TW201803117A - High electron mobility transistor and method for manufacturing high electron mobility transistor - Google Patents
High electron mobility transistor and method for manufacturing high electron mobility transistor Download PDFInfo
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- 238000000034 method Methods 0.000 title claims description 12
- 238000004519 manufacturing process Methods 0.000 title claims description 10
- 239000000758 substrate Substances 0.000 claims abstract description 36
- 230000005533 two-dimensional electron gas Effects 0.000 claims abstract description 16
- 239000013078 crystal Substances 0.000 claims 1
- 238000009413 insulation Methods 0.000 abstract description 6
- 230000008901 benefit Effects 0.000 description 6
- 239000004065 semiconductor Substances 0.000 description 4
- 229910002601 GaN Inorganic materials 0.000 description 3
- 230000007547 defect Effects 0.000 description 3
- 230000007774 longterm Effects 0.000 description 3
- 239000000463 material Substances 0.000 description 3
- PXHVJJICTQNCMI-UHFFFAOYSA-N Nickel Chemical compound [Ni] PXHVJJICTQNCMI-UHFFFAOYSA-N 0.000 description 2
- 239000003990 capacitor Substances 0.000 description 2
- 230000015556 catabolic process Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000005669 field effect Effects 0.000 description 2
- 239000012535 impurity Substances 0.000 description 2
- 230000002441 reversible effect Effects 0.000 description 2
- 229910002704 AlGaN Inorganic materials 0.000 description 1
- 229910000980 Aluminium gallium arsenide Inorganic materials 0.000 description 1
- 229910001218 Gallium arsenide Inorganic materials 0.000 description 1
- JMASRVWKEDWRBT-UHFFFAOYSA-N Gallium nitride Chemical compound [Ga]#N JMASRVWKEDWRBT-UHFFFAOYSA-N 0.000 description 1
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 230000006378 damage Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 description 1
- 229910052737 gold Inorganic materials 0.000 description 1
- 239000010931 gold Substances 0.000 description 1
- 230000002427 irreversible effect Effects 0.000 description 1
- 230000007246 mechanism Effects 0.000 description 1
- 229910052759 nickel Inorganic materials 0.000 description 1
- 230000008569 process Effects 0.000 description 1
- 230000009467 reduction Effects 0.000 description 1
- 239000010936 titanium Substances 0.000 description 1
- 229910052719 titanium Inorganic materials 0.000 description 1
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D30/00—Field-effect transistors [FET]
- H10D30/40—FETs having zero-dimensional [0D], one-dimensional [1D] or two-dimensional [2D] charge carrier gas channels
- H10D30/47—FETs having zero-dimensional [0D], one-dimensional [1D] or two-dimensional [2D] charge carrier gas channels having 2D charge carrier gas channels, e.g. nanoribbon FETs or high electron mobility transistors [HEMT]
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D30/00—Field-effect transistors [FET]
- H10D30/01—Manufacture or treatment
- H10D30/015—Manufacture or treatment of FETs having heterojunction interface channels or heterojunction gate electrodes, e.g. HEMT
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D62/00—Semiconductor bodies, or regions thereof, of devices having potential barriers
- H10D62/10—Shapes, relative sizes or dispositions of the regions of the semiconductor bodies; Shapes of the semiconductor bodies
- H10D62/113—Isolations within a component, i.e. internal isolations
- H10D62/115—Dielectric isolations, e.g. air gaps
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D84/00—Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers
- H10D84/01—Manufacture or treatment
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D84/00—Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers
- H10D84/80—Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers characterised by the integration of at least one component covered by groups H10D12/00 or H10D30/00, e.g. integration of IGFETs
- H10D84/811—Combinations of field-effect devices and one or more diodes, capacitors or resistors
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D62/00—Semiconductor bodies, or regions thereof, of devices having potential barriers
- H10D62/80—Semiconductor bodies, or regions thereof, of devices having potential barriers characterised by the materials
- H10D62/85—Semiconductor bodies, or regions thereof, of devices having potential barriers characterised by the materials being Group III-V materials, e.g. GaAs
- H10D62/8503—Nitride Group III-V materials, e.g. AlN or GaN
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D64/00—Electrodes of devices having potential barriers
- H10D64/20—Electrodes characterised by their shapes, relative sizes or dispositions
- H10D64/23—Electrodes carrying the current to be rectified, amplified, oscillated or switched, e.g. sources, drains, anodes or cathodes
- H10D64/251—Source or drain electrodes for field-effect devices
- H10D64/257—Source or drain electrodes for field-effect devices for lateral devices wherein the source or drain electrodes are characterised by top-view geometrical layouts, e.g. interdigitated, semi-circular, annular or L-shaped electrodes
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- H—ELECTRICITY
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- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D89/00—Aspects of integrated devices not covered by groups H10D84/00 - H10D88/00
- H10D89/10—Integrated device layouts
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Abstract
Description
本發明係關於一種高電子遷移率的電晶體HEMT及用於製造高電子遷移率的電晶體之方法。 The invention relates to a high electron mobility transistor HEMT and a method for manufacturing a high electron mobility transistor.
基於氮化鎵之橫向功率電晶體HEMT並不耐過電壓,因為該HEMT之介電層(例如緩衝層及屏蔽電容)在低於HEMT下方之半導體基板的場強度下經受擊穿。電晶體未呈現突崩。此處,HEMT可安全操作的最大突崩能量對應於可在最大反向電壓下儲存於輸出電容上的能量。 A lateral power transistor HEMT based on gallium nitride is not resistant to overvoltage because the dielectric layers (such as buffer layers and shield capacitors) of the HEMT undergo breakdown at a field strength lower than the semiconductor substrate below the HEMT. The transistor did not show burst. Here, the maximum burst energy that the HEMT can safely operate corresponds to the energy that can be stored on the output capacitor at the maximum reverse voltage.
此處不利的是,若超過該最大反向電壓,則會發生不可逆的介質擊穿且HEMT遭到破壞。 The disadvantage here is that if this maximum reverse voltage is exceeded, irreversible dielectric breakdown occurs and the HEMT is destroyed.
就基於IGBT的組件而言,組件的破壞同樣為已知的。在此情形下,將齊納二極體及突崩二極體互連以用來抵禦過電壓。然而,此做法對於HEMT無法實行,因為齊納二極體及突崩二極體無法整合入HEMT技術。此外,此處不利的是此等二極體不夠快,因為GaN HEMT具有高切換速度。 In the case of IGBT-based components, the destruction of the components is also known. In this case, the Zener diode and the burst diode are interconnected to resist overvoltage. However, this approach cannot be implemented for HEMT, because Zener diodes and burst diodes cannot be integrated into HEMT technology. Furthermore, it is disadvantageous here that these diodes are not fast enough because GaN HEMTs have high switching speeds.
文件DE 10 2013 102 457 A1描述用於合成半導體場效電晶體之過電壓保護的組件。該組件含有配置於合成半導體材料中之植入區。該 植入區具有空間上分佈的捕捉態,該等捕捉態具有使得植入區在臨限電壓下變得導電的作用。因此,根據弗倫克爾-普爾原理(Frenkel-Pool principle),該植入區具有傳導機制。藉助於植入雜質原子,引入高能態(所謂的缺陷),使得跳頻傳導類型成為可能。該等缺陷在通常係自由態的能帶隙之區內形成對於電子而言可能的高能態。藉助於跳頻傳導,電子可越過一個缺陷至下一個。此對應於電流。狀態之高能深度藉由選擇雜質原子來判定。始於在場效電晶體中產生電流之場強度可藉助於該等狀態調整。 Document DE 10 2013 102 457 A1 describes components for overvoltage protection of synthetic semiconductor field effect transistors. The device includes an implanted region disposed in a synthetic semiconductor material. The The implanted region has spatially distributed capture states, which have the effect of making the implanted region conductive under a threshold voltage. Therefore, according to the Frenkel-Pool principle, the implanted region has a conduction mechanism. By implanting impurity atoms, the introduction of high energy states (so-called defects) makes it possible for frequency hopping conduction types. These defects form high energy states that are possible for electrons in the region of the energy band gap of the free state. With frequency hopping conduction, electrons can pass one defect to the next. This corresponds to the current. The high-energy depth of the state is determined by selecting impurity atoms. The field strength that starts with the generation of current in the field effect transistor can be adjusted by means of these states.
此處不利的是可能出現穿過植入之合成半導體材料之電流,使得無法達到過電壓保護組件之長期穩定性。 The disadvantage here is that a current may pass through the implanted synthetic semiconductor material, making it impossible to achieve the long-term stability of the overvoltage protection device.
本發明之目標為提供一種具有長期穩定性的耐過電壓HEMT。 The object of the present invention is to provide an over-voltage resistant HEMT with long-term stability.
高電子遷移率的電晶體包含複數個第一個別單元及至少一個第二個別單元,其中該第二個別單元具有一第一絕緣層。在此情形下,一個別單元應理解為意指具有一源極端子、一閘極端子及一汲極端子之一HEMT的一基本單元。第二絕緣層經配置成垂直於一基板前側且自該基板前側直接延伸至一二維電子氣體中,以使得製造具有一第一閘極端子的一第一個別電晶體及具有一第二閘極端子的一第二個別電晶體。在此情形下,術語基板前側應理解為意指該基板之側面,在該側面上配置HEMT之觸點,亦即閘極、汲極及源極。該第一個別電晶體及該第二個別電晶體並聯電連接且具有一源極端子及一汲極端子。換言之,該第一個別電晶體及該第二個別電晶體具有一共同源極端子或源極觸點及一共同汲極端子或汲 極觸點。根據本發明,一電位觸點配置在該第二個別電晶體之區內的該汲極端子與該源極端子之間。該電位觸點垂直於該基板前側延伸且自該基板前側直接延伸至該第二個別電晶體之該二維電子氣體中。此情形意指該電位觸點經配置成垂直於該基板前側。由於該電位觸點,因此在該汲極端子與該第二閘極端子之間形成或產生一第一電阻,且在該第二閘極端子與該源極端子之間形成或產生一第二電阻。換言之,該電位觸點在該源極端子與該汲極端子之間形成一分壓器,其中該分壓器經由該電位觸點電連接至該第二閘極端子。此情形意指提供將該電位觸點與該第二閘極端子電連接的部件。 The high electron mobility transistor includes a plurality of first individual cells and at least one second individual cell, wherein the second individual cell has a first insulating layer. In this case, a different unit should be understood to mean a basic unit with one HEMT having one source terminal, one gate terminal, and one drain terminal. The second insulating layer is configured to be perpendicular to a substrate front side and directly extends from the substrate front side into a two-dimensional electronic gas, so that a first individual transistor having a first gate electrode terminal and a second gate electrode are manufactured. A second individual transistor for the terminal. In this case, the term substrate front side should be understood to mean the side of the substrate on which the contacts of the HEMT are arranged, that is, the gate, the drain, and the source. The first individual transistor and the second individual transistor are electrically connected in parallel and have a source terminal and a drain terminal. In other words, the first individual transistor and the second individual transistor have a common source terminal or source contact and a common drain terminal or sink Pole contact. According to the present invention, a potential contact is disposed between the drain terminal and the source terminal in the region of the second individual transistor. The potential contact extends perpendicular to the front side of the substrate and directly extends from the front side of the substrate into the two-dimensional electron gas of the second individual transistor. This situation means that the potential contact is configured to be perpendicular to the front side of the substrate. Due to the potential contact, a first resistance is formed or generated between the drain terminal and the second gate terminal, and a second resistance is formed or generated between the second gate terminal and the source terminal. resistance. In other words, the potential contact forms a voltage divider between the source terminal and the drain terminal, wherein the voltage divider is electrically connected to the second gate terminal via the potential contact. This situation means providing a means for electrically connecting the potential contact to the second gate terminal.
此處優勢為所得HEMT功率電晶體耐過電壓。該第二個別電晶體之閘極電壓可藉助於該分壓器調整。若該第二個別電晶體之該閘極電壓超出該第二個別電晶體之臨限電壓,則該第二個別電晶體接通且將過電壓導走。此外,該HEMT具有長期穩定性且過電壓保護可以簡單方式整合入HEMT製程。 The advantage here is that the resulting HEMT power transistor is resistant to overvoltage. The gate voltage of the second individual transistor can be adjusted by the voltage divider. If the gate voltage of the second individual transistor exceeds the threshold voltage of the second individual transistor, the second individual transistor is turned on and the overvoltage is conducted away. In addition, the HEMT has long-term stability and overvoltage protection can be easily integrated into the HEMT process.
在另一組態中,該部件為一閘極場板。 In another configuration, the component is a gate field plate.
此具有經由減小最大場強度以阻止動態Rds起作用的優勢。 This has the advantage of preventing dynamic Rds from working by reducing the maximum field strength.
在一進展中,該第二閘極端子之一區域對應於該電位觸點之一區域。該第二閘極端子之區域及該電位觸點之區域兩者經配置成平行於該基板前側或在該基板前側上。 In a development, a region of the second gate terminal corresponds to a region of the potential contact. Both the region of the second gate terminal and the region of the potential contact are configured to be parallel to or on the front side of the substrate.
此處有利的是該電位觸點可塑造為一較大區域。在此情形下,該電位觸點既不影響該二維電子氣體,也不影響該汲極端子與該第二閘極端子之間的漂移分區。 It is advantageous here that the potential contact can be shaped into a larger area. In this case, the potential contact does not affect the two-dimensional electron gas, nor does it affect the drift zone between the drain terminal and the second gate terminal.
在另一組態中,該第二閘極端子之一區域大於該電位觸點之一區域。該第二閘極端子之區域及該電位觸點之區域兩者經配置成平行於該基板前側或在該基板前側上。 In another configuration, an area of the second gate terminal is larger than an area of the potential contact. Both the region of the second gate terminal and the region of the potential contact are configured to be parallel to or on the front side of the substrate.
此處優勢為由於電位觸點區域較小,因此該電位觸點對該二維電子氣體的影響較低。 The advantage here is that the potential contact has a lower impact on the two-dimensional electron gas because the potential contact area is smaller.
在一進展中,該電位觸點配置於該第二個別電晶體之區內的該汲極端子與該第二閘極端子之間。 In a development, the potential contact is disposed between the drain terminal and the second gate terminal in the region of the second individual transistor.
此處有利的是該HEMT的所需總面積減少。 It is advantageous here that the required total area of the HEMT is reduced.
在另一組態中,該電位觸點配置於該第二個別電晶體之區內的該源極端子與該第二閘極端子之間。 In another configuration, the potential contact is disposed between the source terminal and the second gate terminal in the region of the second individual transistor.
此處優勢為總面積出現減少。 The advantage here is a reduction in the total area.
在一進展中,該第二個別電晶體具有一第二絕緣層,其經配置成垂直於該基板前側且自該基板前側直接延伸至該第二個別電晶體之該二維電子氣體中。 In a development, the second individual transistor has a second insulating layer that is configured to be perpendicular to the front side of the substrate and directly extends from the front side of the substrate into the two-dimensional electron gas of the second individual transistor.
此處有利的是該電位觸點不影響該二維電子氣體,因為該電位觸點與該第二閘極端子電絕緣。 It is advantageous here that the potential contact does not affect the two-dimensional electron gas, since the potential contact is electrically insulated from the second gate terminal.
在另一組態中,該第二個別電晶體之一維持電流可取決於該電位觸點之一位準而調整。 In another configuration, a sustain current of one of the second individual transistors may be adjusted depending on a level of the potential contact.
此處優勢為在過電壓情形下,該第二個別電晶體之該閘極端子可安全切換。 The advantage here is that the gate terminal of the second individual transistor can be safely switched in an over-voltage situation.
根據本發明之用於製造包含複數個第一個別單元之一HEMT的方法包含在至少一個第二個別單元中製造一第一絕緣層,其中該 第一絕緣層經配置成垂直於該基板前側且直接延伸至一二維電子氣體中,以使得製造具有一第一閘極端子的一第一個別電晶體及具有一第二閘極端子的一第二個別電晶體。在該第二個別電晶體之區內製造一電位觸點,該電位觸點經配置成垂直於該基板前側且自該基板前側直接延伸至該第二個別電晶體之該二維電子氣體中。此外,該方法包含在該電位觸點與該第二閘極端子之間產生一電連接。 A method for manufacturing a HEMT including one of a plurality of first individual units according to the present invention includes fabricating a first insulating layer in at least one second individual unit, wherein the The first insulating layer is configured to be perpendicular to the front side of the substrate and directly extends into a two-dimensional electronic gas, so that a first individual transistor having a first gate terminal and a second gate electrode having a second gate terminal are manufactured. The second individual transistor. A potential contact is manufactured in the region of the second individual transistor, and the potential contact is configured to be perpendicular to the front side of the substrate and directly extends from the front side of the substrate into the two-dimensional electron gas of the second individual transistor. In addition, the method includes creating an electrical connection between the potential contact and the second gate terminal.
在另一組態中,製造一第二絕緣層,該第二絕緣層經配置成垂直於該基板前側且直接延伸至該第二個別電晶體之該二維電子氣體中。 In another configuration, a second insulating layer is manufactured, the second insulating layer is configured to be perpendicular to the front side of the substrate and directly extends into the two-dimensional electron gas of the second individual transistor.
其他優勢自以下例示性具體實例之描述及/或自附屬專利申請專利範圍顯而易見。 Other advantages are apparent from the description of the following illustrative specific examples and / or from the scope of patent applications of the subsidiary patents.
100‧‧‧高電子遷移率的電晶體(HEMT) 100‧‧‧High Electron Mobility Transistor (HEMT)
101‧‧‧第一個別單元 101‧‧‧First individual unit
108‧‧‧源極端子 108‧‧‧Source terminal
109‧‧‧汲極端子 109‧‧‧ drain terminal
112‧‧‧閘極端子 112‧‧‧Gate terminal
200‧‧‧高電子遷移率的電晶體(HEMT) 200‧‧‧High Electron Mobility Transistor (HEMT)
201‧‧‧第一個別單元 201‧‧‧ the first individual unit
202‧‧‧第一絕緣層 202‧‧‧First insulation layer
205‧‧‧第一閘極端子 205‧‧‧First Gate Extreme
207‧‧‧第二閘極端子 207‧‧‧Second Gate Extreme
208‧‧‧源極端子 208‧‧‧Source terminal
209‧‧‧汲極端子 209‧‧‧ drain terminal
212‧‧‧閘極端子 212‧‧‧Gate terminal
213‧‧‧電位觸點 213‧‧‧potential contact
214‧‧‧第二個別單元 214‧‧‧Second Individual Unit
302‧‧‧第一絕緣層 302‧‧‧First insulation layer
304‧‧‧第一個別電晶體 304‧‧‧The first individual transistor
305‧‧‧第一閘極端子 305‧‧‧First Gate Extreme
306‧‧‧第二個別電晶體 306‧‧‧Second individual transistor
307‧‧‧第二閘極端子 307‧‧‧Second Gate Extreme
308‧‧‧源極端子 308‧‧‧Source terminal
309‧‧‧汲極端子 309‧‧‧ terminal
313‧‧‧電位觸點 313‧‧‧potential contact
314‧‧‧第二個別單元 314‧‧‧Second Unit
402‧‧‧第一絕緣層 402‧‧‧First insulation layer
403‧‧‧第二絕緣層 403‧‧‧Second insulation layer
404‧‧‧第一個別電晶體 404‧‧‧The first individual transistor
405‧‧‧第一閘極端子 405‧‧‧First Gate Extreme
406‧‧‧第二個別電晶體 406‧‧‧Second individual transistor
407‧‧‧第二閘極端子 407‧‧‧Second Gate Extreme
408‧‧‧源極端子 408‧‧‧source terminal
409‧‧‧汲極端子 409‧‧‧ drain terminal
413‧‧‧電位觸點 413‧‧‧potential contact
414‧‧‧第二個別單元 414‧‧‧Second Individual Unit
500‧‧‧高電子遷移率的電晶體(HEMT) 500‧‧‧High Electron Mobility Transistor (HEMT)
504‧‧‧第一個別電晶體 504‧‧‧The first individual transistor
505‧‧‧第一閘極端子 505‧‧‧First Gate Extreme
506‧‧‧第二個別電晶體 506‧‧‧Second individual transistor
507‧‧‧第二閘極端子 507‧‧‧Second Gate Extreme
508‧‧‧源極端子 508‧‧‧Source terminal
509‧‧‧汲極端子 509‧‧‧ drain terminal
510‧‧‧第一電阻 510‧‧‧first resistor
511‧‧‧第二電阻 511‧‧‧Second resistor
513‧‧‧電位觸點 513‧‧‧potential contact
600‧‧‧方法 600‧‧‧ Method
610‧‧‧步驟 610‧‧‧step
620‧‧‧步驟 620‧‧‧step
630‧‧‧步驟 630‧‧‧step
640‧‧‧步驟 640‧‧‧step
下文基於較佳具體實例及附圖解釋本發明。 The invention is explained below based on preferred specific examples and drawings.
在圖中:圖1展示來自先前技術之HEMT的平面圖,圖2展示根據本發明之HEMT的示意性平面圖,圖3展示第二個別單元之第一組態的平面圖,圖4展示第二個別單元之第二組態的平面圖,圖5展示根據本發明之HEMT的等效電路圖,且圖6展示用於製造根據本發明之HEMT的方法。 In the drawings: FIG. 1 shows a plan view of a prior art HEMT, FIG. 2 shows a schematic plan view of a HEMT according to the present invention, FIG. 3 shows a plan view of a first configuration of a second individual unit, and FIG. 4 shows a second individual unit A plan view of the second configuration, FIG. 5 shows an equivalent circuit diagram of a HEMT according to the present invention, and FIG. 6 shows a method for manufacturing the HEMT according to the present invention.
圖1展示來自先前技術之HEMT 100的平面圖。該HEMT 100包含各自形成至少一個個別電晶體之複數個第一個別單元101。因此,該 HEMT 100包含藉由複數個個別電晶體形成的串聯電路。圖1同樣展示HEMT 100之源極端子108、汲極端子109及閘極端子112。 Figure 1 shows a plan view of a prior art HEMT 100. The HEMT 100 includes a plurality of first individual cells 101 each forming at least one individual transistor. Therefore, the The HEMT 100 includes a series circuit formed by a plurality of individual transistors. Figure 1 also shows the source terminal 108, the drain terminal 109, and the gate terminal 112 of the HEMT 100.
圖2展示根據本發明之HEMT 200的示意性平面圖。該HEMT 200包含源極端子208、汲極端子209及閘極端子212、複數個第一個別單元201及具有第一絕緣層202之至少一個第二個別單元214。藉助於該第一絕緣層202形成具有第一閘極端子205的第一個別電晶體及具有第二閘極端子207的第二個別電晶體。在此情形下,該第一個別電晶體及該第二個別電晶體並聯電連接。電位觸點213配置於該第二個別電晶體之區內。在此情形下,該第二個別電晶體起到對第一個別電晶體進行過電壓保護的作用。 FIG. 2 shows a schematic plan view of a HEMT 200 according to the present invention. The HEMT 200 includes a source terminal 208, a drain terminal 209 and a gate terminal 212, a plurality of first individual units 201, and at least one second individual unit 214 having a first insulating layer 202. A first individual transistor having a first gate terminal 205 and a second individual transistor having a second gate terminal 207 are formed by the first insulating layer 202. In this case, the first individual transistor and the second individual transistor are electrically connected in parallel. The potential contact 213 is disposed in a region of the second individual transistor. In this case, the second individual transistor functions to protect the first individual transistor from overvoltage.
圖3展示第二個別單元314之第一組態。該第二個別單元314具有源極端子308及汲極端子309。此外,其他個別單元314具有第一絕緣層302,使得具有第一閘極端子305的第一個別電晶體304及具有第二閘極端子307的第二個別電晶體306成形。在此情形下,該第一個別電晶體304及該第二個別電晶體306並聯連接。電位觸點313配置於第二個別電晶體306之區內。 FIG. 3 shows a first configuration of the second individual unit 314. The second individual unit 314 has a source terminal 308 and a drain terminal 309. In addition, the other individual units 314 have a first insulating layer 302, so that a first individual transistor 304 having a first gate terminal 305 and a second individual transistor 306 having a second gate terminal 307 are formed. In this case, the first individual transistor 304 and the second individual transistor 306 are connected in parallel. The potential contact 313 is disposed in a region of the second individual transistor 306.
圖4展示第二個別單元414之第二組態。在此情形下,與圖3之參考符號之尾數相一致的參考符號之尾數表示相同特徵。另外,第二個別電晶體406具有第二絕緣層403,其使電位觸點413與第二閘極端子407電絕緣。第二絕緣層406經配置成相對於基板前側成直角且直接延伸至第二個別電晶體406之二維電子氣體中。 FIG. 4 shows a second configuration of the second individual unit 414. In this case, the mantissas of the reference symbols that correspond to the mantissas of the reference symbols in FIG. 3 represent the same characteristics. In addition, the second individual transistor 406 has a second insulating layer 403 that electrically insulates the potential contact 413 from the second gate terminal 407. The second insulating layer 406 is configured to be at a right angle to the front side of the substrate and directly extends into the two-dimensional electronic gas of the second individual transistor 406.
視情況,HEMT可包含複數個第二個別單元314及414。然 而,一個此類第二個別單元314及414足以起到過電壓保護的作用。 Optionally, the HEMT may include a plurality of second individual units 314 and 414. Of course However, one such second individual unit 314 and 414 is sufficient to function as an overvoltage protection.
在一個例示性具體實例中,HEMT包含複數個個別單元。該等個別單元皆並聯連接,以使得其具有一共同汲極端子、源極端子及閘極端子。在此情形下,單獨實施個別單元中之兩者。兩個個別單元經由一絕緣層與其他個別單元絕緣,其中此等個別單元仍具有一共同汲極及源極端子。此等兩個單獨實施之個別單元中的第一者含有另一歐姆觸點作為電位觸點,其處於實際基本單元之漂移分區上。實施兩個個別單元中之第二者,以使得閘極端子連接至第一個別單元之歐姆觸點。 In an illustrative specific example, the HEMT includes a plurality of individual units. The individual units are connected in parallel so that they have a common sink terminal, source terminal, and gate terminal. In this case, both of the individual units are implemented separately. Two individual cells are insulated from other individual cells via an insulating layer, wherein these individual cells still have a common drain and source terminal. The first of these two individually implemented individual units contains another ohmic contact as a potential contact, which is on the drift zone of the actual base unit. The second of the two individual units is implemented so that the gate terminal is connected to the ohmic contact of the first individual unit.
圖5展示根據本發明之HEMT 500的等效電路圖。該HEMT包含具有一第一閘極端子505的一第一個別電晶體504及具有一第二閘極端子507的一第二個別電晶體506。該第一個別電晶體504及該第二個別電晶體506藉助於共同源極端子508及共同汲極端子509並聯電連接。該HEMT包含具有兩個層的異質結構,該等層具有不同量值之能帶隙,例如AlGaN/GaN層或AlGaAs/GaAs,以使得二維電子氣體在主動組件下方形成。在此情形下,該二維電子氣體在汲極端子與源極端子之間形成一歐姆電阻。該HEMT具有一電位觸點513,該電位觸點自基板前側直接延伸至二維電子氣體,以使得歐姆電阻細分為一第一電阻510及一第二電阻511,亦即形成分壓器,該分壓器設定第二個別電晶體506之閘極電壓或維持電流。為了過電壓裝置之可靠功能性,維持電流必須高於閘極之接通電流,以使得第二個別電晶體506在過電壓情形下可用。此情形意指第二個別電晶體506正常為接通的。在此情形下,電位觸點513之位準設定維持電流。 FIG. 5 shows an equivalent circuit diagram of a HEMT 500 according to the present invention. The HEMT includes a first individual transistor 504 having a first gate terminal 505 and a second individual transistor 506 having a second gate terminal 507. The first individual transistor 504 and the second individual transistor 506 are electrically connected in parallel by means of a common source terminal 508 and a common drain terminal 509. The HEMT includes a heterostructure with two layers having band gaps of different magnitudes, such as an AlGaN / GaN layer or AlGaAs / GaAs, so that a two-dimensional electron gas is formed under the active component. In this case, the two-dimensional electron gas forms an ohmic resistance between the drain terminal and the source terminal. The HEMT has a potential contact 513 that extends directly from the front side of the substrate to a two-dimensional electronic gas, so that the ohmic resistance is subdivided into a first resistance 510 and a second resistance 511, that is, a voltage divider is formed. The voltage divider sets a gate voltage or a sustain current of the second individual transistor 506. For the reliable functionality of the over-voltage device, the sustain current must be higher than the on-current of the gate, so that the second individual transistor 506 is available in an over-voltage situation. This situation means that the second individual transistor 506 is normally on. In this case, the level of the potential contact 513 sets a sustain current.
舉例而言,電位觸點513之材料包含鈦/鋁/鎳/金觸點。 For example, the material of the potential contact 513 includes a titanium / aluminum / nickel / gold contact.
圖6展示用於製造包含複數個第一個別單元及至少一個第二個別單元之HEMT的方法600。該方法600以步驟610開始,該步驟610涉及在第二個別單元內製造一第一絕緣層。在此情形下,該第一絕緣層經配置成垂直於基板前側且直接延伸至二維電子氣體中。因此,製造具有一第一閘極端子的一第一個別電晶體及具有一第二閘極端子的一第二個別電晶體。後續步驟630涉及在第二個別電晶體之區內製造一電位觸點。該電位觸點亦經配置成垂直於基板前側且自基板前側直接延伸至第二個別電晶體之二維電子氣體中。後續步驟640涉及在電位觸點與第二閘極端子之間產生一電連接。 FIG. 6 shows a method 600 for manufacturing a HEMT including a plurality of first individual units and at least one second individual unit. The method 600 begins with step 610, which involves fabricating a first insulating layer in a second individual cell. In this case, the first insulating layer is configured to be perpendicular to the front side of the substrate and directly extends into the two-dimensional electronic gas. Therefore, a first individual transistor having a first gate terminal and a second individual transistor having a second gate terminal are manufactured. The subsequent step 630 involves making a potential contact in the region of the second individual transistor. The potential contact is also configured to be perpendicular to the front side of the substrate and directly extends from the front side of the substrate into the two-dimensional electron gas of the second individual transistor. The subsequent step 640 involves creating an electrical connection between the potential contact and the second gate terminal.
在一例示性具體實例中,在步驟610與步驟630之間執行步驟620,該步驟620涉及製造一第二絕緣層,該第二絕緣層經配置成垂直於基板前側且直接延伸至第二個別電晶體之二維電子氣體中。因此,電位觸點與第二閘極端子電隔離。 In an illustrative specific example, step 620 is performed between step 610 and step 630. This step 620 involves manufacturing a second insulating layer that is configured to be perpendicular to the front side of the substrate and directly extends to a second individual. The two-dimensional electron gas of the transistor. Therefore, the potential contact is electrically isolated from the second gate terminal.
200‧‧‧高電子遷移率的電晶體(HEMT) 200‧‧‧High Electron Mobility Transistor (HEMT)
201‧‧‧第一個別單元 201‧‧‧ the first individual unit
202‧‧‧第一絕緣層 202‧‧‧First insulation layer
205‧‧‧第一閘極端子 205‧‧‧First Gate Extreme
207‧‧‧第二閘極端子 207‧‧‧Second Gate Extreme
208‧‧‧源極端子 208‧‧‧Source terminal
209‧‧‧汲極端子 209‧‧‧ drain terminal
212‧‧‧閘極端子 212‧‧‧Gate terminal
213‧‧‧電位觸點 213‧‧‧potential contact
214‧‧‧第二個別單元 214‧‧‧Second Individual Unit
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| TWI889609B (en) * | 2020-05-29 | 2025-07-01 | 瑞典商艾皮諾科技公司 | A vertical hemt and a method to produce a vertical hemt |
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