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WO2018074228A1 - Semiconductor device, and production method therefor - Google Patents

Semiconductor device, and production method therefor Download PDF

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Publication number
WO2018074228A1
WO2018074228A1 PCT/JP2017/036055 JP2017036055W WO2018074228A1 WO 2018074228 A1 WO2018074228 A1 WO 2018074228A1 JP 2017036055 W JP2017036055 W JP 2017036055W WO 2018074228 A1 WO2018074228 A1 WO 2018074228A1
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WO
WIPO (PCT)
Prior art keywords
region
diffusion region
semiconductor substrate
semiconductor device
main surface
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Ceased
Application number
PCT/JP2017/036055
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French (fr)
Japanese (ja)
Inventor
振一郎 柳
野中 裕介
誠二 野間
晋也 櫻井
奨悟 池浦
淳志 笠原
伸 瀧澤
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Denso Corp
Original Assignee
Denso Corp
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Publication date
Priority claimed from JP2017076087A external-priority patent/JP6642507B2/en
Application filed by Denso Corp filed Critical Denso Corp
Priority to CN201780063822.6A priority Critical patent/CN109863581B/en
Publication of WO2018074228A1 publication Critical patent/WO2018074228A1/en
Priority to US16/368,026 priority patent/US11114571B2/en
Anticipated expiration legal-status Critical
Ceased legal-status Critical Current

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    • H10P32/1406
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L21/00Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
    • H01L21/02Manufacture or treatment of semiconductor devices or of parts thereof
    • H01L21/04Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer
    • H01L21/18Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic Table or AIIIBV compounds with or without impurities, e.g. doping materials
    • H01L21/22Diffusion of impurity materials, e.g. doping materials, electrode materials, into or out of a semiconductor body, or between semiconductor regions; Interactions between two or more impurities; Redistribution of impurities
    • H01L21/223Diffusion of impurity materials, e.g. doping materials, electrode materials, into or out of a semiconductor body, or between semiconductor regions; Interactions between two or more impurities; Redistribution of impurities using diffusion into or out of a solid from or into a gaseous phase
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L21/00Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
    • H01L21/02Manufacture or treatment of semiconductor devices or of parts thereof
    • H01L21/04Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer
    • H01L21/18Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic Table or AIIIBV compounds with or without impurities, e.g. doping materials
    • H01L21/26Bombardment with radiation
    • H01L21/263Bombardment with radiation with high-energy radiation
    • H01L21/265Bombardment with radiation with high-energy radiation producing ion implantation
    • 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
    • H10D62/10Shapes, relative sizes or dispositions of the regions of the semiconductor bodies; Shapes of the semiconductor bodies
    • H10D62/124Shapes, relative sizes or dispositions of the regions of semiconductor bodies or of junctions between the regions
    • H10D62/125Shapes of junctions between the regions
    • H10D64/011
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D8/00Diodes
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D8/00Diodes
    • H10D8/01Manufacture or treatment
    • H10D8/021Manufacture or treatment of breakdown diodes
    • H10D8/022Manufacture or treatment of breakdown diodes of Zener diodes
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D8/00Diodes
    • H10D8/20Breakdown diodes, e.g. avalanche diodes
    • H10D8/25Zener diodes 
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D8/00Diodes
    • H10D8/50PIN diodes 
    • H10P32/171
    • 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
    • H10D62/10Shapes, relative sizes or dispositions of the regions of the semiconductor bodies; Shapes of the semiconductor bodies
    • H10D62/124Shapes, relative sizes or dispositions of the regions of semiconductor bodies or of junctions between the regions
    • H10D62/126Top-view geometrical layouts of the regions or the junctions
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D8/00Diodes
    • H10D8/411PN diodes having planar bodies

Definitions

  • the present disclosure relates to a semiconductor device including a Zener diode and a manufacturing method thereof.
  • a constant voltage power supply using a Zener diode is known.
  • a constant voltage power supply is also used for a battery monitoring IC mounted on a vehicle, but high-precision voltage control is required to supply power to the IC.
  • the Zener voltage is uniquely determined depending on the concentration of both.
  • the semiconductor device disclosed in Patent Document 1 the first diffusion region and the second diffusion region are provided in the semiconductor substrate, and the impurity concentration of the two diffusion regions related to the PN junction is arbitrarily controlled. Made possible.
  • the desired Zener characteristic can be obtained by controlling the impurity concentration of the diffusion region.
  • the breakdown voltage due to the overlap is reduced at the junction due to the overlap between the first diffusion region and the second diffusion region. And it is said that yielding occurs in the part corresponding to this overlap.
  • the portion corresponding to the overlap is an area existing three-dimensionally, and the yield phenomenon occurs somewhere in the three-dimensional area, but the position is indefinite. That is, the exact position at which yield occurs cannot be controlled.
  • the occurrence of hot carriers and the state of traps on the surface defects of the hot carriers differ depending on the position where breakdown occurs, so the occurrence position of breakdown is uncertain because it causes the amount of variation in Zener voltage over time to increase. Become. Then, a change in Zener voltage with time may hinder high-accuracy voltage control.
  • an object of the present disclosure is to provide a semiconductor device capable of suppressing a change in Zener voltage and a method for manufacturing the semiconductor device.
  • a semiconductor device includes a semiconductor substrate having a diode formation region, an upper diffusion region of a first conductivity type formed in a surface layer of a main surface of the semiconductor substrate in the diode formation region, and a depth of the semiconductor substrate.
  • a lower diffusion region of a second conductivity type formed at a position deeper than the upper diffusion region with respect to the main surface in the vertical direction, and the lower diffusion region is a PN junction with the upper diffusion region at a position deeper than the main surface And has a local maximum point indicating the local maximum in the impurity concentration profile of the lower diffusion region in the diode formation region.
  • the breakdown phenomenon can be easily generated at the maximum point.
  • the designer can arbitrarily determine the impurity concentration of the lower diffusion region and its peak position, and can control the position where the breakdown phenomenon occurs. That is, the variation factor of the Zener voltage can be suppressed to the minimum.
  • the PN junction surface between the upper diffusion region and the lower diffusion region is formed at a position deeper than the main surface of the semiconductor substrate, it is trapped by surface defects existing on the main surface when hot carriers are generated. Probability can be reduced. That is, the fluctuation amount of the Zener voltage can be reduced.
  • the method for manufacturing a semiconductor device according to the second aspect of the present disclosure is such that a semiconductor substrate is prepared, impurities are implanted into a surface layer of the main surface of the semiconductor substrate, and a rotationally symmetric shape is obtained when the main surface is viewed from the front.
  • An upper implantation region of the first conductivity type is formed at a position shallower to the main surface than the lower implantation region so as to have a rotationally symmetric shape concentric with the lower implantation region, After forming, the lower implantation region is diffused by annealing to form the lower diffusion region, and the upper implantation region is diffused to form the upper diffusion region.
  • the local maximum point where the impurity concentration becomes maximum can be formed on the rotational symmetry axis of the lower implantation region, the variation factor of the Zener voltage can be suppressed to the minimum.
  • a semiconductor device includes a second conductivity type semiconductor substrate having a diode formation region, and a first conductivity type upper diffusion formed in a surface layer of a main surface of the semiconductor substrate in the diode formation region.
  • a second conductivity type lower diffusion region formed at a position deeper than the upper diffusion region with respect to the main surface in the depth direction of the semiconductor substrate and having a higher impurity concentration than the semiconductor substrate; and a diode formation region
  • a second conductivity type counter electrode region formed on a surface layer of the main surface and having an impurity concentration higher than that of the semiconductor substrate, and further, a surface layer of the main surface between the upper diffusion region and the counter electrode region In the region, an inter-electrode region of the second conductivity type having an impurity concentration higher than that of the semiconductor substrate is formed.
  • the method for manufacturing a semiconductor device includes preparing a second conductivity type semiconductor substrate, implanting impurities into the surface layer of the main surface of the semiconductor substrate, and having an impurity concentration higher than that of the semiconductor substrate. Forming a raised second conductivity type lower implantation region; forming a lower implantation region; diffusing the lower implantation region by annealing; and diffusing by annealing of the lower implantation region; Impurities are implanted into the surface layer to form an upper implantation region of the first conductivity type at a position shallower than the main surface of the lower implantation region. After forming the upper implantation region, the lower implantation region is diffused by annealing.
  • FIG. 1 is a diagram illustrating a cross section and an upper surface of the semiconductor device according to the first embodiment.
  • FIG. 2 is a cross-sectional view showing a process of preparing a semiconductor substrate
  • FIG. 3 is a cross-sectional view showing a process of forming the lower implantation region
  • FIG. 4 is a cross-sectional view showing the first annealing step
  • FIG. 5 is a cross-sectional view showing a process of forming the upper implantation region
  • FIG. 6 is a cross-sectional view showing the second annealing step
  • FIG. 7 is a diagram showing a three-dimensional profile of impurity concentration.
  • FIG. 8 is a diagram showing the change over time in the amount of fluctuation of the Zener voltage.
  • FIG. 9 is a cross-sectional view of the semiconductor device according to the second embodiment.
  • FIG. 10 is a cross-sectional view showing a process of forming the lower implantation region
  • FIG. 11 is a cross-sectional view showing the first annealing step
  • FIG. 12 is a cross-sectional view showing the process of forming the upper implantation region
  • FIG. 13 is a cross-sectional view of the semiconductor device according to the third embodiment.
  • FIG. 14 is a cross-sectional view showing a process of forming a lower injection region and a counter electrode injection region
  • FIG. 15 is a cross-sectional view showing the first annealing step
  • FIG. 16 is a cross-sectional view showing a process of forming the upper injection region and the interelectrode injection region
  • FIG. 17 is a cross-sectional view of the semiconductor device according to the fourth embodiment.
  • This semiconductor device includes a Zener diode as an element, and is introduced into a power supply circuit, for example, and functions as a constant voltage power supply.
  • the semiconductor device 100 includes a semiconductor substrate 10, an upper diffusion region 20, a lower diffusion region 30, and a silicide block layer 40.
  • the semiconductor substrate 10 is a part of an N conductivity type semiconductor wafer, and in particular, FIG. 1 shows a part of the main surface 10a side.
  • the semiconductor substrate 10 has a diode formation region Di.
  • a PN junction diode is formed as an element by forming an upper diffusion region 20 and a lower diffusion region 30 described later.
  • the P diffusion type upper diffusion region 20 functions as an anode
  • the N conductivity type semiconductor substrate 10 functions as a cathode.
  • the N conductivity type corresponds to the second conductivity type
  • the P conductivity type corresponds to the first conductivity type.
  • the upper diffusion region 20 is a P conductivity type semiconductor region.
  • the upper diffusion region 20 is formed in the surface layer on the main surface 10 a side of the semiconductor substrate 10 so as to be exposed on the main surface 10 a of the semiconductor substrate 10.
  • the upper diffusion region 20 is formed to be rotationally symmetric with respect to an axis A orthogonal to the main surface 10a.
  • the upper diffusion region 20 in the present embodiment is formed in a substantially perfect circle shape centered on a point passing through the axis A when the main surface 10a is viewed from the front.
  • region 20 has a structure which became depressed so that the axis
  • the upper diffusion region 20 in the present embodiment is a substantially perfect circle when the main surface 10a is viewed from the front, and has a shape like a so-called rotating body, but does not necessarily need to be a rotating body.
  • the shape may be n times symmetrical when the main surface 10a is viewed from the front.
  • an ellipse, a capsule shape (2-fold symmetry), an equilateral triangle (3-fold symmetry), a square (4-fold symmetry), or the like may be employed.
  • the lower diffusion region 30 is an N conductivity type semiconductor region.
  • the lower diffusion region 30 is formed so as to cover the upper diffusion region 20.
  • the lower diffusion region 30 is also rotationally symmetric with respect to the axis A.
  • the lower diffusion region 30 in the present embodiment has an axis when the main surface 10a is viewed from the front. It is formed in a substantially perfect circle shape centered on a point passing through A. Also for the lower diffusion region 30, the shape of the main surface 10 a when viewed from the front is not limited to a perfect circle, but may be formed to be n times symmetrical.
  • a PN junction surface S is formed between the lower diffusion region 30 of N conductivity type and the upper diffusion region of P conductivity type. Yes.
  • the PN junction surface S also has the same shape. That is, the PN junction surface S has a concave shape when the upper diffusion region 20 is mainly used.
  • the lower diffusion region 30 in the present embodiment completely covers the upper diffusion region 20, and a part thereof is exposed to the main surface 10a. That is, when the main surface 10a is viewed from the front, the lower diffusion region 30 is exposed to the main surface 10a in a region beyond the outer edge of the upper diffusion region 20 with respect to the formation center. In other words, when the main surface 10a is viewed from the front, the upper diffusion region 20, the lower diffusion region 30, and the N-conductivity type semiconductor region of the semiconductor substrate 10 are arranged in this order around the point where the axis A intersects the main surface 10a. It is formed in a concentric circle.
  • the P conductivity type semiconductor region of the upper diffusion region 20 and the lower diffusion region 30 and the N conductivity type semiconductor region of the semiconductor substrate 10 form a PN junction to form a diode.
  • the P diffusion type upper diffusion region 20 functions as an anode
  • the N conductivity type semiconductor substrate 10 functions as a cathode.
  • the silicide block layer 40 is an insulating film, and is formed of, for example, SiO 2 in this embodiment.
  • the silicide block layer 40 is formed in an annular shape around the point where the axis A and the main surface 10a intersect.
  • the upper diffusion region 20 and the lower diffusion region 30 are exposed on the main surface 10a, and the semiconductor region of the semiconductor substrate 10 is exposed outside thereof.
  • the silicide block layer 40 is formed so as to cover the surface from the outer edge of the upper diffusion region 20 through the lower diffusion region 30 to the semiconductor region of the semiconductor substrate 10.
  • the silicide block layer 40 functions as an electrode for the anode and the cathode. For example, when a silicide electrode containing cobalt is stacked on the main surface 10a, the silicide block layer 40 and the N diffusion type P diffusion region 20 are formed. It is formed for the purpose of maintaining electrical insulation between the lower diffusion region 30 and the semiconductor substrate 10.
  • a semiconductor substrate 10 having N conductivity type is prepared.
  • an N conductivity type lower implantation region 31 having a diameter R is formed. That is, a disk-shaped N conductivity type region having the axis A as the rotational symmetry axis is formed.
  • the lower implantation region 31 is a region before being diffused by annealing, and becomes the lower diffusion region 30 after two annealing steps described later.
  • the photoresist (not shown) is removed and a first annealing process is performed.
  • impurities forming the lower implantation region 31 diffuse in the semiconductor substrate 10 as shown in FIG.
  • the impurity region 32 in which the lower implantation region 31 is thermally diffused does not diffuse as much as the lower diffusion region 30 shown in FIG.
  • a photoresist (not shown) having the same center as that of the lower implantation region 31 and having a smaller diameter than the impurity region 32 shown in FIG. And boron is ion-implanted.
  • the ion implantation is performed with the same energy on the one surface 10a, and the implantation depth is made substantially constant.
  • a P conductivity type upper implantation region 21 surrounded by the impurity region 32 is formed. That is, a disk-shaped P conductivity type region having the axis A as a rotationally symmetric axis is formed.
  • the upper implantation region 21 is a region before being diffused by annealing, and becomes the upper diffusion region 20 after the second annealing step described later.
  • the photoresist (not shown) is removed and a second annealing step is performed.
  • the second annealing step the upper implantation region 21 is thermally diffused as shown in FIG. 6, and the impurity region 32 in which the lower implantation region 31 is diffused to some extent is further thermally diffused.
  • the upper implantation region 21 diffuses to a region corresponding to the upper diffusion region 20, and the lower implantation region 31 diffuses to a region corresponding to the lower diffusion region 30.
  • the formation depth of the lower diffusion region 30 after thermal diffusion is preferably designed to be substantially the same as the ion implantation diameter R of the lower implantation region 31.
  • Parameters for the annealing temperature, ion implantation energy, and impurity concentration may be determined by making the process common with other elements formed on the semiconductor substrate 10, and it may be difficult to change the values.
  • the formation depth of the lower diffusion region 30 is designed to be substantially the same as the ion implantation diameter R of the lower implantation region 31, the formation radius of the lower implantation region 31 is set to be the same as that of the assumed lower diffusion region 30. It means to match the formation depth.
  • the impurity concentration of the impurity region 32 caused by the lower implantation region 31 has a peak at a position on the axis A and deeper than the upper implantation region 21.
  • the conductivity type is unlikely to be reversed in the vicinity of the center of the disk-shaped upper implantation region 21.
  • the cross-sectional shape passing through the axis A of the upper diffusion region 20 becomes a structure that is recessed toward the vicinity of the axis A as shown in FIG. 1. Yes. That is, the upper diffusion region 20 is formed in a disk shape with a recessed center. That is, the PN junction surface S between the upper diffusion region 20 and the lower diffusion region 30 has a concave shape when the upper diffusion region 20 is mainly used.
  • contour lines shown in the lower diffusion region 30 in FIG. 6 indicate the contour lines of the impurity concentration, and that the peak of the impurity concentration in the lower diffusion region 30 is located below the dent in the upper diffusion region 20. Show.
  • the silicide block layer 40 is formed so as to straddle the boundary line L2 with the substrate 10.
  • the semiconductor device 100 can be manufactured by a manufacturing method including the above steps.
  • the respective impurity profiles are also substantially rotationally symmetric with respect to the axis A. It becomes.
  • the inventor simulated a specific impurity profile using a computer. The simulation results are shown in FIG.
  • the lower diffusion region 30 formed in the diode formation region Di has a maximum point P at which the impurity concentration is maximum.
  • the maximum point P in the present embodiment is on the axis A and is located below the PN junction surface S.
  • the high impurity concentration portion of the lower diffusion region 30 exhibiting N conductivity is not three-dimensionally distributed as in the prior art, but is defined as zero dimension (point). Therefore, it is possible to identify the portion where the yield phenomenon occurs as a point. That is, the yielding phenomenon in the semiconductor device 100 can be fixed at a substantially predetermined position (maximum point P).
  • the cause of increasing the amount of fluctuation of the Zener voltage over time is presumed to be that the generation of the breakdown phenomenon is indefinite because the generation source of the breakdown phenomenon is distributed three-dimensionally.
  • the occurrence position of the breakdown phenomenon can be determined as a point. According to this, as compared with the conventional configuration in which the breakdown phenomenon occurs three-dimensionally, the generation position of the breakdown phenomenon can be limited. As shown in FIG. It can be suppressed compared to.
  • the output voltage can be controlled with high accuracy regardless of the passage of time.
  • the semiconductor device 100 has a concave structure in which the PN junction surface S is recessed when the upper diffusion region 20 is mainly used.
  • the structure is recessed near the axis A. According to this, as shown in FIG. 7, it is possible to easily form an impurity distribution having a peak in the lower diffusion region 30 at the lower portion of the recessed portion of the upper diffusion region 20. In other words, the maximum impurity concentration can be easily formed in a dot shape.
  • the upper diffusion region 20 and the lower diffusion region 30 have a rotationally symmetric shape, particularly a perfect circle shape, when the one surface 10a is viewed from the front.
  • the maximum of the impurity concentration in the lower diffusion region 30 can be on the rotational symmetry axis (axis A in the present embodiment), and the maximum of the impurity concentration can be easily formed in a dot shape.
  • the formation diameter R of the lower implantation region 31 that is a precursor region of the lower diffusion region 30 is substantially the same as the assumed formation depth of the lower diffusion region 30.
  • the maximum of the impurity concentration in the lower diffusion region 30 can be easily formed in a dot shape.
  • the maximum impurity concentration is distributed one-dimensionally or two-dimensionally extending in the direction along the main surface 10a. Cheap.
  • the maximum impurity concentration in the lower diffusion region 30 can be easily formed in a dot shape.
  • the semiconductor device 100 ion-implants impurities with a uniform depth in the manufacturing process, particularly in the formation of the upper implantation region 21.
  • the conductivity type is easily reversed at the portion where the impurity concentration in the impurity region 32 which is the precursor region of the lower diffusion region 30 is low, and the concave structure of the PN junction surface S can be easily formed. it can. That is, as described above, the maximum impurity concentration of the lower diffusion region 30 can be easily formed in a dot shape.
  • the lower diffusion region 30 is formed so as to cover the upper diffusion region 20, and is exposed to the main surface 10a.
  • the depletion layer formed between the P conductivity type upper diffusion region 20 and the N conductivity type region extends in the direction along the main surface 10a. 30 can be suppressed as compared with a configuration in which the main surface is not exposed. Thereby, it is possible to suppress trapping of hot carriers at a level caused by surface defects existing in the vicinity of the main surface 10a, and it is possible to suppress an amount of fluctuation of the Zener voltage with time.
  • the semiconductor device 100 includes the silicide block layer 40 on the main surface 10a.
  • the silicide block layer 40 is formed so as to straddle the PN junction line L1 between the upper diffusion region 20 and the lower diffusion region 30 when the lower diffusion region 30 is exposed to the main surface 10a.
  • it should be formed so as to straddle the boundary line L ⁇ b> 2 between the lower diffusion region 30 and the semiconductor region in the semiconductor substrate 10.
  • the lower diffusion region 30 is not exposed to the main surface 10 a, it should be formed so as to straddle the boundary line between the upper diffusion region 20 and the semiconductor region in the semiconductor substrate 10.
  • the PN junction surface S between the upper diffusion region 20 and the lower diffusion region 30 is a concave surface, but a convex surface may be used.
  • the semiconductor device 110 in this embodiment includes an upper diffusion region 50 and a lower diffusion region 60 having shapes different from those in the first embodiment, as shown in FIG.
  • the semiconductor device 110 has a convex surface portion C that becomes a convex surface in the cross section of the PN junction surface S.
  • the shape of the upper diffusion region 50 and the lower diffusion region 60 when viewed from the main surface 10a is a perfect circle, and an axis B passing through the center of the perfect circle and orthogonal to the main surface 10a is an axis of symmetry.
  • a rotating body is formed.
  • the concave portion C has a convex vertex on the axis B.
  • the impurity concentration of the lower diffusion region 60 has a peak in the vicinity of the lower portion of the concave surface portion formed outside the convex surface portion C of the PN junction surface S. That is, the cross section shown in FIG. 9 has the maximum point of impurity concentration at the points indicated by points P1 and P2.
  • the maximum points P1 and P2 are also part of a circle having the axis B as the symmetry axis. That is, as for the maximum points of the impurity concentration of the lower diffusion region 60 in the present embodiment, a plurality of maximum points are distributed around the axis B in a one-dimensional manner (specifically, in a circular shape).
  • the maximum points of the impurity concentration of the lower diffusion region 60 can be distributed one-dimensionally. Similar to the first embodiment, since the maximum point of the impurity concentration is effective as the occurrence position of the breakdown phenomenon, the occurrence position of the breakdown phenomenon can be defined as a line in the semiconductor device 110. According to this, as compared with the conventional configuration in which the breakdown phenomenon occurs three-dimensionally, the generation position of the breakdown phenomenon can be limited, and the variation of the Zener voltage with time can be suppressed. For example, when a Zener diode included in the semiconductor device 110 is employed as a constant voltage power source, the output voltage can be controlled with high accuracy regardless of the passage of time.
  • a semiconductor substrate 10 is prepared as shown in FIG.
  • the lower injection region 61 is formed in a rotationally symmetric shape with the axis B as the axis of symmetry. In particular, in the present embodiment, it is formed in an annular shape.
  • the lower injection region 31 in the first embodiment is a perfect circle when viewed from the main surface 10a, but the lower injection region 61 in the present embodiment is an annular shape in which the vicinity of the center is hollowed out. Since FIG. 10 is a cross-sectional view, the two lower injection regions 61 are illustrated as being separated from each other, but are actually continuous in the front-rear direction of the paper.
  • the lower implantation region 61 is a region that becomes the lower diffusion region 60 by two thermal diffusions in a later process.
  • the first annealing step is performed.
  • the lower implantation region 61 is thermally diffused to form an N conductivity type impurity region 62. Since the lower implantation region 61 before the annealing step is annular, the impurity concentration structure in the impurity region 62 after the thermal diffusion is a substantially torus structure in which the higher concentration portion is distributed in a circle having the axis B as the symmetry axis. ing.
  • the upper implantation region 51 is formed so as to be included in the impurity region 62. Specifically, the upper implantation region 51 is formed on the upper portion of the impurity region 61 that is the precursor region of the lower diffusion region 60 where the concentration reaches a peak. That is, the upper injection region 51 is formed in a rotationally symmetric shape with the axis B as the axis of symmetry. In particular, in the present embodiment, the upper injection region 51 is formed in an annular shape.
  • the upper injection region 21 in the first embodiment is a perfect circle when viewed from the main surface 10a, but the upper injection region 51 in the present embodiment has an annular shape in which the vicinity of the center is hollowed out. Since FIG. 12 is a cross-sectional view, the two upper injection regions 51 are illustrated so as to be separated from each other, but are actually continuous in the front-rear direction of the drawing.
  • the upper implantation region 51 is a region that becomes the upper diffusion region 50 by two thermal diffusions in a later step.
  • a second annealing step is performed.
  • the upper implantation region 51 is thermally diffused, and the impurity region 62 in which the lower implantation region 61 is diffused to some extent is further thermally diffused.
  • the upper implantation region 51 after the second annealing step is diffused to a region corresponding to the upper diffusion region 50, and the lower implantation region 61 is diffused to a region corresponding to the lower diffusion region 60.
  • the torus shape of the impurity concentration distribution of the impurity region 62 which is a precursor region of the lower diffusion region 60 is substantially maintained, and the maximum impurity concentration of the lower diffusion region 60 is configured in the circular shape as described above.
  • the silicide block layer 40 is formed so as to straddle the PN junction line between the P conductivity type upper diffusion region 50 exposed on the main surface 10a and the N conductivity type semiconductor region, and the boundary line between the lower diffusion region 60 and the semiconductor substrate 10. To do.
  • the semiconductor device 110 in which the PN junction surface S is a convex surface can be manufactured.
  • the depletion layer when the breakdown occurs is the lower diffusion regions 30 and 60 in the surface layer of the semiconductor substrate 10. May extend to a wide area outside. This is presumed to be caused by surface traps in the surface layer of the semiconductor device 10, and an increase in the electrical resistance of the current path between the upper diffusion regions 20 and 50 as the anode and the cathode occurs. This increase in electrical resistance may cause a change in Zener voltage with time.
  • the semiconductor device 120 has a cathode whose impurity concentration is higher than that of the semiconductor substrate 10 in the diode formation region Di in addition to the upper diffusion region 70 and the lower diffusion region 80.
  • a region 90 and an inter-electrode region 91 formed between the upper diffusion region 70 functioning as an anode and the cathode region 90 are provided.
  • the cathode region 90 corresponds to a counter electrode region.
  • the upper diffusion region 70 and the lower diffusion region 80 in the present embodiment are formed in the same manner as the upper diffusion region 20 and the lower diffusion region 30 in the first embodiment, respectively. That is, the upper diffusion region 70 is a P conductivity type semiconductor region formed so as to be exposed on the main surface 10 a, and the lower diffusion region 80 is formed so as to cover the upper diffusion region 70 in the semiconductor substrate 10. This is an N conductivity type semiconductor region. Although a detailed structure has been described in the first embodiment, it will be omitted. However, in this embodiment as well, the PN junction surface S between the upper diffusion region 70 and the lower diffusion region 80 has a concave shape, and the breakpoint is almost the same. It is structurally controlled to be formed as a point (0 dimension).
  • the cathode region 90 which is a counter electrode region is an N conductivity type semiconductor region having a concentration higher than that of the semiconductor substrate 10 and is an annular region concentric with the upper diffusion region 70 when the main surface 10a is viewed from the front. .
  • Cathode region 90 is exposed at main surface 10a, and the cathode electrode is in ohmic contact with the exposed surface.
  • the cathode region 90 and the lower diffusion region 80 are formed by the same process, and the average impurity concentration is substantially the same.
  • the interelectrode region 91 is an N conductivity type semiconductor region formed between the upper diffusion region 70 and the cathode region 90.
  • the interelectrode region 91 has an impurity concentration higher than that of the semiconductor substrate 10.
  • the inter-electrode region 91 is formed so as to be exposed on the main surface 10a, whereby the region surrounded by the cathode region 90 is exposed on the main surface 10a of the N conductivity type region constituting the semiconductor substrate 10. Not done.
  • the distribution of the radial impurities seen from the center of the upper diffusion region 70 is the P conductivity type of the upper diffusion region 70 and the N conductivity type of the lower diffusion region 80 exposed on the main surface 10a.
  • the N conductivity type of the inter-electrode region 91 and the N conductivity type of the cathode region 90 are spread concentrically.
  • the interelectrode region 91 is formed as a separate process from the process of forming the lower diffusion region 80 and the cathode region 90. Therefore, the impurity concentration in the inter-electrode region 91 can be controlled independently of the lower diffusion region 80 and the cathode region 90, and is determined based on the intention of the designer.
  • the impurity concentration of the interelectrode region 91 needs to be lower than that of the cathode region 90 to which the cathode electrode is connected, is higher than that of the semiconductor substrate 10, and is impurity concentration of the lower diffusion region 80. Preferably, the concentration is lower than the maximum value.
  • the place where the impurity concentration of the lower diffusion region 80 in the present embodiment is the maximum is the maximum point of the impurity concentration, which is formed as a point (zero dimension) and becomes a breakpoint.
  • the impurity concentration in the inter-electrode region 91 is set lower than this breakpoint. Thereby, breakdown in the vicinity of the inter-electrode region 91 is prevented. In other words, breakdown is intentionally generated in the lower diffusion region 80.
  • the method for manufacturing the semiconductor device 120 will be described with reference to FIGS. 14 to 16 with reference to the description regarding the method for manufacturing the semiconductor device 100 in the first embodiment.
  • a semiconductor substrate 10 having N conductivity type is prepared.
  • the lower implantation region 81 is formed by ion implantation, as in the first embodiment.
  • the counter electrode injection region 92 is formed by the same or different process as the lower injection region 81. Both lower injection region 81 and counter electrode injection region 92 are formed in the surface layer of main surface 10a. These regions are regions that become the lower diffusion region 80 and the cathode region 90 by an annealing process described later.
  • an annealing process is performed to thermally diffuse impurities.
  • impurities are diffused in the semiconductor substrate 10 to form a semiconductor region having a higher concentration than the semiconductor substrate 10 by the annealing process.
  • ions are implanted into the region where the lower implantation region 81 is thermally diffused by the annealing process, thereby forming a P conductivity type upper implantation region 71. Further, ions are implanted into the surface layer of the main surface 10 a surrounded by the lower implantation region 81 and the counter electrode implantation region 92 to form an N conductivity type interelectrode implantation region 93.
  • the silicide block layer 40 is formed in an annular shape, and the semiconductor device 120 is manufactured.
  • the silicide block layer 40 has an annular inner edge that covers the upper diffusion region 70 and an annular outer edge that covers the cathode region 90. That is, the exposed portion of the lower diffusion region 80 and the inter-electrode region 91 in the main surface 10 a are completely hidden by the silicide block layer 40.
  • the depletion layer when breakdown occurs may extend to a wide region outside the lower diffusion regions 30 and 60 in the surface layer of the semiconductor substrate 10, which is a surface trap in the surface layer of the semiconductor device 10. It is presumed to be caused.
  • the semiconductor device 120 includes the cathode region 90 and the inter-electrode region 91 having a higher concentration than that of the semiconductor substrate 10 so that the N-conductivity type impurity layer constituting the semiconductor substrate 10 is not exposed in the semiconductor substrate 10a. Yes.
  • an interelectrode region 91 is formed as a portion where a lower diffusion region 80 and a cathode region 90 as a counter electrode region overlap.
  • the inter-electrode region 91 is of N conductivity type, and is higher in concentration than the impurity concentration constituting the semiconductor substrate 10 as in the third embodiment.
  • the upper diffusion regions 20, 50, and 70 and the upper implantation regions 21, 51, and 71 are formed in a perfect circle shape with the axis A or the axis B as the symmetry axis.
  • the shapes of the upper diffusion regions 20, 50, 70 and the upper injection regions 21, 51, 71 viewed from the front from the surface 10a are not limited to a perfect circle, and may be n-fold symmetrical shapes. Specifically, an ellipse, capsule shape (2 times symmetry), equilateral triangle (3 times symmetry), square (4 times symmetry), regular pentagon (5 times symmetry), regular hexagon (6 times symmetry), etc. are adopted. Also good.
  • the lower diffusion regions 30, 60, 80 and the lower injection regions 31, 61, 81 are formed in a perfect circle shape with the axis A or the axis B as a symmetry axis is shown.
  • the shapes of the lower diffusion regions 30, 60, 80 and the lower implantation regions 31, 61, 81 are not limited to a perfect circle, but may be any n-fold symmetrical shape. In the two-fold symmetrical shape, the maximum impurity concentration is not a point but a linear shape (one-dimensional) along the long side.
  • the lower diffusion regions 30, 60, 80 corresponding to the upper diffusion regions 20, 50, 70 are preferably similar in shape to each other when viewed from the main surface 10a. Since the upper diffusion regions 20, 50, 70 and the corresponding lower diffusion regions 30, 60, 80 have symmetry, the lower diffusion regions 30, 60, 80 break in one or zero dimensions lower than three dimensions. It is easy to form points.
  • the silicide block layer 40 is formed in the same center as the upper diffusion regions 20, 50, 70 and the lower diffusion regions 30, 60, 80 has been described. However, the formation center may be shifted. It should be noted that the silicide block layer 40 may be unnecessary if the electrode is not formed by silicide, and is not an essential element in such a form.
  • the P conductivity type is adopted for the upper diffusion regions 20 and 50 and the N conductivity type is adopted for the lower diffusion regions 30 and 60.
  • these conductivity types are configured to be reversed to each other. May be.
  • substrate was described as a semiconductor substrate, about the semiconductor substrate, N conductivity type and P conductivity were used irrespective of the conductivity type of the upper diffusion regions 20 and 50 and the lower diffusion regions 30 and 60. Any type of mold may be employed.
  • the inter-electrode region 91 is provided, the counter electrode region corresponding to the cathode region 90, the lower diffusion regions 30, 60, and 80, and the semiconductor substrate 10 need to be of the same conductivity type.
  • the lower diffusion regions 30, 60, 80 are illustrated as being exposed to the main surface 10 a by completely covering the corresponding upper diffusion regions 20, 50, 70 inside the semiconductor substrate 10.
  • the lower diffusion region may be positioned only below the upper diffusion region and not exposed to the main surface 10a.
  • the P conductivity type upper diffusion regions 20, 50, 70 and N The spread of the depletion layer formed between the conductive type region in the direction along the main surface 10a can be suppressed as compared with the configuration in which the lower diffusion regions 30, 60, and 80 are not exposed on the main surface.
  • the diode formation region Di in which a Zener diode is formed in the semiconductor substrate 10 has been described.
  • another element is formed in the semiconductor substrate 10 in a region other than the diode formation region. I will not prevent it.
  • a MOSFET or IGBT may be separately formed on the same semiconductor substrate 10.
  • the joint surface between the upper diffusion regions 20, 50, 70 and the lower diffusion regions 30, 60, 80 has a concave shape, so that the lower diffusion regions 30, 60, 80 are formed.
  • the configuration in which the maximum point indicating the maximum concentration is formed has been described.
  • the bonding surface between the upper diffusion regions 20, 50, 70 and the lower diffusion regions 30, 60, 80 is flat.
  • the formation of the inter-electrode region 91 can provide an effect of suppressing the variation with time of the Zener voltage.
  • the effect of providing the inter-electrode region 91 can be realized independently of the technical idea of forming a maximum point indicating the maximum concentration in the impurity concentration profile of the lower diffusion regions 30, 60, 80. .

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Abstract

This semiconductor device is provided with: a semiconductor substrate (10) provided with a diode-forming region (Di); a first-conductivity-type upper diffusion region (20, 50, 70) which is formed in the surface layer of a main surface (10a) of the semiconductor substrate, and in the diode-forming region; and a second-conductivity-type lower diffusion region (30, 60, 80) which is formed in a deeper position than the upper diffusion region with respect to the main surface in the depth direction of the semiconductor substrate, and which has a higher impurity concentration than the semiconductor substrate. Furthermore, the lower diffusion region forms a PN junction surface (S) with the upper diffusion region at a position deeper than the main surface, and is provided with a maximum point (P, P1, P2) which indicates the maximum concentration in an impurity concentration profile of the lower diffusion region in the diode-forming region.

Description

半導体装置およびその製造方法Semiconductor device and manufacturing method thereof 関連出願の相互参照Cross-reference of related applications

 本出願は、2016年10月18日に出願された日本特許出願番号2016-204668号と、2017年4月6日に出願された日本特許出願番号2017-76087号に基づくもので、ここにそれらの記載内容を援用する。 This application is based on Japanese Patent Application No. 2016-204668 filed on October 18, 2016 and Japanese Patent Application No. 2017-76087 filed on April 6, 2017. The description of is incorporated.

 本開示は、ツェナーダイオードを含む半導体装置およびその製造方法に関する。 The present disclosure relates to a semiconductor device including a Zener diode and a manufacturing method thereof.

 ツェナーダイオードを利用した定電圧電源が知られている。車両に搭載される電池の監視ICなどにも定電圧電源が用いられているが、ICなどへの電源供給には高精度な電圧制御が要求される。 A constant voltage power supply using a Zener diode is known. A constant voltage power supply is also used for a battery monitoring IC mounted on a vehicle, but high-precision voltage control is required to supply power to the IC.

 従来、N導電型のエピタキシャル層とP導電型の拡散層との間のPN接合において、両者の濃度に依存してツェナー電圧が一義的に決まるものであった。これに対して、特許文献1に開示される半導体装置は、半導体基板に第1の拡散領域と第2の拡散領域とを設けて、PN接合に係る2つの拡散領域の不純物濃度を任意に制御可能にした。そして、拡散領域の不純物濃度を制御することにより所望のツェナー特性を得られるとしている。 Conventionally, in a PN junction between an N conductivity type epitaxial layer and a P conductivity type diffusion layer, the Zener voltage is uniquely determined depending on the concentration of both. On the other hand, in the semiconductor device disclosed in Patent Document 1, the first diffusion region and the second diffusion region are provided in the semiconductor substrate, and the impurity concentration of the two diffusion regions related to the PN junction is arbitrarily controlled. Made possible. The desired Zener characteristic can be obtained by controlling the impurity concentration of the diffusion region.

特開2010-239015号公報JP 2010-239015 A

 ところで、ツェナー電圧には降伏による経時的な変動があることが知られている。この特性変動は、降伏現象によって生じるホットキャリアが半導体基板の表面欠陥にトラップされることにより起こると推察されている。 By the way, it is known that the Zener voltage varies over time due to breakdown. This characteristic variation is presumed to occur when hot carriers generated by the breakdown phenomenon are trapped by surface defects of the semiconductor substrate.

 特許文献1に記載の半導体装置にあっては、第1の拡散領域と第2の拡散領域との重なりによる接合部において、その重なりに起因する降伏電圧が低下するとされている。そして、この重なりに相当する部分で降伏が生じるとしている。このような構成では、重なりに相当する部分は3次元的に存在する領域であり、降伏現象は3次元的な領域のうち何処かで生じるが、その位置は不定である。すなわち、降伏の生じる正確な位置は制御不可能である。 In the semiconductor device described in Patent Document 1, the breakdown voltage due to the overlap is reduced at the junction due to the overlap between the first diffusion region and the second diffusion region. And it is said that yielding occurs in the part corresponding to this overlap. In such a configuration, the portion corresponding to the overlap is an area existing three-dimensionally, and the yield phenomenon occurs somewhere in the three-dimensional area, but the position is indefinite. That is, the exact position at which yield occurs cannot be controlled.

 降伏が生じる位置によって、ホットキャリアの発生や該ホットキャリアの表面欠陥へのトラップの状態が異なるため、降伏の発生位置が不定であることは、ツェナー電圧の経時的な変動量を大きくする原因となる。そして、ツェナー電圧の経時的な変動は、高精度な電圧制御を妨げる虞がある。 The occurrence of hot carriers and the state of traps on the surface defects of the hot carriers differ depending on the position where breakdown occurs, so the occurrence position of breakdown is uncertain because it causes the amount of variation in Zener voltage over time to increase. Become. Then, a change in Zener voltage with time may hinder high-accuracy voltage control.

 そこで、本開示は、ツェナー電圧の変動を抑制可能な半導体装置を提供するとともに、その半導体装置の製造方法を提供することを目的とする。 Therefore, an object of the present disclosure is to provide a semiconductor device capable of suppressing a change in Zener voltage and a method for manufacturing the semiconductor device.

 本開示の第一態様に係る半導体装置は、ダイオード形成領域を有する半導体基板と、ダイオード形成領域における半導体基板の主面の表層に形成された第1導電型の上部拡散領域と、半導体基板の深さ方向において主面に対して上部拡散領域よりも深い位置に形成される第2導電型の下部拡散領域と、を備え、下部拡散領域は、主面より深い位置において上部拡散領域とのPN接合面を成すとともに、ダイオード形成領域における下部拡散領域の不純物濃度プロファイルにおいて、濃度の極大を示す極大点を有する。 A semiconductor device according to a first aspect of the present disclosure includes a semiconductor substrate having a diode formation region, an upper diffusion region of a first conductivity type formed in a surface layer of a main surface of the semiconductor substrate in the diode formation region, and a depth of the semiconductor substrate. A lower diffusion region of a second conductivity type formed at a position deeper than the upper diffusion region with respect to the main surface in the vertical direction, and the lower diffusion region is a PN junction with the upper diffusion region at a position deeper than the main surface And has a local maximum point indicating the local maximum in the impurity concentration profile of the lower diffusion region in the diode formation region.

 これによれば、下部拡散領域における不純物濃度の極大点において電界を大きくできるから、該極大点において降伏現象を生じやすくできる。設計者は下部拡散領域の不純物濃度およびそのピーク位置を任意に決定することができ、降伏現象を生じる位置を制御することができる。すなわち、ツェナー電圧の変動因子を最小限に抑制することができる。 According to this, since the electric field can be increased at the maximum point of the impurity concentration in the lower diffusion region, the breakdown phenomenon can be easily generated at the maximum point. The designer can arbitrarily determine the impurity concentration of the lower diffusion region and its peak position, and can control the position where the breakdown phenomenon occurs. That is, the variation factor of the Zener voltage can be suppressed to the minimum.

 また、上部拡散領域と下部拡散領域とのPN接合面は、半導体基板の主面よりも深い位置に形成されているから、ホットキャリアが発生した際に主面に存在する表面欠陥にトラップされる確率を小さくできる。すなわち、ツェナー電圧の変動量を小さくすることができる。 Further, since the PN junction surface between the upper diffusion region and the lower diffusion region is formed at a position deeper than the main surface of the semiconductor substrate, it is trapped by surface defects existing on the main surface when hot carriers are generated. Probability can be reduced. That is, the fluctuation amount of the Zener voltage can be reduced.

 このように、この半導体装置によれば、ツェナー電圧の変動因子を最小限にしつつ、降伏時の特性変動量も抑制できるものである。 Thus, according to this semiconductor device, it is possible to suppress the fluctuation factor of the Zener voltage and to suppress the characteristic fluctuation amount at the breakdown.

 本開示の第二態様に係る半導体装置の製造方法は、半導体基板を準備すること、半導体基板の主面における表層に不純物を注入して、主面を正面視したときに回転対称の形状となるように第2導電型の下部注入領域を形成すること、下部注入領域の形成の後、アニールにより下部注入領域を拡散すること、下部注入領域のアニールによる拡散の後、半導体基板の主面における表層に不純物を注入して、下部注入領域よりも主面に対して浅い位置に、下部注入領域と同心の回転対称形状となるように第1導電型の上部注入領域を形成すること、上部注入領域の形成の後、アニールにより下部注入領域を拡散して下部拡散領域を形成するとともに、上部注入領域を拡散して上部拡散領域を形成すること、を備える。 The method for manufacturing a semiconductor device according to the second aspect of the present disclosure is such that a semiconductor substrate is prepared, impurities are implanted into a surface layer of the main surface of the semiconductor substrate, and a rotationally symmetric shape is obtained when the main surface is viewed from the front. Forming the second conductivity type lower implant region, forming the lower implant region, diffusing the lower implant region by annealing, and after diffusing by annealing the lower implant region, the surface layer on the main surface of the semiconductor substrate An upper implantation region of the first conductivity type is formed at a position shallower to the main surface than the lower implantation region so as to have a rotationally symmetric shape concentric with the lower implantation region, After forming, the lower implantation region is diffused by annealing to form the lower diffusion region, and the upper implantation region is diffused to form the upper diffusion region.

 これによれば、下部注入領域の回転対称軸上に、不純物濃度が極大となる極大点を形成することができるから、ツェナー電圧の変動因子を最小限に抑制することができる。 According to this, since the local maximum point where the impurity concentration becomes maximum can be formed on the rotational symmetry axis of the lower implantation region, the variation factor of the Zener voltage can be suppressed to the minimum.

 また、本開示の第三態様に係る半導体装置は、ダイオード形成領域を有する第2導電型の半導体基板と、ダイオード形成領域における半導体基板の主面の表層に形成された第1導電型の上部拡散領域と、半導体基板の深さ方向において主面に対して上部拡散領域よりも深い位置に形成され、半導体基板よりも不純物濃度が高くされた第2導電型の下部拡散領域と、ダイオード形成領域における主面の表層に形成され、半導体基板よりも不純物濃度が高くされた第2導電型の対極領域と、を備え、さらに、主面の表層であって、上部拡散領域と対極領域との間の領域に、半導体基板よりも不純物濃度の高い第2導電型の極間領域が形成される。 Further, a semiconductor device according to the third aspect of the present disclosure includes a second conductivity type semiconductor substrate having a diode formation region, and a first conductivity type upper diffusion formed in a surface layer of a main surface of the semiconductor substrate in the diode formation region. A second conductivity type lower diffusion region formed at a position deeper than the upper diffusion region with respect to the main surface in the depth direction of the semiconductor substrate and having a higher impurity concentration than the semiconductor substrate; and a diode formation region A second conductivity type counter electrode region formed on a surface layer of the main surface and having an impurity concentration higher than that of the semiconductor substrate, and further, a surface layer of the main surface between the upper diffusion region and the counter electrode region In the region, an inter-electrode region of the second conductivity type having an impurity concentration higher than that of the semiconductor substrate is formed.

 これによれば、ブレークダウン発生時において、上部拡散領域と対極領域との間において、主面表層に進展する空乏層の侵入を抑制でき、電流経路における電気抵抗の上昇を抑制することができる。よって、ツェナー電圧の変動を抑制することができる。 According to this, when a breakdown occurs, it is possible to suppress the intrusion of a depletion layer that progresses to the main surface layer between the upper diffusion region and the counter electrode region, and it is possible to suppress an increase in electrical resistance in the current path. Therefore, fluctuations in the Zener voltage can be suppressed.

 さらに、本開示の第四態様に係る半導体装置の製造方法は、第2導電型の半導体基板を準備すること、半導体基板の主面における表層に不純物を注入して、半導体基板よりも不純物濃度が高くされた第2導電型の下部注入領域を形成すること、下部注入領域の形成の後、アニールにより下部注入領域を拡散すること、下部注入領域のアニールによる拡散の後、拡散した下部注入領域の表層に不純物を注入して、下部注入領域よりも主面に対して浅い位置に、第1導電型の上部注入領域を形成すること、上部注入領域の形成の後、アニールにより下部注入領域を拡散して下部拡散領域を形成するとともに、上部注入領域を拡散して上部拡散領域を形成すること、加えて、半導体基板の表層であって下部注入領域とは離間した位置に不純物を注入して第2導電型の対極注入領域を形成すること、半導体基板の表層であって対極注入領域と下部注入領域の間の領域に半導体基板よりも不純物濃度の高い極間領域を形成すること、を備える。 Furthermore, the method for manufacturing a semiconductor device according to the fourth aspect of the present disclosure includes preparing a second conductivity type semiconductor substrate, implanting impurities into the surface layer of the main surface of the semiconductor substrate, and having an impurity concentration higher than that of the semiconductor substrate. Forming a raised second conductivity type lower implantation region; forming a lower implantation region; diffusing the lower implantation region by annealing; and diffusing by annealing of the lower implantation region; Impurities are implanted into the surface layer to form an upper implantation region of the first conductivity type at a position shallower than the main surface of the lower implantation region. After forming the upper implantation region, the lower implantation region is diffused by annealing. Forming the lower diffusion region, diffusing the upper implantation region to form the upper diffusion region, and in addition, injecting impurities into the surface layer of the semiconductor substrate at a position separated from the lower implantation region. Forming a second conductivity type counter-electrode injection region, forming an inter-electrode region having a higher impurity concentration than the semiconductor substrate in a surface layer of the semiconductor substrate between the counter-electrode injection region and the lower injection region, Is provided.

 これによれば、ブレークダウン発生時において、上部拡散領域と対極領域との間において、主面表層に進展する空乏層の侵入を抑制でき、電流経路における電気抵抗の上昇を抑制することができる。よって、ツェナー電圧の変動を抑制することができる。 According to this, when a breakdown occurs, it is possible to suppress the intrusion of a depletion layer that progresses to the main surface layer between the upper diffusion region and the counter electrode region, and it is possible to suppress an increase in electrical resistance in the current path. Therefore, fluctuations in the Zener voltage can be suppressed.

 本開示についての上記目的およびその他の目的、特徴や利点は、添付の図面を参照しながら下記の詳細な記述により、より明確になる。図面において、
図1は、第1実施形態における半導体装置の断面および上面を示す図であり、 図2は、半導体基板を準備する工程を示す断面図であり、 図3は、下部注入領域の形成工程を示す断面図であり、 図4は、1回目のアニール工程を示す断面図であり、 図5は、上部注入領域の形成工程を示す断面図であり、 図6は、2回目のアニール工程を示す断面図であり、 図7は、不純物濃度の3次元プロファイルを示す図であり、 図8は、ツェナー電圧の変動量の経時変化を示す図であり、 図9は、第2実施形態における半導体装置の断面図であり、 図10は、下部注入領域の形成工程を示す断面図であり、 図11は、1回目のアニール工程を示す断面図であり、 図12は、上部注入領域の形成工程を示す断面図であり、 図13は、第3実施形態における半導体装置の断面図であり、 図14は、下部注入領域および対極注入領域の形成工程を示す断面図であり、 図15は、1回目のアニール工程を示す断面図であり、 図16は、上部注入領域および極間注入領域の形成工程を示す断面図であり、 図17は、第4実施形態における半導体装置の断面図である。
The above and other objects, features and advantages of the present disclosure will become more apparent from the following detailed description with reference to the accompanying drawings. In the drawing
FIG. 1 is a diagram illustrating a cross section and an upper surface of the semiconductor device according to the first embodiment. FIG. 2 is a cross-sectional view showing a process of preparing a semiconductor substrate, FIG. 3 is a cross-sectional view showing a process of forming the lower implantation region, FIG. 4 is a cross-sectional view showing the first annealing step, FIG. 5 is a cross-sectional view showing a process of forming the upper implantation region, FIG. 6 is a cross-sectional view showing the second annealing step, FIG. 7 is a diagram showing a three-dimensional profile of impurity concentration. FIG. 8 is a diagram showing the change over time in the amount of fluctuation of the Zener voltage. FIG. 9 is a cross-sectional view of the semiconductor device according to the second embodiment. FIG. 10 is a cross-sectional view showing a process of forming the lower implantation region, FIG. 11 is a cross-sectional view showing the first annealing step, FIG. 12 is a cross-sectional view showing the process of forming the upper implantation region, FIG. 13 is a cross-sectional view of the semiconductor device according to the third embodiment. FIG. 14 is a cross-sectional view showing a process of forming a lower injection region and a counter electrode injection region, FIG. 15 is a cross-sectional view showing the first annealing step, FIG. 16 is a cross-sectional view showing a process of forming the upper injection region and the interelectrode injection region, FIG. 17 is a cross-sectional view of the semiconductor device according to the fourth embodiment.

 以下、本開示の実施の形態を図面に基づいて説明する。なお、以下の各図相互において、互いに同一もしくは均等である部分に、同一符号を付与する。 Hereinafter, embodiments of the present disclosure will be described with reference to the drawings. In the following drawings, the same reference numerals are given to the same or equivalent parts.

 (第1実施形態)
 最初に、図1を参照して、本実施形態に係る半導体装置の概略構成について説明する。
(First embodiment)
First, a schematic configuration of the semiconductor device according to the present embodiment will be described with reference to FIG.

 この半導体装置は素子としてツェナーダイオードを含み、例えば電源回路に導入されて定電圧電源として機能するものである。 This semiconductor device includes a Zener diode as an element, and is introduced into a power supply circuit, for example, and functions as a constant voltage power supply.

 図1に示すように、半導体装置100は、半導体基板10と、上部拡散領域20と、下部拡散領域30と、シリサイドブロック層40と、を備えている。 As shown in FIG. 1, the semiconductor device 100 includes a semiconductor substrate 10, an upper diffusion region 20, a lower diffusion region 30, and a silicide block layer 40.

 半導体基板10は、N導電型とされた半導体ウェハの一部であり、特に図1においては主面10a側の一部を図示している。半導体基板10はダイオード形成領域Diを有している。ダイオード形成領域Diには、後述の上部拡散領域20および下部拡散領域30が形成されることにより素子としてPN接合ダイオードが形成される。P導電型である上部拡散領域20はアノードとして機能し、N導電型である半導体基板10はカソードとして機能する。なお、本実施形態におけるN導電型は、第2導電型に相当し、P導電型は第1導電型に相当する。 The semiconductor substrate 10 is a part of an N conductivity type semiconductor wafer, and in particular, FIG. 1 shows a part of the main surface 10a side. The semiconductor substrate 10 has a diode formation region Di. In the diode formation region Di, a PN junction diode is formed as an element by forming an upper diffusion region 20 and a lower diffusion region 30 described later. The P diffusion type upper diffusion region 20 functions as an anode, and the N conductivity type semiconductor substrate 10 functions as a cathode. In this embodiment, the N conductivity type corresponds to the second conductivity type, and the P conductivity type corresponds to the first conductivity type.

 上部拡散領域20はP導電型の半導体領域である。上部拡散領域20は、半導体基板10の主面10aに露出するように、半導体基板10の主面10a側表層に形成されている。図1に示すように、上部拡散領域20は、主面10aを直交する軸Aに対して回転対称に形成されている。とくに本実施形態における上部拡散領域20は、主面10aを正面視したとき、軸Aを通る点を中心にした略真円状に形成されている。そして、上部拡散領域20の軸Aを通る断面形状は、図1に示すように、軸A近傍ほど窪んだ構造になっている。すなわち、中央が凹んだ円盤状に形成されている。後述するが、本実施形態における軸Aは対称軸に一致する。なお、本実施形態における上部拡散領域20は主面10aを正面視したときに略真円であって、いわゆる回転体のような形状になっているが、必ずしも回転体状である必要はない。例えば、主面10aを正面視したときに、n回対称形状であればよい。具体的には、楕円やカプセル形状(2回対称)、正三角形(3回対称)、正方形(4回対称)などを採用しても良い。 The upper diffusion region 20 is a P conductivity type semiconductor region. The upper diffusion region 20 is formed in the surface layer on the main surface 10 a side of the semiconductor substrate 10 so as to be exposed on the main surface 10 a of the semiconductor substrate 10. As shown in FIG. 1, the upper diffusion region 20 is formed to be rotationally symmetric with respect to an axis A orthogonal to the main surface 10a. In particular, the upper diffusion region 20 in the present embodiment is formed in a substantially perfect circle shape centered on a point passing through the axis A when the main surface 10a is viewed from the front. And the cross-sectional shape which passes along the axis | shaft A of the upper diffusion area | region 20 has a structure which became depressed so that the axis | shaft A vicinity might be shown in FIG. That is, it is formed in a disk shape with a recessed center. As will be described later, the axis A in this embodiment coincides with the symmetry axis. Note that the upper diffusion region 20 in the present embodiment is a substantially perfect circle when the main surface 10a is viewed from the front, and has a shape like a so-called rotating body, but does not necessarily need to be a rotating body. For example, the shape may be n times symmetrical when the main surface 10a is viewed from the front. Specifically, an ellipse, a capsule shape (2-fold symmetry), an equilateral triangle (3-fold symmetry), a square (4-fold symmetry), or the like may be employed.

 下部拡散領域30はN導電型の半導体領域である。下部拡散領域30は、上部拡散領域20を覆うように形成されている。下部拡散領域30も、上部拡散領域20と同様に、軸Aに対して回転対称に形成されているのであり、とくに本実施形態における下部拡散領域30は、主面10aを正面視したとき、軸Aを通る点を中心にした略真円状に形成されている。下部拡散領域30についても、主面10aを正面視したときの形状は真円に限定されるものではなく、n回対称に形成されていればよい。 The lower diffusion region 30 is an N conductivity type semiconductor region. The lower diffusion region 30 is formed so as to cover the upper diffusion region 20. Similarly to the upper diffusion region 20, the lower diffusion region 30 is also rotationally symmetric with respect to the axis A. In particular, the lower diffusion region 30 in the present embodiment has an axis when the main surface 10a is viewed from the front. It is formed in a substantially perfect circle shape centered on a point passing through A. Also for the lower diffusion region 30, the shape of the main surface 10 a when viewed from the front is not limited to a perfect circle, but may be formed to be n times symmetrical.

 下部拡散領域30は、上部拡散領域20に隣接して形成されているので、N導電型である下部拡散領域30とP導電型である上部拡散領域との間でPN接合面Sが形成されている。上記したように、上部拡散領域20は主面10aに露出しない反対の面において凹んだ形状をしているのであるから、PN接合面Sも同様の形状を成す。すなわち、PN接合面Sは、上部拡散領域20を主体とすれば凹面形状を成している。 Since the lower diffusion region 30 is formed adjacent to the upper diffusion region 20, a PN junction surface S is formed between the lower diffusion region 30 of N conductivity type and the upper diffusion region of P conductivity type. Yes. As described above, since the upper diffusion region 20 has a concave shape on the opposite surface that is not exposed to the main surface 10a, the PN junction surface S also has the same shape. That is, the PN junction surface S has a concave shape when the upper diffusion region 20 is mainly used.

 なお、本実施形態における下部拡散領域30は、上部拡散領域20を完全に覆っており、一部が主面10aに露出している。つまり、主面10aを正面視したとき、下部拡散領域30は、形成中心に対して上部拡散領域20の外縁以遠の領域で主面10aに露出している。換言すれば、主面10aを正面視すると、軸Aと主面10aとが交差する点を中心として、上部拡散領域20、下部拡散領域30、半導体基板10のN導電型半導体領域が、この順で同心円状に広がって形成されている。 Note that the lower diffusion region 30 in the present embodiment completely covers the upper diffusion region 20, and a part thereof is exposed to the main surface 10a. That is, when the main surface 10a is viewed from the front, the lower diffusion region 30 is exposed to the main surface 10a in a region beyond the outer edge of the upper diffusion region 20 with respect to the formation center. In other words, when the main surface 10a is viewed from the front, the upper diffusion region 20, the lower diffusion region 30, and the N-conductivity type semiconductor region of the semiconductor substrate 10 are arranged in this order around the point where the axis A intersects the main surface 10a. It is formed in a concentric circle.

 上記したように、この半導体装置100では、上部拡散領域20のP導電型の半導体領域と、下部拡散領域30および半導体基板10におけるN導電型の半導体領域とがPN接合を形成してダイオードを成す。P導電型である上部拡散領域20はアノードとして機能し、N導電型である半導体基板10はカソードとして機能する。 As described above, in this semiconductor device 100, the P conductivity type semiconductor region of the upper diffusion region 20 and the lower diffusion region 30 and the N conductivity type semiconductor region of the semiconductor substrate 10 form a PN junction to form a diode. . The P diffusion type upper diffusion region 20 functions as an anode, and the N conductivity type semiconductor substrate 10 functions as a cathode.

 シリサイドブロック層40は絶縁膜であり、本実施形態では例えばSiOで形成されている。シリサイドブロック層40は、軸Aと主面10aとが交差する点を中心として円環状に形成されている。本実施形態における半導体装置100は、主面10aにおいて上部拡散領域20、下部拡散領域30が露出し、その外側に半導体基板10の半導体領域が露出している。シリサイドブロック層40は、上部拡散領域20の外縁部から下部拡散領域30を経て半導体基板10の半導体領域に至る面を覆うように形成されている。すなわち、主面10aに露出するP導電型の上部拡散領域20とN導電型の半導体領域とのPN接合線L1、および下部拡散領域30と半導体基板10との境界線L2を跨ぐように形成されている。 The silicide block layer 40 is an insulating film, and is formed of, for example, SiO 2 in this embodiment. The silicide block layer 40 is formed in an annular shape around the point where the axis A and the main surface 10a intersect. In the semiconductor device 100 according to the present embodiment, the upper diffusion region 20 and the lower diffusion region 30 are exposed on the main surface 10a, and the semiconductor region of the semiconductor substrate 10 is exposed outside thereof. The silicide block layer 40 is formed so as to cover the surface from the outer edge of the upper diffusion region 20 through the lower diffusion region 30 to the semiconductor region of the semiconductor substrate 10. That is, it is formed so as to straddle the PN junction line L1 between the P conductivity type upper diffusion region 20 and the N conductivity type semiconductor region exposed on the main surface 10a and the boundary line L2 between the lower diffusion region 30 and the semiconductor substrate 10. ing.

 なお、シリサイドブロック層40は、アノードとカソードについて電極として機能する、例えばコバルトを含むシリサイド電極を主面10aに積層して形成する際に、P導電型である上部拡散領域20と、N導電型である下部拡散領域30あるいは半導体基板10との間の電気的絶縁を維持する目的で形成されている。 The silicide block layer 40 functions as an electrode for the anode and the cathode. For example, when a silicide electrode containing cobalt is stacked on the main surface 10a, the silicide block layer 40 and the N diffusion type P diffusion region 20 are formed. It is formed for the purpose of maintaining electrical insulation between the lower diffusion region 30 and the semiconductor substrate 10.

 次に、図2~図6、および図1を参照して、半導体装置100の製造方法について説明する。 Next, a method for manufacturing the semiconductor device 100 will be described with reference to FIGS. 2 to 6 and FIG.

 最初に、図2に示すようにN導電型にされた半導体基板10を用意する。 First, as shown in FIG. 2, a semiconductor substrate 10 having N conductivity type is prepared.

 その後、直径がRとされた真円状にくり貫かれたフォトレジスト(図示せず)を主面10aに積層し、リンあるいはヒ素をイオン注入する。イオン注入は一面10aにおいて同一のエネルギーで実施し、注入深さを略一定とする。これにより、図3に示すように、直径がRとされたN導電型の下部注入領域31が形成される。つまり、軸Aを回転対称軸とする円盤状のN導電型領域が形成される。なお、下部注入領域31は、アニールにより拡散する前の領域であり、後述の2回のアニール工程後は下部拡散領域30となる。 Thereafter, a photoresist (not shown) cut into a perfect circle having a diameter of R is laminated on the main surface 10a, and phosphorus or arsenic is ion-implanted. The ion implantation is performed with the same energy on the one surface 10a, and the implantation depth is made substantially constant. As a result, as shown in FIG. 3, an N conductivity type lower implantation region 31 having a diameter R is formed. That is, a disk-shaped N conductivity type region having the axis A as the rotational symmetry axis is formed. The lower implantation region 31 is a region before being diffused by annealing, and becomes the lower diffusion region 30 after two annealing steps described later.

 下部注入領域31の形成後、図示しないフォトレジストを除去し、1回目のアニール工程を実施する。アニール工程により、図4に示すように下部注入領域31を形成する不純物が半導体基板10中を拡散する。なお、1回目のアニール工程では、下部注入領域31が熱拡散した不純物領域32は図1に示す下部拡散領域30程度には拡散しない。 After the formation of the lower implantation region 31, the photoresist (not shown) is removed and a first annealing process is performed. By the annealing process, impurities forming the lower implantation region 31 diffuse in the semiconductor substrate 10 as shown in FIG. In the first annealing step, the impurity region 32 in which the lower implantation region 31 is thermally diffused does not diffuse as much as the lower diffusion region 30 shown in FIG.

 1回目のアニール工程の後、下部注入領域31と同じ中心を有し、図4に示す不純物領域32よりも直径の小さい真円状にくり貫かれたフォトレジスト(図示せず)を主面10aに積層し、ホウ素をイオン注入する。イオン注入は一面10aにおいて同一のエネルギーで実施し、注入深さを略一定とする。これにより、図5に示すように、不純物領域32に取り囲まれたP導電型の上部注入領域21が形成される。つまり、軸Aを回転対称軸とする円盤状のP導電型領域が形成される。なお、上部注入領域21は、アニールにより拡散する前の領域であり、後述の2回目のアニール工程後は上部拡散領域20となる。 After the first annealing step, a photoresist (not shown) having the same center as that of the lower implantation region 31 and having a smaller diameter than the impurity region 32 shown in FIG. And boron is ion-implanted. The ion implantation is performed with the same energy on the one surface 10a, and the implantation depth is made substantially constant. As a result, as shown in FIG. 5, a P conductivity type upper implantation region 21 surrounded by the impurity region 32 is formed. That is, a disk-shaped P conductivity type region having the axis A as a rotationally symmetric axis is formed. The upper implantation region 21 is a region before being diffused by annealing, and becomes the upper diffusion region 20 after the second annealing step described later.

 上部注入領域21の形成後、図示しないフォトレジストを除去し、2回目のアニール工程を実施する。2回目のアニール工程により、図6に示すように上部注入領域21が熱拡散するとともに、下部注入領域31がある程度拡散した不純物領域32がさらに熱拡散する。2回目のアニール工程を実施した後の上部注入領域21は上部拡散領域20に相当する領域に至るまで拡散し、下部注入領域31は下部拡散領域30に相当する領域まで拡散する。 After the formation of the upper implantation region 21, the photoresist (not shown) is removed and a second annealing step is performed. By the second annealing step, the upper implantation region 21 is thermally diffused as shown in FIG. 6, and the impurity region 32 in which the lower implantation region 31 is diffused to some extent is further thermally diffused. After performing the second annealing step, the upper implantation region 21 diffuses to a region corresponding to the upper diffusion region 20, and the lower implantation region 31 diffuses to a region corresponding to the lower diffusion region 30.

 なお、熱拡散後の下部拡散領域30の形成深さは、下部注入領域31のイオン注入の直径Rと略同一になるように設計することが好ましい。アニール温度やイオン注入のエネルギーおよび不純物濃度は半導体基板10に形成される他の素子との工程共通化などによりパラメータが決められることが有り得、値の変更が困難な場合がある。このため、下部拡散領域30の形成深さを下部注入領域31のイオン注入の直径Rと略同一になるように設計するとは、下部注入領域31の形成半径を、想定される下部拡散領域30の形成深さに合わせることを意味する。 It should be noted that the formation depth of the lower diffusion region 30 after thermal diffusion is preferably designed to be substantially the same as the ion implantation diameter R of the lower implantation region 31. Parameters for the annealing temperature, ion implantation energy, and impurity concentration may be determined by making the process common with other elements formed on the semiconductor substrate 10, and it may be difficult to change the values. For this reason, if the formation depth of the lower diffusion region 30 is designed to be substantially the same as the ion implantation diameter R of the lower implantation region 31, the formation radius of the lower implantation region 31 is set to be the same as that of the assumed lower diffusion region 30. It means to match the formation depth.

 ところで、2回目のアニール工程を実施する前において、下部注入領域31に起因する不純物領域32の不純物濃度は、軸A上であって上部注入領域21よりも深い位置にピークが存在する。このため、2回目のアニール工程を経て上部注入領域21が熱拡散する際には、円盤状の上部注入領域21の中央近傍は導電型が反転しにくい。これにより、2回目のアニール工程を実施した後、図6に示すように、上部拡散領域20の軸Aを通る断面形状は、図1に示すように、軸A近傍ほど窪んだ構造になっている。すなわち、上部拡散領域20は中央が凹んだ円盤状に形成されている。すなわち、上部拡散領域20と下部拡散領域30のPN接合面Sは、上部拡散領域20を主体とすれば凹面形状を成す。 Incidentally, before the second annealing step is performed, the impurity concentration of the impurity region 32 caused by the lower implantation region 31 has a peak at a position on the axis A and deeper than the upper implantation region 21. For this reason, when the upper implantation region 21 is thermally diffused through the second annealing step, the conductivity type is unlikely to be reversed in the vicinity of the center of the disk-shaped upper implantation region 21. Thus, after performing the second annealing step, as shown in FIG. 6, the cross-sectional shape passing through the axis A of the upper diffusion region 20 becomes a structure that is recessed toward the vicinity of the axis A as shown in FIG. 1. Yes. That is, the upper diffusion region 20 is formed in a disk shape with a recessed center. That is, the PN junction surface S between the upper diffusion region 20 and the lower diffusion region 30 has a concave shape when the upper diffusion region 20 is mainly used.

 なお、図6において下部拡散領域30に示した等高線は、不純物濃度の等高線を示しており、下部拡散領域30における不純物濃度のピークが、上部拡散領域20における凹みの下部に位置していることを示している。 Note that the contour lines shown in the lower diffusion region 30 in FIG. 6 indicate the contour lines of the impurity concentration, and that the peak of the impurity concentration in the lower diffusion region 30 is located below the dent in the upper diffusion region 20. Show.

 2回目のアニール工程の後、図1に示すように、主面10aに露出するP導電型の上部拡散領域20とN導電型の半導体領域とのPN接合線L1、および下部拡散領域30と半導体基板10との境界線L2を跨ぐようにシリサイドブロック層40を形成する。 After the second annealing step, as shown in FIG. 1, the PN junction line L1 between the P conductivity type upper diffusion region 20 and the N conductivity type semiconductor region exposed on the main surface 10a, and the lower diffusion region 30 and the semiconductor The silicide block layer 40 is formed so as to straddle the boundary line L2 with the substrate 10.

 以上の工程を含む製造方法を以って、半導体装置100を製造することができる。 The semiconductor device 100 can be manufactured by a manufacturing method including the above steps.

 次に、本実施形態における半導体装置100およびその製造方法について作用効果を説明する。 Next, functions and effects of the semiconductor device 100 and the manufacturing method thereof in the present embodiment will be described.

 図1および図6に示す半導体装置100は、上部拡散領域20および下部拡散領域30が軸Aに対して略回転対称に形成されているので、それぞれの不純物プロファイルも軸Aに対して略回転対称となる。発明者は、具体的な不純物プロファイルを、コンピュータを用いてシミュレーションした。シミュレーションの結果を図7に示す。 In the semiconductor device 100 shown in FIGS. 1 and 6, since the upper diffusion region 20 and the lower diffusion region 30 are formed in substantially rotational symmetry with respect to the axis A, the respective impurity profiles are also substantially rotationally symmetric with respect to the axis A. It becomes. The inventor simulated a specific impurity profile using a computer. The simulation results are shown in FIG.

 図7に示すように、ダイオード形成領域Di内に形成された下部拡散領域30において、不純物濃度が極大となる極大点Pを有している。本実施形態では、とくに下部拡散領域30内にただ一つの極大点Pを有している。本実施形態における極大点Pは軸A上にあって、PN接合面Sの下部に位置する。 As shown in FIG. 7, the lower diffusion region 30 formed in the diode formation region Di has a maximum point P at which the impurity concentration is maximum. In this embodiment, in particular, there is only one maximum point P in the lower diffusion region 30. The maximum point P in the present embodiment is on the axis A and is located below the PN junction surface S.

 一般に、PN接合ツェナーダイオードにおいては、逆バイアスが印加されるとき、N導電型の領域とP導電型の領域の、それぞれ不純物濃度の高い部分の間で電界が大きくなり降伏現象を生じやすい。本実施形態における半導体装置100にあっては、N導電性を示す下部拡散領域30の不純物濃度の高い部分が、従来のように3次元的に分布するのではなく、0次元(点)として規定されているので、降伏現象が生じる部分を点として特定することができる。すなわち、半導体装置100における降伏現象は、その発生位置をほぼ所定の位置(極大点P)で固定することができる。 In general, in a PN junction Zener diode, when a reverse bias is applied, an electric field is increased between portions with high impurity concentrations in an N conductivity type region and a P conductivity type region, and a breakdown phenomenon is likely to occur. In the semiconductor device 100 according to the present embodiment, the high impurity concentration portion of the lower diffusion region 30 exhibiting N conductivity is not three-dimensionally distributed as in the prior art, but is defined as zero dimension (point). Therefore, it is possible to identify the portion where the yield phenomenon occurs as a point. That is, the yielding phenomenon in the semiconductor device 100 can be fixed at a substantially predetermined position (maximum point P).

 ツェナー電圧の経時的な変動量を大きくする原因は、降伏現象の発生源が3次元的に分布することで降伏現象の発生が不定であることにあると推察されているが、本実施形態における半導体装置100では、降伏現象の発生位置を点として定めることができる。これによれば、従来のように3次元的に降伏現象が生じる構成に較べて、降伏現象の発生位置を制限することができ、図8に示すように、ツェナー電圧の経時的な変動を従来に較べて抑制することができる。そして、例えば、半導体装置100に含まれるツェナーダイオードを定圧電源に採用すれば、出力電圧を時間経過によらず高精度に制御することができる。 The cause of increasing the amount of fluctuation of the Zener voltage over time is presumed to be that the generation of the breakdown phenomenon is indefinite because the generation source of the breakdown phenomenon is distributed three-dimensionally. In the semiconductor device 100, the occurrence position of the breakdown phenomenon can be determined as a point. According to this, as compared with the conventional configuration in which the breakdown phenomenon occurs three-dimensionally, the generation position of the breakdown phenomenon can be limited. As shown in FIG. It can be suppressed compared to. For example, when a Zener diode included in the semiconductor device 100 is used as a constant voltage power source, the output voltage can be controlled with high accuracy regardless of the passage of time.

 また、本実施形態に係る半導体装置100は、上部拡散領域20を主体としたとき、PN接合面Sが窪んだ凹面構造となっている。とくに本実施形態では軸A近傍で窪んだ構造となっている。これによれば、図7に示すように、下部拡散領域30における、上部拡散領域20の窪んだ部分の下部でピークを持つような不純物分布を形成させやすくできる。換言すれば、不純物濃度の極大を点状に形成しやすくできる。 Further, the semiconductor device 100 according to the present embodiment has a concave structure in which the PN junction surface S is recessed when the upper diffusion region 20 is mainly used. In particular, in this embodiment, the structure is recessed near the axis A. According to this, as shown in FIG. 7, it is possible to easily form an impurity distribution having a peak in the lower diffusion region 30 at the lower portion of the recessed portion of the upper diffusion region 20. In other words, the maximum impurity concentration can be easily formed in a dot shape.

 また、本実施形態に係る半導体装置100は、上部拡散領域20および下部拡散領域30が、一面10aを正面視したときに回転対称形状、特には真円状になっている。これによれば、下部拡散領域30における不純物濃度の極大を回転対称軸(本実施形態では軸A)上にすることができ、不純物濃度の極大を点状に形成しやすくできる。 Further, in the semiconductor device 100 according to the present embodiment, the upper diffusion region 20 and the lower diffusion region 30 have a rotationally symmetric shape, particularly a perfect circle shape, when the one surface 10a is viewed from the front. According to this, the maximum of the impurity concentration in the lower diffusion region 30 can be on the rotational symmetry axis (axis A in the present embodiment), and the maximum of the impurity concentration can be easily formed in a dot shape.

 また、本実施形態に係る半導体装置100は、その製造工程において、下部拡散領域30の前駆領域である下部注入領域31の形成直径Rを、下部拡散領域30の想定される形成深さと略同一にする。これによれば、下部拡散領域30における不純物濃度の極大を点状に形成しやすくできる。例えば、下部注入領域31の形成直径Rが下部拡散領域30の想定される形成深さよりも大きいと、不純物濃度の極大部分は主面10aに沿う方向に延びた1次元あるいは2次元的に分布しやすい。あるいは、下部注入領域31の形成直径Rが下部拡散領域30の想定される形成深さよりも小さいと、不純物濃度の極大部分は半導体基板10の深さ方向に延びた1次元あるいは2次元的に分布しやすい。これに対して、下部注入領域31の形成直径Rを、下部拡散領域30の想定される形成深さと略同一にすると、下部拡散領域30における不純物濃度の極大を点状に形成しやすくできる。 In addition, in the manufacturing process of the semiconductor device 100 according to the present embodiment, the formation diameter R of the lower implantation region 31 that is a precursor region of the lower diffusion region 30 is substantially the same as the assumed formation depth of the lower diffusion region 30. To do. According to this, the maximum of the impurity concentration in the lower diffusion region 30 can be easily formed in a dot shape. For example, when the formation diameter R of the lower implantation region 31 is larger than the assumed formation depth of the lower diffusion region 30, the maximum impurity concentration is distributed one-dimensionally or two-dimensionally extending in the direction along the main surface 10a. Cheap. Alternatively, when the formation diameter R of the lower implantation region 31 is smaller than the assumed formation depth of the lower diffusion region 30, the maximum impurity concentration is distributed one-dimensionally or two-dimensionally extending in the depth direction of the semiconductor substrate 10. It's easy to do. On the other hand, when the formation diameter R of the lower implantation region 31 is substantially the same as the assumed formation depth of the lower diffusion region 30, the maximum impurity concentration in the lower diffusion region 30 can be easily formed in a dot shape.

 また、本実施形態に係る半導体装置100は、その製造工程、とくに上部注入領域21の形成において、均一な深さで不純物をイオン注入する。これによれば、2回目のアニール工程において、下部拡散領域30の前駆領域である不純物領域32における不純物濃度が小さい部分で導電型を反転させやすくなり、PN接合面Sの凹面構造を形成しやすくできる。つまり、上記したように、下部拡散領域30の不純物濃度の極大を点状に形成しやすくできる。 Further, the semiconductor device 100 according to the present embodiment ion-implants impurities with a uniform depth in the manufacturing process, particularly in the formation of the upper implantation region 21. According to this, in the second annealing step, the conductivity type is easily reversed at the portion where the impurity concentration in the impurity region 32 which is the precursor region of the lower diffusion region 30 is low, and the concave structure of the PN junction surface S can be easily formed. it can. That is, as described above, the maximum impurity concentration of the lower diffusion region 30 can be easily formed in a dot shape.

 さらに、本実施形態に係る半導体装置100は、下部拡散領域30が上部拡散領域20を覆うように形成され、主面10aに露出している。これによれば、主面10aの表層において、P導電型の上部拡散領域20と、N導電型の領域との間に形成される空乏層の主面10aに沿う方向の広がりを、下部拡散領域30が主面に露出していない構成に較べて抑制することができる。これにより、主面10a近傍に存在する表面欠陥に起因する準位に、ホットキャリアがトラップされることを抑制でき、ツェナー電圧の経時的変動量を抑制することができる。 Furthermore, in the semiconductor device 100 according to the present embodiment, the lower diffusion region 30 is formed so as to cover the upper diffusion region 20, and is exposed to the main surface 10a. According to this, in the surface layer of the main surface 10a, the depletion layer formed between the P conductivity type upper diffusion region 20 and the N conductivity type region extends in the direction along the main surface 10a. 30 can be suppressed as compared with a configuration in which the main surface is not exposed. Thereby, it is possible to suppress trapping of hot carriers at a level caused by surface defects existing in the vicinity of the main surface 10a, and it is possible to suppress an amount of fluctuation of the Zener voltage with time.

 ところで、本実施形態に係る半導体装置100は主面10aにシリサイドブロック層40を備えている。これによれば、シリサイド電極を主面10aに積層して形成する際に、P導電型である上部拡散領域20と、N導電型である下部拡散領域30あるいは半導体基板10との間で、シリサイドによる電気的導通が生じることを防止できる。このような目的のため、シリサイドブロック層40は、下部拡散領域30が主面10aに露出している場合は、上部拡散領域20と下部拡散領域30のPN接合線L1を跨ぐように形成されるとともに、下部拡散領域30と半導体基板10における半導体領域との境界線L2を跨ぐように形成されるべきである。また、下部拡散領域30が主面10aに露出していない場合は、上部拡散領域20と半導体基板10における半導体領域との境界線を跨ぐように形成されるべきである。 Incidentally, the semiconductor device 100 according to the present embodiment includes the silicide block layer 40 on the main surface 10a. According to this, when the silicide electrode is stacked on the main surface 10a, the silicide is formed between the P diffusion type upper diffusion region 20 and the N conductivity type lower diffusion region 30 or the semiconductor substrate 10. It is possible to prevent electrical continuity due to. For this purpose, the silicide block layer 40 is formed so as to straddle the PN junction line L1 between the upper diffusion region 20 and the lower diffusion region 30 when the lower diffusion region 30 is exposed to the main surface 10a. At the same time, it should be formed so as to straddle the boundary line L <b> 2 between the lower diffusion region 30 and the semiconductor region in the semiconductor substrate 10. Further, when the lower diffusion region 30 is not exposed to the main surface 10 a, it should be formed so as to straddle the boundary line between the upper diffusion region 20 and the semiconductor region in the semiconductor substrate 10.

 (第2実施形態)
 第1実施形態においては、上部拡散領域20を主体としたとき、上部拡散領域20と下部拡散領域30とのPN接合面Sが凹面である例を示したが、凸面であっても良い。
(Second Embodiment)
In the first embodiment, when the upper diffusion region 20 is mainly used, the PN junction surface S between the upper diffusion region 20 and the lower diffusion region 30 is a concave surface, but a convex surface may be used.

 本実施形態における半導体装置110は、図9に示すように、第1実施形態とは異なる形状の上部拡散領域50および下部拡散領域60を備えている。半導体装置110はPN接合面Sの断面において凸面となる凸面部Cを有している。半導体装置110も、主面10aから正面視したときの上部拡散領域50および下部拡散領域60の形状は真円状であり、該真円の中心を通り主面10aに直交する軸Bを対称軸とする回転体を成している。凹面部Cは軸B上に凸面の頂点を有する。 The semiconductor device 110 in this embodiment includes an upper diffusion region 50 and a lower diffusion region 60 having shapes different from those in the first embodiment, as shown in FIG. The semiconductor device 110 has a convex surface portion C that becomes a convex surface in the cross section of the PN junction surface S. Also in the semiconductor device 110, the shape of the upper diffusion region 50 and the lower diffusion region 60 when viewed from the main surface 10a is a perfect circle, and an axis B passing through the center of the perfect circle and orthogonal to the main surface 10a is an axis of symmetry. A rotating body is formed. The concave portion C has a convex vertex on the axis B.

 本実施形態において、下部拡散領域60の不純物濃度は、PN接合面Sの凸面部Cよりも外側に形成された凹面部の下部近傍にピークを有する。すなわち、図9に示す断面においては、点P1および点P2に示す点に不純物濃度の極大点を有している。実際には、上部拡散領域50および下部拡散領域60は円盤状であるから、極大点P1,P2も軸Bを対称軸とする円の一部である。つまり、本実施形態における下部拡散領域60の不純物濃度の極大点は、複数の極大点が軸Bの周りに1次元的(具体的には円状)に分布している。 In this embodiment, the impurity concentration of the lower diffusion region 60 has a peak in the vicinity of the lower portion of the concave surface portion formed outside the convex surface portion C of the PN junction surface S. That is, the cross section shown in FIG. 9 has the maximum point of impurity concentration at the points indicated by points P1 and P2. Actually, since the upper diffusion region 50 and the lower diffusion region 60 are disk-shaped, the maximum points P1 and P2 are also part of a circle having the axis B as the symmetry axis. That is, as for the maximum points of the impurity concentration of the lower diffusion region 60 in the present embodiment, a plurality of maximum points are distributed around the axis B in a one-dimensional manner (specifically, in a circular shape).

 このように、PN接合面Sを凸面形状にすることによって、下部拡散領域60の不純物濃度の極大点を1次元的に分布させることができる。第1実施形態と同様、不純物濃度の極大点は降伏現象の発生位置として有力であるから、半導体装置110においては降伏現象の発生位置を線として定めることができる。これによれば、従来のように3次元的に降伏現象が生じる構成に較べて、降伏現象の発生位置を制限することができ、ツェナー電圧の経時的な変動を抑制することができる。そして、例えば、半導体装置110に含まれるツェナーダイオードを定圧電源に採用すれば、出力電圧を時間経過によらず高精度に制御することができる。 Thus, by making the PN junction surface S convex, the maximum points of the impurity concentration of the lower diffusion region 60 can be distributed one-dimensionally. Similar to the first embodiment, since the maximum point of the impurity concentration is effective as the occurrence position of the breakdown phenomenon, the occurrence position of the breakdown phenomenon can be defined as a line in the semiconductor device 110. According to this, as compared with the conventional configuration in which the breakdown phenomenon occurs three-dimensionally, the generation position of the breakdown phenomenon can be limited, and the variation of the Zener voltage with time can be suppressed. For example, when a Zener diode included in the semiconductor device 110 is employed as a constant voltage power source, the output voltage can be controlled with high accuracy regardless of the passage of time.

 以下、半導体装置110の製造方法について簡単に説明する。 Hereinafter, a method for manufacturing the semiconductor device 110 will be briefly described.

 先ず、第1実施形態と同様に、図2に示すがごとく半導体基板10を用意する。 First, as in the first embodiment, a semiconductor substrate 10 is prepared as shown in FIG.

 次いで、図10に示すように、リンあるいはヒ素をイオン注入して下部注入領域61を形成する。下部注入領域61を、軸Bを対称軸とした回転対称形状に形成する。特に、本実施形態においては、円環状に形成する。第1実施形態における下部注入領域31は主面10aから正面視すると真円であったが、本実施形態における下部注入領域61は、中心付近がくり貫かれた円環状である。なお、図10は断面図であるから2つの下部注入領域61が離間するように図示しているが、実際は紙面前後方向において連続している。下部注入領域61は後工程の2回の熱拡散により下部拡散領域60となる領域である。 Next, as shown in FIG. 10, phosphorus or arsenic is ion-implanted to form a lower implantation region 61. The lower injection region 61 is formed in a rotationally symmetric shape with the axis B as the axis of symmetry. In particular, in the present embodiment, it is formed in an annular shape. The lower injection region 31 in the first embodiment is a perfect circle when viewed from the main surface 10a, but the lower injection region 61 in the present embodiment is an annular shape in which the vicinity of the center is hollowed out. Since FIG. 10 is a cross-sectional view, the two lower injection regions 61 are illustrated as being separated from each other, but are actually continuous in the front-rear direction of the paper. The lower implantation region 61 is a region that becomes the lower diffusion region 60 by two thermal diffusions in a later process.

 次いで、1回目のアニール工程を実施する。これにより、図11に示すように、下部注入領域61は熱拡散してN導電型の不純物領域62が形成される。アニール工程前の下部注入領域61は円環状なので、熱拡散後の不純物領域62における不純物の濃度構造は、より高濃度の部分が軸Bを対称軸とする円状に分布する略トーラス構造となっている。 Next, the first annealing step is performed. As a result, as shown in FIG. 11, the lower implantation region 61 is thermally diffused to form an N conductivity type impurity region 62. Since the lower implantation region 61 before the annealing step is annular, the impurity concentration structure in the impurity region 62 after the thermal diffusion is a substantially torus structure in which the higher concentration portion is distributed in a circle having the axis B as the symmetry axis. ing.

 次いで、図12に示すように、ホウ素をイオン注入して上部注入領域51を形成する。上部注入領域51は不純物領域62に内包されるように形成する。具体的には、下部拡散領域60の前駆領域である不純物領域61において濃度がピークとなる部分の上部に上部注入領域51を形成する。つまり、上部注入領域51は軸Bを対称軸とした回転対称形状に形成される。特に、本実施形態においては、上部注入領域51は円環状に形成される。第1実施形態における上部注入領域21は主面10aから正面視すると真円であったが、本実施形態における上部注入領域51は、中心付近がくり貫かれた円環状である。なお、図12は断面図であるから2つの上部注入領域51が離間するように図示しているが、実際は紙面前後方向において連続している。上部注入領域51は後工程の2回の熱拡散により上部拡散領域50となる領域である。 Next, as shown in FIG. 12, boron is ion-implanted to form an upper implantation region 51. The upper implantation region 51 is formed so as to be included in the impurity region 62. Specifically, the upper implantation region 51 is formed on the upper portion of the impurity region 61 that is the precursor region of the lower diffusion region 60 where the concentration reaches a peak. That is, the upper injection region 51 is formed in a rotationally symmetric shape with the axis B as the axis of symmetry. In particular, in the present embodiment, the upper injection region 51 is formed in an annular shape. The upper injection region 21 in the first embodiment is a perfect circle when viewed from the main surface 10a, but the upper injection region 51 in the present embodiment has an annular shape in which the vicinity of the center is hollowed out. Since FIG. 12 is a cross-sectional view, the two upper injection regions 51 are illustrated so as to be separated from each other, but are actually continuous in the front-rear direction of the drawing. The upper implantation region 51 is a region that becomes the upper diffusion region 50 by two thermal diffusions in a later step.

 次いで、2回目のアニール工程を実施する。これにより、図9に示すように、上部注入領域51が熱拡散するとともに、下部注入領域61がある程度拡散した不純物領域62がさらに熱拡散する。2回目のアニール工程を実施した後の上部注入領域51は上部拡散領域50に相当する領域に至るまで拡散し、下部注入領域61は下部拡散領域60に相当する領域まで拡散する。 Next, a second annealing step is performed. As a result, as shown in FIG. 9, the upper implantation region 51 is thermally diffused, and the impurity region 62 in which the lower implantation region 61 is diffused to some extent is further thermally diffused. The upper implantation region 51 after the second annealing step is diffused to a region corresponding to the upper diffusion region 50, and the lower implantation region 61 is diffused to a region corresponding to the lower diffusion region 60.

 このとき、下部拡散領域60の前駆領域である不純物領域62の不純物濃度分布のトーラス形状はほぼ維持され、下部拡散領域60の不純物濃度の極大は、上記したような円形状に構成されることになる。主面10aに露出するP導電型の上部拡散領域50とN導電型の半導体領域とのPN接合線、および下部拡散領域60と半導体基板10との境界線を跨ぐようにシリサイドブロック層40を形成する。 At this time, the torus shape of the impurity concentration distribution of the impurity region 62 which is a precursor region of the lower diffusion region 60 is substantially maintained, and the maximum impurity concentration of the lower diffusion region 60 is configured in the circular shape as described above. Become. The silicide block layer 40 is formed so as to straddle the PN junction line between the P conductivity type upper diffusion region 50 exposed on the main surface 10a and the N conductivity type semiconductor region, and the boundary line between the lower diffusion region 60 and the semiconductor substrate 10. To do.

 以上のようにして、PN接合面Sが凸面となる半導体装置110を製造することができる。 As described above, the semiconductor device 110 in which the PN junction surface S is a convex surface can be manufactured.

 (第3実施形態)
 第1実施形態および第2実施形態に例示したような下部拡散領域30,60を有する構成においては、ブレークダウンが発生した際の空乏層が、半導体基板10の表層における下部拡散領域30,60の外側の広い領域まで及ぶ場合がある。これは、半導体装置10の表層における表面トラップに起因すると推察され、アノードとしての上部拡散領域20,50とカソードとの間の電流経路の電気抵抗の上昇が生じる。そして、この電気抵抗の上昇は、ツェナー電圧の経時的変動の要因となる虞がある。
(Third embodiment)
In the configuration having the lower diffusion regions 30 and 60 exemplified in the first embodiment and the second embodiment, the depletion layer when the breakdown occurs is the lower diffusion regions 30 and 60 in the surface layer of the semiconductor substrate 10. May extend to a wide area outside. This is presumed to be caused by surface traps in the surface layer of the semiconductor device 10, and an increase in the electrical resistance of the current path between the upper diffusion regions 20 and 50 as the anode and the cathode occurs. This increase in electrical resistance may cause a change in Zener voltage with time.

 そこで、本実施形態における半導体装置120は、図13に示すように、上部拡散領域70と下部拡散領域80に加えて、ダイオード形成領域Di内において、半導体基板10よりも不純物濃度が高くされたカソード領域90と、アノードとして機能する上部拡散領域70とカソード領域90との間に形成された極間領域91を備えている。なお、カソード領域90は、対極領域に相当する。 Therefore, as shown in FIG. 13, the semiconductor device 120 according to the present embodiment has a cathode whose impurity concentration is higher than that of the semiconductor substrate 10 in the diode formation region Di in addition to the upper diffusion region 70 and the lower diffusion region 80. A region 90 and an inter-electrode region 91 formed between the upper diffusion region 70 functioning as an anode and the cathode region 90 are provided. The cathode region 90 corresponds to a counter electrode region.

 本実施形態における上部拡散領域70および下部拡散領域80は、それぞれ、第1実施形態における上部拡散領域20および下部拡散領域30と同様に形成されている。すなわち、上部拡散領域70は、主面10aに露出するように形成されたP導電型の半導体領域であり、下部拡散領域80は、半導体基板10内において上部拡散領域70を覆うように形成されたN導電型の半導体領域である。詳しい構造は第1実施形態において説明しているので省略するが、本実施形態においても、上部拡散領域70と下部拡散領域80とのPN接合面Sは凹面形状となっており、ブレークポイントがほぼ点(0次元)として形成されるように、構造的に制御されている。 The upper diffusion region 70 and the lower diffusion region 80 in the present embodiment are formed in the same manner as the upper diffusion region 20 and the lower diffusion region 30 in the first embodiment, respectively. That is, the upper diffusion region 70 is a P conductivity type semiconductor region formed so as to be exposed on the main surface 10 a, and the lower diffusion region 80 is formed so as to cover the upper diffusion region 70 in the semiconductor substrate 10. This is an N conductivity type semiconductor region. Although a detailed structure has been described in the first embodiment, it will be omitted. However, in this embodiment as well, the PN junction surface S between the upper diffusion region 70 and the lower diffusion region 80 has a concave shape, and the breakpoint is almost the same. It is structurally controlled to be formed as a point (0 dimension).

 対極領域たるカソード領域90は、半導体基板10よりも高濃度のN導電型の半導体領域であり、主面10aを正面視したときに、上部拡散領域70と同心円の円環状の領域となっている。カソード領域90は主面10aに露出しており、その露出面においてカソード電極がオーミック接合されている。なお、本実施形態では、カソード領域90と下部拡散領域80とが同一の工程によって形成されており、平均した不純物濃度は略同一になっている。 The cathode region 90 which is a counter electrode region is an N conductivity type semiconductor region having a concentration higher than that of the semiconductor substrate 10 and is an annular region concentric with the upper diffusion region 70 when the main surface 10a is viewed from the front. . Cathode region 90 is exposed at main surface 10a, and the cathode electrode is in ohmic contact with the exposed surface. In the present embodiment, the cathode region 90 and the lower diffusion region 80 are formed by the same process, and the average impurity concentration is substantially the same.

 極間領域91は、上部拡散領域70とカソード領域90との間に形成されたN導電型の半導体領域である。極間領域91は、不純物濃度が半導体基板10の不純物濃度よりも高くされている。極間領域91は主面10aに露出するように形成されており、これにより、カソード領域90に囲まれた領域は、その主面10aにおいて、半導体基板10を構成するN導電型の領域は露出していない。換言すれば、主面10aにおいて、上部拡散領域70の中心から見た動径方向の不純物の分布は、上部拡散領域70のP導電型、主面10aに露出した下部拡散領域80のN導電型、極間領域91のN導電型、カソード領域90のN導電型の順で同心円状に広がっている。 The interelectrode region 91 is an N conductivity type semiconductor region formed between the upper diffusion region 70 and the cathode region 90. The interelectrode region 91 has an impurity concentration higher than that of the semiconductor substrate 10. The inter-electrode region 91 is formed so as to be exposed on the main surface 10a, whereby the region surrounded by the cathode region 90 is exposed on the main surface 10a of the N conductivity type region constituting the semiconductor substrate 10. Not done. In other words, on the main surface 10a, the distribution of the radial impurities seen from the center of the upper diffusion region 70 is the P conductivity type of the upper diffusion region 70 and the N conductivity type of the lower diffusion region 80 exposed on the main surface 10a. In addition, the N conductivity type of the inter-electrode region 91 and the N conductivity type of the cathode region 90 are spread concentrically.

 本実施形態の半導体装置120では、極間領域91が、下部拡散領域80やカソード領域90を形成する工程とは別の工程として形成されるものである。よって、極間領域91の不純物濃度は、下部拡散領域80やカソード領域90とは独立して制御可能であり、設計者の意図に基づいて決定される。極間領域91の不純物濃度は、カソード電極が接続されるカソード領域90よりも低濃度とすることが必要であり、半導体基板10よりも高濃度であって、且つ、下部拡散領域80の不純物濃度の最大値よりも低濃度とすることが好ましい。本実施形態における下部拡散領域80の不純物濃度が最大となる場所は不純物濃度の極大点であり、ほぼ点(0次元)として形成されてブレークポイントとなる。極間領域91の不純物濃度は、このブレークポイントよりも低濃度とされる。これにより、極間領域91の近傍でのブレークダウンを防止している。換言すれば、下部拡散領域80において、意図的にブレークダウンを発生させるようになっている。 In the semiconductor device 120 of the present embodiment, the interelectrode region 91 is formed as a separate process from the process of forming the lower diffusion region 80 and the cathode region 90. Therefore, the impurity concentration in the inter-electrode region 91 can be controlled independently of the lower diffusion region 80 and the cathode region 90, and is determined based on the intention of the designer. The impurity concentration of the interelectrode region 91 needs to be lower than that of the cathode region 90 to which the cathode electrode is connected, is higher than that of the semiconductor substrate 10, and is impurity concentration of the lower diffusion region 80. Preferably, the concentration is lower than the maximum value. The place where the impurity concentration of the lower diffusion region 80 in the present embodiment is the maximum is the maximum point of the impurity concentration, which is formed as a point (zero dimension) and becomes a breakpoint. The impurity concentration in the inter-electrode region 91 is set lower than this breakpoint. Thereby, breakdown in the vicinity of the inter-electrode region 91 is prevented. In other words, breakdown is intentionally generated in the lower diffusion region 80.

 半導体装置120の製造方法について、第1実施形態における半導体装置100の製造方法に関する記述を引用しつつ、図14~図16を参照して説明する。 The method for manufacturing the semiconductor device 120 will be described with reference to FIGS. 14 to 16 with reference to the description regarding the method for manufacturing the semiconductor device 100 in the first embodiment.

 まず、N導電型とされた半導体基板10を用意する。 First, a semiconductor substrate 10 having N conductivity type is prepared.

 その後、図14に示すように、第1実施形態と同様、イオン注入によって下部注入領域81を形成する。このとき、下部注入領域81と同一または別の工程によって、対極注入領域92を形成する。下部注入領域81と対極注入領域92はともに主面10aの表層に形成される。これらの領域はそれぞれ、後述のアニール工程によって下部拡散領域80とカソード領域90になる領域である。 Thereafter, as shown in FIG. 14, the lower implantation region 81 is formed by ion implantation, as in the first embodiment. At this time, the counter electrode injection region 92 is formed by the same or different process as the lower injection region 81. Both lower injection region 81 and counter electrode injection region 92 are formed in the surface layer of main surface 10a. These regions are regions that become the lower diffusion region 80 and the cathode region 90 by an annealing process described later.

 その後、アニール工程を実行して不純物の熱拡散を行う。図15に示すように、アニール工程によって、下部注入領域81と対極注入領域92は、不純物が半導体基板10内を拡散して半導体基板10よりも高濃度の半導体領域を形成する。 Then, an annealing process is performed to thermally diffuse impurities. As shown in FIG. 15, in the lower implantation region 81 and the counter electrode implantation region 92, impurities are diffused in the semiconductor substrate 10 to form a semiconductor region having a higher concentration than the semiconductor substrate 10 by the annealing process.

 その後、下部注入領域81がアニール工程によって熱拡散した領域にイオン注入して、P導電型の上部注入領域71を形成する。さらに、下部注入領域81と対極注入領域92とに囲まれた主面10aの表層にイオン注入して、N導電型の極間注入領域93を形成する。 Thereafter, ions are implanted into the region where the lower implantation region 81 is thermally diffused by the annealing process, thereby forming a P conductivity type upper implantation region 71. Further, ions are implanted into the surface layer of the main surface 10 a surrounded by the lower implantation region 81 and the counter electrode implantation region 92 to form an N conductivity type interelectrode implantation region 93.

 その後、再びアニール工程を実施して各半導体領域の不純物を熱拡散させる。これにより、不純物の分布は、図13に示すような分布となる。その後、シリサイドブロック層40を円環状に形成して半導体装置120が製造される。シリサイドブロック層40は、円環の内縁が上部拡散領域70にかかるようになっているとともに、円環の外縁がカソード領域90にかかるようになっている。つまり、主面10aにおける下部拡散領域80の露出部と極間領域91は、シリサイドブロック層40によって完全に隠されている。 Thereafter, an annealing process is performed again to thermally diffuse impurities in each semiconductor region. As a result, the impurity distribution is as shown in FIG. Thereafter, the silicide block layer 40 is formed in an annular shape, and the semiconductor device 120 is manufactured. The silicide block layer 40 has an annular inner edge that covers the upper diffusion region 70 and an annular outer edge that covers the cathode region 90. That is, the exposed portion of the lower diffusion region 80 and the inter-electrode region 91 in the main surface 10 a are completely hidden by the silicide block layer 40.

 本実施形態における半導体装置120を採用することによる作用効果について説明する。 The effect by adopting the semiconductor device 120 in this embodiment will be described.

 上記した通り、ブレークダウンが発生した際の空乏層が、半導体基板10の表層における下部拡散領域30,60の外側の広い領域まで及ぶ場合があり、これは、半導体装置10の表層における表面トラップに起因すると推察されている。半導体装置120は、カソード領域90を備えるとともに、半導体基板10aにおいて、半導体基板10を構成するN導電型の不純物層が露出しないように、半導体基板10よりも高濃度の極間領域91を備えている。これにより、上部拡散領域70から延びる空乏層が極間領域91に侵入しにくい状況を作ることができる。したがって、上部拡散領域70とカソード領域90との間の電気抵抗の上昇を抑制することができる。これに伴って、ツェナー電圧の経時的変動を抑制できる。 As described above, the depletion layer when breakdown occurs may extend to a wide region outside the lower diffusion regions 30 and 60 in the surface layer of the semiconductor substrate 10, which is a surface trap in the surface layer of the semiconductor device 10. It is presumed to be caused. The semiconductor device 120 includes the cathode region 90 and the inter-electrode region 91 having a higher concentration than that of the semiconductor substrate 10 so that the N-conductivity type impurity layer constituting the semiconductor substrate 10 is not exposed in the semiconductor substrate 10a. Yes. As a result, it is possible to create a situation in which a depletion layer extending from the upper diffusion region 70 hardly enters the inter-electrode region 91. Therefore, an increase in electrical resistance between the upper diffusion region 70 and the cathode region 90 can be suppressed. Along with this, it is possible to suppress the variation with time of the Zener voltage.

 (第4実施形態)
 第3実施形態では、極間領域91の形成に際して、下部拡散領域80とカソード領域90の形成に係るイオン注入とは別の工程として、極間注入領域93を形成する例について説明したが、下部拡散領域80とカソード領域90の形成位置を近接させることよって、極間注入領域93を形成する工程を省略することができる。
(Fourth embodiment)
In the third embodiment, an example in which the interelectrode implantation region 93 is formed as a process different from the ion implantation for forming the lower diffusion region 80 and the cathode region 90 when forming the interelectrode region 91 has been described. By bringing the formation positions of the diffusion region 80 and the cathode region 90 close to each other, the step of forming the interelectrode injection region 93 can be omitted.

 図17に示すように、本実施形態における半導体装置130は、下部拡散領域80と対極領域としてのカソード領域90とが重なった部分として、極間領域91が形成されている。極間領域91はN導電型であり、第3実施形態と同様に、半導体基板10を構成する不純物濃度よりも高濃度になっている。 As shown in FIG. 17, in the semiconductor device 130 in the present embodiment, an interelectrode region 91 is formed as a portion where a lower diffusion region 80 and a cathode region 90 as a counter electrode region overlap. The inter-electrode region 91 is of N conductivity type, and is higher in concentration than the impurity concentration constituting the semiconductor substrate 10 as in the third embodiment.

 このような態様を実現するためには、例えば第3実施形態において図14を参照して説明した下部注入領域81と対極注入領域92の形成において、互いの離間距離を短くレイアウトする。これにより、イオン注入後のアニール工程によって不純物が熱拡散していく領域が互いにオーバーラップすることとなり、極間領域91が形成される。この態様および方法を採用すれば、極間注入領域93を形成するためのイオン注入の工程を削減できるとともに、上部拡散領域70から延びる空乏層が極間領域91に侵入しにくい状況を作ることができる。 In order to realize such an aspect, for example, in the formation of the lower injection region 81 and the counter electrode injection region 92 described in the third embodiment with reference to FIG. As a result, regions where impurities are thermally diffused by the annealing process after ion implantation overlap each other, and an inter-electrode region 91 is formed. By adopting this mode and method, it is possible to reduce the number of ion implantation steps for forming the interelectrode region 93 and to create a situation in which a depletion layer extending from the upper diffusion region 70 hardly enters the interelectrode region 91. it can.

 (その他の実施形態)
 本開示は、実施形態に準拠して記述されたが、本開示は当該実施形態や構造に限定されるものではないと理解される。本開示は、様々な変形例や均等範囲内の変形をも包含する。加えて、様々な組み合わせや形態、さらには、それらに一要素のみ、それ以上、あるいはそれ以下、を含む他の組み合わせや形態をも、本開示の範疇や思想範囲に入るものである。
(Other embodiments)
Although the present disclosure has been described based on the embodiments, it is understood that the present disclosure is not limited to the embodiments and structures. The present disclosure includes various modifications and modifications within the equivalent range. In addition, various combinations and forms, as well as other combinations and forms including only one element, more or less, are within the scope and spirit of the present disclosure.

 上記した各実施形態においては、上部拡散領域20,50,70、および、上部注入領域21,51,71を軸Aあるいは軸Bを対称軸として真円状に形成する例を示したが、主面10aから正面視した上部拡散領域20,50,70および上部注入領域21,51,71の形状は真円に限定されるものではなく、n回対称形状であればよい。具体的には、楕円やカプセル形状(2回対称)、正三角形(3回対称)、正方形(4回対称)、正五角形(5回対称)、正六角形(6回対称)などを採用しても良い。 In each of the above embodiments, the upper diffusion regions 20, 50, and 70 and the upper implantation regions 21, 51, and 71 are formed in a perfect circle shape with the axis A or the axis B as the symmetry axis. The shapes of the upper diffusion regions 20, 50, 70 and the upper injection regions 21, 51, 71 viewed from the front from the surface 10a are not limited to a perfect circle, and may be n-fold symmetrical shapes. Specifically, an ellipse, capsule shape (2 times symmetry), equilateral triangle (3 times symmetry), square (4 times symmetry), regular pentagon (5 times symmetry), regular hexagon (6 times symmetry), etc. are adopted. Also good.

 同様に、下部拡散領域30,60,80、および、下部注入領域31,61,81を軸Aあるいは軸Bを対称軸として真円状に形成する例を示したが、主面10aから正面視した下部拡散領域30,60,80および下部注入領域31,61,81の形状は真円に限定されるものではなく、n回対称形状であればよい。なお、2回対称の形状では、不純物濃度の極大は点ではなく長辺に沿う線状(1次元)になる。 Similarly, an example in which the lower diffusion regions 30, 60, 80 and the lower injection regions 31, 61, 81 are formed in a perfect circle shape with the axis A or the axis B as a symmetry axis is shown. The shapes of the lower diffusion regions 30, 60, 80 and the lower implantation regions 31, 61, 81 are not limited to a perfect circle, but may be any n-fold symmetrical shape. In the two-fold symmetrical shape, the maximum impurity concentration is not a point but a linear shape (one-dimensional) along the long side.

 加えて、上部拡散領域20,50,70と対応する下部拡散領域30,60,80は、主面10aから正面視したときに、互いの形状が相似形であることが好ましい。上部拡散領域20,50,70と対応する下部拡散領域30,60,80とが対称性を有することにより、下部拡散領域30,60,80において、3次元よりも低い1次元や0次元でブレークポイントを形成しやすくできる。 In addition, the lower diffusion regions 30, 60, 80 corresponding to the upper diffusion regions 20, 50, 70 are preferably similar in shape to each other when viewed from the main surface 10a. Since the upper diffusion regions 20, 50, 70 and the corresponding lower diffusion regions 30, 60, 80 have symmetry, the lower diffusion regions 30, 60, 80 break in one or zero dimensions lower than three dimensions. It is easy to form points.

 また、上記した各実施形態では、シリサイドブロック層40が、上部拡散領域20,50,70や下部拡散領域30,60,80と中心を同じくして形成される例について説明したが、これに限定されず、形成中心がずれていてもよい。なお、シリサイドブロック層40は、シリサイドによる電極形成を行わない場合には不要な場合があり、このような形態では必須な要素ではない。 In each of the above-described embodiments, the example in which the silicide block layer 40 is formed in the same center as the upper diffusion regions 20, 50, 70 and the lower diffusion regions 30, 60, 80 has been described. However, the formation center may be shifted. It should be noted that the silicide block layer 40 may be unnecessary if the electrode is not formed by silicide, and is not an essential element in such a form.

 また、上記した各実施形態では、上部拡散領域20,50にP導電型を採用し、下部拡散領域30,60にN導電型を採用したが、これらの導電型は相互に反転して構成されても良い。なお、半導体基板にはN導電型の基板を採用する例を記載したが、半導体基板については、上部拡散領域20,50や下部拡散領域30,60の導電型に依らずN導電型、P導電型のいずれを採用してもよい。だたし、極間領域91を有する場合には、カソード領域90に相当する対極領域と、下部拡散領域30,60,80と、半導体基板10とは同一の導電型である必要がある。 Further, in each of the above-described embodiments, the P conductivity type is adopted for the upper diffusion regions 20 and 50 and the N conductivity type is adopted for the lower diffusion regions 30 and 60. However, these conductivity types are configured to be reversed to each other. May be. In addition, although the example which employ | adopts an N conductivity type board | substrate was described as a semiconductor substrate, about the semiconductor substrate, N conductivity type and P conductivity were used irrespective of the conductivity type of the upper diffusion regions 20 and 50 and the lower diffusion regions 30 and 60. Any type of mold may be employed. However, when the inter-electrode region 91 is provided, the counter electrode region corresponding to the cathode region 90, the lower diffusion regions 30, 60, and 80, and the semiconductor substrate 10 need to be of the same conductivity type.

 また、上記した各実施形態においては、下部拡散領域30,60,80が、対応する上部拡散領域20,50,70を半導体基板10内部で完全に覆うことで主面10aに露出する形態について例示したが、下部拡散領域が上部拡散領域の下部にのみ位置し、主面10aに露出しないように構成しても良い。ただし、下部拡散領域が上部拡散領域を完全に覆って主面10aに露出するように構成されることにより、主面10aの表層において、P導電型の上部拡散領域20,50,70と、N導電型の領域との間に形成される空乏層の主面10aに沿う方向の広がりを、下部拡散領域30,60,80が主面に露出していない構成に較べて抑制することができる。これにより、主面10a近傍に存在する表面欠陥に起因する準位に、ホットキャリアがトラップされることを抑制でき、ツェナー電圧の経時的変動量を抑制することができる。この点において、極間領域91を有していると、さらに有利である。 Further, in each of the above-described embodiments, the lower diffusion regions 30, 60, 80 are illustrated as being exposed to the main surface 10 a by completely covering the corresponding upper diffusion regions 20, 50, 70 inside the semiconductor substrate 10. However, the lower diffusion region may be positioned only below the upper diffusion region and not exposed to the main surface 10a. However, since the lower diffusion region completely covers the upper diffusion region and is exposed to the main surface 10a, in the surface layer of the main surface 10a, the P conductivity type upper diffusion regions 20, 50, 70 and N The spread of the depletion layer formed between the conductive type region in the direction along the main surface 10a can be suppressed as compared with the configuration in which the lower diffusion regions 30, 60, and 80 are not exposed on the main surface. Thereby, it is possible to suppress trapping of hot carriers at a level caused by surface defects existing in the vicinity of the main surface 10a, and it is possible to suppress an amount of fluctuation of the Zener voltage with time. In this respect, it is further advantageous to have the inter-electrode region 91.

 また、上記した各実施形態では、半導体基板10においてツェナーダイオードが形成されるダイオード形成領域Diに注目して記載したが、半導体基板10にダイオード形成領域以外の領域において別の素子が形成されていることを妨げない。例えば、同一の半導体基板10にMOSFETやIGBTが別途形成されていても良い。 In each of the above-described embodiments, the diode formation region Di in which a Zener diode is formed in the semiconductor substrate 10 has been described. However, another element is formed in the semiconductor substrate 10 in a region other than the diode formation region. I will not prevent it. For example, a MOSFET or IGBT may be separately formed on the same semiconductor substrate 10.

 また、第3実施形態および第4実施形態においては、上部拡散領域20,50,70と下部拡散領域30,60,80との接合面が凹面形状となって、下部拡散領域30,60,80の不純物濃度プロファイルにおいて、濃度の極大を示す極大点が形成されるようにされる構成について説明したが、上部拡散領域20,50,70と下部拡散領域30,60,80との接合面が平面形状である従来の態様に対して、極間領域91が形成されることによってツェナー電圧の経時的変動を抑制する効果を奏することができる。すなわち、極間領域91を備えることによる効果は、下部拡散領域30,60,80の不純物濃度プロファイルにおいて、濃度の極大を示す極大点を形成する技術的思想とは独立して実現することができる。 Further, in the third embodiment and the fourth embodiment, the joint surface between the upper diffusion regions 20, 50, 70 and the lower diffusion regions 30, 60, 80 has a concave shape, so that the lower diffusion regions 30, 60, 80 are formed. In the impurity concentration profile, the configuration in which the maximum point indicating the maximum concentration is formed has been described. However, the bonding surface between the upper diffusion regions 20, 50, 70 and the lower diffusion regions 30, 60, 80 is flat. In contrast to the conventional shape having the shape, the formation of the inter-electrode region 91 can provide an effect of suppressing the variation with time of the Zener voltage. In other words, the effect of providing the inter-electrode region 91 can be realized independently of the technical idea of forming a maximum point indicating the maximum concentration in the impurity concentration profile of the lower diffusion regions 30, 60, 80. .

Claims (28)

 ダイオード形成領域(Di)を有する半導体基板(10)と、
 前記ダイオード形成領域における前記半導体基板の主面(10a)の表層に形成された第1導電型の上部拡散領域(20,50,70)と、
 前記半導体基板の深さ方向において前記主面に対して前記上部拡散領域よりも深い位置に形成され、前記半導体基板よりも不純物濃度が高くされた第2導電型の下部拡散領域(30,60,80)と、を備え、
 前記下部拡散領域は、前記主面より深い位置において前記上部拡散領域とのPN接合面(S)を成すとともに、
 前記ダイオード形成領域における前記下部拡散領域の不純物濃度プロファイルにおいて、濃度の極大を示す極大点(P,P1,P2)を有する半導体装置。
A semiconductor substrate (10) having a diode formation region (Di);
An upper diffusion region (20, 50, 70) of the first conductivity type formed in the surface layer of the main surface (10a) of the semiconductor substrate in the diode formation region;
A second conductivity type lower diffusion region (30, 60, 30) formed at a position deeper than the upper diffusion region with respect to the main surface in the depth direction of the semiconductor substrate and having an impurity concentration higher than that of the semiconductor substrate. 80)
The lower diffusion region forms a PN junction surface (S) with the upper diffusion region at a position deeper than the main surface,
A semiconductor device having a maximum point (P, P1, P2) indicating a maximum concentration in the impurity concentration profile of the lower diffusion region in the diode formation region.
 前記上部拡散領域および前記下部拡散領域は、前記極大点を通り前記深さ方向に沿う仮想線を対称軸(A,B)として回転対称に分布し、前記PN接合面は、凹面または凸面である請求項1に記載の半導体装置。 The upper diffusion region and the lower diffusion region are distributed rotationally symmetrically with an imaginary line passing through the maximum point and extending along the depth direction as symmetry axes (A, B), and the PN junction surface is a concave surface or a convex surface. The semiconductor device according to claim 1.  前記主面を正面視したとき、前記上部拡散領域と前記下部拡散領域とは互いに相似形である請求項2に記載の半導体装置。 3. The semiconductor device according to claim 2, wherein the upper diffusion region and the lower diffusion region are similar to each other when the main surface is viewed from the front.  前記上部拡散領域および前記下部拡散領域は、前記主面を正面視したとき、前記対称軸を中心とする真円状に分布する請求項2または請求項3に記載の半導体装置。 4. The semiconductor device according to claim 2, wherein the upper diffusion region and the lower diffusion region are distributed in a perfect circle centered on the symmetry axis when the main surface is viewed from the front.  前記下部拡散領域は、前記上部拡散領域を覆うように形成され、前記下部拡散領域の一部が前記主面に露出する請求項1~4のいずれか1項に記載の半導体装置。 5. The semiconductor device according to claim 1, wherein the lower diffusion region is formed so as to cover the upper diffusion region, and a part of the lower diffusion region is exposed to the main surface.  前記主面上に設けられたシリサイドブロック層(40)をさらに備え、
 前記シリサイドブロック層は、前記主面に露出する前記上部拡散領域と第2導電型の半導体領域とのPN接合線(L1,L2)を跨ぐように形成される請求項1~5のいずれか1項に記載の半導体装置。
A silicide block layer (40) provided on the main surface;
The silicide block layer is formed so as to straddle a PN junction line (L1, L2) between the upper diffusion region exposed on the main surface and the second conductivity type semiconductor region. The semiconductor device according to item.
 前記半導体基板は第2導電型であり、
 前記ダイオード形成領域における前記主面の表層に形成され、前記半導体基板よりも不純物濃度が高くされた第2導電型の対極領域(90)を、さらに備え、
 前記主面の表層であって、前記上部拡散領域と前記対極領域との間の領域に、前記半導体基板よりも不純物濃度の高い第2導電型の極間領域(91)が形成される請求項1~6のいずれか1項に記載の半導体装置。
The semiconductor substrate is of a second conductivity type;
A second conductivity type counter electrode region (90) formed on a surface layer of the main surface in the diode formation region and having an impurity concentration higher than that of the semiconductor substrate;
The inter-electrode region (91) of the second conductivity type having a higher impurity concentration than the semiconductor substrate is formed in a surface layer of the main surface and between the upper diffusion region and the counter electrode region. 7. The semiconductor device according to any one of 1 to 6.
 前記極間領域の不純物濃度は、前記下部拡散領域における不純物濃度の前記極大点よりも低い濃度とされる請求項7に記載の半導体装置。 8. The semiconductor device according to claim 7, wherein the impurity concentration in the inter-electrode region is lower than the maximum point of the impurity concentration in the lower diffusion region.  前記極間領域は、前記下部拡散領域および前記対極領域とは独立した不純物領域として形成される請求項7または請求項8に記載の半導体装置。 9. The semiconductor device according to claim 7, wherein the inter-electrode region is formed as an impurity region independent of the lower diffusion region and the counter electrode region.  前記極間領域は、前記下部拡散領域および前記対極領域を第2導電型たらしめる不純物がオーバーラップすることによって形成される請求項7または請求項8に記載の半導体装置。 9. The semiconductor device according to claim 7, wherein the inter-electrode region is formed by overlapping impurities that cause the lower diffusion region and the counter electrode region to have a second conductivity type.  ダイオード形成領域(Di)を有する第2導電型の半導体基板(10)と、
 前記ダイオード形成領域における前記半導体基板の主面(10a)の表層に形成された第1導電型の上部拡散領域(20,50,70)と、
 前記半導体基板の深さ方向において前記主面に対して前記上部拡散領域よりも深い位置に形成され、前記半導体基板よりも不純物濃度が高くされた第2導電型の下部拡散領域(30,60,80)と、
 前記ダイオード形成領域における前記主面の表層に形成され、前記半導体基板よりも不純物濃度が高くされた第2導電型の対極領域(90)と、を備え、
 さらに、前記主面の表層であって、前記上部拡散領域と前記対極領域との間の領域に、前記半導体基板よりも不純物濃度の高い第2導電型の極間領域(91)が形成される半導体装置。
A second conductivity type semiconductor substrate (10) having a diode formation region (Di);
An upper diffusion region (20, 50, 70) of the first conductivity type formed in the surface layer of the main surface (10a) of the semiconductor substrate in the diode formation region;
A second conductivity type lower diffusion region (30, 60, 30) formed at a position deeper than the upper diffusion region with respect to the main surface in the depth direction of the semiconductor substrate and having an impurity concentration higher than that of the semiconductor substrate. 80)
A second conductive type counter electrode region (90) formed on a surface layer of the main surface in the diode forming region and having an impurity concentration higher than that of the semiconductor substrate;
Further, a second conductivity type inter-electrode region (91) having an impurity concentration higher than that of the semiconductor substrate is formed in a surface layer of the main surface and between the upper diffusion region and the counter electrode region. Semiconductor device.
 前記極間領域の不純物濃度は、前記下部拡散領域における不純物濃度の最大値のよりも低い濃度とされる請求項11に記載の半導体装置。 12. The semiconductor device according to claim 11, wherein the impurity concentration in the inter-electrode region is lower than the maximum impurity concentration in the lower diffusion region.  前記極間領域は、前記下部拡散領域および前記対極領域とは独立した不純物領域として形成される請求項11または請求項12に記載の半導体装置。 13. The semiconductor device according to claim 11, wherein the inter-electrode region is formed as an impurity region independent of the lower diffusion region and the counter electrode region.  前記極間領域は、前記下部拡散領域および前記対極領域を第2導電型たらしめる不純物がオーバーラップすることによって形成される請求項11または請求項12に記載の半導体装置。 13. The semiconductor device according to claim 11, wherein the interelectrode region is formed by overlapping impurities that cause the lower diffusion region and the counter electrode region to have a second conductivity type.  半導体基板(10)を準備すること、
 前記半導体基板の主面における表層に不純物を注入して、前記主面を正面視したときに回転対称の形状となるように前記半導体基板よりも不純物濃度が高くされた第2導電型の下部注入領域(31,61,81)を形成すること、
 前記下部注入領域の形成の後、アニールにより前記下部注入領域を拡散すること、
 前記下部注入領域のアニールによる拡散の後、前記半導体基板の主面における表層に不純物を注入して、前記下部注入領域よりも前記主面に対して浅い位置に、前記下部注入領域と同心の回転対称形状となるように第1導電型の上部注入領域(21,51,71)を形成すること、
 前記上部注入領域の形成の後、アニールにより前記下部注入領域を拡散して下部拡散領域(30,60,80)を形成するとともに、前記上部注入領域を拡散して上部拡散領域(20,50,70)を形成すること、を備える半導体装置の製造方法。
Preparing a semiconductor substrate (10);
Impurities are implanted into the surface layer of the main surface of the semiconductor substrate, and the second conductivity type lower implantation in which the impurity concentration is higher than that of the semiconductor substrate so as to have a rotationally symmetrical shape when the main surface is viewed from the front. Forming regions (31, 61, 81);
After forming the lower implant region, diffusing the lower implant region by annealing;
After diffusion by annealing of the lower implantation region, impurities are implanted into the surface layer of the main surface of the semiconductor substrate, and concentric rotation with the lower implantation region is performed at a position shallower than the main surface than the lower implantation region. Forming an upper implantation region (21, 51, 71) of the first conductivity type so as to have a symmetrical shape;
After the formation of the upper implantation region, the lower implantation region is diffused by annealing to form a lower diffusion region (30, 60, 80), and the upper implantation region is diffused to diffuse the upper diffusion region (20, 50, 80). 70). A method for manufacturing a semiconductor device.
 前記主面を正面視したとき、前記上部拡散領域と前記下部拡散領域とが互いに相似形となるように、前記下部注入領域および前記上部注入領域とを相似形に形成する、請求項15に記載の半導体装置の製造方法。 The lower injection region and the upper injection region are formed in a similar shape so that the upper diffusion region and the lower diffusion region are similar to each other when the main surface is viewed from the front. Semiconductor device manufacturing method.  前記上部注入領域および前記下部注入領域は、前記主面を正面視したとき、回転対称に係る対称軸を中心とする真円状に分布するように形成する請求項15または請求項16に記載の半導体装置の製造方法。 The upper injection region and the lower injection region are formed so as to be distributed in a perfect circle centered on a rotational symmetry axis when the main surface is viewed from the front. A method for manufacturing a semiconductor device.  前記上部注入領域の形成において、均一な深さで不純物を注入する請求項15~17のいずれか1項に記載の半導体装置の製造方法。 18. The method of manufacturing a semiconductor device according to claim 15, wherein impurities are implanted at a uniform depth in the formation of the upper implantation region.  前記下部注入領域の形成において、前記主面を正面視したときの直径(R)は、前記半導体基板の深さ方向における前記下部拡散領域の形成深さと同一に設定する請求項15~18のいずれか1項に記載の半導体装置の製造方法。 In the formation of the lower implantation region, the diameter (R) when the main surface is viewed from the front is set to be the same as the formation depth of the lower diffusion region in the depth direction of the semiconductor substrate. A method for manufacturing a semiconductor device according to claim 1.  前記主面に露出する前記上部拡散領域と第2導電型の半導体領域とのPN接合線を跨ぐように、前記主面上にシリサイドブロック層(40)を形成すること、をさらに備える請求項15~19のいずれか1項に記載の半導体装置の製造方法。 The silicide block layer (40) is further formed on the main surface so as to straddle the PN junction line between the upper diffusion region exposed to the main surface and the semiconductor region of the second conductivity type. 20. A method for manufacturing a semiconductor device according to any one of items 19 to 19.  前記半導体基板は第2導電型であり、
 さらに、前記半導体基板の表層であって前記下部注入領域とは離間した位置に不純物を注入して第2導電型の対極注入領域(92)と形成すること、
 前記半導体基板の表層であって前記対極注入領域と前記下部注入領域の間の領域に前記半導体基板よりも不純物濃度の高い極間領域(91)を形成すること、を備える請求項15~20のいずれか1項に記載の半導体装置の製造方法。
The semiconductor substrate is of a second conductivity type;
Furthermore, a second conductive type counter electrode implantation region (92) is formed by implanting impurities into a surface layer of the semiconductor substrate and spaced from the lower implantation region;
The inter-electrode region (91) having an impurity concentration higher than that of the semiconductor substrate is formed in a surface layer of the semiconductor substrate and between the counter electrode injection region and the lower injection region. A manufacturing method of a semiconductor device given in any 1 paragraph.
 前記極間領域の不純物濃度を、前記下部拡散領域における不純物濃度の最大値のよりも低い濃度とする請求項21に記載の半導体装置の製造方法。 The method of manufacturing a semiconductor device according to claim 21, wherein the impurity concentration in the inter-electrode region is lower than the maximum impurity concentration in the lower diffusion region.  前記極間領域を、前記下部注入領域および前記対極注入領域とは独立した極間注入領域(93)を形成し、アニールによる拡散により形成する請求項21または請求項22に記載の半導体装置の製造方法。 23. The manufacturing method of a semiconductor device according to claim 21, wherein the interelectrode region is formed by forming an interelectrode injection region (93) independent of the lower injection region and the counter electrode injection region and performing diffusion by annealing. Method.  前記極間領域を、前記下部注入領域のアニールにより拡散した不純物と、前記対極注入領域のアニールにより拡散した不純物とによって形成する請求項21または請求項22に記載の半導体装置の製造方法。 23. The method of manufacturing a semiconductor device according to claim 21, wherein the inter-electrode region is formed by an impurity diffused by annealing of the lower implantation region and an impurity diffused by annealing of the counter electrode implantation region.  第2導電型の半導体基板(10)を準備すること、
 前記半導体基板の主面における表層に不純物を注入して、前記半導体基板よりも不純物濃度が高くされた第2導電型の下部注入領域(31,61,81)を形成すること、
 前記下部注入領域の形成の後、アニールにより前記下部注入領域を拡散すること、
 前記下部注入領域のアニールによる拡散の後、拡散した前記下部注入領域の表層に不純物を注入して、前記下部注入領域よりも前記主面に対して浅い位置に、第1導電型の上部注入領域(21,51,71)を形成すること、
 前記上部注入領域の形成の後、アニールにより前記下部注入領域を拡散して下部拡散領域(30,60,80)を形成するとともに、前記上部注入領域を拡散して上部拡散領域(20,50,70)を形成すること、
 加えて、前記半導体基板の表層であって前記下部注入領域とは離間した位置に不純物を注入して第2導電型の対極注入領域(92)を形成すること、
 前記半導体基板の表層であって前記対極注入領域と前記下部注入領域の間の領域に前記半導体基板よりも不純物濃度の高い極間領域(91)を形成すること、を備える半導体装置の製造方法。
Preparing a second conductivity type semiconductor substrate (10);
Implanting impurities into the surface layer of the main surface of the semiconductor substrate to form a second conductivity type lower implantation region (31, 61, 81) having a higher impurity concentration than the semiconductor substrate;
After forming the lower implant region, diffusing the lower implant region by annealing;
After the diffusion of the lower implantation region by annealing, an impurity is implanted into the surface layer of the diffused lower implantation region, and the first conductivity type upper implantation region is located at a position shallower than the main surface than the lower implantation region. Forming (21, 51, 71),
After the formation of the upper implantation region, the lower implantation region is diffused by annealing to form a lower diffusion region (30, 60, 80), and the upper implantation region is diffused to diffuse the upper diffusion region (20, 50, 80). 70),
In addition, a second conductive type counter electrode injection region (92) is formed by injecting impurities into a surface layer of the semiconductor substrate and spaced from the lower injection region.
A method of manufacturing a semiconductor device comprising: forming an inter-electrode region (91) having a higher impurity concentration than the semiconductor substrate in a surface layer of the semiconductor substrate and between the counter-electrode injection region and the lower injection region.
 前記極間領域の不純物濃度を、前記下部拡散領域における不純物濃度の最大値のよりも低い濃度とする請求項25に記載の半導体装置の製造方法。 26. The method of manufacturing a semiconductor device according to claim 25, wherein the impurity concentration in the inter-electrode region is lower than the maximum impurity concentration in the lower diffusion region.  前記極間領域を、前記下部注入領域および前記対極注入領域とは独立した極間注入領域(93)を形成し、アニールによる拡散により形成する請求項25または請求項26に記載の半導体装置の製造方法。 27. The method of manufacturing a semiconductor device according to claim 25, wherein the interelectrode region is formed by forming an interelectrode injection region (93) independent of the lower injection region and the counter electrode injection region, and performing diffusion by annealing. Method.  前記極間領域を、前記下部注入領域のアニールにより拡散した不純物と、前記対極注入領域のアニールにより拡散した不純物とによって形成する請求項25または請求項26に記載の半導体装置の製造方法。 27. The method of manufacturing a semiconductor device according to claim 25, wherein the inter-electrode region is formed by impurities diffused by annealing of the lower implantation region and impurities diffused by annealing of the counter electrode implantation region.
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