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WO2007007589A1 - Field effect transistor and method for manufacturing same - Google Patents

Field effect transistor and method for manufacturing same Download PDF

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Publication number
WO2007007589A1
WO2007007589A1 PCT/JP2006/313296 JP2006313296W WO2007007589A1 WO 2007007589 A1 WO2007007589 A1 WO 2007007589A1 JP 2006313296 W JP2006313296 W JP 2006313296W WO 2007007589 A1 WO2007007589 A1 WO 2007007589A1
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Prior art keywords
effect transistor
nitride semiconductor
semiconductor layer
field effect
layer structure
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PCT/JP2006/313296
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French (fr)
Japanese (ja)
Inventor
Yasuhiro Murase
Hironobu Miyamoto
Kazuki Ota
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NEC Corp
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NEC Corp
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Priority to JP2007524583A priority Critical patent/JPWO2007007589A1/en
Publication of WO2007007589A1 publication Critical patent/WO2007007589A1/en
Anticipated expiration legal-status Critical
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    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D30/00Field-effect transistors [FET]
    • H10D30/40FETs having zero-dimensional [0D], one-dimensional [1D] or two-dimensional [2D] charge carrier gas channels
    • H10D30/47FETs having zero-dimensional [0D], one-dimensional [1D] or two-dimensional [2D] charge carrier gas channels having 2D charge carrier gas channels, e.g. nanoribbon FETs or high electron mobility transistors [HEMT]
    • H10D30/471High electron mobility transistors [HEMT] or high hole mobility transistors [HHMT]
    • H10D30/475High electron mobility transistors [HEMT] or high hole mobility transistors [HHMT] having wider bandgap layer formed on top of lower bandgap active layer, e.g. undoped barrier HEMTs such as i-AlGaN/GaN HEMTs
    • H10D30/4755High electron mobility transistors [HEMT] or high hole mobility transistors [HHMT] having wider bandgap layer formed on top of lower bandgap active layer, e.g. undoped barrier HEMTs such as i-AlGaN/GaN HEMTs having wide bandgap charge-carrier supplying layers, e.g. modulation doped HEMTs such as n-AlGaAs/GaAs HEMTs
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D30/00Field-effect transistors [FET]
    • H10D30/01Manufacture or treatment
    • H10D30/015Manufacture or treatment of FETs having heterojunction interface channels or heterojunction gate electrodes, e.g. HEMT
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D62/00Semiconductor bodies, or regions thereof, of devices having potential barriers
    • H10D62/80Semiconductor bodies, or regions thereof, of devices having potential barriers characterised by the materials
    • H10D62/85Semiconductor bodies, or regions thereof, of devices having potential barriers characterised by the materials being Group III-V materials, e.g. GaAs
    • H10D62/8503Nitride Group III-V materials, e.g. AlN or GaN

Definitions

  • the present invention relates to a field effect transistor using a group m nitride semiconductor and a method of manufacturing the same.
  • GaN and other group III nitride semiconductors have a large band gap, a high breakdown electric field, and a large saturation drift velocity of electrons compared to GaAs semiconductors. Therefore, high-temperature operation, high-speed switching operation, and high-power operation It is expected to be a material that realizes excellent electronic devices in terms of
  • group III nitride semiconductors have piezoelectricity, they can utilize high-concentration two-dimensional carrier gas generated at the heterojunction due to spontaneous polarization and piezoelectric polarization force due to the heterojunction structure. It has the feature that it can operate by a mechanism different from that of a GaAs-based semiconductor field effect transistor driven by carriers generated by doping.
  • FIG. 28 is a cross-sectional view showing a configuration of a conventional hetero-junction field effect transistor (hereinafter referred to as HJFET).
  • HJFET hetero-junction field effect transistor
  • a buffer layer 211 made of A1N, a GaN channel layer 212 and an AlGaN electron supply layer 213 are stacked in this order on a sapphire substrate 209.
  • a source electrode 201 and a drain electrode 203 are formed, and these electrodes are in ohmic contact with the AlGaN electron supply layer 213.
  • a gate electrode 202 is formed between the source electrode 201 and the drain electrode 203, and the gate electrode 202 is in Schottky contact with the AlGaN electron supply layer 213.
  • a SiN film 221 is formed as a surface protective film.
  • a method for manufacturing HJFET 200 will be described.
  • a semiconductor is grown by, for example, a molecular beam epitaxy (MBE) growth method or a metal organic vapor phase epitaxy (MOVPE) growth method.
  • MBE molecular beam epitaxy
  • MOVPE metal organic vapor phase epitaxy
  • a part of the epitaxial layer structure is etched away until the GaN channel layer 212 is exposed, thereby forming an element isolation mesa (not shown). Then, after forming a photoresist in a predetermined region of the AlGaN electron supply layer 213, a metal such as TiZAl is deposited on the AlGaN electron supply layer 213, and a source electrode 201 and a drain electrode are formed using a lift-off method or the like. 203 is formed. And by annealing it at 650 ° C, An ohmic junction is formed between these electrodes and the AlGaN electron supply layer 213.
  • Non-Patent Document 1 UK Mishra, P.
  • Non-Patent Document 2 International 'Electron' Device 'Meeting' Digest (IEDM01—381-384), Ando (Y. Ando)
  • the inventors of the present invention have studied the HJFET obtained by the above-described manufacturing method, and even when a surface protective film is provided, the characteristics of the obtained transistor may vary, or sufficient drainage may occur. It became clear that the current could not be obtained.
  • the present inventor has inferred such a cause as follows.
  • the current collapse has a trade-off relationship with the gate breakdown voltage.
  • the negative polarization charge generated on the AlGaN surface has a great influence on the transistor characteristics depending on the electrical properties of the protective film (passivation film) deposited on the AlGaN surface.
  • the protective film passivation film
  • the negative charge amount on the surface is small, the gate breakdown voltage is low, but the current collab is small.
  • the variation in transistor characteristics that still occurs even when the SiN film 221 is provided includes, for example, a variation in efficiency during the operation of the transistor.
  • the variation in the gate leakage current of the HJFET 200 is caused by the variation in the Schottky characteristics of the gate electrode 202 as the cause of the variation in efficiency during the operation of the transistor.
  • impurities introduced into the interface between the AlGaN electron supply layer 213 and the SiN film 221 also affected the Schottky characteristics. It was found. This point will be described below.
  • the surface of the AlGaN electron supply layer 213 is exposed. For this reason, a photoresist is formed on the surface of the AlGaN electron supply layer 213 in the manufacturing process. Also, when removing the resist, it is exposed several times to plasma damage due to plasma ashing. In addition, high-temperature annealing during ohmic electrode formation is performed with the surface of the AlGaN electron supply layer 213 exposed.
  • the concentration of impurities such as oxygen at the interface between the surface of the group III nitride semiconductor layer 213 of the HJFET 200 and the gate electrode 202 obtained through such a manufacturing process is determined by SIMS (secondary ion mass spectrometry). When measured, it was about lE18atomsZcm 3 to lE19atomsZcm 3 .
  • the impurity concentration increases as described above because the surface force of the AlGaN electron supply layer 213 is more damaged by plasma damage during the electrode formation process described above or by exposure to the atmosphere after high-temperature annealing. This is thought to be easy to be done.
  • the surface state of the AlGaN electron supply layer is easily affected by the process. For this reason, the surface of the AlGaN electron supply layer 213 is in a state different from the initial clean state due to a change in crystallinity of the semiconductor. Examples of such states are:
  • FIG. 25 (a) and FIG. 25 (b) are graphs comparing the characteristics of the HJFET 200 (FIG. 28) obtained by the conventional manufacturing method and the HJFET 100 (FIG. 1) of an example described later.
  • Schottky barrier height ⁇ (eV) Fig. 25 (a)
  • idealization factor in HJFET obtained with 10 3-inch wafers.
  • the idealization factor n is an index that indicates the degree of deviation of the Schottky barrier height ⁇ force when an ideal Schottky junction is used.
  • the n value should be close to 1 and the crystal state should be made uniform, that is, the crystallinity of the semiconductor surface forming the gate electrode. It is important to control this.
  • the present inventor has proceeded to study such viewpoint power, and by providing a surface protective film on the group III nitride semiconductor transistor and improving the cleanliness of the semiconductor surface, the current collab is reduced and the Schottky characteristic is excellent. It was found that a transistor can be realized. Main departure Akira was made based on these new findings.
  • a gate electrode disposed between the source electrode and the drain electrode
  • an insulating film is provided on the group III nitride semiconductor layer structure,
  • an impurity concentration in the group VIII nitride semiconductor layer structure at the interface between the insulating film and the group VIII nitride semiconductor layer structure is lE17 atoms Zcm 3 or less.
  • an insulating film provided on a group III nitride semiconductor layer structure having a heterointerface in a region between the gate electrode and the drain electrode, and a group II group nitride semiconductor layer The impurity concentration at the interface with the structure is lE17atom S Zcm 3 or less. For this reason, in the transistor of the present invention, formation of interface states due to impurities in the group III nitride semiconductor layer structure is suppressed, and current collab is effectively suppressed. In addition, the transistor of the present invention has excellent Schottky characteristics.
  • the crystallinity of the group III nitride semiconductor layer structure is improved as the reason why the Schottky characteristics are excellent by setting the impurity concentration at the interface to 1 E17 atoms / cm 3 or less.
  • the transistor of the present invention is excellent in operational stability and can be manufactured stably with a high yield.
  • the impurity concentration can be measured, for example, by SIMS (secondary ion mass spectrometry).
  • the insulating film can be, for example, an insulating film containing nitrogen, preferably a SiN film having a nitrogen force with silicon.
  • a method for producing the field effect transistor comprising:
  • Forming a group III nitride semiconductor layer structure including a heterojunction in a deposition chamber Forming the insulating film on the group m nitride semiconductor layer structure; selectively removing a predetermined region of the insulating film by etching to form an opening; and forming the opening on the group m nitride semiconductor layer structure And forming the gate electrode so as to fill the opening,
  • a method of manufacturing a field effect transistor is provided.
  • the present invention it is possible to suppress current collapse due to oxidation of the m-group nitride semiconductor layer.
  • a field effect transistor with excellent uniformity of the Schottky interface can be stably manufactured.
  • the crystal state of the surface of the group m nitride semiconductor layer in the region between the gate electrode and the drain electrode can be improved.
  • the uniformity of the crystalline state can be improved.
  • a step of forming the insulating film without taking out the film forming chamber force after the step of forming the group m nitride semiconductor layer structure is performed.
  • a manufacturing method is provided.
  • a method of manufacturing a field effect transistor is provided.
  • the insulating film is formed in a state where the surface of the group m nitride semiconductor layer structure is clean.
  • the insulating film is usually formed after the electrode is formed.
  • the interface order was formed by impurities on the surface of the physical semiconductor layer structure.
  • a field effect transistor having a clean interface can be obtained by devising a process for forming an insulating film on the m-group nitride semiconductor layer structure. . For this reason, the current collaborative effect caused by the oxidation of the interface is suppressed, and a field effect transistor having excellent Schottky characteristics can be stably manufactured.
  • a predetermined region of the insulating film is selectively removed by etching to be removed on the group III nitride semiconductor layer structure.
  • the source electrode and the drain electrode may be formed so as to be embedded in the region.
  • either the step of forming the source electrode and the drain electrode or the step of forming the gate electrode may be performed first.
  • FIG. 1 is a cross-sectional view showing a configuration of a field effect transistor according to an example.
  • FIG. 2 is a cross-sectional view showing a configuration of a field effect transistor according to an example.
  • FIG. 3 is a cross-sectional view showing a configuration of a field effect transistor according to an example.
  • FIG. 4 is a cross-sectional view showing a configuration of a field effect transistor according to an example.
  • FIG. 5 is a cross-sectional view showing a configuration of a field effect transistor according to an example.
  • FIG. 6 is a cross-sectional view showing a configuration of a field effect transistor according to an example.
  • FIG. 7 is a cross-sectional view showing a manufacturing process of the field effect transistor of FIG.
  • FIG. 8 is a cross-sectional view showing a manufacturing process of the field effect transistor of FIG.
  • FIG. 9 is a cross-sectional view showing a manufacturing process of the field effect transistor of FIG.
  • FIG. 10 A sectional view showing a manufacturing process of the field effect transistor of FIG.
  • FIG. 11 A sectional view showing a manufacturing process of the field effect transistor of FIG.
  • FIG. 13 A sectional view showing a manufacturing process of the field effect transistor of FIG.
  • FIG. 16 A sectional view showing a manufacturing process of the field effect transistor of FIG.
  • FIG. 17 A sectional view showing a manufacturing process of the field effect transistor of FIG.
  • FIG. 18 A sectional view showing a manufacturing process of the field effect transistor of FIG.
  • FIG. 19 A sectional view showing a manufacturing process of the field effect transistor of FIG.
  • FIG. 20 is a cross-sectional view showing a manufacturing step of the field effect transistor of FIG. 4.
  • FIG. 20 is a cross-sectional view showing a manufacturing step of the field effect transistor of FIG. 4.
  • FIG. 21 is a cross-sectional view showing a manufacturing process of the field effect transistor of FIG.
  • FIG. 22 A sectional view showing a manufacturing process of the field effect transistor of FIG.
  • FIG. 23 A sectional view showing a manufacturing process of the field effect transistor of FIG.
  • FIG. 24 A sectional view showing a manufacturing process of the field effect transistor of FIG.
  • FIG. 25 is a diagram comparing the method of manufacturing an example and a conventional field effect transistor.
  • FIG. 26 is a diagram for comparing the method of manufacturing an example and a conventional field effect transistor.
  • FIG. 27 is a cross-sectional view showing a configuration of a field effect transistor according to an example.
  • FIG. 28 is a cross-sectional view showing a configuration of a conventional field effect transistor.
  • an embodiment of the present invention will be described by taking an HJFET having an AlGaN electron supply layer, a ZGaN channel layer, and a surface protective film (hereinafter also simply referred to as “protective film”) as an example of a group III nitride semiconductor structure.
  • protective film a surface protective film
  • the laminated structure is expressed as “upper layer Z lower layer (substrate side) J”.
  • FIG. 1 is a diagram showing a basic configuration of the field effect transistor of the present embodiment.
  • This field effect transistor HJFET100
  • This field effect transistor is separated from the group III nitride semiconductor layer structure (GaN channel layer 112, AlGaN electron supply layer 113) including the heterojunction, and these group III nitride semiconductor layer structures.
  • the source electrode 101 and the drain electrode 103 formed, and the gate electrode 102 disposed between the source electrode 101 and the drain electrode 103 are provided. Since the HJFET 100 has a heterojunction structure, it is possible to use a high-concentration two-dimensional carrier gas generated at the heterojunction with spontaneous polarization and piezoelectric polarization force.
  • the group III nitride semiconductor layer structure includes a channel layer made of InGaN (0 ⁇ x ⁇ 1) and an electron supply layer made of AlGaN (0 ⁇ y ⁇ 1), and includes a heterointerface. Is the interface between InGaN and AlGaN. However, in the above formula, l -y so that X and y do not become zero at the same time.
  • the HJFET 100 has an insulating film (SiN film 121) as a protective film on the laminated structure of the GaN channel layer 112 and the AlGaN electron supply layer 113 in the region between the gate electrode 102 and the drain electrode 103.
  • SiN film 121 insulating film
  • the protective film also has an insulating material strength.
  • the SiN film 121 may be provided on the entire surface of the region between the gate electrode 102 and the drain electrode 103 or may be provided on a part of the region.
  • the SiN film 121 is an insulating film containing nitrogen as at least one of the elements constituting the laminated structure of the GaN channel layer 112 and the AlGaN electron supply layer 113.
  • Elements in protective film May move to the interface between the AlGaN electron supply layer 113 and the protective film, there is a concern that a level is formed as an impurity at the interface, but nitrogen in the SiN film 121 is common to N constituting the AlGaN electron supply layer 113 Therefore, it does not become an impurity with respect to the AlGaN electron supply layer 113, and an interface state can be prevented from being formed. For this reason, generation
  • the SiN film 121 as the protective film it is possible to use the same material as the AlGaN electron supply layer 113.
  • the SiN film 121 is a film including a region grown epitaxially on the laminated structure of the GaN channel layer 112 and the AlGaN electron supply layer 113.
  • the group III nitride semiconductor layer structure and the SiN film 121 can be manufactured in a continuous process. Further, the stability of the film quality of the obtained SiN film 121 can be improved.
  • the SiN film 121 is a film that substantially does not contain oxygen as a constituent element. Since oxygen tends to form a level in a group III nitride semiconductor, the generation of current collabs can be more reliably suppressed by employing a structure that does not substantially contain oxygen. Note that “substantially free of oxygen” means that no oxygen is intentionally contained in the film, as long as current Collabs generation due to the formation of impurity levels of oxygen can be suppressed. Unintentionally included oxygen may be present. Moreover, it is preferable that the oxygen concentration is below the detection limit in SIMS.
  • the thickness of the SiN film 121 is, for example, not less than 5 nm and not more than 200 nm, more specifically not less than 5 nm and not more than lOOnm. By setting the thickness to 5 nm or more, current collapse at the interface can be more reliably suppressed.
  • the thickness of the SiN film 121 is, for example, 200 nm or less, preferably 150 nm or less, more preferably lOOnm or less. By doing this, current collaboratives can be suppressed and the gate breakdown voltage can be improved, and the trade-off problem between the two can be solved more effectively.
  • the SiN film 121 is a film grown on the surface of the clean AlGaN electron supply layer 113.
  • the impurity concentration is the total concentration of carbon and oxygen contained in the interface.
  • the impurity concentration can be measured, for example, by SIMS (secondary ion mass spectrometry).
  • the SiN film 121 is used as a surface protective film that effectively suppresses the generation of current collabs, and the SiN film 121 is formed while the surface of the AlGaN electron supply layer 113 is clean. HJFET100 having the above impurity concentration can be obtained.
  • a method of forming the SiN film 121 while the surface of the AlGaN electron supply layer 113 is clean for example,
  • an HJFET having an impurity concentration of lE15 atoms Zcm 3 or less at the interface between the surface of the A1GaN electron supply layer 113 and the SiN film 121 and the gate electrode 102 was obtained by the method (i).
  • an HJFET having an impurity concentration of lE17 atoms Zcm 3 or less at the interface between the surface of the AlGaN electron supply layer 113 and the SiN film 121 and the gate electrode 102 was obtained. Note that these methods will be described in more detail in Examples described later.
  • the SiN film 121 is formed after the AlGaN electron supply layer 113 is formed and before the electrode is formed, the source electrode 101 and the drain electrode 103 run on the SiN film 121. It has a structure. As a result, the concentration of the electric field at the gate electrode side end of the drain electrode 103 during high-voltage operation is alleviated, and the gate breakdown voltage is improved.
  • the HJ FET 100 is formed on a substrate 110 such as SiC.
  • a buffer layer 111 having a semiconductor layer force is formed on the substrate 110.
  • a GaN channel layer 112 is formed on the buffer layer 111.
  • an eight-and-one electron supply layer 113 is formed on the AlGaN electron supply layer 113.
  • the source electrode 101 and the drain electrode 103 are in ohmic contact, and the surface of the AlGaN electron supply layer 113 is covered with the SiN film 121.
  • FIGS. 7 to 9 are diagrams showing a method for manufacturing the HJFET 100 of this example.
  • This manufacturing method includes the following steps.
  • Step 101 A process of forming a III-nitride semiconductor layer structure including a heterojunction (laminated structure of AlGaN electron supply layer 113 and GaN channel layer 112), specifically, an epitaxial growth method on the substrate 110 Sequentially forming a GaN channel layer 112 and an AlGaN electron supply layer 113 by
  • Step 103 forming a protective film (SiN film 121) while the surface of the AlGaN electron supply layer 113 is clean,
  • Step 105 A predetermined region of the SiN film 121 is selectively removed by etching to form an opening, and the gate is embedded on the stacked structure of the AlGaN electron supply layer 113 and the GaN channel layer 112. Forming electrode 102; and
  • Step 107 After the step of forming the SiN film 121, a predetermined region of the SiN film 121 is selectively removed by etching, and the source electrode 101 and the AlGaN electron supply layer 113 are embedded so as to embed the removed region. Forming the drain electrode 103 apart from each other;
  • Step 105 the force gate illustrated in the case of the procedure of forming the source electrode 101 and the drain electrode 103 in Step 107 after forming the gate electrode 102 in Step 105.
  • the SiN film 121 is formed before the formation of the first electrode 102, the source electrode 101, and the drain electrode 103, either Step 105 or Step 107 may be performed first. For example, it is possible to decide which step force to perform in consideration of the type of metal used for each electrode.
  • the SiN film 121 in step 103 is formed at least between the formation region of the gate electrode 102 and the formation region of the drain electrode 103.
  • the step of subsequently forming the SiN film 121 in a clean atmosphere that is not taken out from the film forming chamber. 103 processes are performed.
  • the clean atmosphere is an atmosphere substantially free of oxygen.
  • eight &? ⁇ Do be exposed to the atmosphere the surface of the electron supply layer 113 is on the way, so further effectively an impurity concentration at the interface between the AlGaN electron supply layer 113 and the SiN film 1 21
  • the current collab can be more effectively suppressed.
  • the film formation chamber is composed of a single chamber! Or may include a plurality of small chambers.
  • the substrate 110 is transferred to another chamber without exposure to the atmosphere by releasing the vacuum, and the SiN film 121 is formed. You may go. Do not expose to the atmosphere by releasing the vacuum! Therefore, surface contamination of the AlGaN electron supply layer 113 can be effectively suppressed.
  • a semiconductor layer is grown on a substrate 110 having SiC force by using an epitaxial growth method, and the buffer layer 111 (thickness of the substrate 110 side force and also undoped A1N force is sequentially formed. 20 nm), an undoped GaN channel layer 112 (thickness 2 ⁇ m), and an AlGaN electron supply layer 113 (thickness 25 nm) with undoped Al GaN force are obtained (FIG. 7 (a)).
  • the epitaxy growth method for example, a molecular beam epitaxy (MBE) growth method or a metal organic vapor phase epitaxy (MOVPE) growth method is used.
  • a SiN film 121 (film thickness 60 nm) is formed on the AlGaN electron supply layer 113 (FIG. 7B). At this time, after the AlGaN electron supply layer 113 is formed, it is not exposed to the atmosphere in the same film forming apparatus. A SiN film 121 is formed.
  • the SiN film 121 is formed by the same growth method as the growth method of the AlGaN electron supply layer 113 and the GaN channel layer 112.
  • a part of the SiN film 121 is etched away until the GaN channel layer 112 is exposed, thereby forming an element isolation mesa (not shown). Then, a photoresist is formed in a predetermined region on the surface of the SiN film 121, and the exposed portion of the SiN film 121 is selectively etched away to expose the AlGaN electron supply layer 113 (FIG. 8 (c)).
  • a source electrode 101 and a drain electrode 103 are formed on the AlGaN electron supply layer 113 by evaporating a metal such as TiZAl (FIG. 8 (d)), and annealing is performed at 650 ° C.
  • a metal such as TiZAl (FIG. 8 (d)
  • a photoresist is formed in a predetermined region on the surface of the SiN film 121, and the exposed portion of the SiN film 121 is selectively removed by etching to provide an exposed portion of the AlGaN electron supply layer 113 (FIG. 9 (e)).
  • a gate metal of, for example, NiZAu is deposited to form a Schottky contact gate electrode 102 (FIG. 9 (f)).
  • FIG. 25 and FIG. 26 are diagrams for comparing the manufacturing method of this example with the conventional manufacturing method.
  • FIG. 25 (a) and FIG. 25 (b) show 10 3 inches each in the manufacturing method of the HJFET 100 of this embodiment and the manufacturing method of the conventional HJFET 200 (FIG. 28). Shows Schottky barrier height ⁇ and idealization factor n in HJFET obtained in woofer
  • FIG. 1 A first figure.
  • FIG. 26 is a diagram showing the amount of current collabs when a device is prototyped on each of 10 3-inch wafers in the manufacturing method of this example and the conventional manufacturing method.
  • the surface of the AlGaN electron supply layer 213 provided between the gate electrode 202 and the drain electrode 203 undergoes various processes. It is difficult to control the negative charge induced on the surface, and even if a current film is suppressed by forming a protective film by the SiN film 221, there is a variation in the degree of current current reduction.
  • the SiN film 121 is continuously grown without being exposed to the atmosphere or plasma. Therefore, the SiN film 121 is formed before the gate electrode 102 is formed, and the interface between the semiconductor and the SiN film 121 is formed with a uniform and high-quality interface that is not damaged by the process. From the above, the influence of negative surface charge becomes a big problem, especially as in the present invention! / In the Group III nitride semiconductor device, the current interface is reduced due to this uniform interface formation and low interface impurity concentration. And the effect of improving the uniformity of characteristics is remarkable.
  • the oxygen concentration in the AlGaN electron supply layer at the interface between the SiN film and the AlGaN electron supply layer was analyzed, in the case of the HJFET 100 of this example, it was 1E15 atoms / cm 3 or less. It was.
  • the thickness of the SiN film 121 was about 5 to 200 nm, the AlGaN electron supply layer 113 and the SiN film 121 having such an impurity concentration at the interface could be formed.
  • the SiN film 121 and the AlGaN electron supply layer 113 are formed.
  • the oxygen concentration in the AlGaN electron supply layer 113 at the interface was about lE19 atoms Zcm 3 .
  • the HJFET 100 of this example As described above, in the HJFET 100 of this example, after the AlGaN electron supply layer 113 is formed, the SiN film 121 is formed in the same film formation chamber without being exposed to the atmosphere. Therefore, the HJFET 100 has excellent Schottky properties. In addition, current collabs are suppressed, high output and high reliability Have a configuration. In addition, since the variation between wafers is suppressed, the HJFET 100 has a structure capable of stably manufacturing a structure as designed with a high yield.
  • the SiN film 121 functioning as a protective film contains nitrogen, which is a constituent element of the AlGaN electron supply layer 113, which is a group III nitride semiconductor layer, after the formation of the AlGaN electron supply layer 113, The SiN film 121 can be formed in a continuous process without exposure to the atmosphere. Further, the stability of the film quality of the obtained SiN film 121 can be improved.
  • the source electrode 101 and the gate electrode 102 have a structure that rides on the SiN film 121 that is a protective film, so that the drain electrode 103 is not damaged during high-voltage operation. Electric field concentration at the gate electrode side end can be alleviated. Therefore, the gate breakdown voltage is improved! /.
  • FIG. 2 is a cross-sectional view showing the configuration of the HJFET of this example.
  • the basic configuration of the HJFET 130 shown in FIG. 2 is the same as the HJFET 100 (FIG. 1) of the first embodiment.
  • the buffer layer 111, the GaN channel layer 112, the AlGaN electron supply layer 113, and the SiN film 121 are on the substrate 110 side.
  • the structure is such that the source electrode 101, the drain electrode 103, and the gate electrode 102 are provided on the AlGaN electron supply layer 113, and the cleanliness of the interface between the AlGaN electron supply layer 113 and the SiN film 121 is increased.
  • the method of maintaining is different from Example 1.
  • Such an HJFET 130 is manufactured by the following procedure.
  • Example 10 to 13 are diagrams showing a method for manufacturing the HJFET in this example.
  • the SiN film was formed without being exposed to the contaminated atmosphere (for example, air).
  • the manufacturing method of this example is based on the group III nitride semiconductor. This is a case where the group III nitride semiconductor layer structure is exposed to a contaminated atmosphere after the step of forming the layer structure.
  • step 109 wet etching using an acid, Surface of III-nitride semiconductor layer structure Cleaning process,
  • molecular beam epitaxy (Molecular Beam) is formed on a substrate 110 made of SiC.
  • Semiconductors are grown by epitaxy (MBE) growth method or metal organic vapor phase epitaxy (MOVPE) growth method.
  • MBE epitaxy
  • MOVPE metal organic vapor phase epitaxy
  • the AlGaN electron supply layer 113 Even if the AlGaN electron supply layer 113 was exposed to the atmosphere or the like by the cleaning process in Fig. 10 (b), the surface was cleaned, and in the completed HJFET 130, the AlGaN electron supply layer 113
  • the impurity concentration at the interface between the SiN film 121 and the SiN film 121 can be set to lE17 atoms Zcm 3 or less.
  • an element isolation mesa (not shown) is formed by etching away a part of the SiN film 121 and a part of the epitaxial layer structure until the GaN channel layer 112 is exposed. Then, a photoresist is formed in a predetermined region on the surface of the SiN film 121, and the exposed portion of the SiN film 121 is selectively etched away to expose the AlGaN electron supply layer 113 (FIG. 11 (d)). A source electrode 101 and a drain electrode 103 are formed on the electron supply layer 113 by evaporating a metal such as TiZAl (FIG. 12E). Then, annealing is performed at 650 ° C.
  • a photoresist is formed in a predetermined region on the surface of the SiN film 12 1, and the exposed portion of the SiN film 121 is selectively etched away to provide an opening to expose the AlGaN electron supply layer 113 (FIG. 12 (f)) .
  • a gate metal such as NiZAu is deposited to form a Schottky contact gate electrode 102 (FIG. 13).
  • the HJFET13 shown in Fig. 2 0 is obtained.
  • the semiconductor surface is cleaned by etching with an acid or the like (FIG. 10B). In addition, it can also be terminated so as to suppress subsequent oxidation of the surface by the cleaning treatment with acid. Even if the AlGaN electron supply layer 113 is slightly contaminated after the surface of the AlGaN electron supply layer 113 is etched with acid or the like and before the SiN film 121 is formed, the SiN film is formed by plasma CVD. When the film 121 is formed, contaminants can be removed by plasma irradiation.
  • the SiN film 121 is formed on the surface of the AlGaN electron supply layer 113, the influence of the negative surface charge is a serious problem. Current collab in the child is suppressed.
  • the portion of the AlGaN electron supply layer 113 that was exposed to the atmosphere before the formation of the gate electrode 102 and was contaminated with the atmosphere was removed by etching.
  • the SiN film 121 is formed on the AlGaN electron supply layer 113 when the gate electrode 102 and the drain electrode 103 are formed, the surface of the AlGaN electron supply layer 113 is exposed to plasma at the time of electrode formation. There is nothing to do. Therefore, in the subsequent manufacturing process, a photoresist is formed on the AlGaN electron supply layer 113, and the gate electrode 102 having a nearly ideal Schottky property is obtained without the AlGaN electron supply layer 113 being attacked by plasma.
  • the crystal state of the surface of the AlGaN electron supply layer 113 in the region between the gate electrode 102 and the drain electrode 103 is good and uniform, and the surface state can be stabilized. It is. For this reason, it is possible to obtain a configuration that has excellent Schottky properties and can be stably manufactured at a high yield.
  • the source electrode 101 and the gate electrode 102 are structured on the SiN film 121, so that the drain electrode can be used during high-voltage operation. This makes it possible to produce a device with improved gate breakdown voltage due to relaxation of the electric field concentration at the end of the gate electrode.
  • FIG. 3 is a diagram showing a cross-sectional structure of the HJFET of this example.
  • the basic configuration of the HJFET 132 shown in FIG. 3 is the same as that of the HJFET of Example 1 or Example 2, but a protective film is stacked on the first insulating film (SiN film 121) and the SiN film 121. It differs from the second insulating film (SiO film 122) in that the force is configured.
  • SiO film 122 is Si
  • another insulating film may be provided as an intervening layer between the first insulating film and the second insulating film.
  • the HJFET 132 is formed on a substrate 110 such as SiC.
  • a buffer layer 111 made of a semiconductor layer is formed on the substrate 110.
  • a GaN channel layer 112 is formed on the buffer layer 111.
  • an AlGaN electron supply layer 113 is formed on the GaN channel layer 112, an AlGaN electron supply layer 113 is formed.
  • a source electrode 101 and a drain electrode 103 are ohmic-bonded on the AlGaN electron supply layer 113, and the surface of the AlGaN electron supply layer 113 is covered with a SiN film 121. Covered with 122.
  • FIG. 14 to 17 are diagrams showing a method for manufacturing the HJFET shown in FIG.
  • a semiconductor is grown on the substrate 110 having SiC force by, for example, MBE growth method, metal organic vapor phase epitaxy MOVPE growth method, or the like.
  • the buffer layer 111 thinness 20 nm
  • the undoped GaN channel layer 112 thinness 2 ⁇ m
  • the AlGaN electron supply layer 113 made of undoped AlGaN ( A semiconductor layer structure with a thickness of 25 nm) is obtained (Fig. 14 (a)).
  • a SiN film 121 (60 nm) is subsequently formed on the AlGaN electron supply layer 113 by plasma CVD or the like without exposure to the atmosphere (FIG. 14 (b)).
  • etching is performed with an acid or the like to clean the surface of the semiconductor layer, and the SiN film 121 is formed as in the second embodiment.
  • a SiO film 122 (100 nm) is formed on the SiN film 121 by an atmospheric pressure CVD method or the like (see FIG.
  • An element isolation mesa (not shown) is formed by etching until the N channel layer 112 is exposed. Then, a photoresist is formed in a predetermined region on the surface of the SiO film 122,
  • the predetermined regions of the SiN film 121 and the SiO film 122 are exposed until the AlGaN electron supply layer 113 is exposed. Then, the source electrode 101 and the drain electrode 103 are formed on the AlGaN electron supply layer 113 by evaporating, for example, Ti ZA1 metal (FIG. 16 (e)). An ohmic bond is formed by annealing at 650 ° C.
  • a photoresist is formed in a predetermined region on the surface of the SiO film 122, and the SiN film 121 is formed.
  • FIG. 16 (f) An exposed opening of the electron supply layer 113 is provided (FIG. 16 (f)).
  • a NiZAu gate metal is deposited to form a Schottky-junction gate electrode 102 (FIG. 17).
  • the HJFET 132 shown in FIG. 3 is obtained.
  • the SiN film 121 formed on the surface of the group III nitride semiconductor layer is covered with the SiO 2 film 122, the deterioration with time of the SiN film 121 is further reliably suppressed.
  • the SiO film 122 may be formed using the same film forming apparatus as the SiN film 121, or may be different.
  • the film forming apparatus may be used.
  • the planar shape of the SiO film 122 is the same as that of the SiN film 121.
  • a field plate portion 105 may be formed in a region between the gate electrode 102 and the drain electrode 103 via a SiN film 121 above the AlGaN electron supply layer 113. This configuration will be described later in Example 4 and Example 5.
  • FIG. 4 is a cross-sectional view showing the configuration of the HJFET of this example.
  • the basic configuration of the HJFET 134 shown in FIG. 4 is the same as that of the HJFET 100 of Example 1, except that the gate electrode 102 protrudes in a bowl shape on the drain electrode 103 side and is formed on the SiN film 121. Is different from HJFET100.
  • the HJFET 134 is formed on a substrate 110 such as SiC.
  • a buffer layer 111 made of a semiconductor layer is formed on the substrate 110.
  • a GaN channel layer 112 Is formed on the substrate 110.
  • an eight-and-a-half electron supply layer 113 is formed on the GaN channel layer 112, an eight-and-a-half electron supply layer 113 is formed.
  • the source electrode 101 and the drain electrode 103 are joined in ohmic contact.
  • a gate electrode 102 is provided between these electrodes.
  • the gate electrode 102 has a field plate portion 105 and is joined to the eight &? ⁇ Electron supply layer 113 in a Siykey key junction.
  • the surface of the AlGaN electron supply layer 113 is covered with the SiN film 121.
  • the length of the field plate portion 105 in the gate length direction is, for example, 0.3 ⁇ m or more, preferably 0. 0 or more. In this way, current collab can be more reliably suppressed.
  • the field plate portion 105 is configured so as not to overlap the drain electrode 103, and preferably the length of the field plate portion 105 in the gate length direction is 70% or less of the distance between the gate electrode and the drain electrode. The greater the length of the extension of the field plate portion 105, the greater the effect of suppressing current collabs. The withstand voltage decreases. Note that the distance between the gate electrode 102 and the drain electrode 103 refers to the length from the drain electrode side end of the gate electrode 102 to the gate electrode side end of the drain electrode 103.
  • FIG. 18 to 20 are views showing a method for manufacturing the HJFET of FIG.
  • a semiconductor is grown on a substrate 110 made of SiC by, for example, MBE growth method or MOCVD growth method.
  • the buffer 110 side force in the order of the substrate 110 is also an undoped A1N buffer layer 111 (film thickness 20 nm), an undoped GaN channel layer 112 (film thickness 2 ⁇ m), and an undoped AlGaN force AlGaN electron supply layer 113 (film thickness)
  • a semiconductor layer structure in which 25 nm) is stacked is obtained (Fig. 18 (a)).
  • a SiN film 121 (60 nm) is subsequently formed on the AlGaN electron supply layer 113 by plasma CVD or the like without exposure to the atmosphere (FIG. 18B).
  • etching is performed with an acid or the like to clean the surface of the semiconductor layer, and the SiN film 121 is formed as in the second embodiment.
  • part of the SiN film 121 and part of the epitaxial layer structure are etched away until the GaN channel layer 112 is exposed, thereby forming an element isolation mesa (not shown).
  • a photoresist is formed in a predetermined region of the SiN film 121, and the exposed portion of the SiN film 121 is removed. Etching is selectively removed until the AlGaN electron supply layer 113 is exposed (FIG. 19 (c)).
  • a metal such as TiZAl is deposited on the exposed AlGaN electron supply layer 113 to form the source electrode 101 and the drain electrode 103 (Fig. 19 (d)), and annealing is performed at 650 ° C.
  • the electrode and the AlGaN electron supply layer 113 are joined in ohmic contact.
  • a photoresist is formed in a predetermined region of the SiN film 121, and an exposed portion of the SiN film 121 is selectively removed by etching to provide an opening to expose the AlGaN electron supply layer 113 (FIG. 20 (e)).
  • NiZAu is vapor-deposited on the exposed AlGaN electron supply layer 113 as a metal film to be the gate electrode 102 to form the Schottky contact gate electrode 102 (FIG. 20 (f)) 0 or
  • a field plate portion 105 made of NiZAu is formed integrally with the gate electrode 102.
  • the HJFET 134 shown in FIG. 4 is obtained.
  • the gate electrode 102 and the field plate portion 105 are formed at the same time. These may be performed in separate steps. It is also possible to form a resist having an opening at a predetermined position on the SiN film 121 and form the field plate portion 105 so as to fill the opening. In this case, the gap between the gate electrode 102 and the field plate portion 105 can be formed with a narrower gap.
  • the HJFET 134 has a field plate portion 105. Therefore, even when a high reverse voltage is applied between the gate electrode 102 and the drain electrode 103, the electric field force applied to the drain electrode side end of the gate electrode 102 is mitigated by the action of the field plate portion 105. . Therefore, the electric field concentration at the drain electrode side end of the gate electrode 102 can be further reliably suppressed, and the gate breakdown voltage can be improved. Furthermore, since the surface potential can be modulated by the field plate portion 105 during a large signal operation, the response speed of the surface trap can be increased and the current collab can be suppressed. Therefore, according to the present invention, the balance of current collabs, gate breakdown voltage, and gain can be remarkably improved. In addition, even if the surface condition fluctuates due to variations in the manufacturing process, such good performance should be realized stably. Can do.
  • the force electric field control unit described as an example in which the same member member as the gate electrode 102 is configured and the field plate unit 105 functioning as an electric field control unit is provided is the gate electrode In the region between the gate electrode 102 and the drain electrode 103, the electric field is independent of the gate electrode 102 via the SiN film 121 above the group III nitride semiconductor layer structure in the region between the gate electrode 102 and the drain electrode 103.
  • a configuration in which a control electrode is provided may be employed.
  • FIG. 27 is a cross-sectional view showing the configuration of such an HJFET.
  • a gate electrode 102 and an electric field control electrode 106 provided apart from the gate electrode 102 are provided.
  • the electric field control electrode 106 may be formed at the same time as the gate electrode 102 or may be formed in a separate process. In another process, a resist having an opening at a predetermined position is formed on the SiN film 121, and the electric field control electrode 106 can be formed so as to fill the opening. In this case, the gap between the gate electrode 102 and the electric field control electrode 106 can be formed with a narrower gap.
  • the electric field control electrode 106 may apply different potentials to the electric field control electrode 106 and the gate electrode 102, which may be independently controllable to the gate electrode 102. it can. With such a structure, the field effect transistor can be driven under optimum conditions. Since the surface trap response can be suppressed by fixing the surface potential, the electric field control electrode 106 is set to the same potential as the gate electrode 102, and the current collab can be suppressed more effectively than when the surface potential is modulated. . In particular, the effect of being able to control the electric field control electrode 106 independently is remarkable in the group III nitride semiconductor device in which the influence of the negative surface charge is a serious problem.
  • the insulating film may have a laminated structure.
  • FIG. 5 is a cross-sectional view showing the configuration of the HJFET of this example.
  • the HJFET 136 shown in FIG. 5 is formed on a substrate 110 such as SiC.
  • a buffer layer 111 having a semiconductor layer force is formed on the substrate 110.
  • a GaN channel layer 112 force S is formed on the noffer layer 111.
  • an AlGaN electron supply layer 113 is formed on the GaN channel layer 112, an AlGaN electron supply layer 113 is formed.
  • the source electrode 101 and the drain electrode 103 are ohmic-bonded.
  • a gate electrode 102 is provided between these electrodes.
  • the gate electrode 102 has a field plate portion 105 and is in Schottky junction with the AIGaN electron supply layer 113.
  • the surface of the AlGaN electron supply layer 113 is covered with a SiN film 121, and a SiO film 122 is further provided thereon.
  • the field plate portion 105 is provided on the SiO film 122 and the field plate portion 105.
  • the SiN film 121 and the SiO film 122 are provided immediately below.
  • FIG. 21 to 24 are diagrams showing a method for manufacturing the HJFET 136.
  • FIG. 21 to 24 are diagrams showing a method for manufacturing the HJFET 136.
  • a semiconductor is grown on a substrate 110 made of SiC by, for example, MBE growth method or MOVPE growth method.
  • the substrate 110 side force also has an undoped A1N force buffer layer 111 (film thickness 20 nm), an undoped GaN channel layer 112 (film thickness 2 m), and an undoped AlGaN force AlGaN electron supply layer 113 (film)
  • a semiconductor layer structure with a thickness of 25 nm) is obtained (Fig. 21 (a)).
  • an SiN film 121 (60 nm) is formed on the AlGaN electron supply layer 113 without exposing it to the atmosphere by plasma CVD or the like (FIG. 21 (b )).
  • the SiN film 121 is formed after etching with an acid or the like to clean the surface of the semiconductor layer.
  • an SiO film 122 (10011111) is formed on the SiN film 121 by atmospheric pressure CVD or the like (
  • An element isolation mesa (not shown) is formed by etching until the N channel layer 112 is exposed. Then, a photoresist is formed in a predetermined region on the surface of the SiO film 122.
  • AlGaN electron supply layer 113 is exposed in a predetermined region of SiN film 121 and SiO film 122 Until the source electrode 101 and the drain electrode 103 are formed by depositing a metal such as TiZAl on the AlGaN electron supply layer 113 (FIG. 23 (e)). ))) Annealing is performed at 650 ° C., and these electrodes and the AlGaN child supply layer 113 are joined in ohmic contact.
  • a metal such as TiZAl
  • a photoresist is formed in a predetermined region on the surface of the SiO film 122, and the SiN film 121 is formed.
  • NiZAu is vapor-deposited as a metal film to be the gate electrode 102 to form the gate electrode 102 that is Schottky-bonded to the AlGaN electron supply layer 113 ( ( Figure 24).
  • a field plate portion 105 made of NiZAu is also formed. In this way, the HJFET 136 shown in FIG. 5 is obtained.
  • the gate electrode 102 and the field plate portion 105 are formed at the same time.
  • the step of forming may be performed separately).
  • the gap between the gate electrode 102 and the field plate portion 105 can be formed with a narrower gap.
  • the following effects can be obtained. That is, in the HJFET 136, the SiN film 121 and the SiO film 122 are directly under the field plate portion 105.
  • a protective film consisting of a laminated film is provided. Compared to the configuration in which the protective film is only the SiN film 121, the field plate portion 105 can
  • the SiN film 121 is formed thin enough not to change the film quality over time (150 nm or less, more preferably lOOnm or less), and the SiO film 122 is thickly laminated, thereby further suppressing the increase in capacitance. It is possible
  • the gate electrode 102 having the field plate portion 105 may be replaced with the gate electrode 102 and the electric field control electrode 106 provided apart from the gate electrode 102. .
  • the electric field control electrode 106 may be formed simultaneously with the gate electrode 102 or may be formed in a separate process. In a separate process, a resist with an opening at a predetermined position is removed from SiN. The electric field control electrode 106 may be formed on the film 121 so as to fill the opening. In this case, the gap between the gate electrode 102 and the electric field control electrode 106 can be formed with a narrower gap.
  • the SiN film 121 formed on the surface of the group III nitride semiconductor layer is formed of SiO.sub.
  • the lifetime of the element characteristics can be extended.
  • the structure is such that the source electrode 101 and the gate electrode 102 ride on the SiN film 121 and the SiO film 122. For this reason,
  • the electric field concentration at the gate side end of the drain electrode 103 can be relaxed, and the gate breakdown voltage can be improved.
  • the surface protective film has an SiO film 122 as an upper layer.
  • low dielectric constant film having a relative dielectric constant of 4 or less.
  • low dielectric constant materials include SiOC (sometimes called SiOCH), BCB (benzocyclobutene), FSG (Flouro Silicate Glass: SiOF), HS (Hydrogen— 3 ⁇ 4ilisesquioxane ⁇ MS (Methyl— 3 ⁇ 4iisesquioxane) ⁇ machine polymer, or The material which made these porous is illustrated.
  • the protective film more specifically, the insulating film that forms the upper layer of the surface protective film contains C (carbon) as a constituent element, the interface between the AlGaN electron supply layer 113 and the SiN film 121 is formed.
  • C carbon
  • This embodiment is an example of an HJFET that employs a wide recess structure.
  • FIG. 6 is a cross-sectional view showing the configuration of the HJFET of this example.
  • the contact layer composed of an undoped AlGaN layer is provided between the source electrode 101 and the AlGaN electron supply layer 113 and between the drain electrode 103 and the AlGaN electron supply layer 113.
  • 114 intervenes.
  • a contact layer 114 is provided on the AlGaN electron supply layer 113 in the formation region of the source electrode 101 and the drain electrode 103.
  • the contact layer 114 has an opening, and the AlGaN electron supply layer 113 is exposed from the opening.
  • the bottom surface of the opening is a recess surface with respect to the upper surface of the contact layer 114.
  • a source electrode 101 and a drain electrode 103 are provided in contact with the upper surface of the tact layer 114.
  • a gate electrode 102 is provided in contact with the exposed portion of the AlGaN electron supply layer 113.
  • the bottom force of the source electrode 101 and the drain electrode 103 is located above the bottom surface of the gate electrode 102 (on the side away from the substrate 110).
  • the HJFET 138 is formed on a substrate 110 such as SiC.
  • a buffer layer 111 made of a semiconductor layer is formed on the substrate 110.
  • a GaN channel layer 112 is formed on the buffer layer 111.
  • an eight-and-a-half electron supply layer 113 is formed on the GaN channel layer 112, an eight-and-a-half electron supply layer 113 is formed.
  • a contact layer 114 is formed on the AlGaN electron supply layer 113.
  • the source electrode 101 and the drain electrode 103 are ohmic-bonded to the surface of the contact layer 114.
  • the surface of the AlGaN electron supply layer 113 is covered with a SiN film 121! /.
  • the HJFET 138 in FIG. 6 has a configuration in which a contact layer 114 is added to the HJFET 100 (FIG. 1) of the first embodiment. With this configuration, in addition to the effects described in the first embodiment, there is an effect of further reducing the contact resistance.
  • Example 1 As in Example 1, Example 2, and Example 4, the source electrode 101 and the gate electrode 102 are on the SiN film 121, so that the high voltage operation is possible. In this case, the electric field concentration at the gate electrode side end of the drain electrode 103 can be relaxed to improve the gate breakdown voltage.
  • the protective film provided on the AlGaN electron supply layer 113 is a single layer.
  • two insulating films are provided.
  • a layer structure can be formed, or the field plate portion 105 can be formed.
  • the field plate portion 105 has a two-layer structure composed of a SiN film 121 and a SiO film 122 as a protective film.
  • the rate part 105 may be provided on the SiO film 122. In this case as well, the same as in Example 3.
  • the SiO film 122 is preferably an insulating film having a lower dielectric constant than the SiN film 121.
  • the first insulating film is SiN
  • a film containing no nitrogen can be used.
  • the field plate portion 105 may extend to the top of the contact layer 114. By doing so, the electric field concentration at the drain side end of the gate electrode 102 can be more effectively dispersed and relaxed. If a recess structure is used, a multi-stage recess can be used.
  • a gate recess structure in which a part of the drain electrode 103 is embedded in the AlGaN electron supply layer 113 can also be adopted.
  • the force has been described by taking the case where the contact layer 114 is composed of an undoped AlGaN layer as an example.
  • the contact layer 114 may be doped with a predetermined impurity. .
  • a substrate or the like may be used.
  • the SiN film is provided as an insulating protective film containing at least one of the elements constituting the group-III nitride semiconductor layer structure has been described as an example.
  • the material of the insulating film containing at least one of the elements constituting the nitride semiconductor layer structure is not limited to SiN, and other examples include nitrides such as BN. Even when such a film is used, the generation of current collabs can be suppressed.
  • the structure of the semiconductor layer below the gate electrode 102 is not limited to that illustrated, and various modes are possible.
  • a structure in which the AlGaN electron supply layer 113 is also provided in the lower part of the GaN channel layer 112 is also possible.
  • a group II nitride semiconductor layer structure includes a channel layer made of InGaN (0 ⁇ x ⁇ 1), an electron supply layer with AlGaN (0 ⁇ y ⁇ 1) force, and a cap layer with GaN force.
  • Laminate in order It can be set as the structure which has another structure. In this way, the effective Schottky height can be increased and a higher gate breakdown voltage can be realized.
  • a so-called gate recess structure in which a part of the lower portion of the gate electrode 102 is embedded in the AlGaN electron supply layer 113 can be employed. As a result, an excellent gate breakdown voltage can be obtained.
  • the distance between the gate electrode 102 and the drain electrode 103 can be made longer than that between the gate electrode 102 and the source electrode 101. This is a so-called offset structure, and the electric field concentration at the end on the drain electrode side of the gate electrode 102 can be more effectively dispersed and relaxed.

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  • Junction Field-Effect Transistors (AREA)

Abstract

Disclosed is a group III nitride semiconductor field effect transistor having excellent operation stability which is able to be manufactured at high yield. Specifically disclosed is an HJFET (100) comprising a group III nitride semiconductor layer structure including a heterojunction between a GaN channel layer (112) and an AlGaN electron supply layer (113), a source electrode (101) and a drain electrode (103) formed separately from each other on the group III nitride semiconductor layer structure, and a gate electrode (102) arranged between the source electrode (101) and the drain electrode (103). An SiN film (121) is provided on the group III nitride semiconductor layer structure in a region between the gate electrode (102) and the drain electrode (103). At the interface between the SiN film (121) and the AlGaN electron supply layer (113), the impurity concentration in the AlGaN electron supply layer (113) is not more than 1E17 atoms/cm3.

Description

明 細 書  Specification

電界効果トランジスタおよびその製造方法  Field effect transistor and manufacturing method thereof

技術分野  Technical field

[oooi] 本発明は、 m族窒化物半導体を用いた電界効果トランジスタおよびその製造方法 に関するものである。  [oooi] The present invention relates to a field effect transistor using a group m nitride semiconductor and a method of manufacturing the same.

背景技術  Background art

[0002] GaNをはじめとする ΠΙ族窒化物半導体は、 GaAs系半導体に比べ大きなバンドギ ヤップ、高い絶縁破壊電界、そして大きな電子の飽和ドリフト速度を有するため、高温 動作、高速スイッチング動作、大電力動作等の点で優れた電子素子を実現する材料 として期待^^めている。  [0002] GaN and other group III nitride semiconductors have a large band gap, a high breakdown electric field, and a large saturation drift velocity of electrons compared to GaAs semiconductors. Therefore, high-temperature operation, high-speed switching operation, and high-power operation It is expected to be a material that realizes excellent electronic devices in terms of

[0003] また、 III族窒化物半導体は、圧電性を有するため、ヘテロ接合構造によって、自発 分極とピエゾ分極力 ヘテロ接合部に生成される高濃度二次元キャリアガスの利用 が可能であり、不純物ドーピングによる発生したキャリアによって駆動する GaAs系半 導体電界効果トランジスタとは異なった機構での動作が可能であるという特徴を持つ ている。  [0003] In addition, since group III nitride semiconductors have piezoelectricity, they can utilize high-concentration two-dimensional carrier gas generated at the heterojunction due to spontaneous polarization and piezoelectric polarization force due to the heterojunction structure. It has the feature that it can operate by a mechanism different from that of a GaAs-based semiconductor field effect transistor driven by carriers generated by doping.

[0004] このような III族窒化物半導体素子においては、ヘテロ接合部でキャリアガスが発生 するのに伴い、半導体層構造表面に負電荷が誘起され、これがトランジスタの諸特 性に大きな影響を及ぼすことから、表面負電荷の制御技術の開発が重要である。以 下、この点について説明する。  [0004] In such a group III nitride semiconductor device, as carrier gas is generated at the heterojunction, a negative charge is induced on the surface of the semiconductor layer structure, which greatly affects various characteristics of the transistor. Therefore, the development of surface negative charge control technology is important. This point will be explained below.

[0005] ヘテロ接合を含む III族窒化物半導体の積層構造では、ピエゾ分極等によりチヤネ ル層に大きな電荷が発生する一方、 AlGaN等の半導体層表面に負電荷が発生する ことが知られている(非特許文献 1)。こうした負電荷は、ドレイン電流に直接作用し、 素子性能に強い影響を及ぼす。具体的には、表面に大きな負電荷が発生すると、交 流動作時の最大ドレイン電流が直流時に比べ劣化する。この現象を以下、電流コラ ブスと称する。電流コラブスは、 GaAs系へテロ接合素子においては、分極電荷の発 生が極めて小さ!/、ためみられず、 III族窒化物半導体素子にぉ 、て顕著にみられる 特有の現象である。 [0006] こうした問題に対し、従来、表面保護層を形成することで電流コラブスの低減がなさ れていた。保護膜を設けない構造では、電流コラブスのため、高電圧印加時に充分 なドレイン電流が得られず、 ΠΙ族窒化物半導体材料を用いる利点を得ることが困難 である。また、電流コラブス抑制の効果は、保護膜を用いる材料によっても異なって おり、一般には SiNが電流コラブス抑制の効果が高いことが知られている。以下、保 護膜を有する従来のトランジスタの一例について説明する。 [0005] It is known that in a layered structure of a group III nitride semiconductor including a heterojunction, a large charge is generated in the channel layer due to piezoelectric polarization or the like, while a negative charge is generated on the surface of the semiconductor layer such as AlGaN. (Non-patent document 1). These negative charges directly affect the drain current and have a strong effect on device performance. Specifically, when a large negative charge is generated on the surface, the maximum drain current during the alternating current operation is deteriorated as compared with direct current. This phenomenon is hereinafter referred to as current collapse. Current collabs are a peculiar phenomenon that is not so common in GaAs heterojunction devices and is not observed, and is notably observed in group III nitride semiconductor devices. [0006] Conventionally, current collabs have been reduced by forming a surface protective layer to solve these problems. In a structure without a protective film, sufficient drain current cannot be obtained when a high voltage is applied because of current collabs, and it is difficult to obtain the advantage of using a group III nitride semiconductor material. In addition, the effect of suppressing current collabs differs depending on the material using the protective film, and it is generally known that SiN is highly effective in suppressing current collabs. Hereinafter, an example of a conventional transistor having a protective film will be described.

[0007] 図 28は、従来のへテロ接合電界効果トランジスタ(Hetero— Junction Field Ef feet Transistor:以下 HJFETと称する)の構成を示す断面図である。図 28に示し た HJFETは、たとえば非特許文献 2に報告されて 、る。  FIG. 28 is a cross-sectional view showing a configuration of a conventional hetero-junction field effect transistor (hereinafter referred to as HJFET). The HJFET shown in FIG. 28 is reported in Non-Patent Document 2, for example.

[0008] 図 28の HJFET200においては、サファイア基板 209の上に A1Nからなるバッファ 層 211、 GaNチャネル層 212および AlGaN電子供給層 213がこの順で積層されて いる。その上に、ソース電極 201とドレイン電極 203とが形成されており、これらの電 極は、 AlGaN電子供給層 213とオーム性接触している。また、ソース電極 201とドレ イン電極 203の間にゲート電極 202が形成され、このゲート電極 202は、 AlGaN電 子供給層 213にショットキー性接触している。最上層には、表面保護膜として SiN膜 221が形成されている。  In the HJFET 200 of FIG. 28, a buffer layer 211 made of A1N, a GaN channel layer 212 and an AlGaN electron supply layer 213 are stacked in this order on a sapphire substrate 209. On top of this, a source electrode 201 and a drain electrode 203 are formed, and these electrodes are in ohmic contact with the AlGaN electron supply layer 213. A gate electrode 202 is formed between the source electrode 201 and the drain electrode 203, and the gate electrode 202 is in Schottky contact with the AlGaN electron supply layer 213. In the uppermost layer, a SiN film 221 is formed as a surface protective film.

[0009] 次に、 HJFET200の製造方法を説明する。まず、サファイア力もなる基板 209上に 、たとえば分子線ェピタキシ(Molecular Beam Epitaxy : MBE)成長法や有機金 属気相ェピタキシ(Metal Organic Vapor Phase Epitaxy : MOVPE)成長法 等によって半導体を成長させる。このようにして、基板側から順に、アンドープ A1Nか らなるバッファ層 211 (膜厚 20nm)、アンドープの GaNチャネル層 212 (膜厚 2 μ m) 、およびアンドープ AlGaNからなる AlGaN電子供給層 213 (膜厚 25nm)が積層し た半導体層構造が得られる。  Next, a method for manufacturing HJFET 200 will be described. First, on a substrate 209 having sapphire power, a semiconductor is grown by, for example, a molecular beam epitaxy (MBE) growth method or a metal organic vapor phase epitaxy (MOVPE) growth method. In this way, in order from the substrate side, the buffer layer 211 (film thickness 20 nm) made of undoped A1N, the undoped GaN channel layer 212 (film thickness 2 μm), and the AlGaN electron supply layer 213 (film) made of undoped AlGaN A semiconductor layer structure with a thickness of 25 nm) is obtained.

[0010] 次いで、 GaNチャネル層 212が露出するまでェピタキシャル層構造の一部をエツ チング除去することにより、素子間分離メサ (不図示)を形成する。そして、 AlGaN電 子供給層 213の所定の領域にフォトレジストを形成した後、 AlGaN電子供給層 213 上にたとえば TiZAl等の金属を蒸着し、リフトオフ法等を用い、ソース電極 201およ びドレイン電極 203を形成する。そして、これを 650°Cでァニールすることにより、これ らの電極と AlGaN電子供給層 213との間にオーム性接合を形成する。 Next, a part of the epitaxial layer structure is etched away until the GaN channel layer 212 is exposed, thereby forming an element isolation mesa (not shown). Then, after forming a photoresist in a predetermined region of the AlGaN electron supply layer 213, a metal such as TiZAl is deposited on the AlGaN electron supply layer 213, and a source electrode 201 and a drain electrode are formed using a lift-off method or the like. 203 is formed. And by annealing it at 650 ° C, An ohmic junction is formed between these electrodes and the AlGaN electron supply layer 213.

[0011] つづいて、 AlGaN電子供給層 213の所定の領域にフォトレジストを形成した後、 A1 GaN電子供給層 213上に、たとえばゲート電極用の金属膜として Ni (上層) ZAu( 下層)を蒸着し、リフトオフすることにより、 AlGaN電子供給層 213とショットキー接合 されたゲート電極 202を形成する。そして、プラズマ CVD法等により、 Sii^l22l 03I 厚 50nm)を形成する。以上の手順により、図 28に示した HJFET200が得られる。 非特許文献 1 :U. K. Mishra, P. Parikh, and Yi— Feng Wu, 「AlGa N/GaN HEMTs —An overview of device operation and application s.」 Proc. IEEE, vol. 90, No. 6, pp. 1022—1031, 2002 非特許文献 2 : 2001年インターナショナル'エレクトロン'デバイス'ミーティング 'ダイ ジェスト(IEDM01— 381〜384)、安藤 (Y. Ando) [0011] Subsequently, after forming a photoresist in a predetermined region of the AlGaN electron supply layer 213, Ni (upper layer) ZAu (lower layer) is deposited on the A1 GaN electron supply layer 213 as a metal film for a gate electrode, for example. Then, by lift-off, the gate electrode 202 which is in Schottky junction with the AlGaN electron supply layer 213 is formed. Then, Sii ^ 22l03I thickness 50 nm) is formed by plasma CVD method or the like. With the above procedure, the HJFET 200 shown in FIG. 28 is obtained. Non-Patent Document 1: UK Mishra, P. Parikh, and Yi— Feng Wu, “AlGa N / GaN HEMTs —An overview of device operation and application s.” Proc. IEEE, vol. 90, No. 6, pp. 1022 —1031, 2002 Non-Patent Document 2: International 'Electron' Device 'Meeting' Digest (IEDM01—381-384), Ando (Y. Ando)

発明の開示  Disclosure of the invention

[0012] ところが、上述した製造方法で得られた HJFETについて本発明者が検討したとこ ろ、表面保護膜を設けた場合においても、得られたトランジスタの特性にばらつきが 生じる場合や、充分なドレイン電流が得られない場合があることが明らかになった。  [0012] However, the inventors of the present invention have studied the HJFET obtained by the above-described manufacturing method, and even when a surface protective film is provided, the characteristics of the obtained transistor may vary, or sufficient drainage may occur. It became clear that the current could not be obtained.

[0013] 本発明者は、こうした原因について以下のように推察した。  [0013] The present inventor has inferred such a cause as follows.

第一に、充分なドレイン電流が流れない原因として、製造過程で AlGaN電子供給 層 213と SiN膜 221との界面に導入された不純物が界面準位を形成し、キャリアがト ラップされてしまうことが推察された。不純物により界面準位が形成されると、電流コラ ブスが発生するため、ドレイン電流を低下させる要因となる。  First, the reason why sufficient drain current does not flow is that impurities introduced into the interface between the AlGaN electron supply layer 213 and the SiN film 221 during the manufacturing process form interface states, and carriers are trapped. Was inferred. When interface states are formed by impurities, current collapse occurs, which causes the drain current to decrease.

[0014] ここで、電流コラプスは、ゲート耐圧とトレードオフの関係となっている。 AlGaN表面 に発生する負の分極電荷は、その上に堆積する保護膜 (パッシベーシヨン膜)の電気 的性質によっては、そのトランジスタ特性に大きな影響を与える。一般に、表面に大き な負の固定電荷が存在すると、高いゲート耐圧が得られるが、交流動作時の電流コ ラブスが大きくなる傾向が見られる。一方、表面の負電荷量が少ないと、ゲート耐圧 は低いが、電流コラブスが小さい。トランジスタの動作は、一般にこのトレードオフ関 係に支配されるが、 AlGaN (上層) ZGaN (下層)ヘテロ構造では、たとえば表面に 1 E13atomsZcm2オーダーの負電荷が発生するため、表面パッシベーシヨンの品質 により、前述のトレードオフ関係が極めて顕著に現れる。耐圧の値が、表面パッシベ ーシヨンの状態により 1桁以上変化することも珍しくない。このような大きな変化は、 Ga As系トランジスタでは見られない現象である。逆に言えば、 III族窒化物半導体系トラ ンジスタは表面状態に極めて敏感なデバイスであり、その電気特性にぉ 、て高 ヽ性 能を高歩留まりで安定的に得るためには、表面状態の制御に細心の注意を払う必要 がある。 Here, the current collapse has a trade-off relationship with the gate breakdown voltage. The negative polarization charge generated on the AlGaN surface has a great influence on the transistor characteristics depending on the electrical properties of the protective film (passivation film) deposited on the AlGaN surface. In general, when a large negative fixed charge is present on the surface, a high gate breakdown voltage can be obtained, but current collaboration during AC operation tends to increase. On the other hand, when the negative charge amount on the surface is small, the gate breakdown voltage is low, but the current collab is small. Transistor operation is generally governed by this trade-off, but the AlGaN (upper layer) ZGaN (lower layer) heterostructure generates negative charges on the surface, for example, on the order of 1 E13 atoms Zcm 2, so the quality of the surface passivation As a result, the above-described trade-off relationship appears very markedly. It is not uncommon for the pressure resistance value to change by an order of magnitude depending on the state of surface passivation. Such a large change is a phenomenon that cannot be seen in a Ga As transistor. Conversely, Group III nitride semiconductor transistors are devices that are extremely sensitive to surface conditions, and in order to stably obtain high performance with a high yield, it is necessary to improve the surface conditions. It is necessary to pay close attention to control.

[0015] 第二に、 SiN膜 221を設けてもなお生じるトランジスタ特性のばらつきとしては、たと えば、トランジスタの動作時の効率のばらつきが挙げられる。これについて本発明者 が検討した結果、トランジスタの動作時の効率がばらつく原因として、ゲート電極 202 のショットキー特性のばらつきにより HJFET200のゲートリーク電流にばらつきが生じ ることが推察された。そこで、 HJFET200のショットキー特性のばらつきの原因につ いてさらに検討を行つたところ、 AlGaN電子供給層 213と SiN膜 221との界面に導 入された不純物がショットキー特性にも影響を与えていることが見出された。以下、こ の点について説明する。  [0015] Secondly, the variation in transistor characteristics that still occurs even when the SiN film 221 is provided includes, for example, a variation in efficiency during the operation of the transistor. As a result of the examination by the present inventors, it has been inferred that the variation in the gate leakage current of the HJFET 200 is caused by the variation in the Schottky characteristics of the gate electrode 202 as the cause of the variation in efficiency during the operation of the transistor. Thus, when the cause of the variation in the Schottky characteristics of the HJFET 200 was further investigated, impurities introduced into the interface between the AlGaN electron supply layer 213 and the SiN film 221 also affected the Schottky characteristics. It was found. This point will be described below.

[0016] 従来の HJFET200の製造途中においては、 AlGaN電子供給層 213の表面が剥 き出しの状態となる。このため、製造工程において、 AlGaN電子供給層 213の表面 にフォトレジストが形成さる。また、レジストを除去する際に、プラズマアツシングによる プラズマダメージに数回曝される。さら〖こは、 AlGaN電子供給層 213の表面が剥き 出しのまま、オーム性電極形成時の高温ァニールが行われる。  [0016] During the manufacturing of the conventional HJFET 200, the surface of the AlGaN electron supply layer 213 is exposed. For this reason, a photoresist is formed on the surface of the AlGaN electron supply layer 213 in the manufacturing process. Also, when removing the resist, it is exposed several times to plasma damage due to plasma ashing. In addition, high-temperature annealing during ohmic electrode formation is performed with the surface of the AlGaN electron supply layer 213 exposed.

[0017] このような製造工程を経て得られた HJFET200の III族窒化物半導体層 213の表 面とゲート電極 202との界面における酸素等の不純物濃度を SIMS (二次イオン質 量分析法)により測定したところ、 lE18atomsZcm3〜lE19atomsZcm3程度であ つた。このように不純物濃度が高くなるのは、 AlGaN電子供給層 213の表面力 前 述した電極形成工程時のプラズマダメージを受けたり、高温ァニールの後大気に曝 されたりすることで、より酸ィ匕されやすくなるためであると考えられる。 AlGaN電子供 給層 213の表面を清浄な状態にするためには、酸等によるエッチングが有効である 力 オーム性電極等を形成した後では、レジストで覆っていてもエッチング液の周り込 みがあり、金属が侵され、ォーミック性の劣化等が起きる。このため電極形成後はエツ チングにより表面状態を充分に清浄な状態することは困難である。 [0017] The concentration of impurities such as oxygen at the interface between the surface of the group III nitride semiconductor layer 213 of the HJFET 200 and the gate electrode 202 obtained through such a manufacturing process is determined by SIMS (secondary ion mass spectrometry). When measured, it was about lE18atomsZcm 3 to lE19atomsZcm 3 . The impurity concentration increases as described above because the surface force of the AlGaN electron supply layer 213 is more damaged by plasma damage during the electrode formation process described above or by exposure to the atmosphere after high-temperature annealing. This is thought to be easy to be done. In order to clean the surface of the AlGaN electrode layer 213, etching with an acid or the like is effective for etching. Yes, metal is attacked and ohmic deterioration occurs. For this reason, It is difficult to sufficiently clean the surface state by ching.

[0018] このように、 HJFET200において、 AlGaN電子供給層の表面状態はプロセスによ る影響を受けやすい。このため、 AlGaN電子供給層 213の表面は、半導体の結晶 性の変化等を受け、初期の清浄な状態と異なった状態となる。こうした状態としては、 たとえば、 [0018] Thus, in the HJFET 200, the surface state of the AlGaN electron supply layer is easily affected by the process. For this reason, the surface of the AlGaN electron supply layer 213 is in a state different from the initial clean state due to a change in crystallinity of the semiconductor. Examples of such states are:

(i)プラズマダメージや高温ァニールによって半導体結晶が変化した状態、および (i) a state in which the semiconductor crystal has changed due to plasma damage or high-temperature annealing, and

(ii)大気に曝されることによって AlGaN電子供給層表面に酸素が混入した状態 が挙げられる。 (ii) A state in which oxygen is mixed into the surface of the AlGaN electron supply layer by exposure to the atmosphere.

[0019] 次に、得られた HJFET200のショットキー特性の測定結果を説明する。図 25 (a)お よび図 25 (b)は、従来の製造方法で得られた HJFET200 (図 28)と、後述する実施 例の HJFET100 (図 1)との特性を比較する図である。ここでは、 3インチウエーハ 10 枚で得られた HJFETでのショットキー障壁高さ φ (eV) (図 25 (a) )および理想化因  Next, measurement results of the Schottky characteristics of the obtained HJFET 200 will be described. FIG. 25 (a) and FIG. 25 (b) are graphs comparing the characteristics of the HJFET 200 (FIG. 28) obtained by the conventional manufacturing method and the HJFET 100 (FIG. 1) of an example described later. Here, Schottky barrier height φ (eV) (Fig. 25 (a)) and idealization factor in HJFET obtained with 10 3-inch wafers.

B  B

子 n (図 25 (b) )が示されている。理想化因子 nは、理想的にショットキー接合した場 合のショットキー障壁高さ φ 力 のずれの程度を示す指標であり、 n= lの場合が理  Child n (Fig. 25 (b)) is shown. The idealization factor n is an index that indicates the degree of deviation of the Schottky barrier height φ force when an ideal Schottky junction is used.

B  B

想的にショットキー接合されている場合に対応し、 n値が 1に近いほど、ショットキー性 は良好である。図 25より、従来の製造方法で得られた HJFET200においては、理想 的なショットキー接合に比べ φ が下がり、また、 nが 1から大きくずれている。  This corresponds to the case where the Schottky junction is ideal, and the closer the n value is to 1, the better the Schottky property. From Fig. 25, in the HJFET200 obtained by the conventional manufacturing method, φ is lower than that of an ideal Schottky junction, and n is significantly different from 1.

B  B

[0020] 以上の検討より、実際のデバイスにおいては、表面に結晶欠陥等が存在するため、 n値が理想値 n= lからずれ、結果として、見かけ上の φ を低下させることがゎカゝる。  [0020] From the above examination, since there are crystal defects on the surface in an actual device, the n value deviates from the ideal value n = l, and as a result, the apparent φ is reduced. The

B  B

これは、交流動作時のゲートリーク電流の増加を引き起こし、素子の安定動作の妨げ になる。また、結晶欠陥に何らかの分布がある場合、それに伴いショットキー特性に ばらつきが生じ、素子特性の再現性を劣化させる。したがって、素子の安定動作と特 性の再現性を向上するためには、 n値を 1に近づけることと、および、結晶状態を均一 にすること、つまりはゲート電極を形成する半導体表面の結晶性を制御することが重 要である。  This causes an increase in gate leakage current during AC operation, which hinders stable operation of the device. In addition, if there is some distribution of crystal defects, the Schottky characteristics will vary accordingly, degrading the reproducibility of the element characteristics. Therefore, in order to improve the stable operation of the device and the reproducibility of the characteristics, the n value should be close to 1 and the crystal state should be made uniform, that is, the crystallinity of the semiconductor surface forming the gate electrode. It is important to control this.

[0021] 本発明者は、こうした観点力 検討を進め、 III族窒化物半導体トランジスタに表面 保護膜を設けるとともに半導体表面の清浄度を向上させることにより、電流コラブスが 少なぐまたショットキー特性に優れたトランジスタを実現できることを見出した。本発 明はこうした新規な知見に基づきなされたものである。 [0021] The present inventor has proceeded to study such viewpoint power, and by providing a surface protective film on the group III nitride semiconductor transistor and improving the cleanliness of the semiconductor surface, the current collab is reduced and the Schottky characteristic is excellent. It was found that a transistor can be realized. Main departure Akira was made based on these new findings.

[0022] 本発明によれば、  [0022] According to the present invention,

ヘテロ接合を含む III族窒化物半導体層構造と、  A group III nitride semiconductor layer structure including a heterojunction;

該 III族窒化物半導体層構造上に離間して形成されたソース電極およびドレイン電 極と、  A source electrode and a drain electrode formed separately on the group III nitride semiconductor layer structure;

前記ソース電極と前記ドレイン電極の間に配置されたゲート電極と、  A gate electrode disposed between the source electrode and the drain electrode;

を備え、  With

前記ゲート電極と前記ドレイン電極との間の領域にお!ヽて、前記 III族窒化物半導 体層構造上に絶縁膜を有し、  In the region between the gate electrode and the drain electrode, an insulating film is provided on the group III nitride semiconductor layer structure,

前記絶縁膜と前記 ΠΙ族窒化物半導体層構造との界面における前記 ΠΙ族窒化物半 導体層構造中の不純物濃度が、 lE17atomsZcm3以下であることを特徴とする電 界効果トランジスタが提供される。 There is provided a field effect transistor characterized in that an impurity concentration in the group VIII nitride semiconductor layer structure at the interface between the insulating film and the group VIII nitride semiconductor layer structure is lE17 atoms Zcm 3 or less.

[0023] 本発明の電界効果トランジスタにおいては、ゲート電極とドレイン電極との間の領域 において、ヘテロ界面を有する III族窒化物半導体層構造上に設けられた絶縁膜と II I族窒化物半導体層構造との界面における不純物濃度が、 lE17atomSZcm3以下 である。このため、本発明のトランジスタにおいては、 III族窒化物半導体層構造にお ける不純物による界面準位形成が抑制され、電流コラブスが効果的に抑制される。ま た、本発明のトランジスタは優れたショットキー特性を有する。界面の不純物濃度を 1 E17atoms/cm3以下とすることによりショットキー特性が優れる理由として、 III族窒 化物半導体層構造の結晶性が向上することが推察される。また、本発明のトランジス タは、動作安定性に優れ、高い歩留まりで安定的に製造可能な構成となっている。 In the field effect transistor of the present invention, an insulating film provided on a group III nitride semiconductor layer structure having a heterointerface in a region between the gate electrode and the drain electrode, and a group II group nitride semiconductor layer The impurity concentration at the interface with the structure is lE17atom S Zcm 3 or less. For this reason, in the transistor of the present invention, formation of interface states due to impurities in the group III nitride semiconductor layer structure is suppressed, and current collab is effectively suppressed. In addition, the transistor of the present invention has excellent Schottky characteristics. It is presumed that the crystallinity of the group III nitride semiconductor layer structure is improved as the reason why the Schottky characteristics are excellent by setting the impurity concentration at the interface to 1 E17 atoms / cm 3 or less. In addition, the transistor of the present invention is excellent in operational stability and can be manufactured stably with a high yield.

[0024] なお、本発明にお 、て、不純物濃度は、たとえば SIMS (二次イオン質量分析法) により測定することができる。  In the present invention, the impurity concentration can be measured, for example, by SIMS (secondary ion mass spectrometry).

[0025] 本発明にお 、て、電流コラブスの抑制の観点では、前記絶縁膜を、たとえば窒素を 含む絶縁膜、好ましくはシリコンと窒素力もなる SiN膜とすることができる。  In the present invention, from the viewpoint of suppressing current collabs, the insulating film can be, for example, an insulating film containing nitrogen, preferably a SiN film having a nitrogen force with silicon.

[0026] また、本発明によれば、  [0026] Further, according to the present invention,

上記電界効果トランジスタの製造方法であって、  A method for producing the field effect transistor, comprising:

成膜室中で、ヘテロ接合を含む III族窒化物半導体層構造を形成する工程と、 前記 m族窒化物半導体層構造上に前記絶縁膜を形成する工程と、 前記絶縁膜の所定の領域をエッチングにより選択的に除去して開口部を形成し、 前記 m族窒化物半導体層構造上に、前記開口部を埋め込むように前記ゲート電極 を形成する工程と、 Forming a group III nitride semiconductor layer structure including a heterojunction in a deposition chamber; Forming the insulating film on the group m nitride semiconductor layer structure; selectively removing a predetermined region of the insulating film by etching to form an opening; and forming the opening on the group m nitride semiconductor layer structure And forming the gate electrode so as to fill the opening,

を含むことを特徴とする電界効果トランジスタの製造方法が提供される。  A method of manufacturing a field effect transistor is provided.

[0027] 本発明の方法によれば、絶縁膜がゲート電極作製前に形成される。従来の方法に おいては、背景技術の項で図 28を参照して前述したように、ゲート電極形成後、表 面保護膜が形成されるのに対し、この方法によれば、絶縁膜形成後の製造工程で、 I II族窒化物半導体層表面にフォトレジストが形成されたり、表面がプラズマに侵される ことがない。よって、本発明の製造方法によれば、経時変化による窒化物半導体表 面の酸ィ匕を抑制することができる。したがって、絶縁膜と m族窒化物半導体層構造と の界面が清浄な電界効果トランジスタを安定して製造することができる。このため、本 発明によれば、 m族窒化物半導体層の酸ィ匕による電流コラブスを抑制することがで きる。また、ショットキー界面の均一性に優れた電界効果トランジスタを安定的に製造 することができる。また、ゲート電極とドレイン電極との間の領域における m族窒化物 半導体層表面の結晶状態を良好なものとすることができる。また、結晶状態の均一性 を向上させることができる。 According to the method of the present invention, the insulating film is formed before the gate electrode is manufactured. In the conventional method, as described above with reference to FIG. 28 in the background art section, the surface protective film is formed after the formation of the gate electrode. In the subsequent manufacturing process, a photoresist is not formed on the surface of the group II II nitride semiconductor layer, and the surface is not affected by plasma. Therefore, according to the manufacturing method of the present invention, it is possible to suppress the oxidation of the nitride semiconductor surface due to change with time. Therefore, a field effect transistor having a clean interface between the insulating film and the m-group nitride semiconductor layer structure can be stably manufactured. Therefore, according to the present invention, it is possible to suppress current collapse due to oxidation of the m-group nitride semiconductor layer. In addition, a field effect transistor with excellent uniformity of the Schottky interface can be stably manufactured. In addition, the crystal state of the surface of the group m nitride semiconductor layer in the region between the gate electrode and the drain electrode can be improved. In addition, the uniformity of the crystalline state can be improved.

[0028] また、本発明によれば、  [0028] Further, according to the present invention,

成膜室中でヘテロ接合を含む III族窒化物半導体層構造を形成する工程と、 前記 III族窒化物半導体層構造上に絶縁膜を形成する工程と、  Forming a group III nitride semiconductor layer structure including a heterojunction in a film forming chamber; forming an insulating film on the group III nitride semiconductor layer structure;

前記絶縁膜の所定の領域をエッチングにより選択的に除去して開口部を形成し、 前記 m族窒化物半導体層構造上に、前記開口部を埋め込むようにゲート電極を形 成する工程と、  A step of selectively removing a predetermined region of the insulating film by etching to form an opening, and forming a gate electrode on the group m nitride semiconductor layer structure so as to embed the opening;

を含み、  Including

前記 m族窒化物半導体層構造を形成する工程の後、前記 m族窒化物半導体層 構造を前記成膜室力 取り出すことなく前記絶縁膜を形成する工程を行うことを特徴 とする電界効果トランジスタの製造方法が提供される。  A step of forming the insulating film without taking out the film forming chamber force after the step of forming the group m nitride semiconductor layer structure is performed. A manufacturing method is provided.

[0029] また、本発明によれば、 成膜室中でヘテロ接合を含む III族窒化物半導体層構造を形成する工程と、 前記 III族窒化物半導体層構造上に絶縁膜を形成する工程と、 [0029] Further, according to the present invention, Forming a group III nitride semiconductor layer structure including a heterojunction in a film forming chamber; forming an insulating film on the group III nitride semiconductor layer structure;

前記絶縁膜の所定の領域をエッチングにより選択的に除去して開口部を形成し、 前記 m族窒化物半導体層構造上に、前記開口部を埋め込むようにゲート電極を形 成する工程と、  A step of selectively removing a predetermined region of the insulating film by etching to form an opening, and forming a gate electrode on the group m nitride semiconductor layer structure so as to embed the opening;

前記 in族窒化物半導体層構造を形成する工程の後、前記絶縁膜を形成する工程 の前に、  After the step of forming the in-group nitride semiconductor layer structure and before the step of forming the insulating film,

酸を用いたウエットエッチングにより、前記 m族窒化物半導体層構造の表面を洗浄 する工程と、  Cleaning the surface of the group m nitride semiconductor layer structure by wet etching using an acid;

を含むことを特徴とする電界効果トランジスタの製造方法が提供される。  A method of manufacturing a field effect transistor is provided.

[0030] 本発明の製造方法においては、 m族窒化物半導体層構造の表面が清浄な状態で 絶縁膜を形成する。電流コラブスを抑制するために in族窒化物半導体層構造上に 絶縁膜を形成する従来の製造方法においては、絶縁膜の形成を電極形成後に行つ ていたのが通常であったため、 m族窒化物半導体層構造の表面の不純物により界 面順位が形成されてしまっていた。これに対し、本発明の製造方法によれば、 m族 窒化物半導体層構造上に絶縁膜を成膜する工程を工夫することにより、これらの界 面が清浄な電界効果トランジスタを得ることができる。このため、界面の酸ィ匕により生 じる電流コラブスが抑制され、またショットキー特性に優れた電界効果トランジスタを 安定的に製造することができる。 [0030] In the manufacturing method of the present invention, the insulating film is formed in a state where the surface of the group m nitride semiconductor layer structure is clean. In the conventional manufacturing method in which an insulating film is formed on the in-group nitride semiconductor layer structure to suppress current collabs, the insulating film is usually formed after the electrode is formed. The interface order was formed by impurities on the surface of the physical semiconductor layer structure. On the other hand, according to the manufacturing method of the present invention, a field effect transistor having a clean interface can be obtained by devising a process for forming an insulating film on the m-group nitride semiconductor layer structure. . For this reason, the current collaborative effect caused by the oxidation of the interface is suppressed, and a field effect transistor having excellent Schottky characteristics can be stably manufactured.

[0031] なお、本発明において、前記絶縁膜を形成する工程の後、前記絶縁膜の所定の領 域をエッチングにより選択的に除去し、前記 III族窒化物半導体層構造上に、除去さ れた領域を埋め込むようにソース電極とドレイン電極とを離間して形成してもよ ヽ。こ のとき、ソース電極とドレイン電極とを形成する工程と、ゲート電極を形成する工程は 、どちらを先に行ってもよい。  In the present invention, after the step of forming the insulating film, a predetermined region of the insulating film is selectively removed by etching to be removed on the group III nitride semiconductor layer structure. Alternatively, the source electrode and the drain electrode may be formed so as to be embedded in the region. At this time, either the step of forming the source electrode and the drain electrode or the step of forming the gate electrode may be performed first.

[0032] 以上説明したように、本発明によれば、動作安定性に優れ、高い歩留まりで製造可 能な ΠΙ族窒化物半導体電界効果トランジスタが実現される。  As described above, according to the present invention, it is possible to realize a group III nitride semiconductor field effect transistor that is excellent in operational stability and can be manufactured with a high yield.

図面の簡単な説明  Brief Description of Drawings

[0033] 上述した目的、およびその他の目的、特徴および利点は、以下に述べる好適な実 施の形態、およびそれに付随する以下の図面によってさらに明らかになる。 [0033] The above objects and other objects, features and advantages will The present invention will be further clarified by embodiments and the following drawings attached thereto.

[図 1]実施例に係る電界効果トランジスタの構成を示す断面図である。  FIG. 1 is a cross-sectional view showing a configuration of a field effect transistor according to an example.

[図 2]実施例に係る電界効果トランジスタの構成を示す断面図である。  FIG. 2 is a cross-sectional view showing a configuration of a field effect transistor according to an example.

[図 3]実施例に係る電界効果トランジスタの構成を示す断面図である。  FIG. 3 is a cross-sectional view showing a configuration of a field effect transistor according to an example.

[図 4]実施例に係る電界効果トランジスタの構成を示す断面図である。  FIG. 4 is a cross-sectional view showing a configuration of a field effect transistor according to an example.

[図 5]実施例に係る電界効果トランジスタの構成を示す断面図である。  FIG. 5 is a cross-sectional view showing a configuration of a field effect transistor according to an example.

[図 6]実施例に係る電界効果トランジスタの構成を示す断面図である。  FIG. 6 is a cross-sectional view showing a configuration of a field effect transistor according to an example.

圆 7]図 1の電界効果トランジスタの製造工程を示す断面図である。 7] FIG. 7 is a cross-sectional view showing a manufacturing process of the field effect transistor of FIG.

圆 8]図 1の電界効果トランジスタの製造工程を示す断面図である。 8] FIG. 8 is a cross-sectional view showing a manufacturing process of the field effect transistor of FIG.

圆 9]図 1の電界効果トランジスタの製造工程を示す断面図である。 9] FIG. 9 is a cross-sectional view showing a manufacturing process of the field effect transistor of FIG.

圆 10]図 2の電界効果トランジスタの製造工程を示す断面図である。 FIG. 10] A sectional view showing a manufacturing process of the field effect transistor of FIG.

圆 11]図 2の電界効果トランジスタの製造工程を示す断面図である。 FIG. 11] A sectional view showing a manufacturing process of the field effect transistor of FIG.

圆 12]図 2の電界効果トランジスタの製造工程を示す断面図である。 12] A sectional view showing a manufacturing process of the field effect transistor of FIG.

圆 13]図 2の電界効果トランジスタの製造工程を示す断面図である。 13] A sectional view showing a manufacturing process of the field effect transistor of FIG.

圆 14]図 3の電界効果トランジスタの製造工程を示す断面図である。 14] A sectional view showing a manufacturing process of the field effect transistor of FIG.

圆 15]図 3の電界効果トランジスタの製造工程を示す断面図である。 15] A sectional view showing a manufacturing process of the field effect transistor of FIG.

圆 16]図 3の電界効果トランジスタの製造工程を示す断面図である。 FIG. 16] A sectional view showing a manufacturing process of the field effect transistor of FIG.

圆 17]図 3の電界効果トランジスタの製造工程を示す断面図である。 FIG. 17] A sectional view showing a manufacturing process of the field effect transistor of FIG.

圆 18]図 4の電界効果トランジスタの製造工程を示す断面図である。 FIG. 18] A sectional view showing a manufacturing process of the field effect transistor of FIG.

圆 19]図 4の電界効果トランジスタの製造工程を示す断面図である。 FIG. 19] A sectional view showing a manufacturing process of the field effect transistor of FIG.

[図 20]図 4の電界効果トランジスタの製造工程を示す断面図である。  20 is a cross-sectional view showing a manufacturing step of the field effect transistor of FIG. 4. FIG.

圆 21]図 5の電界効果トランジスタの製造工程を示す断面図である。 FIG. 21 is a cross-sectional view showing a manufacturing process of the field effect transistor of FIG.

圆 22]図 5の電界効果トランジスタの製造工程を示す断面図である。 FIG. 22] A sectional view showing a manufacturing process of the field effect transistor of FIG.

圆 23]図 5の電界効果トランジスタの製造工程を示す断面図である。 FIG. 23] A sectional view showing a manufacturing process of the field effect transistor of FIG.

圆 24]図 5の電界効果トランジスタの製造工程を示す断面図である。 FIG. 24] A sectional view showing a manufacturing process of the field effect transistor of FIG.

圆 25]実施例および従来の電界効果トランジスタの製造方法を比較する図である。 圆 26]実施例および従来の電界効果トランジスタの製造方法を比較する図である。 [25] FIG. 25 is a diagram comparing the method of manufacturing an example and a conventional field effect transistor. [26] FIG. 26 is a diagram for comparing the method of manufacturing an example and a conventional field effect transistor.

[図 27]実施例に係る電界効果トランジスタの構成を示す断面図である。 [図 28]従来の電界効果トランジスタの構成を示す断面図である。 FIG. 27 is a cross-sectional view showing a configuration of a field effect transistor according to an example. FIG. 28 is a cross-sectional view showing a configuration of a conventional field effect transistor.

発明を実施するための最良の形態  BEST MODE FOR CARRYING OUT THE INVENTION

[0035] 以下、 III族窒化物半導体構造として、 AlGaN電子供給層 ZGaNチャネル層およ び表面保護膜 (以下、単に「保護膜」とも呼ぶ。)を有する HJFETを例に、本発明の 実施形態について図面を参照して説明する。なお、すべての図面において、共通の 構成要素には同じ符号を付し、適宜説明を省略する。また、本明細書においては、 積層構造を「上層 Z下層 (基板側) Jと表記する。  Hereinafter, an embodiment of the present invention will be described by taking an HJFET having an AlGaN electron supply layer, a ZGaN channel layer, and a surface protective film (hereinafter also simply referred to as “protective film”) as an example of a group III nitride semiconductor structure. Will be described with reference to the drawings. In all the drawings, common constituent elements are denoted by the same reference numerals, and description thereof will be omitted as appropriate. Further, in this specification, the laminated structure is expressed as “upper layer Z lower layer (substrate side) J”.

[0036] 図 1は、本実施形態の電界効果トランジスタの基本構成を示す図である。この電界 効果トランジスタ (HJFET100)は、ヘテロ接合を含む III族窒化物半導体層構造 (G aNチャネル層 112、 AlGaN電子供給層 113)と、これらの III族窒化物半導体層構 造上に離間して形成されたソース電極 101およびドレイン電極 103と、ソース電極 10 1とドレイン電極 103との間に配置されたゲート電極 102と、を備える。 HJFET100は 、ヘテロ接合構造を有するため、自発分極とピエゾ分極力 ヘテロ接合部に生成され る高濃度二次元キャリアガスの利用が可能である。  FIG. 1 is a diagram showing a basic configuration of the field effect transistor of the present embodiment. This field effect transistor (HJFET100) is separated from the group III nitride semiconductor layer structure (GaN channel layer 112, AlGaN electron supply layer 113) including the heterojunction, and these group III nitride semiconductor layer structures. The source electrode 101 and the drain electrode 103 formed, and the gate electrode 102 disposed between the source electrode 101 and the drain electrode 103 are provided. Since the HJFET 100 has a heterojunction structure, it is possible to use a high-concentration two-dimensional carrier gas generated at the heterojunction with spontaneous polarization and piezoelectric polarization force.

[0037] III族窒化物半導体層構造は、 In Ga N (0≤x≤ 1)からなるチャネル層と、 Al G a N (0≤y≤ 1)とからなる電子供給層を含み、ヘテロ界面は、 In Ga Nと Al Ga Nとの界面である。ただし、上記式において、 Xと yが同時にゼロにならないように l -y  [0037] The group III nitride semiconductor layer structure includes a channel layer made of InGaN (0≤x≤1) and an electron supply layer made of AlGaN (0≤y≤1), and includes a heterointerface. Is the interface between InGaN and AlGaN. However, in the above formula, l -y so that X and y do not become zero at the same time.

することが必要である。  It is necessary to.

[0038] HJFET100は、ゲート電極 102とドレイン電極 103との間の領域において、 GaNチ ャネル層 112および AlGaN電子供給層 113の積層構造上に保護膜として絶縁膜 (S iN膜 121)を有する。  The HJFET 100 has an insulating film (SiN film 121) as a protective film on the laminated structure of the GaN channel layer 112 and the AlGaN electron supply layer 113 in the region between the gate electrode 102 and the drain electrode 103.

[0039] 保護膜は、上記 SiN膜 121のように、絶縁材料力も構成される。 SiN膜 121は、ゲ ート電極 102とドレイン電極 103との間の領域の全面に設けられていてもよいし、当 該領域の一部に設けられていてもよい。ゲート電極 102とドレイン電極 103との間の 領域全面を SiN膜 121が被覆する構成とすることにより、電流コラブスをさらに効果的 に抑制することができる。  [0039] Like the SiN film 121, the protective film also has an insulating material strength. The SiN film 121 may be provided on the entire surface of the region between the gate electrode 102 and the drain electrode 103 or may be provided on a part of the region. By adopting a configuration in which the entire region between the gate electrode 102 and the drain electrode 103 is covered with the SiN film 121, the current collab can be more effectively suppressed.

[0040] SiN膜 121は、 GaNチャネル層 112および AlGaN電子供給層 113の積層構造を 構成する元素のうち少なくとも一つとして窒素を含む絶縁膜である。保護膜中の元素 が AlGaN電子供給層 113と保護膜との界面に移動すると、界面の不純物として準位 が形成される懸念があるが、 SiN膜 121中の窒素は AlGaN電子供給層 113を構成 する Nと共通するため、 AlGaN電子供給層 113に対して不純物とならず、界面準位 が形成されないようにすることができる。このため、電流コラブスの発生をさらに効果 的に抑制できる。また、保護膜を SiN膜 121とすることにより、 AlGaN電子供給層 11 3と共通の材料を用いることが可能となる。 The SiN film 121 is an insulating film containing nitrogen as at least one of the elements constituting the laminated structure of the GaN channel layer 112 and the AlGaN electron supply layer 113. Elements in protective film May move to the interface between the AlGaN electron supply layer 113 and the protective film, there is a concern that a level is formed as an impurity at the interface, but nitrogen in the SiN film 121 is common to N constituting the AlGaN electron supply layer 113 Therefore, it does not become an impurity with respect to the AlGaN electron supply layer 113, and an interface state can be prevented from being formed. For this reason, generation | occurrence | production of current collaboration can be suppressed more effectively. In addition, by using the SiN film 121 as the protective film, it is possible to use the same material as the AlGaN electron supply layer 113.

[0041] また、 AlGaN電子供給層 113である AlGaNェピタキシャル層上に SiNを成長させ る場合、成長条件に応じて、成長初期に、下層の AlGaNと格子整合しょうとして下地 の結晶性を反映するように SiNがいわゆるェピタキシャル成長する。このとき、 SiN膜 121は、 GaNチャネル層 112および AlGaN電子供給層 113の積層構造上に、ェピ タキシャル成長した領域を含む膜である。ェピタキシャル成長した領域を含む膜とす ることにより、 III族窒化物半導体層構造と SiN膜 121とを連続工程で製造することが 可能となる。また、得られた SiN膜 121の膜質の安定性を向上させることができる。  [0041] When SiN is grown on the AlGaN epitaxial layer, which is the AlGaN electron supply layer 113, the crystallinity of the underlying layer is reflected in the initial stage of growth depending on the growth conditions so as to lattice match with the underlying AlGaN. So SiN grows so-called epitaxy. At this time, the SiN film 121 is a film including a region grown epitaxially on the laminated structure of the GaN channel layer 112 and the AlGaN electron supply layer 113. By using a film including an epitaxially grown region, the group III nitride semiconductor layer structure and the SiN film 121 can be manufactured in a continuous process. Further, the stability of the film quality of the obtained SiN film 121 can be improved.

[0042] SiN膜 121は、構成元素として酸素を実質的に含まない膜である。酸素は、 III族窒 化物半導体中で準位を形成しやすいため、酸素を実質的に含まない構成とすること により、電流コラブスの発生をさらに確実に抑制することができる。なお、「酸素を実質 的に含まない」とは、膜中に酸素を意図的に含有させていないことをいい、酸素の不 純物準位形成による電流コラブスの発生を抑制できる程度であれば、非意図的に含 まれる酸素が存在してもよい。また、酸素濃度が SIMSにおける検出限界以下である ことが好ましい。  The SiN film 121 is a film that substantially does not contain oxygen as a constituent element. Since oxygen tends to form a level in a group III nitride semiconductor, the generation of current collabs can be more reliably suppressed by employing a structure that does not substantially contain oxygen. Note that “substantially free of oxygen” means that no oxygen is intentionally contained in the film, as long as current Collabs generation due to the formation of impurity levels of oxygen can be suppressed. Unintentionally included oxygen may be present. Moreover, it is preferable that the oxygen concentration is below the detection limit in SIMS.

[0043] SiN膜 121の厚さは、たとえば 5nm以上 200nm以下、さらに具体的には 5nm以上 lOOnm以下である。 5nm以上とすることにより、界面における電流コラプスをさらに 確実に抑制することができる。また、 SiN膜 121の厚さは、たとえば 200nm以下、好 ましくは 150nm以下、さらに好ましくは lOOnm以下とする。こうすることによって、電 流コラブスを抑制するとともに、ゲート耐圧を向上させることが可能となり、両者のトレ ードオフの問題をさらに有効に解決することができる。  [0043] The thickness of the SiN film 121 is, for example, not less than 5 nm and not more than 200 nm, more specifically not less than 5 nm and not more than lOOnm. By setting the thickness to 5 nm or more, current collapse at the interface can be more reliably suppressed. The thickness of the SiN film 121 is, for example, 200 nm or less, preferably 150 nm or less, more preferably lOOnm or less. By doing this, current collaboratives can be suppressed and the gate breakdown voltage can be improved, and the trade-off problem between the two can be solved more effectively.

[0044] また、 SiN膜 121は、清浄な AlGaN電子供給層 113の表面に成長した膜である。  Further, the SiN film 121 is a film grown on the surface of the clean AlGaN electron supply layer 113.

HJFET100にお!/、ては、 SiN膜 121と GaNチャネル層 112および AlGaN電子供給 層 113の積層構造との界面における不純物濃度力 lE17atomsZcm3以下、好ま しくは lE15atomsZcm3以下である。こうすることにより、 AlGaN電子供給層 113に おける界面準位形成を抑制し、電流コラブスの発生を抑制できる。また、ショットキー 特性を向上させることができる。なお、本明細書において、不純物濃度は、界面に含 まれる炭素と酸素の合計濃度である。本実施形態および以下の実施例において、不 純物濃度は、たとえば SIMS (二次イオン質量分析法)により測定することができる。 HJFET100! /, SiN film 121, GaN channel layer 112 and AlGaN electron supply Impurity concentration force LE17atomsZcm 3 below at the interface between the laminated structure of the layer 113, is favored properly is LE15atomsZcm 3 or less. By doing so, it is possible to suppress the formation of interface states in the AlGaN electron supply layer 113 and to suppress the generation of current collabs. In addition, Schottky characteristics can be improved. In this specification, the impurity concentration is the total concentration of carbon and oxygen contained in the interface. In this embodiment and the following examples, the impurity concentration can be measured, for example, by SIMS (secondary ion mass spectrometry).

[0045] ただし、上記界面不純物濃度を満たす HJFET100を、上述の従来の方法で得るこ とは困難である。本実施形態においては、電流コラブスの発生を効果的に抑制する 表面保護膜として SiN膜 121を用いるとともに、 AlGaN電子供給層 113の表面が清 浄な状態で SiN膜 121の形成を行うことにより、上記不純物濃度の HJFET100を得 ることができる。 AlGaN電子供給層 113の表面が清浄な状態で SiN膜 121の形成を 行う方法として、たとえば、 [0045] However, it is difficult to obtain the HJFET 100 satisfying the interface impurity concentration by the above-described conventional method. In the present embodiment, the SiN film 121 is used as a surface protective film that effectively suppresses the generation of current collabs, and the SiN film 121 is formed while the surface of the AlGaN electron supply layer 113 is clean. HJFET100 having the above impurity concentration can be obtained. As a method of forming the SiN film 121 while the surface of the AlGaN electron supply layer 113 is clean, for example,

(i) AlGaN電子供給層 113形成後、大気暴露することなく同じ成膜室内で SiN膜 12 1を形成する方法、  (i) After forming the AlGaN electron supply layer 113, a method of forming the SiN film 121 in the same deposition chamber without exposing to the atmosphere,

(ii) AlGaN電子供給層 113の表面を酸等でエッチングした後 SiN膜 121を形成する 方法、  (ii) a method of forming the SiN film 121 after etching the surface of the AlGaN electron supply layer 113 with an acid or the like,

が挙げられる。これらの方法により HJFETを作製したところ、上記 (i)の方法では A1G aN電子供給層 113表面と SiN膜 121およびゲート電極 102との界面における不純 物濃度が lE15atomsZcm3以下の HJFETが得られた。また、上記(ii)の方法では AlGaN電子供給層 113表面と SiN膜 121およびゲート電極 102との界面における 不純物濃度が lE17atomsZcm3以下の HJFETが得られた。なお、これらの方法に ついては、後述する実施例においてさらに詳細に説明する。 Is mentioned. When an HJFET was fabricated by these methods, an HJFET having an impurity concentration of lE15 atoms Zcm 3 or less at the interface between the surface of the A1GaN electron supply layer 113 and the SiN film 121 and the gate electrode 102 was obtained by the method (i). In the method (ii), an HJFET having an impurity concentration of lE17 atoms Zcm 3 or less at the interface between the surface of the AlGaN electron supply layer 113 and the SiN film 121 and the gate electrode 102 was obtained. Note that these methods will be described in more detail in Examples described later.

[0046] また、上記方法によれば、 AlGaN電子供給層 113形成後、電極形成前に SiN膜 1 21が形成されるため、ソース電極 101とドレイン電極 103とが SiN膜 121の上に乗り 上げた構造になっている。このことによって、高電圧動作時のドレイン電極 103のゲ ート電極側端部での電界集中が緩和され、ゲート耐圧が改善される効果が得られる In addition, according to the above method, since the SiN film 121 is formed after the AlGaN electron supply layer 113 is formed and before the electrode is formed, the source electrode 101 and the drain electrode 103 run on the SiN film 121. It has a structure. As a result, the concentration of the electric field at the gate electrode side end of the drain electrode 103 during high-voltage operation is alleviated, and the gate breakdown voltage is improved.

[0047] (実施例) 以下、 m族窒化物半導体層の成長基板として c面 Sicを用いる場合を例に、本発 明の実施例について図面を参照して説明する。なお、すべての図面において、共通 の構成要素には同一の符号を付し、以下の説明において共通する説明を適宜省略 する。 [0047] (Example) Hereinafter, an example of the present invention will be described with reference to the drawings, taking as an example the case where c-plane Sic is used as a growth substrate for a group m nitride semiconductor layer. In all the drawings, common constituent elements are denoted by the same reference numerals, and common description is omitted as appropriate in the following description.

[0048] (実施例 1)  [0048] (Example 1)

本実施例は、図 1に示した構成を有する HJFETに関する。本実施例において、 HJ FET100は、 SiC等の基板 110上に形成される。基板 110上には半導体層力もなる バッファ層 111が形成されて 、る。このバッファ層 111上に GaNチャネル層 112が形 成されている。 GaNチャネル層 112の上には、八10&?^電子供給層113が形成され ている。この AlGaN電子供給層 113上には、ソース電極 101とドレイン電極 103とが オーム性接触しており、 AlGaN電子供給層 113の表面は SiN膜 121で覆われて ヽ る。  This example relates to an HJFET having the configuration shown in FIG. In this embodiment, the HJ FET 100 is formed on a substrate 110 such as SiC. A buffer layer 111 having a semiconductor layer force is formed on the substrate 110. A GaN channel layer 112 is formed on the buffer layer 111. On the GaN channel layer 112, an eight-and-one electron supply layer 113 is formed. On the AlGaN electron supply layer 113, the source electrode 101 and the drain electrode 103 are in ohmic contact, and the surface of the AlGaN electron supply layer 113 is covered with the SiN film 121.

[0049] 図 7〜図 9は、本実施例の HJFET100の製造方法を示す図である。  7 to 9 are diagrams showing a method for manufacturing the HJFET 100 of this example.

この製造方法は、以下の工程を含む。  This manufacturing method includes the following steps.

ステップ 101:ヘテロ接合を含む III族窒化物半導体層構造 (AlGaN電子供給層 11 3と GaNチャネル層 112との積層構造)を形成する工程、具体的には、基板 110上に 、ェピタキシャル成長法により GaNチャネル層 112および AlGaN電子供給層 113を 順次形成する工程、  Step 101: A process of forming a III-nitride semiconductor layer structure including a heterojunction (laminated structure of AlGaN electron supply layer 113 and GaN channel layer 112), specifically, an epitaxial growth method on the substrate 110 Sequentially forming a GaN channel layer 112 and an AlGaN electron supply layer 113 by

ステップ 103 :AlGaN電子供給層 113の表面が清浄な状態で保護膜 (SiN膜 121) を形成する工程、  Step 103: forming a protective film (SiN film 121) while the surface of the AlGaN electron supply layer 113 is clean,

ステップ 105: SiN膜 121の所定の領域をエッチングにより選択的に除去して開口部 を形成し、 AlGaN電子供給層 113と GaNチャネル層 112との積層構造上に、当該 開口部を埋め込むようにゲート電極 102を形成する工程、および  Step 105: A predetermined region of the SiN film 121 is selectively removed by etching to form an opening, and the gate is embedded on the stacked structure of the AlGaN electron supply layer 113 and the GaN channel layer 112. Forming electrode 102; and

ステップ 107 : SiN膜 121を形成する工程の後、 SiN膜 121の所定の領域をエツチン グにより選択的に除去し、 AlGaN電子供給層 113上に、除去された領域を埋め込む ようにソース電極 101とドレイン電極 103とを離間して形成する工程。  Step 107: After the step of forming the SiN film 121, a predetermined region of the SiN film 121 is selectively removed by etching, and the source electrode 101 and the AlGaN electron supply layer 113 are embedded so as to embed the removed region. Forming the drain electrode 103 apart from each other;

[0050] なお、ここでは、ステップ 105においてゲート電極 102を形成した後、ステップ 107 にてソース電極 101とドレイン電極 103とを形成する手順の場合を例示した力 ゲー ト電極 102、ソース電極 101およびドレイン電極 103の形成前に SiN膜 121が形成さ れる手順であれば、ステップ 105およびステップ 107のどちらを先に行ってもよい。た とえば各電極に用いる金属の種類等を考慮して、いずれのステップ力 行うかを決め ることがでさる。 Here, the force gate illustrated in the case of the procedure of forming the source electrode 101 and the drain electrode 103 in Step 107 after forming the gate electrode 102 in Step 105. As long as the SiN film 121 is formed before the formation of the first electrode 102, the source electrode 101, and the drain electrode 103, either Step 105 or Step 107 may be performed first. For example, it is possible to decide which step force to perform in consideration of the type of metal used for each electrode.

[0051] ステップ 103の SiN膜 121は、少なくともゲート電極 102の形成領域とドレイン電極 103の形成領域との間に形成される。  [0051] The SiN film 121 in step 103 is formed at least between the formation region of the gate electrode 102 and the formation region of the drain electrode 103.

[0052] 本実施例では、ステップ 101において、ェピタキシャル成長法により III族窒化物半 導体層構造を形成した後、成膜室から取り出すことなぐ清浄な雰囲気で、引き続き SiN膜 121を形成するステップ 103の工程を行っている。清浄な雰囲気とは、具体的 には実質的に酸素を含まない雰囲気である。こうすれば、八 &?^電子供給層113の 表面が途中で大気中に曝されることがな 、ので、 AlGaN電子供給層 113と SiN膜 1 21との界面における不純物濃度をさらに効果的に低減させ、電流コラブスをさらに効 果的に抑制可能な構成とすることができる。 In this embodiment, after forming the group III nitride semiconductor layer structure by the epitaxial growth method in step 101, the step of subsequently forming the SiN film 121 in a clean atmosphere that is not taken out from the film forming chamber. 103 processes are performed. Specifically, the clean atmosphere is an atmosphere substantially free of oxygen. In this way, eight &? ^ Do be exposed to the atmosphere the surface of the electron supply layer 113 is on the way, so further effectively an impurity concentration at the interface between the AlGaN electron supply layer 113 and the SiN film 1 21 Thus, the current collab can be more effectively suppressed.

[0053] なお、本明細書にぉ 、て、成膜室は、一つの室から構成されて!、てもよ 、し、複数 の小室を含んでいてもよい。複数の小室を含む成膜室を用いる場合、一つの AlGa N電子供給層 113を形成した後、真空解除による大気暴露をせずに基板 110を他の 小室に搬送し、 SiN膜 121の形成を行ってもよい。真空解除による大気暴露を行わ な!、ため、 AlGaN電子供給層 113の表面汚染を効果的に抑制することができる。  [0053] Note that, in the present specification, the film formation chamber is composed of a single chamber! Or may include a plurality of small chambers. In the case of using a film formation chamber including a plurality of chambers, after forming one AlGaN electron supply layer 113, the substrate 110 is transferred to another chamber without exposure to the atmosphere by releasing the vacuum, and the SiN film 121 is formed. You may go. Do not expose to the atmosphere by releasing the vacuum! Therefore, surface contamination of the AlGaN electron supply layer 113 can be effectively suppressed.

[0054] 以下、 HJFET100の製造工程をさらに具体的に説明する。  Hereinafter, the manufacturing process of the HJFET 100 will be described more specifically.

まず、図 7 (a)に示したように、 SiC力 なる基板 110上に、ェピタキシャル成長法を 用いて半導体を成長させて、基板 110側力も順に、アンドープ A1N力もなるバッファ 層 111 (膜厚 20nm)、アンドープの GaNチャネル層 112 (膜厚 2 μ m)、アンドープ Al GaN力もなる AlGaN電子供給層 113 (膜厚 25nm)が積層した半導体層構造を得る (図 7 (a) )。ェピタキシャル成長法として、たとえば、分子線ェピタキシ(Molecular Beam Epitaxy : MBE)成長法や有機金属気相ェピタキシ(Metal Organic Va por Phase Epitaxy : MOVPE)成長法を用いる。  First, as shown in FIG. 7 (a), a semiconductor layer is grown on a substrate 110 having SiC force by using an epitaxial growth method, and the buffer layer 111 (thickness of the substrate 110 side force and also undoped A1N force is sequentially formed. 20 nm), an undoped GaN channel layer 112 (thickness 2 μm), and an AlGaN electron supply layer 113 (thickness 25 nm) with undoped Al GaN force are obtained (FIG. 7 (a)). As the epitaxy growth method, for example, a molecular beam epitaxy (MBE) growth method or a metal organic vapor phase epitaxy (MOVPE) growth method is used.

[0055] そして、 AlGaN電子供給層 113上に SiN膜 121 (膜厚 60nm)を形成する(図 7 (b) )。このとき、 AlGaN電子供給層 113形成後、大気曝露せずに同一の成膜装置内で SiN膜 121を形成する。 SiN膜 121は、 AlGaN電子供給層 113および GaNチヤネ ル層 112の成長法と同一の成長法により形成される。 Then, a SiN film 121 (film thickness 60 nm) is formed on the AlGaN electron supply layer 113 (FIG. 7B). At this time, after the AlGaN electron supply layer 113 is formed, it is not exposed to the atmosphere in the same film forming apparatus. A SiN film 121 is formed. The SiN film 121 is formed by the same growth method as the growth method of the AlGaN electron supply layer 113 and the GaN channel layer 112.

[0056] つづいて、 SiN膜 121の一部を GaNチャネル層 112が露出するまでエッチング除 去することにより、素子間分離メサ (不図示)を形成する。そして、 SiN膜 121表面の 所定の領域にフォトレジストを形成し、 SiN膜 121の露出部を選択的にエッチング除 去して AlGaN電子供給層 113を露出させる(図 8 (c) )。  Subsequently, a part of the SiN film 121 is etched away until the GaN channel layer 112 is exposed, thereby forming an element isolation mesa (not shown). Then, a photoresist is formed in a predetermined region on the surface of the SiN film 121, and the exposed portion of the SiN film 121 is selectively etched away to expose the AlGaN electron supply layer 113 (FIG. 8 (c)).

[0057] そして、 AlGaN電子供給層 113上に、たとえば TiZAl等の金属を蒸着することに より、ソース電極 101およびドレイン電極 103を形成し(図 8 (d) )、 650°Cでァニール を行うことにより、 AlGaN電子供給層 113とオーム性接合させる。  [0057] Then, a source electrode 101 and a drain electrode 103 are formed on the AlGaN electron supply layer 113 by evaporating a metal such as TiZAl (FIG. 8 (d)), and annealing is performed at 650 ° C. Thus, the AlGaN electron supply layer 113 is ohmic-bonded.

[0058] 次いで、 SiN膜 121表面の所定の領域にフォトレジストを形成し、 SiN膜 121の露 出部を選択的にエッチング除去して、 AlGaN電子供給層 113の露出する開口部を 設ける(図 9 (e) )。露出した AlGaN電子供給層 113上に、たとえば NiZAuのゲート 金属を蒸着して、ショットキー接触のゲート電極 102を形成する(図 9 (f) )。以上の手 順により、図 1に示した HJFET100が得られる。  [0058] Next, a photoresist is formed in a predetermined region on the surface of the SiN film 121, and the exposed portion of the SiN film 121 is selectively removed by etching to provide an exposed portion of the AlGaN electron supply layer 113 (FIG. 9 (e)). On the exposed AlGaN electron supply layer 113, a gate metal of, for example, NiZAu is deposited to form a Schottky contact gate electrode 102 (FIG. 9 (f)). With the above procedure, the HJFET 100 shown in Fig. 1 is obtained.

[0059] 図 25および図 26は、本実施例の製造方法と従来の製造方法とを比較する図であ る。  FIG. 25 and FIG. 26 are diagrams for comparing the manufacturing method of this example with the conventional manufacturing method.

[0060] まず、図 25 (a)および図 25 (b)は、それぞれ、上述した本実施例の HJFET100の 製造方法と、従来の HJFET200 (図 28)の製造方法において、各々 10枚の 3インチ ゥエーハで得られた HJFETでのショットキー障壁高さ φ および理想化因子 nを示す  [0060] First, FIG. 25 (a) and FIG. 25 (b) show 10 3 inches each in the manufacturing method of the HJFET 100 of this embodiment and the manufacturing method of the conventional HJFET 200 (FIG. 28). Shows Schottky barrier height φ and idealization factor n in HJFET obtained in woofer

B  B

図である。  FIG.

[0061] 図 25 (a)および図 25 (b)からわかるように、本実施例の HJFET100では、理想的 なショットキー接合に近い優れたショットキー性が得られ、さらに、ゥエーハ間のばらつ きが抑制されて均一性が向上していることがわかる。これは、ゲート電極 102形成領 域における AlGaN電子供給層 113の表面力 ゲート電極 102の形成時まで大気や プラズマに曝されず、 AlGaN電子供給層 113表面が汚染されな 、ためと推察される  [0061] As can be seen from FIGS. 25 (a) and 25 (b), in the HJFET 100 of this example, an excellent Schottky property close to an ideal Schottky junction can be obtained, and the variation between wafers can be improved. It can be seen that cracks are suppressed and the uniformity is improved. This is presumably because the surface force of the AlGaN electron supply layer 113 in the region where the gate electrode 102 is formed is not exposed to the atmosphere or plasma until the gate electrode 102 is formed, and the surface of the AlGaN electron supply layer 113 is not contaminated.

[0062] また、図 26は、本実施例の作製方法と従来の作製方法において、各々 10枚の 3ィ ンチウエーハに素子を試作した時の電流コラブス量を示す図である。 [0063] 図 26に示した従来の作製方法で得られた電界効果トランジスタ 200では、ゲート電 極 202とドレイン電極 203と間に設けられる AlGaN電子供給層 213の表面は様々な 工程を経るため、その表面に誘起される負電荷の制御は困難であり、 SiN膜 221に よる保護膜を形成し電流コラブスの抑制を行っても、電流コラブスの低減の程度にば らつきが生じている。 [0062] FIG. 26 is a diagram showing the amount of current collabs when a device is prototyped on each of 10 3-inch wafers in the manufacturing method of this example and the conventional manufacturing method. In the field effect transistor 200 obtained by the conventional manufacturing method shown in FIG. 26, the surface of the AlGaN electron supply layer 213 provided between the gate electrode 202 and the drain electrode 203 undergoes various processes. It is difficult to control the negative charge induced on the surface, and even if a current film is suppressed by forming a protective film by the SiN film 221, there is a variation in the degree of current current reduction.

[0064] これに対し、本実施例の HJFET100では、電流コラプス量が少なぐかつ、そのば らつきが小さいことがわかる。本実施例においては、半導体層と同じ成長装置にて、 AlGaN電子供給層 113を形成後、大気やプラズマ中に暴露することなぐ引き続き S iN膜 121を成長させる。このため、ゲート電極 102の形成前に SiN膜 121が形成され 、半導体と SiN膜 121との界面はプロセスによる損傷を受けることなぐ均一で良質な 界面が形成されている。以上より、特に本発明の如く表面負電荷の影響が大きな問 題となって!/、る III族窒化物半導体素子では、この均一な界面形成と界面不純物濃 度が低 、ことによる電流コラブス低減と特性の均一性向上の効果は著 U、。  In contrast, in the HJFET 100 of this example, it can be seen that the amount of current collapse is small and the variation is small. In this embodiment, after the AlGaN electron supply layer 113 is formed using the same growth apparatus as the semiconductor layer, the SiN film 121 is continuously grown without being exposed to the atmosphere or plasma. Therefore, the SiN film 121 is formed before the gate electrode 102 is formed, and the interface between the semiconductor and the SiN film 121 is formed with a uniform and high-quality interface that is not damaged by the process. From the above, the influence of negative surface charge becomes a big problem, especially as in the present invention! / In the Group III nitride semiconductor device, the current interface is reduced due to this uniform interface formation and low interface impurity concentration. And the effect of improving the uniformity of characteristics is remarkable.

[0065] さらに、得られた HJFETにおいて、 SiN膜と AlGaN電子供給層との界面における AlGaN電子供給層中の酸素濃度を分析したところ、本実施例の HJFET100の場合 、 lE15atoms/cm3以下であった。 SiN膜 121の膜厚が 5〜200nm程度である場 合にっ 、て、このような不純物濃度を界面にぉ 、て有する AlGaN電子供給層 113 および SiN膜 121を形成することができた。 [0065] Further, in the obtained HJFET, when the oxygen concentration in the AlGaN electron supply layer at the interface between the SiN film and the AlGaN electron supply layer was analyzed, in the case of the HJFET 100 of this example, it was 1E15 atoms / cm 3 or less. It was. When the thickness of the SiN film 121 was about 5 to 200 nm, the AlGaN electron supply layer 113 and the SiN film 121 having such an impurity concentration at the interface could be formed.

[0066] これに対し、図 28〖こ示した HJFET200〖こついて、電極形成後、 SiN膜 221をプラ ズマ CVD法により形成した結果、 AlGaN電子供給層 213と SiN膜 221との界面に おける AlGaN電子供給層 213中の酸素濃度が IE 19atomsZcm3程度であつた。 [0066] On the other hand, as a result of forming the SiN film 221 by the plasma CVD method after forming the electrodes for the HJFET 200 shown in FIG. 28, AlGaN at the interface between the AlGaN electron supply layer 213 and the SiN film 221 is formed. The oxygen concentration in the electron supply layer 213 was about IE 19 atoms Zcm 3 .

[0067] また、 HJFET100の製造工程において、ェピタキシャル成長法により AlGaN電子 供給層 113を形成した後、 SiN膜 121を形成する前に大気暴露を行った場合、 SiN 膜 121と AlGaN電子供給層 113との界面における AlGaN電子供給層 113中の酸 素濃度が lE19atomsZcm3程度であった。 [0067] Further, in the manufacturing process of the HJFET 100, when the AlGaN electron supply layer 113 is formed by the epitaxial growth method and then exposed to the atmosphere before the SiN film 121 is formed, the SiN film 121 and the AlGaN electron supply layer 113 are formed. The oxygen concentration in the AlGaN electron supply layer 113 at the interface was about lE19 atoms Zcm 3 .

[0068] このように、本実施例の HJFET100においては、 AlGaN電子供給層 113形成後、 大気暴露することなく同じ成膜室内で SiN膜 121が形成されるため、 HJFET100は 、ショットキー性に優れるとともに、電流コラブスが抑制され、高出力で信頼性に優れ た構成を有する。また、 HJFET100は、ゥエーハ間のばらつきが抑制されているため 、設計通りの構造を高い歩留まりで安定的に製造可能な構成となっている。本実施 例の方法で HJFETを作製したところ、 AlGaN電子供給層 113と SiN膜 121との界面 における不純物濃度、ここでは酸素濃度が、 lE15atomsZcm3以下のトランジスタ が得られた。 As described above, in the HJFET 100 of this example, after the AlGaN electron supply layer 113 is formed, the SiN film 121 is formed in the same film formation chamber without being exposed to the atmosphere. Therefore, the HJFET 100 has excellent Schottky properties. In addition, current collabs are suppressed, high output and high reliability Have a configuration. In addition, since the variation between wafers is suppressed, the HJFET 100 has a structure capable of stably manufacturing a structure as designed with a high yield. When an HJFET was fabricated by the method of this example, a transistor having an impurity concentration at the interface between the AlGaN electron supply layer 113 and the SiN film 121, here an oxygen concentration of lE15 atoms Zcm 3 or less, was obtained.

[0069] また、本実施例では、保護膜として機能する SiN膜 121が、 ΠΙ族窒化物半導体層 である AlGaN電子供給層 113の構成元素である窒素を含むため、 AlGaN電子供給 層 113形成後、大気暴露することなく連続工程で SiN膜 121を形成することができる 。また、得られる SiN膜 121の膜質の安定性を向上させることができる。  [0069] In this example, since the SiN film 121 functioning as a protective film contains nitrogen, which is a constituent element of the AlGaN electron supply layer 113, which is a group III nitride semiconductor layer, after the formation of the AlGaN electron supply layer 113, The SiN film 121 can be formed in a continuous process without exposure to the atmosphere. Further, the stability of the film quality of the obtained SiN film 121 can be improved.

[0070] また、本実施例においては、ソース電極 101およびゲート電極 102が、保護膜であ る SiN膜 121上に乗り上げた構造になっているため、高電圧動作時において、ドレイ ン電極 103のゲート電極側端部での電界集中を緩和することができる。よって、ゲー ト耐圧が改善された構成となって!/、る。  In the present embodiment, the source electrode 101 and the gate electrode 102 have a structure that rides on the SiN film 121 that is a protective film, so that the drain electrode 103 is not damaged during high-voltage operation. Electric field concentration at the gate electrode side end can be alleviated. Therefore, the gate breakdown voltage is improved! /.

[0071] (実施例 2)  [0071] (Example 2)

図 2は、本実施例の HJFETの構成を示す断面図である。図 2に示した HJFET130 の基本構成は実施例 1の HJFET100 (図 1)と同様、基板 110上に、バッファ層 111 、 GaNチャネル層 112、 AlGaN電子供給層 113および SiN膜 121が基板 110側か らこの順に積層され、 AlGaN電子供給層 113上に、ソース電極 101、ドレイン電極 1 03およびゲート電極 102が設けられた構成である力 AlGaN電子供給層 113と SiN 膜 121との界面の清浄度を保つ方法が実施例 1と異なる。  FIG. 2 is a cross-sectional view showing the configuration of the HJFET of this example. The basic configuration of the HJFET 130 shown in FIG. 2 is the same as the HJFET 100 (FIG. 1) of the first embodiment. On the substrate 110, the buffer layer 111, the GaN channel layer 112, the AlGaN electron supply layer 113, and the SiN film 121 are on the substrate 110 side. In this order, the structure is such that the source electrode 101, the drain electrode 103, and the gate electrode 102 are provided on the AlGaN electron supply layer 113, and the cleanliness of the interface between the AlGaN electron supply layer 113 and the SiN film 121 is increased. The method of maintaining is different from Example 1.

[0072] このような HJFET130は、以下の手順で製造される。  [0072] Such an HJFET 130 is manufactured by the following procedure.

図 10〜図 13は、本実施例における HJFETの製造方法を示す図である。実施例 1 では、 ΠΙ族窒化物半導体層構造を形成する工程の後、汚染雰囲気 (たとえば大気) に曝露せずに SiNを成膜したが、本実施例の製造方法は、 III族窒化物半導体層構 造を形成する工程の後、 III族窒化物半導体層構造を汚染雰囲気に曝す場合を考 慮したものである。本実施例においては、 ΠΙ族窒化物半導体層構造の表面で界面 準位を形成する不純物を除去するために SiN膜 121を形成する工程の前に、 ステップ 109 :酸を用いたウエットエッチングにより、 III族窒化物半導体層構造の表面 を洗浄する工程、 10 to 13 are diagrams showing a method for manufacturing the HJFET in this example. In Example 1, after the step of forming the group III nitride semiconductor layer structure, the SiN film was formed without being exposed to the contaminated atmosphere (for example, air). However, the manufacturing method of this example is based on the group III nitride semiconductor. This is a case where the group III nitride semiconductor layer structure is exposed to a contaminated atmosphere after the step of forming the layer structure. In this embodiment, before the step of forming the SiN film 121 in order to remove impurities that form interface states on the surface of the group III nitride semiconductor layer structure, step 109: wet etching using an acid, Surface of III-nitride semiconductor layer structure Cleaning process,

を含んでいる。  Is included.

[0073] まず、 SiCからなる基板 110上にたとえば分子線ェピタキシ(Molecular Beam [0073] First, for example, molecular beam epitaxy (Molecular Beam) is formed on a substrate 110 made of SiC.

Epitaxy : MBE)成長法や有機金属気相ェピタキシ(Metal Organic Vapor Ph ase Epitaxy : MOVPE)成長法等によって半導体を成長させる。このようにして、基 板 110側から順に、アンドープ A1N力 なるバッファ層 111 (膜厚 20nm)、アンドープ の GaNチャネル層 112 (膜厚 2 μ m)、アンドープ AlGaNからなる AlGaN電子供給 層 113 (膜厚 25nm)が積層した半導体層構造が得られる(図 10 (a) )。 Semiconductors are grown by epitaxy (MBE) growth method or metal organic vapor phase epitaxy (MOVPE) growth method. Thus, in order from the substrate 110 side, an undoped A1N force buffer layer 111 (film thickness 20 nm), an undoped GaN channel layer 112 (film thickness 2 μm), and an undoped AlGaN AlGaN electron supply layer 113 (film) A semiconductor layer structure with a thickness of 25 nm) is obtained (Fig. 10 (a)).

[0074] 次いで、 AlGaN電子供給層 113の表面が大気等により汚染される場合は、 AlGa N電子供給層 113上を酸等によりウエットエッチングして半導体層表面を清浄ィ匕した 後(図 10 (b) )、清浄な雰囲気でプラズマ CVD法等により SiN膜 121 (60nm)を形成 する(図 l l (c) )。具体的には、酸としてフッ酸または塩酸を用い、たとえば室温中で 30秒〜 1分程度エッチングした後、水洗し、乾燥する。  [0074] Next, when the surface of the AlGaN electron supply layer 113 is contaminated by the air or the like, the surface of the semiconductor layer is cleaned by wet etching on the AlGaN electron supply layer 113 with an acid or the like (FIG. 10 ( b)) SiN film 121 (60 nm) is formed by a plasma CVD method etc. in a clean atmosphere (Fig. ll (c)). Specifically, hydrofluoric acid or hydrochloric acid is used as the acid. For example, etching is performed at room temperature for about 30 seconds to 1 minute, followed by washing with water and drying.

[0075] 図 10 (b)における清浄ィ匕の処理により、 AlGaN電子供給層 113が大気等に曝され ていた場合にも、その表面を洗浄し、完成した HJFET130において、 AlGaN電子供 給層 113と SiN膜 121との界面における不純物の濃度を lE17atomsZcm3以下と することができる。 [0075] Even if the AlGaN electron supply layer 113 was exposed to the atmosphere or the like by the cleaning process in Fig. 10 (b), the surface was cleaned, and in the completed HJFET 130, the AlGaN electron supply layer 113 The impurity concentration at the interface between the SiN film 121 and the SiN film 121 can be set to lE17 atoms Zcm 3 or less.

[0076] 続いて、 GaNチャネル層 112が露出するまで、 SiN膜 121の一部とェピタキシャル 層構造の一部をエッチング除去することにより、素子間分離メサ (不図示)を形成する 。そして、 SiN膜 121表面の所定の領域にフォトレジストを形成し、 SiN膜 121の露出 部を選択的にエッチング除去して AlGaN電子供給層 113を露出させ(図 11 (d) )、 露出した AlGaN電子供給層 113上に、たとえば TiZAl等の金属を蒸着することによ り、ソース電極 101およびドレイン電極 103を形成する(図 12 (e) )。そして、 650°Cで ァニールを行うことにより、 AlGaN電子供給層 113とオーム性接合させる。 SiN膜 12 1表面の所定の領域にフォトレジストを形成し、 SiN膜 121の露出部を選択的にエツ チング除去し、 AlGaN電子供給層 113の露出する開口部を設ける(図 12 (f) )。露出 した AlGaN電子供給層 113上にたとえば NiZAuのゲート金属を蒸着して、ショット キー接触のゲート電極 102を形成する(図 13)。以上により、図 2に示した HJFET13 0が得られる。 Subsequently, an element isolation mesa (not shown) is formed by etching away a part of the SiN film 121 and a part of the epitaxial layer structure until the GaN channel layer 112 is exposed. Then, a photoresist is formed in a predetermined region on the surface of the SiN film 121, and the exposed portion of the SiN film 121 is selectively etched away to expose the AlGaN electron supply layer 113 (FIG. 11 (d)). A source electrode 101 and a drain electrode 103 are formed on the electron supply layer 113 by evaporating a metal such as TiZAl (FIG. 12E). Then, annealing is performed at 650 ° C. to form ohmic contact with the AlGaN electron supply layer 113. A photoresist is formed in a predetermined region on the surface of the SiN film 12 1, and the exposed portion of the SiN film 121 is selectively etched away to provide an opening to expose the AlGaN electron supply layer 113 (FIG. 12 (f)) . On the exposed AlGaN electron supply layer 113, a gate metal such as NiZAu is deposited to form a Schottky contact gate electrode 102 (FIG. 13). As a result, the HJFET13 shown in Fig. 2 0 is obtained.

[0077] 本実施例においては、電極構造を形成する前に、半導体表面を酸等でエッチング することにより清浄ィ匕している(図 10 (b) )。なお、酸による清浄化処理により、その後 の表面の酸ィ匕を抑制するように終端させることもできる。また、酸等により AlGaN電子 供給層 113の表面をエッチングした後、 SiN膜 121を成膜するまでの間に、 AlGaN 電子供給層 113にわずかに汚染が生じた場合にも、プラズマ CVD法により SiN膜 1 21を成膜すれば、プラズマ照射により汚染物を除去することができる。  In this example, before the electrode structure is formed, the semiconductor surface is cleaned by etching with an acid or the like (FIG. 10B). In addition, it can also be terminated so as to suppress subsequent oxidation of the surface by the cleaning treatment with acid. Even if the AlGaN electron supply layer 113 is slightly contaminated after the surface of the AlGaN electron supply layer 113 is etched with acid or the like and before the SiN film 121 is formed, the SiN film is formed by plasma CVD. When the film 121 is formed, contaminants can be removed by plasma irradiation.

[0078] このように、本実施例では、 AlGaN電子供給層 113の清浄ィ匕表面に SiN膜 121が 形成されるため、表面負電荷の影響が大きな問題となっている ΠΙ族窒化物半導体素 子における電流コラブスが抑制される。  As described above, in this example, since the SiN film 121 is formed on the surface of the AlGaN electron supply layer 113, the influence of the negative surface charge is a serious problem. Current collab in the child is suppressed.

[0079] また、本実施例では、ゲート電極 102の形成前にー且大気に曝された AlGaN電子 供給層 113の大気等で汚染された箇所がエッチングにより除去されている。また、ゲ ート電極 102およびドレイン電極 103の形成時に、 AlGaN電子供給層 113上に SiN 膜 121が形成されて!ヽるため、電極形成時に AlGaN電子供給層 113の表面がブラ ズマに曝されることがない。よって、その後の製造工程で AlGaN電子供給層 113上 にフォトレジストが形成されたり、 AlGaN電子供給層 113がプラズマに侵されることな ぐ理想的に近いショットキー性を有するゲート電極 102が得られる。また、清浄化処 理をしているため、ゲート電極 102とドレイン電極 103との間の領域における AlGaN 電子供給層 113の表面の結晶状態が良好で均一であり、表面状態の安定ィ匕が可能 である。このため、優れたショットキー性を有するとともに、高歩留まりで安定的に製造 可能な構成とすることができる。本実施例の方法で HJFETを作製したところ、 AlGa N電子供給層 113と SiN膜 121との界面における不純物濃度、ここでは酸素濃度が 、 lE17atomsZcm3以下のトランジスタが得られた。 Further, in this example, the portion of the AlGaN electron supply layer 113 that was exposed to the atmosphere before the formation of the gate electrode 102 and was contaminated with the atmosphere was removed by etching. In addition, since the SiN film 121 is formed on the AlGaN electron supply layer 113 when the gate electrode 102 and the drain electrode 103 are formed, the surface of the AlGaN electron supply layer 113 is exposed to plasma at the time of electrode formation. There is nothing to do. Therefore, in the subsequent manufacturing process, a photoresist is formed on the AlGaN electron supply layer 113, and the gate electrode 102 having a nearly ideal Schottky property is obtained without the AlGaN electron supply layer 113 being attacked by plasma. In addition, since the cleaning process is performed, the crystal state of the surface of the AlGaN electron supply layer 113 in the region between the gate electrode 102 and the drain electrode 103 is good and uniform, and the surface state can be stabilized. It is. For this reason, it is possible to obtain a configuration that has excellent Schottky properties and can be stably manufactured at a high yield. When an HJFET was fabricated by the method of this example, a transistor having an impurity concentration at the interface between the AlGaN electron supply layer 113 and the SiN film 121, here an oxygen concentration of lE17 atoms Zcm 3 or less, was obtained.

[0080] また、本実施例においても、実施例 1の場合と同様に、ソース電極 101およびゲート 電極 102が SiN膜 121上に乗り上げた構造になっているため、高電圧動作時におい てドレイン電極のゲート電極側端部での電界集中の緩和が起き、ゲート耐圧が改善 された素子の作製が可能である。  [0080] Also in this embodiment, as in the case of Embodiment 1, the source electrode 101 and the gate electrode 102 are structured on the SiN film 121, so that the drain electrode can be used during high-voltage operation. This makes it possible to produce a device with improved gate breakdown voltage due to relaxation of the electric field concentration at the end of the gate electrode.

[0081] (実施例 3) 図 3は、本実施例の HJFETの断面構造を示す図である。 [Example 3] FIG. 3 is a diagram showing a cross-sectional structure of the HJFET of this example.

図 3に示した HJFET132の基本構成は、実施例 1または実施例 2の HJFETと同様 であるが、保護膜が、第一の絶縁膜 (SiN膜 121)と、 SiN膜 121上に積層された第 二の絶縁膜 (SiO膜 122)と、力 構成される点が異なる。ここでは、 SiO膜 122が Si  The basic configuration of the HJFET 132 shown in FIG. 3 is the same as that of the HJFET of Example 1 or Example 2, but a protective film is stacked on the first insulating film (SiN film 121) and the SiN film 121. It differs from the second insulating film (SiO film 122) in that the force is configured. Here, SiO film 122 is Si

2 2  twenty two

N膜 121に直接接して設けられているが、第一の絶縁膜と第二の絶縁膜との間に、 介在層としてさらに別の絶縁膜が設けられていてもよい。  Although provided in direct contact with the N film 121, another insulating film may be provided as an intervening layer between the first insulating film and the second insulating film.

[0082] さらに具体的には、 HJFET132は、 SiC等の基板 110上に形成される。基板 110 上には半導体層からなるバッファ層 111が形成されて 、る。このバッファ層 111上に GaNチャネル層 112が形成されている。 GaNチャネル層 112の上には、 AlGaN電 子供給層 113が形成されている。この AlGaN電子供給層 113上には、ソース電極 1 01およびドレイン電極 103がオーム性接合されており、 AlGaN電子供給層 113の表 面は SiN膜 121で覆われ、さらにその SiN膜 121は SiO膜 122で覆われている。 More specifically, the HJFET 132 is formed on a substrate 110 such as SiC. A buffer layer 111 made of a semiconductor layer is formed on the substrate 110. A GaN channel layer 112 is formed on the buffer layer 111. On the GaN channel layer 112, an AlGaN electron supply layer 113 is formed. A source electrode 101 and a drain electrode 103 are ohmic-bonded on the AlGaN electron supply layer 113, and the surface of the AlGaN electron supply layer 113 is covered with a SiN film 121. Covered with 122.

2  2

[0083] 図 14〜図 17は、図 3に示した HJFETの製造方法を示す図である。  14 to 17 are diagrams showing a method for manufacturing the HJFET shown in FIG.

まず、 SiC力もなる基板 110上にたとえば MBE成長法や有機金属気相ェピタキシ MOVPE成長法等によって半導体を成長させる。このようにして、基板 110側から順 に、アンドープ A1Nからなるバッファ層 111 (膜厚 20nm)、アンドープの GaNチヤネ ル層 112 (膜厚 2 μ m)、アンドープ AlGaNからなる AlGaN電子供給層 113 (膜厚 25 nm)が積層した半導体層構造が得られる(図 14 (a) )。  First, a semiconductor is grown on the substrate 110 having SiC force by, for example, MBE growth method, metal organic vapor phase epitaxy MOVPE growth method, or the like. In this way, in order from the substrate 110 side, the buffer layer 111 (thickness 20 nm) made of undoped A1N, the undoped GaN channel layer 112 (thickness 2 μm), and the AlGaN electron supply layer 113 made of undoped AlGaN ( A semiconductor layer structure with a thickness of 25 nm) is obtained (Fig. 14 (a)).

[0084] 次いで、実施例 1と同様に、大気暴露を行わずに引き続き AlGaN電子供給層 113 上に、プラズマ CVD法等により SiN膜 121 (60nm)を形成する(図 14 (b) )。なお、 A IGaN電子供給層 113が大気に曝された場合は、実施例 2と同様に、酸等によりエツ チングを施し、半導体層表面を清浄ィ匕した後に SiN膜 121を形成する。  Next, as in Example 1, a SiN film 121 (60 nm) is subsequently formed on the AlGaN electron supply layer 113 by plasma CVD or the like without exposure to the atmosphere (FIG. 14 (b)). When the A IGaN electron supply layer 113 is exposed to the atmosphere, etching is performed with an acid or the like to clean the surface of the semiconductor layer, and the SiN film 121 is formed as in the second embodiment.

[0085] そして、 SiN膜 121上に常圧 CVD法等により SiO膜 122 (100nm)を形成する(図  Then, a SiO film 122 (100 nm) is formed on the SiN film 121 by an atmospheric pressure CVD method or the like (see FIG.

2  2

15 (c) ) 0 15 (c)) 0

[0086] その後、 SiN膜 121および SiO膜 122の一部とェピタキシャル層構造の一部を Ga  [0086] After that, a part of the SiN film 121 and the SiO film 122 and a part of the epitaxial layer structure were removed by Ga.

2  2

Nチャネル層 112が露出するまでエッチング除去することにより、素子間分離メサ(不 図示)を形成する。そして、 SiO膜 122表面の所定の領域にフォトレジストを形成し、  An element isolation mesa (not shown) is formed by etching until the N channel layer 112 is exposed. Then, a photoresist is formed in a predetermined region on the surface of the SiO film 122,

2  2

SiN膜 121および SiO膜 122の所定の領域を AlGaN電子供給層 113が露出するま で選択的にエッチング除去し(図 15 (d) )、 AlGaN電子供給層 113上に、たとえば Ti ZA1金属を蒸着することにより、ソース電極 101およびドレイン電極 103を形成し(図 16 (e) )、 650°Cでァニールを行うことによりオーム性接合を形成する。 The predetermined regions of the SiN film 121 and the SiO film 122 are exposed until the AlGaN electron supply layer 113 is exposed. Then, the source electrode 101 and the drain electrode 103 are formed on the AlGaN electron supply layer 113 by evaporating, for example, Ti ZA1 metal (FIG. 16 (e)). An ohmic bond is formed by annealing at 650 ° C.

[0087] つづいて、 SiO膜 122表面の所定の領域にフォトレジストを形成し、 SiN膜 121お [0087] Subsequently, a photoresist is formed in a predetermined region on the surface of the SiO film 122, and the SiN film 121 is formed.

2  2

よび SiO膜 122の所定の領域を選択的にエッチング除去することによって、 AlGaN And by selectively etching away a predetermined region of the SiO film 122, AlGaN

2 2

電子供給層 113の露出する開口部を設ける(図 16 (f) )。露出した AlGaN電子供給 層 113上にたとえば NiZAuのゲート金属を蒸着して、ショットキー接合されたゲート 電極 102を形成する(図 17)。以上により、図 3に示した HJFET132が得られる。  An exposed opening of the electron supply layer 113 is provided (FIG. 16 (f)). On the exposed AlGaN electron supply layer 113, for example, a NiZAu gate metal is deposited to form a Schottky-junction gate electrode 102 (FIG. 17). As a result, the HJFET 132 shown in FIG. 3 is obtained.

[0088] 本実施例にお!、ても、電極構造の形成前に大気暴露を行わな!/ヽか、または、 AlGa N電子供給層 113の表面を酸等により洗浄する方法を採用することにより、 AlGaN 電子供給層 113と SiN膜 121との界面が清浄な状態に保たれている。このため、実 施例 1または実施例 2と同様の効果が得られる。  [0088] In this embodiment, however, do not expose to the atmosphere before forming the electrode structure! Or use a method of cleaning the surface of the AlGa N electron supply layer 113 with an acid or the like. Thus, the interface between the AlGaN electron supply layer 113 and the SiN film 121 is kept clean. For this reason, the same effect as in Example 1 or Example 2 can be obtained.

[0089] さらに、本実施例では、 III族窒化物半導体層の表面に形成された SiN膜 121を Si O膜 122で覆う構成になっているため、 SiN膜 121の経時劣化をさらに確実に抑制 Furthermore, in this example, since the SiN film 121 formed on the surface of the group III nitride semiconductor layer is covered with the SiO 2 film 122, the deterioration with time of the SiN film 121 is further reliably suppressed.

2 2

することができる。よって、素子特性の長寿命化を図ることができる。  can do. Therefore, the lifetime of element characteristics can be extended.

[0090] なお、 SiO膜 122は、 SiN膜 121と同じ成膜装置を用いて形成してもよいし、異な Note that the SiO film 122 may be formed using the same film forming apparatus as the SiN film 121, or may be different.

2  2

る成膜装置を用いて形成してもよい。また、 SiO膜 122の平面形状は、 SiN膜 121と  The film forming apparatus may be used. The planar shape of the SiO film 122 is the same as that of the SiN film 121.

2  2

同じでも異なる構成でもよい。また、ゲート電極 102とドレイン電極 103との間の領域 にお!/、て、 AlGaN電子供給層 113の上部の SiN膜 121を介してフィールドプレート 部 105が形成されていてもよい。この構成については、実施例 4および実施例 5にて 後述する。  The same or different configurations may be used. In addition, a field plate portion 105 may be formed in a region between the gate electrode 102 and the drain electrode 103 via a SiN film 121 above the AlGaN electron supply layer 113. This configuration will be described later in Example 4 and Example 5.

[0091] (実施例 4) [0091] (Example 4)

図 4は、本実施例の HJFETの構成を示す断面図である。  FIG. 4 is a cross-sectional view showing the configuration of the HJFET of this example.

図 4に示した HJFET134の基本構成は、実施例 1の HJFET100と同様であるが、 ゲート電極 102が、ドレイン電極 103側に庇状に張り出して SiN膜 121の上部に形成 されたフィールドプレート部 105を有する点が HJFET100と異なる。  The basic configuration of the HJFET 134 shown in FIG. 4 is the same as that of the HJFET 100 of Example 1, except that the gate electrode 102 protrudes in a bowl shape on the drain electrode 103 side and is formed on the SiN film 121. Is different from HJFET100.

[0092] HJFET134は、 SiC等の基板 110上に形成される。基板 110上には半導体層から なるバッファ層 111が形成されて 、る。このバッファ層 111上に GaNチャネル層 112 が形成されている。 GaNチャネル層 112の上には、八10&?^電子供給層113が形成 されている。この八 &?^電子供給層113上に、ソース電極 101およびドレイン電極 1 03がオーム性接合されている。これらの電極の間に、ゲート電極 102が設けられてい る。ゲート電極 102は、フィールドプレート部 105を有し、八 &?^電子供給層113とシ ヨットキー接合して 、る。 AlGaN電子供給層 113の表面は SiN膜 121で覆われて ヽ る。 [0092] The HJFET 134 is formed on a substrate 110 such as SiC. A buffer layer 111 made of a semiconductor layer is formed on the substrate 110. On this buffer layer 111, a GaN channel layer 112 Is formed. On the GaN channel layer 112, an eight-and-a-half electron supply layer 113 is formed. On the eight &? ^ Electron supply layer 113, the source electrode 101 and the drain electrode 103 are joined in ohmic contact. A gate electrode 102 is provided between these electrodes. The gate electrode 102 has a field plate portion 105 and is joined to the eight &? ^ Electron supply layer 113 in a Siykey key junction. The surface of the AlGaN electron supply layer 113 is covered with the SiN film 121.

[0093] フィールドプレート部 105のゲート長方向の長さは、たとえば 0. 3 μ m以上、好まし くは 0. 以上とする。こうすることにより、さらに確実に電流コラブスを抑制できる 。また、フィールドプレート部 105力 ドレイン電極 103とオーバーラップしない構成と し、好ましくは、フィールドプレート部 105のゲート長方向の長さを、ゲート電極とドレ イン電極との間隔の 70%以下とする。フィールドプレート部 105の延出部の長さが大 きいほど電流コラブス抑制の効果は高いが、フィールドプレート部 105が長すぎると、 フィールドプレート部 105とドレイン電極 103との間の電界集中により、ゲート耐圧が 低下する。なお、ゲート電極 102とドレイン電極 103との間隔とは、ゲート電極 102の ドレイン電極側端部からドレイン電極 103のゲート電極側端部までの長さを指す。  [0093] The length of the field plate portion 105 in the gate length direction is, for example, 0.3 µm or more, preferably 0. 0 or more. In this way, current collab can be more reliably suppressed. The field plate portion 105 is configured so as not to overlap the drain electrode 103, and preferably the length of the field plate portion 105 in the gate length direction is 70% or less of the distance between the gate electrode and the drain electrode. The greater the length of the extension of the field plate portion 105, the greater the effect of suppressing current collabs. The withstand voltage decreases. Note that the distance between the gate electrode 102 and the drain electrode 103 refers to the length from the drain electrode side end of the gate electrode 102 to the gate electrode side end of the drain electrode 103.

[0094] 図 18〜図 20は、図 4の HJFETの製造方法を示す図である。  18 to 20 are views showing a method for manufacturing the HJFET of FIG.

まず、 SiCからなる基板 110上に、たとえば MBE成長法や MOCVD成長法等によ つて半導体を成長させる。このようにして、基板 110側力も順に、アンドープ A1Nから なるバッファ層 111 (膜厚 20nm)、アンドープの GaNチャネル層 112 (膜厚 2 μ m)、 アンドープ AlGaN力もなる AlGaN電子供給層 113 (膜厚 25nm)が積層した半導体 層構造が得られる(図 18 (a) )。  First, a semiconductor is grown on a substrate 110 made of SiC by, for example, MBE growth method or MOCVD growth method. In this way, the buffer 110 side force in the order of the substrate 110 is also an undoped A1N buffer layer 111 (film thickness 20 nm), an undoped GaN channel layer 112 (film thickness 2 μm), and an undoped AlGaN force AlGaN electron supply layer 113 (film thickness) A semiconductor layer structure in which 25 nm) is stacked is obtained (Fig. 18 (a)).

[0095] 次いで、実施例 1と同様に、大気暴露を行わずに引き続き AlGaN電子供給層 113 上に、プラズマ CVD法等により SiN膜 121 (60nm)を形成する(図 18 (b) )。なお、 A IGaN電子供給層 113が大気に曝された場合は、実施例 2と同様に、酸等によりエツ チングを施し、半導体層表面を清浄ィ匕した後に SiN膜 121を形成する。  Next, similarly to Example 1, a SiN film 121 (60 nm) is subsequently formed on the AlGaN electron supply layer 113 by plasma CVD or the like without exposure to the atmosphere (FIG. 18B). When the A IGaN electron supply layer 113 is exposed to the atmosphere, etching is performed with an acid or the like to clean the surface of the semiconductor layer, and the SiN film 121 is formed as in the second embodiment.

[0096] 続いて、 SiN膜 121の一部とェピタキシャル層構造の一部を GaNチャネル層 112 が露出するまでエッチング除去することにより、素子間分離メサ (不図示)を形成する 。そして、 SiN膜 121の所定の領域にフォトレジストを形成し、 SiN膜 121の露出部を AlGaN電子供給層 113が露出するまで選択的にエッチング除去する(図 19 (c) )。 露出した AlGaN電子供給層 113上に、たとえば TiZAl等の金属を蒸着して、ソース 電極 101およびドレイン電極 103を形成し(図 19 (d) )、 650°Cでァニールを行うこと により、これらの電極と AlGaN電子供給層 113とをオーム性接合させる。 SiN膜 121 の所定の領域にフォトレジストを形成し、 SiN膜 121の露出部を選択的にエッチング 除去して開口部を設け、 AlGaN電子供給層 113を露出させる(図 20 (e) )。 Subsequently, part of the SiN film 121 and part of the epitaxial layer structure are etched away until the GaN channel layer 112 is exposed, thereby forming an element isolation mesa (not shown). Then, a photoresist is formed in a predetermined region of the SiN film 121, and the exposed portion of the SiN film 121 is removed. Etching is selectively removed until the AlGaN electron supply layer 113 is exposed (FIG. 19 (c)). A metal such as TiZAl is deposited on the exposed AlGaN electron supply layer 113 to form the source electrode 101 and the drain electrode 103 (Fig. 19 (d)), and annealing is performed at 650 ° C. The electrode and the AlGaN electron supply layer 113 are joined in ohmic contact. A photoresist is formed in a predetermined region of the SiN film 121, and an exposed portion of the SiN film 121 is selectively removed by etching to provide an opening to expose the AlGaN electron supply layer 113 (FIG. 20 (e)).

[0097] そして、露出した AlGaN電子供給層 113上に、ゲート電極 102となる金属膜として 、たとえば NiZAuを蒸着して、ショットキー接触のゲート電極 102を形成する(図 20 ( f) ) 0またこれと同時に、 NiZAuよりなるフィールドプレート部 105をゲート電極 102と 連続一体に形成する。以上により、図 4に示した HJFET134が得られる。 Then, for example, NiZAu is vapor-deposited on the exposed AlGaN electron supply layer 113 as a metal film to be the gate electrode 102 to form the Schottky contact gate electrode 102 (FIG. 20 (f)) 0 or At the same time, a field plate portion 105 made of NiZAu is formed integrally with the gate electrode 102. As a result, the HJFET 134 shown in FIG. 4 is obtained.

[0098] なお、本実施例ではゲート電極 102とフィールドプレート部 105を同時に形成する 例を示したが、これらを別々の工程で行ってもよい。所定の位置に開口部が設けられ たレジストを SiN膜 121上に形成し、開口部を埋め込むようにフィールドプレート部 10 5を形成することもできる。この場合、ゲート電極 102とフィールドプレート部 105との 間隔をより狭い間隔で形成できる。  Note that although an example in which the gate electrode 102 and the field plate portion 105 are formed at the same time has been described in this embodiment, these may be performed in separate steps. It is also possible to form a resist having an opening at a predetermined position on the SiN film 121 and form the field plate portion 105 so as to fill the opening. In this case, the gap between the gate electrode 102 and the field plate portion 105 can be formed with a narrower gap.

[0099] 本実施例にお!、ても、電極構造の形成前に大気暴露を行わな!/ヽか、または、 AlGa N電子供給層 113の表面を酸等により洗浄する方法を採用することにより、 AlGaN 電子供給層 113と SiN膜 121との界面が清浄な状態に保たれている。このため、実 施例 1または実施例 2と同様の効果が得られる。  [0099] In this embodiment, however, exposure to the atmosphere is not performed before the formation of the electrode structure! / Alternatively, a method of cleaning the surface of the AlGa N electron supply layer 113 with an acid or the like should be employed. Thus, the interface between the AlGaN electron supply layer 113 and the SiN film 121 is kept clean. For this reason, the same effect as in Example 1 or Example 2 can be obtained.

[0100] さらに、 HJFET134は、フィールドプレート部 105を有する。このため、ゲート電極 1 02とドレイン電極 103の間に高い逆方向電圧が力かった場合にも、ゲート電極 102 のドレイン電極側端部に力かる電界力 フィールドプレート部 105の働きにより緩和さ れる。よって、ゲート電極 102のドレイン電極側端部における電界集中をさらに確実 に抑制し、ゲート耐圧を向上させることができる。さらに、大信号動作時には、表面電 位をフィールドプレート部 105によって変調できるため、表面トラップの応答速度を速 めて電流コラブスを抑制する効果がある。したがって、本発明によれば、電流コラブス 、ゲート耐圧および利得のバランスを顕著に改善できる。また、製造プロセス上のばら つきにより表面状態が変動した場合でも、こうした良好な性能を安定して実現すること ができる。 Further, the HJFET 134 has a field plate portion 105. Therefore, even when a high reverse voltage is applied between the gate electrode 102 and the drain electrode 103, the electric field force applied to the drain electrode side end of the gate electrode 102 is mitigated by the action of the field plate portion 105. . Therefore, the electric field concentration at the drain electrode side end of the gate electrode 102 can be further reliably suppressed, and the gate breakdown voltage can be improved. Furthermore, since the surface potential can be modulated by the field plate portion 105 during a large signal operation, the response speed of the surface trap can be increased and the current collab can be suppressed. Therefore, according to the present invention, the balance of current collabs, gate breakdown voltage, and gain can be remarkably improved. In addition, even if the surface condition fluctuates due to variations in the manufacturing process, such good performance should be realized stably. Can do.

[0101] なお、以上においては、ゲート電極 102と同じ部材カも構成されるとともに電界制御 部として機能するフィールドプレート部 105が設けられた場合を例に説明した力 電 界制御部がゲート電極と連続一体である構成には限られず、ゲート電極 102と前記ド レイン電極 103との間の領域において、 III族窒化物半導体層構造の上部に SiN膜 1 21を介してゲート電極 102と独立に電界制御電極が設けられた構成とすることもでき る。  [0101] In the above description, the force electric field control unit described as an example in which the same member member as the gate electrode 102 is configured and the field plate unit 105 functioning as an electric field control unit is provided is the gate electrode In the region between the gate electrode 102 and the drain electrode 103, the electric field is independent of the gate electrode 102 via the SiN film 121 above the group III nitride semiconductor layer structure in the region between the gate electrode 102 and the drain electrode 103. A configuration in which a control electrode is provided may be employed.

[0102] 図 27は、このような HJFETの構成を示す断面図である。図 27においては、フィー ルドプレート部 105を有するゲート電極 102にかえて、ゲート電極 102と、ゲート電極 102から離隔して設けられた電界制御電極 106とを有する。  FIG. 27 is a cross-sectional view showing the configuration of such an HJFET. In FIG. 27, instead of the gate electrode 102 having the field plate portion 105, a gate electrode 102 and an electric field control electrode 106 provided apart from the gate electrode 102 are provided.

[0103] なお、電界制御電極 106はゲート電極 102と同時に形成してもよいし、別工程で形 成してもよい。別工程とする場合、所定の位置に開口部が設けられたレジストを SiN 膜 121上に形成し、開口部を埋め込むように電界制御電極 106を形成することもでき る。この場合、ゲート電極 102と電界制御電極 106との間隔をより狭い間隔で形成で きる。  Note that the electric field control electrode 106 may be formed at the same time as the gate electrode 102 or may be formed in a separate process. In another process, a resist having an opening at a predetermined position is formed on the SiN film 121, and the electric field control electrode 106 can be formed so as to fill the opening. In this case, the gap between the gate electrode 102 and the electric field control electrode 106 can be formed with a narrower gap.

[0104] また、図 27において、電界制御電極 106が、ゲート電極 102に対して独立に制御 可能であってもよぐ電界制御電極 106およびゲート電極 102に対して互いに異なる 電位を付与することもできる。こうした構成とすることにより、電界効果トランジスタを最 適な条件で駆動することが可能である。そして、表面電位を固定することにより、表面 トラップの応答を抑止できるため、電界制御電極 106をゲート電極 102と同電位とし、 表面電位を変調した場合よりも、さらに効果的に電流コラブスを抑制できる。特に、表 面負電荷の影響が大きな問題となる ΠΙ族窒化物半導体素子では、この電界制御電 極 106を独立に制御できることの効果は著しい。  [0104] In FIG. 27, the electric field control electrode 106 may apply different potentials to the electric field control electrode 106 and the gate electrode 102, which may be independently controllable to the gate electrode 102. it can. With such a structure, the field effect transistor can be driven under optimum conditions. Since the surface trap response can be suppressed by fixing the surface potential, the electric field control electrode 106 is set to the same potential as the gate electrode 102, and the current collab can be suppressed more effectively than when the surface potential is modulated. . In particular, the effect of being able to control the electric field control electrode 106 independently is remarkable in the group III nitride semiconductor device in which the influence of the negative surface charge is a serious problem.

[0105] また、上記のように電界制御電極 106の電位を固定した場合、ゲート電極 102の電 位が変化してもゲート容量がほとんど変化しないため、利得の低下を大幅に抑制す ることがでさる。  [0105] Further, when the electric potential of the electric field control electrode 106 is fixed as described above, the gate capacitance hardly changes even if the electric potential of the gate electrode 102 is changed, so that a decrease in gain can be significantly suppressed. I'll do it.

[0106] (実施例 5)  [0106] (Example 5)

フィールドプレート部 105を有する実施例 4の HJFET134において、さらに、実施 例 3のように、絶縁膜を積層構造としてもよい。図 5は、本実施例の HJFETの構成を 示す断面図である。 In the HJFET 134 of Example 4 having the field plate part 105, further implementation As in Example 3, the insulating film may have a laminated structure. FIG. 5 is a cross-sectional view showing the configuration of the HJFET of this example.

[0107] 図 5に示した HJFET136は、 HJFET136は、 SiC等の基板 110上に形成される。  The HJFET 136 shown in FIG. 5 is formed on a substrate 110 such as SiC.

基板 110上には、半導体層力もなるバッファ層 111が形成されている。このノッファ 層 111上に GaNチャネル層 112力 S形成されて 、る。 GaNチャネル層 112の上には、 AlGaN電子供給層 113が形成されている。この AlGaN電子供給層 113上に、ソー ス電極 101およびドレイン電極 103がオーム性接合している。これらの電極間にゲー ト電極 102が設けられている。ゲート電極 102は、フィールドプレート部 105を有し、 A IGaN電子供給層 113とショットキー性接合して 、る。 AlGaN電子供給層 113の表面 は SiN膜 121で覆われており、さらにその上層には SiO膜 122が設けられている。フ  A buffer layer 111 having a semiconductor layer force is formed on the substrate 110. A GaN channel layer 112 force S is formed on the noffer layer 111. On the GaN channel layer 112, an AlGaN electron supply layer 113 is formed. On this AlGaN electron supply layer 113, the source electrode 101 and the drain electrode 103 are ohmic-bonded. A gate electrode 102 is provided between these electrodes. The gate electrode 102 has a field plate portion 105 and is in Schottky junction with the AIGaN electron supply layer 113. The surface of the AlGaN electron supply layer 113 is covered with a SiN film 121, and a SiO film 122 is further provided thereon. F

2  2

ィールドプレート部 105は SiO膜 122上に設けられており、フィールドプレート部 105  The field plate portion 105 is provided on the SiO film 122 and the field plate portion 105.

2  2

の直下にはこの SiN膜 121および SiO膜 122が設けられている。  The SiN film 121 and the SiO film 122 are provided immediately below.

2  2

[0108] 図 21〜図 24は、 HJFET136の製造方法を示す図である。  21 to 24 are diagrams showing a method for manufacturing the HJFET 136. FIG.

まず、 SiCからなる基板 110上にたとえば MBE成長法や MOVPE成長法等によつ て半導体を成長させる。このようにして、基板 110側力も順に、アンドープ A1N力もな るバッファ層 111 (膜厚 20nm)、アンドープの GaNチャネル層 112 (膜厚 2 m)、ァ ンドープ AlGaN力もなる AlGaN電子供給層 113 (膜厚 25nm)が積層した半導体層 構造が得られる(図 21 (a) )。  First, a semiconductor is grown on a substrate 110 made of SiC by, for example, MBE growth method or MOVPE growth method. In this way, the substrate 110 side force also has an undoped A1N force buffer layer 111 (film thickness 20 nm), an undoped GaN channel layer 112 (film thickness 2 m), and an undoped AlGaN force AlGaN electron supply layer 113 (film) A semiconductor layer structure with a thickness of 25 nm) is obtained (Fig. 21 (a)).

[0109] 次 、で、 AlGaN電子供給層 113形成後、これを大気暴露することなぐ AlGaN電 子供給層 113上に、プラズマ CVD法等により SiN膜 121 (60nm)を形成する(図 21 (b) )。なお、 AlGaN電子供給層 113が大気に曝された場合には、酸等によりエッチ ングを施し、半導体層表面を清浄ィ匕した後に SiN膜 121を形成する。  Next, after the AlGaN electron supply layer 113 is formed, an SiN film 121 (60 nm) is formed on the AlGaN electron supply layer 113 without exposing it to the atmosphere by plasma CVD or the like (FIG. 21 (b )). When the AlGaN electron supply layer 113 is exposed to the atmosphere, the SiN film 121 is formed after etching with an acid or the like to clean the surface of the semiconductor layer.

[0110] 続いて、 SiN膜 121上に常圧 CVD法等により SiO膜 122 ( 10011111)を形成する(  [0110] Subsequently, an SiO film 122 (10011111) is formed on the SiN film 121 by atmospheric pressure CVD or the like (

2  2

図 22 (c) )。  Figure 22 (c)).

[0111] そして、 SiN膜 121および SiO膜 122の一部とェピタキシャル層構造の一部を Ga  [0111] Then, a part of the SiN film 121 and the SiO film 122 and a part of the epitaxial layer structure are made Ga.

2  2

Nチャネル層 112が露出するまでエッチング除去することにより、素子間分離メサ(不 図示)を形成する。そして、 SiO膜 122の表面の所定の領域にフォトレジストを形成し  An element isolation mesa (not shown) is formed by etching until the N channel layer 112 is exposed. Then, a photoresist is formed in a predetermined region on the surface of the SiO film 122.

2  2

、 SiN膜 121および SiO膜 122の所定の領域を AlGaN電子供給層 113が露出する まで選択的にエッチング除去し(図 22 (d) )、 AlGaN電子供給層 113上に、たとえば TiZAl等の金属を蒸着することにより、ソース電極 101およびドレイン電極 103を形 成し(図 23 (e) )、 650°Cでァニールを行うことにより、これらの電極と AlGaN電子供 給層 113とをオーム性接合させる。 AlGaN electron supply layer 113 is exposed in a predetermined region of SiN film 121 and SiO film 122 Until the source electrode 101 and the drain electrode 103 are formed by depositing a metal such as TiZAl on the AlGaN electron supply layer 113 (FIG. 23 (e)). ))) Annealing is performed at 650 ° C., and these electrodes and the AlGaN child supply layer 113 are joined in ohmic contact.

[0112] つづいて、 SiO膜 122の表面の所定の領域にフォトレジストを形成し、 SiN膜 121 [0112] Next, a photoresist is formed in a predetermined region on the surface of the SiO film 122, and the SiN film 121 is formed.

2  2

および SiO膜 122の所定の領域を選択的にエッチング除去することによって、 AlGa  And by selectively etching away a predetermined region of the SiO film 122, AlGa

2  2

N電子供給層 113の露出する開口部を設ける(図 23 (f) )。  An exposed opening of the N electron supply layer 113 is provided (FIG. 23 (f)).

[0113] 次に、露出した AlGaN電子供給層 113上に、ゲート電極 102となる金属膜として、 たとえば NiZAuを蒸着して、 AlGaN電子供給層 113とショットキー接合されたゲート 電極 102を形成する(図 24)。またこれと同時に NiZAuよりなるフィールドプレート部 105も形成する。このようにして、図 5に示した HJFET136が得られる。  Next, on the exposed AlGaN electron supply layer 113, for example, NiZAu is vapor-deposited as a metal film to be the gate electrode 102 to form the gate electrode 102 that is Schottky-bonded to the AlGaN electron supply layer 113 ( (Figure 24). At the same time, a field plate portion 105 made of NiZAu is also formed. In this way, the HJFET 136 shown in FIG. 5 is obtained.

[0114] なお、本実施例ではゲート電極 102とフィールドプレート部 105を同時に形成する 例を示したが、別々の工程(開口を設けたレジストを形成し、開口部にフィールドプレ ート部 105を形成する工程を別々に行う)で形成してもよい。この場合、ゲート電極 10 2とフィールドプレート部 105との間隔をより狭い間隔で形成できる。  [0114] In this embodiment, an example in which the gate electrode 102 and the field plate portion 105 are formed at the same time has been shown. The step of forming may be performed separately). In this case, the gap between the gate electrode 102 and the field plate portion 105 can be formed with a narrower gap.

[0115] 本実施例によれば、実施例 4の効果に加えて、以下の効果が得られる。すなわち、 HJFET136では、フィールドプレート部 105の直下に、 SiN膜 121と SiO膜 122の  According to the present embodiment, in addition to the effects of the fourth embodiment, the following effects can be obtained. That is, in the HJFET 136, the SiN film 121 and the SiO film 122 are directly under the field plate portion 105.

2 積層膜からなる保護膜が設けられている。保護膜が SiN膜 121のみカゝらなる構成に 比べて、誘電率の低い SiO膜 122を用いることにより、フィールドプレート部 105によ  2 A protective film consisting of a laminated film is provided. Compared to the configuration in which the protective film is only the SiN film 121, the field plate portion 105 can

2  2

り生じる寄生容量の増大を抑制することができる。また、特に、 SiN膜 121を膜質経時 変化しない程度に薄く形成し(150nm以下、より好ましくは lOOnm以下)、そして Si O膜 122を厚く積層することにより、容量の増大をさらに効果的に抑制することができ Increase in parasitic capacitance can be suppressed. In particular, the SiN film 121 is formed thin enough not to change the film quality over time (150 nm or less, more preferably lOOnm or less), and the SiO film 122 is thickly laminated, thereby further suppressing the increase in capacitance. It is possible

2 2

る。  The

[0116] なお、本実施例においても、フィールドプレート部 105を有するゲート電極 102にか えて、ゲート電極 102と、ゲート電極 102から離隔して設けられた電界制御電極 106 とを有する構成としてもよい。  [0116] In this embodiment, the gate electrode 102 having the field plate portion 105 may be replaced with the gate electrode 102 and the electric field control electrode 106 provided apart from the gate electrode 102. .

[0117] また、電界制御電極 106はゲート電極 102と同時に形成してもよいし、別工程で形 成してもよい。別工程とする場合、所定の位置に開口部が設けられたレジストを SiN 膜 121上に形成し、開口部を埋め込むように電界制御電極 106を形成することもでき る。この場合、ゲート電極 102と電界制御電極 106との間隔をより狭い間隔で形成で きる。 [0117] The electric field control electrode 106 may be formed simultaneously with the gate electrode 102 or may be formed in a separate process. In a separate process, a resist with an opening at a predetermined position is removed from SiN. The electric field control electrode 106 may be formed on the film 121 so as to fill the opening. In this case, the gap between the gate electrode 102 and the electric field control electrode 106 can be formed with a narrower gap.

[0118] また、本実施例では、 III族窒化物半導体層の表面に形成された SiN膜 121を SiO  [0118] In this example, the SiN film 121 formed on the surface of the group III nitride semiconductor layer is formed of SiO.sub.

2 膜 122で覆う構成になっているため、 SiN膜 121の経時劣化をさらに確実に抑制す ることができる。よって、実施例 3と同様に、素子特性の長寿命化を図ることができる。  2 Since the structure is covered with the film 122, the deterioration with time of the SiN film 121 can be further reliably suppressed. Therefore, as in Example 3, the lifetime of the element characteristics can be extended.

[0119] また、本実施例においても、実施例 3と同様に、ソース電極 101およびゲート電極 1 02が SiN膜 121および SiO膜 122に乗り上げた構造になっている。このため、高電 Also in this example, as in Example 3, the structure is such that the source electrode 101 and the gate electrode 102 ride on the SiN film 121 and the SiO film 122. For this reason,

2  2

圧動作時において、ドレイン電極 103のゲート側端部における電界集中を緩和させ て、ゲート耐圧を向上させることができる。  During the pressure operation, the electric field concentration at the gate side end of the drain electrode 103 can be relaxed, and the gate breakdown voltage can be improved.

[0120] なお、本実施例では表面保護膜が、上層として、 SiO膜 122を有する例を示したが [0120] In this example, the surface protective film has an SiO film 122 as an upper layer.

2  2

、利得の向上および信頼性の向上の観点から、比誘電率が 4以下の低誘電率膜を 用いることがさらに好ましい。こうした低誘電率材料として、 SiOC (SiOCHと呼ばれる 場合もある)、 BCB (ベンゾシクロブテン)、 FSG (Flouro Silicate Glass: SiOF)、 HS (Hydrogen— ¾ilisesquioxane ^ MS (Methyl— ¾iisesquioxane) ^ 機 ポリマー、あるいはこれらをポーラス化した材料が例示される。  From the viewpoint of improving gain and reliability, it is more preferable to use a low dielectric constant film having a relative dielectric constant of 4 or less. Such low dielectric constant materials include SiOC (sometimes called SiOCH), BCB (benzocyclobutene), FSG (Flouro Silicate Glass: SiOF), HS (Hydrogen— ¾ilisesquioxane ^ MS (Methyl— ¾iisesquioxane) ^ machine polymer, or The material which made these porous is illustrated.

[0121] 保護膜、さらに具体的には、表面保護膜の上層を構成する絶縁膜が構成元素とし て C (炭素)を含む場合にも、 AlGaN電子供給層 113と SiN膜 121との界面を清浄ィ匕 することにより、上述した効果を得ることができる。  [0121] Even when the protective film, more specifically, the insulating film that forms the upper layer of the surface protective film contains C (carbon) as a constituent element, the interface between the AlGaN electron supply layer 113 and the SiN film 121 is formed. The effects described above can be obtained by cleaning.

[0122] (実施例 6)  [0122] (Example 6)

本実施例は、ワイドリセス構造を採用した HJFETの例である。  This embodiment is an example of an HJFET that employs a wide recess structure.

図 6は、本実施例の HJFETの構成を示す断面図である。図 6に示した HJFET138 にお 、ては、ソース電極 101と AlGaN電子供給層 113との間およびドレイン電極 10 3と AlGaN電子供給層 113との間に、アンドープ AlGaN層により構成されたコンタク ト層 114が介在する。 HJFET138においては、ソース電極 101およびドレイン電極 1 03の形成領域にお!、て、 AlGaN電子供給層 113上にコンタクト層 114が設けられて いる。コンタクト層 114は開口部を有し、開口部から AlGaN電子供給層 113が露出し ている。コンタクト層 114の上面に対して開口部の底面がリセス面となっている。コン タクト層 114の上面に接してソース電極 101およびドレイン電極 103が設けられてい る。そして、 AlGaN電子供給層 113の露出部に接してゲート電極 102が設けられて いる。ソース電極 101およびドレイン電極 103の底面力 ゲート電極 102の底面よりも 上方 (基板 110から遠ざ力る側)に位置する。 FIG. 6 is a cross-sectional view showing the configuration of the HJFET of this example. In the HJFET 138 shown in FIG. 6, the contact layer composed of an undoped AlGaN layer is provided between the source electrode 101 and the AlGaN electron supply layer 113 and between the drain electrode 103 and the AlGaN electron supply layer 113. 114 intervenes. In the HJFET 138, a contact layer 114 is provided on the AlGaN electron supply layer 113 in the formation region of the source electrode 101 and the drain electrode 103. The contact layer 114 has an opening, and the AlGaN electron supply layer 113 is exposed from the opening. The bottom surface of the opening is a recess surface with respect to the upper surface of the contact layer 114. Con A source electrode 101 and a drain electrode 103 are provided in contact with the upper surface of the tact layer 114. A gate electrode 102 is provided in contact with the exposed portion of the AlGaN electron supply layer 113. The bottom force of the source electrode 101 and the drain electrode 103 is located above the bottom surface of the gate electrode 102 (on the side away from the substrate 110).

[0123] HJFET138は、 SiC等の基板 110上に形成される。基板 110上には半導体層から なるバッファ層 111が形成されて 、る。このバッファ層 111上に GaNチャネル層 112 が形成されている。 GaNチャネル層 112の上には、八10&?^電子供給層113が形成 されている。この AlGaN電子供給層 113上にコンタクト層 114が形成されている。コ ンタクト層 114の表面にソース電極 101およびドレイン電極 103がオーム性接合され て!、る。 AlGaN電子供給層 113の表面は SiN膜 121で覆われて!/、る。  [0123] The HJFET 138 is formed on a substrate 110 such as SiC. A buffer layer 111 made of a semiconductor layer is formed on the substrate 110. A GaN channel layer 112 is formed on the buffer layer 111. On the GaN channel layer 112, an eight-and-a-half electron supply layer 113 is formed. A contact layer 114 is formed on the AlGaN electron supply layer 113. The source electrode 101 and the drain electrode 103 are ohmic-bonded to the surface of the contact layer 114. The surface of the AlGaN electron supply layer 113 is covered with a SiN film 121! /.

[0124] 図 6の HJFET138は、実施例 1の HJFET100 (図 1)にコンタクト層 114を追加した 構成である。この構成により、実施例 1で述べた効果に加え、さらにコンタクト抵抗を 低減する効果を奏する。  The HJFET 138 in FIG. 6 has a configuration in which a contact layer 114 is added to the HJFET 100 (FIG. 1) of the first embodiment. With this configuration, in addition to the effects described in the first embodiment, there is an effect of further reducing the contact resistance.

[0125] また、ワイドリセス構造の採用により、ゲート電極 102のドレイン電極側端部の電界 分布が変化するため、より一層優れた電界緩和効果が得られる。  [0125] Further, by adopting the wide recess structure, the electric field distribution at the end of the gate electrode 102 on the drain electrode side changes, so that an even better electric field relaxation effect can be obtained.

[0126] さらに、本実施例においても、実施例 1、実施例 2および実施例 4同様、ソース電極 101およびゲート電極 102が SiN膜 121に乗り上げた構造になっているため、高電 圧動作時においてドレイン電極 103のゲート電極側端部での電界集中を緩和させて 、ゲート耐圧を向上させることができる。  [0126] Furthermore, in this example, as in Example 1, Example 2, and Example 4, the source electrode 101 and the gate electrode 102 are on the SiN film 121, so that the high voltage operation is possible. In this case, the electric field concentration at the gate electrode side end of the drain electrode 103 can be relaxed to improve the gate breakdown voltage.

[0127] なお、本実施例では、 AlGaN電子供給層 113上に設ける保護膜が単層である例 を示したが、前述した実施例 3や実施例 4の場合のように、絶縁膜を二層構造としたり 、フィールドプレート部 105を形成することもできる。たとえば、フィールドプレート部 1 05は保護膜を SiN膜 121と SiO膜 122とから構成される二層構造とし、フィールドプ  [0127] In this example, the protective film provided on the AlGaN electron supply layer 113 is a single layer. However, as in the case of Example 3 and Example 4 described above, two insulating films are provided. A layer structure can be formed, or the field plate portion 105 can be formed. For example, the field plate portion 105 has a two-layer structure composed of a SiN film 121 and a SiO film 122 as a protective film.

2  2

レート部 105が SiO膜 122上に設けられていてもよい。この場合にも、実施例 3と同  The rate part 105 may be provided on the SiO film 122. In this case as well, the same as in Example 3.

2  2

様に、 SiO膜 122を、 SiN膜 121よりも低い誘電率を有する絶縁膜とすることが好ま  Thus, the SiO film 122 is preferably an insulating film having a lower dielectric constant than the SiN film 121.

2  2

しい。このような絶縁膜として、たとえば、第一の絶縁膜が SiNであった場合、窒素を 含まない膜を用いることができる。こうすることにより、フィールドプレート部 105の下方 の領域における絶縁膜の膜質の経時変化および容量増大を有効に抑制することが できる。よって、 HJFET138の信頼性および高周波特性をさらに向上させることがで きる。また、フィールドプレート部 105は、コンタクト層 114の上部まで延在していても よい。こうすることにより、ゲート電極 102のドレイン側端部の電界集中をより効果的に 分散 '緩和することができる。なおリセス構造とする場合、多段リセスとすることもできる That's right. As such an insulating film, for example, when the first insulating film is SiN, a film containing no nitrogen can be used. In this way, it is possible to effectively suppress the change over time in the film quality of the insulating film in the region below the field plate portion 105 and the increase in capacitance. it can. Therefore, the reliability and high frequency characteristics of the HJFET 138 can be further improved. Further, the field plate portion 105 may extend to the top of the contact layer 114. By doing so, the electric field concentration at the drain side end of the gate electrode 102 can be more effectively dispersed and relaxed. If a recess structure is used, a multi-stage recess can be used.

[0128] また、本実施例において、ドレイン電極 103の一部が AlGaN電子供給層 113中に 埋設されたゲートリセス構造を採用することもできる。 In this embodiment, a gate recess structure in which a part of the drain electrode 103 is embedded in the AlGaN electron supply layer 113 can also be adopted.

[0129] また、以上においてはコンタクト層 114がアンドープ AlGaN層により構成された場 合を例に説明した力 本実施例において、コンタクト層 114に所定の不純物がドーピ ングされた構成とすることもできる。 Further, in the above description, the force has been described by taking the case where the contact layer 114 is composed of an undoped AlGaN layer as an example. In this embodiment, the contact layer 114 may be doped with a predetermined impurity. .

[0130] 以上、本発明について実施形態および実施例をもとに説明した。これらの実施例は 例示であり、各構成要素や各処理プロセスの組み合わせに 、ろ 、ろな変形例が可能 なこと、また、そうした変形例も本発明の範囲にあることは当業者に理解されるところ である。 [0130] The present invention has been described based on the embodiments and examples. It is understood by those skilled in the art that these embodiments are exemplifications, and that various modifications are possible for each component and combination of each processing process, and that such modifications are also within the scope of the present invention. This is where it is.

[0131] たとえば、上記実施例では、基板 110の材料として SiCを用いた場合を例に説明し た力 他に、サファイア等他の異種基板材料や GaN、 AlGaN等の III族窒化物半導 体基板等を用いてもよい。  [0131] For example, in the above embodiment, the force described in the case where SiC is used as the material of the substrate 110, as well as other dissimilar substrate materials such as sapphire, and Group III nitride semiconductors such as GaN and AlGaN. A substrate or the like may be used.

[0132] また、以上の実施例では、 ΠΙ族窒化物半導体層構造を構成する元素のうち少なく とも一つを含む絶縁性の保護膜として SiN膜を設ける場合を例に説明したが、 III族 窒化物半導体層構造を構成する元素のうち少なくとも一つを含む絶縁膜の材料は、 SiNには限られず、他に、たとえば BN等の窒化物が挙げられる。こうした膜を用いた 場合にも、電流コラブスの発生を抑制できる。  [0132] In the above embodiment, the case where the SiN film is provided as an insulating protective film containing at least one of the elements constituting the group-III nitride semiconductor layer structure has been described as an example. The material of the insulating film containing at least one of the elements constituting the nitride semiconductor layer structure is not limited to SiN, and other examples include nitrides such as BN. Even when such a film is used, the generation of current collabs can be suppressed.

[0133] また、ゲート電極 102の下部における半導体層の構造としては、例示したものに限 られず種々の態様が可能である。たとえば GaNチャネル層 112の上部だけでなぐ 下部にも AlGaN電子供給層 113を併設した構造とすることも可能である。  [0133] Further, the structure of the semiconductor layer below the gate electrode 102 is not limited to that illustrated, and various modes are possible. For example, a structure in which the AlGaN electron supply layer 113 is also provided in the lower part of the GaN channel layer 112 is also possible.

[0134] また、この半導体層構造に、適宜、中間層やキャップ層を設けてもよい。たとえば、 I II族窒化物半導体層構造が、 In Ga N (0≤x≤ 1)からなるチャネル層、 Al Ga N (0≤y≤ 1)力もなる電子供給層および GaN力もなるキャップ層がこの順で積層し た構造を有する構成とすることができる。このようにすれば、実効的なショットキー高さ を高くでき、さらに高いゲート耐圧が実現できる。ただし、上記式において、 x=y=0 の場合は除く。 [0134] Further, an intermediate layer and a cap layer may be appropriately provided in this semiconductor layer structure. For example, a group II nitride semiconductor layer structure includes a channel layer made of InGaN (0≤x≤1), an electron supply layer with AlGaN (0≤y≤1) force, and a cap layer with GaN force. Laminate in order It can be set as the structure which has another structure. In this way, the effective Schottky height can be increased and a higher gate breakdown voltage can be realized. However, in the above formula, the case where x = y = 0 is excluded.

[0135] また、以上の各実施例において、ゲート電極 102の下部を一部、 AlGaN電子供給 層 113中に埋め込んだ、いわゆるゲートリセス構造を採用することができる。これによ り、優れたゲート耐圧が得られる。  In each of the above embodiments, a so-called gate recess structure in which a part of the lower portion of the gate electrode 102 is embedded in the AlGaN electron supply layer 113 can be employed. As a result, an excellent gate breakdown voltage can be obtained.

[0136] また、以上の各実施例において、ゲート電極 102とドレイン電極 103との距離を、ゲ ート電極 102とソース電極 101との間よりも長くすることもできる。いわゆるオフセット構 造と呼ばれるものであり、ゲート電極 102のドレイン電極側端部の電界集中をより効 果的に分散 ·緩和することができる。  Further, in each of the above embodiments, the distance between the gate electrode 102 and the drain electrode 103 can be made longer than that between the gate electrode 102 and the source electrode 101. This is a so-called offset structure, and the electric field concentration at the end on the drain electrode side of the gate electrode 102 can be more effectively dispersed and relaxed.

Claims

請求の範囲 The scope of the claims [1] ヘテロ接合を含む m族窒化物半導体層構造と、  [1] Group m nitride semiconductor layer structure including heterojunction, 該 in族窒化物半導体層構造上に離間して形成されたソース電極およびドレイン電 極と、  A source electrode and a drain electrode formed separately on the in-group nitride semiconductor layer structure; 前記ソース電極と前記ドレイン電極との間に配置されたゲート電極と、  A gate electrode disposed between the source electrode and the drain electrode; を備え、  With 前記ゲート電極と前記ドレイン電極との間の領域にお!ヽて、前記 in族窒化物半導 体層構造上に絶縁膜を有し、  In the region between the gate electrode and the drain electrode, an insulating film is provided on the in-group nitride semiconductor layer structure, 前記絶縁膜と前記 in族窒化物半導体層構造との界面における前記 in族窒化物半 導体層構造中の不純物濃度が、 lE17atomsZcm3以下であることを特徴とする電 界効果トランジスタ。 A field effect transistor, wherein an impurity concentration in the in-group nitride semiconductor layer structure at the interface between the insulating film and the in-group nitride semiconductor layer structure is lE17 atoms Zcm 3 or less. [2] 請求項 1に記載の電界効果トランジスタにお 、て、 [2] In the field effect transistor according to claim 1, 前記絶縁膜が、前記 III族窒化物半導体層構造を構成する元素のうち少なくとも一 つを含む絶縁膜であることを特徴とする電界効果トランジスタ。  A field effect transistor, wherein the insulating film is an insulating film containing at least one of elements constituting the group III nitride semiconductor layer structure. [3] 請求項 2に記載の電界効果トランジスタにおいて、 [3] The field effect transistor according to claim 2, III族窒化物半導体層構造を構成する前記元素が窒素であることを特徴とする電界 効果トランジスタ。  A field effect transistor, wherein the element constituting the group III nitride semiconductor layer structure is nitrogen. [4] 請求項 1乃至 3いずれかに記載の電界効果トランジスタにおいて、  [4] The field effect transistor according to any one of claims 1 to 3, 前記絶縁膜が、構成元素として酸素を実質的に含まない膜であることを特徴とする 電界効果トランジスタ。  The field effect transistor, wherein the insulating film is a film that substantially does not contain oxygen as a constituent element. [5] 請求項 1乃至 4いずれかに記載の電界効果トランジスタにおいて、 [5] The field effect transistor according to any one of claims 1 to 4, 前記ゲート電極と前記ドレイン電極との間の領域にお!ヽて、前記 III族窒化物半導 体層構造の上部に前記絶縁膜を介して電界制御電極が設けられたことを特徴とする 電界効果トランジスタ。  An electric field control electrode is provided on the region between the gate electrode and the drain electrode above the group III nitride semiconductor layer structure via the insulating film. Effect transistor. [6] 請求項 5に記載の電界効果トランジスタにおいて、 [6] The field effect transistor according to claim 5, 前記電界制御電極が、前記ゲート電極に対して独立に制御可能であることを特徴 とする電界効果トランジスタ。  The field effect transistor, wherein the field control electrode can be controlled independently of the gate electrode. [7] 請求項 1乃至 4いずれかに記載の電界効果トランジスタにおいて、前記ゲート電極 力 前記ドレイン電極側に庇状に張り出して前記絶縁膜の上部に形成されたフィー ルドプレート部を有することを特徴とする電界効果トランジスタ。 7. The field effect transistor according to claim 1, wherein the gate electrode is used. A field-effect transistor comprising a field plate portion that extends in a bowl shape on the drain electrode side and is formed on the insulating film. [8] 請求項 1乃至 7いずれかに記載の電界効果トランジスタにおいて、  [8] The field effect transistor according to any one of claims 1 to 7, 前記絶縁膜の厚さが、 5nm以上 lOOnm以下であることを特徴とする電界効果トラ ンジスタ。  A field effect transistor, wherein the insulating film has a thickness of 5 nm to lOO nm. [9] 請求項 1乃至 8いずれかに記載の電界効果トランジスタにおいて、  [9] The field effect transistor according to any one of claims 1 to 8, 前記絶縁膜が、第一の絶縁膜と、該第一の絶縁膜上に積層された第二の絶縁膜と 、力も構成されることを特徴とする電界効果トランジスタ。  2. The field effect transistor according to claim 1, wherein the first insulating film and a second insulating film laminated on the first insulating film are also configured with force. [10] 請求項 1乃至 9いずれかに記載の電界効果トランジスタにおいて、 [10] The field effect transistor according to any one of claims 1 to 9, 前記ソース電極と前記 III族窒化物半導体層構造との間および前記ドレイン電極と 前記 III族窒化物半導体層構造との間に、コンタクト層が介在することを特徴とする電 界効果トランジスタ。  A field effect transistor, wherein a contact layer is interposed between the source electrode and the group III nitride semiconductor layer structure and between the drain electrode and the group III nitride semiconductor layer structure. [11] 請求項 10に記載の電界効果トランジスタにおいて、 [11] The field effect transistor according to claim 10, 前記コンタクト層がアンドープ AlGaN層により構成されていることを特徴とする電界 効果トランジスタ。  A field effect transistor, wherein the contact layer comprises an undoped AlGaN layer. [12] 請求項 1乃至 11いずれかに記載の電界効果トランジスタにおいて、前記絶縁膜と 前記 ΠΙ族窒化物半導体層構造との界面における前記 III族窒化物半導体層構造中 の不純物濃度が、 lE15atomsZcm3以下であることを特徴とする電界効果トランジ スタ。 12. The field effect transistor according to claim 1, wherein an impurity concentration in the group III nitride semiconductor layer structure at an interface between the insulating film and the group III nitride semiconductor layer structure is lE15atomsZcm 3. A field-effect transistor characterized by: [13] 請求項 1乃至 12いずれかに記載の電界効果トランジスタの製造方法であって、 成膜室中でヘテロ接合を含む前記 III族窒化物半導体層構造を形成する工程と、 前記 ΠΙ族窒化物半導体層構造上に前記絶縁膜を形成する工程と、  [13] The method of manufacturing a field effect transistor according to any one of claims 1 to 12, wherein the group III nitride semiconductor layer structure including a heterojunction is formed in a film formation chamber; Forming the insulating film on the physical semiconductor layer structure; 前記絶縁膜の所定の領域をエッチングにより選択的に除去して開口部を形成し、 前記 ΠΙ族窒化物半導体層構造上に、前記開口部を埋め込むように前記ゲート電極 を形成する工程と、  A step of selectively removing a predetermined region of the insulating film by etching to form an opening; and forming the gate electrode so as to embed the opening on the group III nitride semiconductor layer structure; を含むことを特徴とする電界効果トランジスタの製造方法。  A method of manufacturing a field effect transistor comprising: [14] 成膜室中でヘテロ接合を含む III族窒化物半導体層構造を形成する工程と、 [14] forming a group III nitride semiconductor layer structure including a heterojunction in the deposition chamber; 前記 III族窒化物半導体層構造上に絶縁膜を形成する工程と、 前記絶縁膜の所定の領域をエッチングにより選択的に除去して開口部を形成し、 前記 ΠΙ族窒化物半導体層構造上に、前記開口部を埋め込むようにゲート電極を形 成する工程と、 Forming an insulating film on the group III nitride semiconductor layer structure; A step of selectively removing a predetermined region of the insulating film by etching to form an opening, and forming a gate electrode so as to embed the opening on the group III nitride semiconductor layer structure; を含み、  Including 前記 m族窒化物半導体層構造を形成する工程の後、前記 m族窒化物半導体層 構造を前記成膜室力 取り出すことなく前記絶縁膜を形成する工程を行うことを特徴 とする電界効果トランジスタの製造方法。  A step of forming the insulating film without taking out the film forming chamber force after the step of forming the group m nitride semiconductor layer structure is performed. Production method. [15] 成膜室中でヘテロ接合を含む m族窒化物半導体層構造を形成する工程と、 [15] forming a group m nitride semiconductor layer structure including a heterojunction in the deposition chamber; 前記 in族窒化物半導体層構造上に絶縁膜を形成する工程と、  Forming an insulating film on the in-group nitride semiconductor layer structure; 前記絶縁膜の所定の領域をエッチングにより選択的に除去して開口部を形成し、 前記 m族窒化物半導体層構造上に、前記開口部を埋め込むようにゲート電極を形 成する工程と、  A step of selectively removing a predetermined region of the insulating film by etching to form an opening, and forming a gate electrode on the group m nitride semiconductor layer structure so as to embed the opening; 前記 in族窒化物半導体層構造を形成する工程の後、前記絶縁膜を形成する工程 の前に、  After the step of forming the in-group nitride semiconductor layer structure and before the step of forming the insulating film, 酸を用いたウエットエッチングにより、前記 m族窒化物半導体層構造の表面を洗浄 する工程と、  Cleaning the surface of the group m nitride semiconductor layer structure by wet etching using an acid; を含むことを特徴とする電界効果トランジスタの製造方法。  A method of manufacturing a field effect transistor comprising: [16] 請求項 13乃至 15いずれかに記載の電界効果トランジスタの製造方法において、 前記絶縁膜を形成する工程の後、前記絶縁膜の所定の領域をエッチングにより選 択的に除去し、前記 in族窒化物半導体層構造上に、除去された領域を埋め込むよう にソース電極とドレイン電極とを離間して形成する工程を含むことを特徴とする電界 効果トランジスタの製造方法。 [16] In the method of manufacturing a field effect transistor according to any one of claims 13 to 15, after the step of forming the insulating film, a predetermined region of the insulating film is selectively removed by etching, and the in A method for manufacturing a field effect transistor, comprising: forming a source electrode and a drain electrode separately on a group nitride semiconductor layer structure so as to embed a removed region.
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