TWI533451B - Silicon power device and power conversion equipment provided with the same - Google Patents
Silicon power device and power conversion equipment provided with the same Download PDFInfo
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- TWI533451B TWI533451B TW102147959A TW102147959A TWI533451B TW I533451 B TWI533451 B TW I533451B TW 102147959 A TW102147959 A TW 102147959A TW 102147959 A TW102147959 A TW 102147959A TW I533451 B TWI533451 B TW I533451B
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- 238000006243 chemical reaction Methods 0.000 title claims description 15
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 title 1
- 229910052710 silicon Inorganic materials 0.000 title 1
- 239000010703 silicon Substances 0.000 title 1
- 239000004065 semiconductor Substances 0.000 claims description 44
- 239000000758 substrate Substances 0.000 claims description 40
- 239000012535 impurity Substances 0.000 claims description 9
- 238000009792 diffusion process Methods 0.000 claims description 5
- 230000004888 barrier function Effects 0.000 claims description 3
- 230000005669 field effect Effects 0.000 claims 1
- 230000003071 parasitic effect Effects 0.000 description 15
- 239000000969 carrier Substances 0.000 description 10
- 238000002347 injection Methods 0.000 description 5
- 239000007924 injection Substances 0.000 description 5
- 230000009471 action Effects 0.000 description 2
- 230000015556 catabolic process Effects 0.000 description 2
- 230000000052 comparative effect Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- BASFCYQUMIYNBI-UHFFFAOYSA-N platinum Chemical compound [Pt] BASFCYQUMIYNBI-UHFFFAOYSA-N 0.000 description 2
- 238000004904 shortening Methods 0.000 description 2
- 229910000831 Steel Inorganic materials 0.000 description 1
- 238000009825 accumulation Methods 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 230000001186 cumulative effect Effects 0.000 description 1
- 238000010894 electron beam technology Methods 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
- 229910001385 heavy metal Inorganic materials 0.000 description 1
- 230000006872 improvement Effects 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- NFFIWVVINABMKP-UHFFFAOYSA-N methylidynetantalum Chemical compound [Ta]#C NFFIWVVINABMKP-UHFFFAOYSA-N 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 229910052697 platinum Inorganic materials 0.000 description 1
- 238000003825 pressing Methods 0.000 description 1
- 230000008569 process Effects 0.000 description 1
- 230000005855 radiation Effects 0.000 description 1
- 238000011084 recovery Methods 0.000 description 1
- 239000010959 steel Substances 0.000 description 1
- 229910003468 tantalcarbide Inorganic materials 0.000 description 1
- 229910052715 tantalum Inorganic materials 0.000 description 1
- GUVRBAGPIYLISA-UHFFFAOYSA-N tantalum atom Chemical compound [Ta] GUVRBAGPIYLISA-UHFFFAOYSA-N 0.000 description 1
Classifications
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
- H01L29/02—Semiconductor bodies ; Multistep manufacturing processes therefor
- H01L29/06—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions
- H01L29/08—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions with semiconductor regions connected to an electrode carrying current to be rectified, amplified or switched and such electrode being part of a semiconductor device which comprises three or more electrodes
- H01L29/083—Anode or cathode regions of thyristors or gated bipolar-mode devices
- H01L29/0834—Anode regions of thyristors or gated bipolar-mode devices, e.g. supplementary regions surrounding anode regions
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
- H01L29/02—Semiconductor bodies ; Multistep manufacturing processes therefor
- H01L29/06—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions
- H01L29/0603—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions characterised by particular constructional design considerations, e.g. for preventing surface leakage, for controlling electric field concentration or for internal isolations regions
- H01L29/0642—Isolation within the component, i.e. internal isolation
- H01L29/0649—Dielectric regions, e.g. SiO2 regions, air gaps
- H01L29/0653—Dielectric regions, e.g. SiO2 regions, air gaps adjoining the input or output region of a field-effect device, e.g. the source or drain region
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
- H01L29/40—Electrodes ; Multistep manufacturing processes therefor
- H01L29/402—Field plates
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
- H01L29/66—Types of semiconductor device ; Multistep manufacturing processes therefor
- H01L29/68—Types of semiconductor device ; Multistep manufacturing processes therefor controllable by only the electric current supplied, or only the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched
- H01L29/70—Bipolar devices
- H01L29/72—Transistor-type devices, i.e. able to continuously respond to applied control signals
- H01L29/739—Transistor-type devices, i.e. able to continuously respond to applied control signals controlled by field-effect, e.g. bipolar static induction transistors [BSIT]
- H01L29/7393—Insulated gate bipolar mode transistors, i.e. IGBT; IGT; COMFET
- H01L29/7395—Vertical transistors, e.g. vertical IGBT
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
- H01L29/66—Types of semiconductor device ; Multistep manufacturing processes therefor
- H01L29/86—Types of semiconductor device ; Multistep manufacturing processes therefor controllable only by variation of the electric current supplied, or only the electric potential applied, to one or more of the electrodes carrying the current to be rectified, amplified, oscillated or switched
- H01L29/861—Diodes
- H01L29/8611—Planar PN junction diodes
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- Engineering & Computer Science (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Power Engineering (AREA)
- Physics & Mathematics (AREA)
- Ceramic Engineering (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Computer Hardware Design (AREA)
- Metal-Oxide And Bipolar Metal-Oxide Semiconductor Integrated Circuits (AREA)
Description
本發明有關於半導體裝置及使用其之電力轉換裝置,特別有關於適合於具有絕緣閘構造之絕緣閘型雙極電晶體(Insulated Gate Bipolar Transistor:以下,略為IGBT)的半導體裝置及使用其之電力轉換裝置。 The present invention relates to a semiconductor device and a power conversion device using the same, and more particularly to a semiconductor device suitable for an insulated gate bipolar transistor (hereinafter, slightly IGBT) having an insulating gate structure and power using the same Conversion device.
IGBT係藉於閘極電極施加電壓以控制流通於集一射極間之電流的切換元件。由於IGBT可控制之電力及於從數十瓦特至數十萬瓦特之廣範圍,切換頻率亦廣泛為超過數十赫茲至幾百千赫,故使用於空調等之小電力機器甚至於鐵道和鋼鐵廠等之大電力機器。在此等電力機器方面,為了系統的高效化、小型化,強烈要求IGBT的導通損失與切換損失之減低。 The IGBT is a switching element that applies a voltage to the gate electrode to control the current flowing between the collector and the emitter. Because the IGBT can control the power and the wide range from tens of watts to hundreds of thousands of watts, the switching frequency is also widely exceeded tens of hertz to hundreds of kilohertz, so it is used in small electric machines such as air conditioners and even railways and steel. Large power machines such as factories. In terms of such power equipment, in order to increase the efficiency and miniaturization of the system, the conduction loss of the IGBT and the switching loss are strongly required to be reduced.
導通損失係ON時之電壓降(導通電壓)的減低為有效的,累積於漂移層之少數載子濃度越高,越可減低。此外,關斷損失係所累積之少數載子濃度越低越小, 於導通電壓與關斷損失之間存在抵換的關係。為了改善抵換,雖提高IE(電子注入促進)效果為有效的,惟IGBT的特性正在接近極限,進一步之特性改善處於艱難的狀況。 The decrease in the voltage drop (on-voltage) when the conduction loss is ON is effective, and the higher the concentration of the minority carrier accumulated in the drift layer, the lower it can be. In addition, the lower the concentration of the minority carriers accumulated by the shutdown loss, the smaller the smaller, There is a relationship between the turn-on voltage and the turn-off loss. In order to improve the resistance, although the effect of improving the IE (Electronic Injection Promotion) is effective, the characteristics of the IGBT are approaching the limit, and further improvement in characteristics is in a difficult state.
為了進一步改善特性,於專利文獻1(日本發明專利公開平3-268363號公報)揭露如圖15所示之4端子之IGBT構造。本構造係在集極側鄰接著高濃度p型射極層7與高濃度n+層25,於該各區域連接著個別之電極。藉作成如此之構成,ON時由於少數載子從高濃度p型射極層7被高量注入,故可提高平均載子濃度,可降低導通電壓。此外,關斷時由於藉使高濃度n+層25動作以可減低少數載子的累積,並可縮小尾電流,故關斷損失可減低。亦即,由於ON時作為IGBT而動作,關斷時作為切換速度快之MOSFET而動作,故可改善導通電壓與關斷損失之抵換。 In order to further improve the characteristics, a four-terminal IGBT structure as shown in FIG. 15 is disclosed in Patent Document 1 (Japanese Laid-Open Patent Publication No. Hei-3-268363). In this structure, a high-concentration p-type emitter layer 7 and a high-concentration n+ layer 25 are adjacent to the collector side, and individual electrodes are connected to the respective regions. With such a configuration, since a small amount of carriers are injected from the high-concentration p-type emitter layer 7 at a high level during ON, the average carrier concentration can be increased and the on-voltage can be lowered. In addition, the turn-off loss can be reduced by turning on the high-concentration n+ layer 25 to reduce the accumulation of minority carriers and to reduce the tail current. In other words, since it operates as an IGBT at the time of ON and operates as a MOSFET having a fast switching speed at the time of turning off, it is possible to improve the resistance between the on-voltage and the turn-off loss.
[專利文獻1]日本發明專利公開平3-268363號公報 [Patent Document 1] Japanese Patent Laid-Open Publication No. Hei-3-268363
然而,在圖15所示之IGBT構造方面,OFF時由於作為MOSFET而動作,故有集一射極間的反彈電 壓大的問題。此外,使高濃度n+層25動作之期間由於無電洞注入,故亦有即將關斷之前的導通損失增大之問題。 However, in the IGBT structure shown in FIG. 15, since it operates as a MOSFET during OFF, there is a rebound between the emitters. The problem of pressing down. Further, since there is no hole injection during the operation of the high-concentration n+ layer 25, there is a problem that the conduction loss immediately before the turn-off is increased.
本發明係鑑於上述之點而為之者,該目的在於提供一種半導體裝置及使用其之電力轉換裝置,可抑制反彈電壓之增大,同時可改善導通電壓與關斷損失之抵換。 The present invention has been made in view of the above circumstances, and an object thereof is to provide a semiconductor device and a power conversion device using the same, which can suppress an increase in a bounce voltage and can improve a resistance between a turn-on voltage and a turn-off loss.
為了解決上述問題,依照了本發明的半導體裝置為了在半導體裝置內注入載子而具備互相分離而設之第2導電型高濃度射極層及第2導電型低濃度射極層,並具備分別個別地電性連接於第2導電型高濃度射極層與第2導電型低濃度射極層的主電極。 In order to solve the above problems, the semiconductor device according to the present invention includes a second conductivity type high concentration emitter layer and a second conductivity type low concentration emitter layer which are provided separately from each other in order to inject a carrier into the semiconductor device. Each of the main electrodes of the second conductivity type high concentration emitter layer and the second conductivity type low concentration emitter layer is electrically connected to each other.
根據本發明,由於可在半導體裝置的動作中抑制累積於半導體裝置內之載子之量,故可一面抑制反彈電壓增大,一面改善導通電壓與關斷損失之抵換。此外,只要將依照了本發明的半導體裝置使用於電力轉換裝置,即可提升電力轉換裝置的可靠性,同時可減低電力損失。 According to the present invention, since the amount of carriers accumulated in the semiconductor device can be suppressed during the operation of the semiconductor device, it is possible to improve the resistance between the on-voltage and the turn-off loss while suppressing an increase in the buckling voltage. Further, as long as the semiconductor device according to the present invention is used in a power conversion device, the reliability of the power conversion device can be improved while power loss can be reduced.
1‧‧‧n-基板 1‧‧‧n-substrate
2‧‧‧p型基極層 2‧‧‧p-type base layer
3‧‧‧n型源極層 3‧‧‧n source layer
4‧‧‧射極電極 4‧‧ ‧ emitter electrode
5‧‧‧氧化膜 5‧‧‧Oxide film
6‧‧‧閘極電極 6‧‧‧Gate electrode
7‧‧‧p型高濃度射極層 7‧‧‧p type high concentration emitter layer
8‧‧‧p型低濃度射極層 8‧‧‧p type low concentration emitter layer
9‧‧‧連接於p型高濃度射極層之集極電極 9‧‧‧ Collector electrode connected to p-type high concentration emitter layer
10‧‧‧連接於p型低濃度射極層之集極電極 10‧‧‧ Collector electrode connected to p-type low concentration emitter layer
11‧‧‧外置切換元件 11‧‧‧External switching elements
12‧‧‧緩衝層 12‧‧‧ Buffer layer
13‧‧‧高濃度n+層 13‧‧‧High concentration n+ layer
14‧‧‧絕緣層 14‧‧‧Insulation
15‧‧‧電洞阻障層 15‧‧‧ hole barrier
16‧‧‧外置MOSFET 16‧‧‧External MOSFET
17‧‧‧第2之閘極氧化膜 17‧‧‧2nd gate oxide film
18‧‧‧第2閘極電極 18‧‧‧2nd gate electrode
19‧‧‧p型反轉層 19‧‧‧p type inversion layer
20‧‧‧集極電極 20‧‧‧ Collector electrode
21‧‧‧陰極側n+層 21‧‧‧ cathode side n+ layer
22‧‧‧陰極電極 22‧‧‧Cathode electrode
23‧‧‧連接於高濃度p型射極層之陽極電極 23‧‧‧Anode electrode connected to a high concentration p-type emitter layer
24‧‧‧連接於低濃度p型射極層之陽極電極 24‧‧‧Anode electrode connected to a low concentration p-type emitter layer
25‧‧‧高濃度n+層 25‧‧‧High concentration n+ layer
101、102‧‧‧直流端子 101, 102‧‧‧ DC terminals
103、104、105‧‧‧交流端子 103, 104, 105‧‧‧ AC terminals
106‧‧‧閘極驅動電路 106‧‧‧ gate drive circuit
107‧‧‧IGBT 107‧‧‧IGBT
108‧‧‧二極體 108‧‧‧ diode
201‧‧‧IGBT 201‧‧‧IGBT
202‧‧‧外置MOSFET 202‧‧‧External MOSFET
203‧‧‧驅動IC 203‧‧‧Drive IC
204‧‧‧內置於射極側之MOS電晶體 204‧‧‧MOS transistor built into the emitter side
205‧‧‧漂移電阻 205‧‧‧drift resistance
206、207‧‧‧內置於集極之pn二極體 206, 207‧‧‧ pn diodes built into the collector
208‧‧‧電源端子 208‧‧‧Power terminal
209‧‧‧輸出端子 209‧‧‧Output terminal
210‧‧‧射極端子 210‧‧‧ shot extremes
211‧‧‧閘極電極 211‧‧‧gate electrode
212‧‧‧閘極電極 212‧‧‧gate electrode
[圖1]繪示是本發明之實施之形態1之IGBT。 Fig. 1 is a view showing an IGBT according to a first embodiment of the present invention.
[圖2]係使用了實施之形態1之IGBT之電路的一例。 FIG. 2 is an example of a circuit using the IGBT of the first embodiment.
[圖3]繪示實施之形態1之驅動序列。 FIG. 3 shows a driving sequence of the embodiment 1 of the embodiment.
[圖4]繪示實施之形態1之導通電壓與關斷損失之抵換關係。 FIG. 4 is a diagram showing the relationship between the on-voltage and the turn-off loss of the first embodiment.
[圖5]繪示是本發明之實施之形態2之IGBT。 Fig. 5 is a view showing an IGBT according to a second embodiment of the present invention.
[圖6]繪示是本發明之實施之形態3之IGBT。 Fig. 6 is a view showing an IGBT according to a third embodiment of the present invention.
[圖7]繪示是實施之形態3之變化例之IGBT。 Fig. 7 is a view showing an IGBT according to a variation of Embodiment 3 of the embodiment.
[圖8]繪示是本發明之實施之形態4之IGBT。 Fig. 8 is a view showing an IGBT according to a fourth embodiment of the present invention.
[圖9]繪示是實施之形態4之變化例之IGBT。 Fig. 9 is a view showing an IGBT according to a variation of Embodiment 4 of the embodiment.
[圖10]繪示是本發明之實施之形態5之IGBT。 Fig. 10 is a view showing an IGBT according to a fifth embodiment of the present invention.
[圖11]繪示是本發明之實施之形態6之IGBT。 Fig. 11 is a view showing an IGBT according to a sixth embodiment of the present invention.
[圖12]繪示是實施之形態6之變化例之IGBT。 Fig. 12 is a view showing an IGBT according to a variation of Embodiment 6 of the embodiment.
[圖13]繪示本發明之實施之形態7之IGBT。 Fig. 13 is a view showing an IGBT of a seventh embodiment of the present invention.
[圖14]繪示是本發明之實施之形態9之電力轉換裝置。 Fig. 14 is a diagram showing a power conversion device according to a ninth embodiment of the present invention.
[圖15]繪示揭露於專利文獻1之歷來的IGBT。 FIG. 15 shows an IGBT disclosed in Patent Document 1.
[圖16]繪示是本發明之實施之形態8之二極體。 Fig. 16 is a view showing a diode of the eighth aspect of the present invention.
以下,根據圖示之實施例詳細地說明本發明之半導體裝置。另外,於供以說明實施之形態的全圖,對於相同的構件原則上附加相同的符號,並省略其重複的說明。另外,圖中、p-、p、p+此等標記表示半導體層為p 型,且依此順序表示雜質濃度相對地高。此外,n-、n、n+此等標記表示半導體層為n型,且依此順序表示雜質濃度相對地高。 Hereinafter, a semiconductor device of the present invention will be described in detail based on the illustrated embodiments. In the entire drawings, the same components are denoted by the same reference numerals, and the repeated description thereof will be omitted. In addition, in the figure, p-, p, p+, etc. indicate that the semiconductor layer is p Type, and in this order, the impurity concentration is relatively high. Further, the marks n-, n, n+ indicate that the semiconductor layer is n-type, and in this order, the impurity concentration is relatively high.
在圖1繪示是本發明之實施之形態1之IGBT的剖面構造。 Fig. 1 is a cross-sectional view showing an IGBT of a first embodiment of the present invention.
在本實施之形態1之IGBT方面,設有n-基板1、選擇性形成於此n-基板1之表面之p型基極層2、形成於p型基極層的表面之n+型源極層3、及電性連接於p型基極層2與n+型源極層3且形成於n+型源極層3的表面之射極電極4,並在被n-基板1與n+型源極層3夾住之p型基極層2的表面隔著閘極氧化膜5而設有閘極電極6。另外在本實施之形態1之IGBT方面,在n-基板1的另一側之表面,p+型高濃度射極層7及p-型低濃度射極層8因n-層1的一部分介入此等之間而分別互相分離為個別的p型導電類型的半導體層。並且,在p+型高濃度射極層7與p-型低濃度射極層8分別電性連接著個別之電極9及10。亦即,此IGBT成為4端子元件。 In the IGBT of the first aspect of the present invention, the n-substrate 1, the p-type base layer 2 selectively formed on the surface of the n-substrate 1, and the n+-type source formed on the surface of the p-type base layer are provided. a layer 3 and an emitter electrode 4 electrically connected to the p-type base layer 2 and the n + -type source layer 3 and formed on the surface of the n + -type source layer 3, and being n-substrate 1 and n+ type source The gate electrode 6 is provided on the surface of the p-type base layer 2 sandwiched by the layer 3 via the gate oxide film 5. Further, in the IGBT of the first embodiment of the present embodiment, the p + -type high-concentration emitter layer 7 and the p-type low-concentration emitter layer 8 are interposed by a part of the n-layer 1 on the other surface of the n-substrate 1 . They are separated from each other into individual p-type conductivity type semiconductor layers. Further, the respective electrodes 9 and 10 are electrically connected to the p + -type high-concentration emitter layer 7 and the p-type low-concentration emitter layer 8 , respectively. That is, this IGBT becomes a 4-terminal element.
圖2係使用了圖1的IGBT之電路的一例,集極端子c1對應於連接於圖1的p+型高濃度射極層7之端子,端子c2對應於連接於p-型低濃度射極層8之端子。在此例方面,IGBT201的集極端子c2隔著作為開關而工作之MOSFET202而連接於輸出端子209(C),再另一方 面之集極端子c1係直接連接於輸出端子209(C)。但是,集極端子c1可隔著與MOSFET202相異之切換元件而連接於輸出端子209(C),使切換元件為MOSFET和IGBT等之絕緣閘型的元件最理想。此外,亦可代替MOSFET202而使用IGBT等之其他的絕緣閘控制型之元件。 2 is an example of a circuit using the IGBT of FIG. 1. The collector terminal c1 corresponds to a terminal connected to the p+ type high concentration emitter layer 7 of FIG. 1, and the terminal c2 corresponds to a p-type low concentration emitter layer. 8 terminal. In this example, the collector terminal c2 of the IGBT 201 is connected to the output terminal 209 (C) via the MOSFET 202 operating as a switch, and the other side The set terminal c1 of the face is directly connected to the output terminal 209 (C). However, the collector terminal c1 can be connected to the output terminal 209 (C) via a switching element different from the MOSFET 202, and the switching element is preferably an insulating gate type element such as a MOSFET or an IGBT. Further, instead of the MOSFET 202, another insulating gate control type element such as an IGBT may be used.
IGBT201之ON時係於閘極電極6(端子G1)施加電壓(例如15V),於端子G2輸入MOSFET202成為OFF之電壓(例如0V),以使電流流通於集極端子c1與射極端子210之間。藉此,由於少數載子(電洞)從連接於端子c1之p+型高濃度射極層7高量注入n-基板1,故促進傳導度調變,導通電壓減低。從使端子G1(IGBT201)OFF之數μs跟前在端子G2輸入ON信號,電流主要在集極端子c2與射極端子210之間流通。集極端子c1與c2雖係共同連接於輸出端子209(C),惟由於雜質濃度為低的p型低濃度射極層8內建電壓為低的,故電子電流容易流進p-型低濃度射極層8(端子c2)。為此,由於從集極所注入之少數載子變少,累積於n-基板1之電荷減低,故關斷損失可減低。再者,OFF時由於作為低量注入之IGBT而動作,故可抑制尾電流產生,集極-射極間之反彈電壓增大。 When the IGBT 201 is turned on, a voltage (for example, 15 V) is applied to the gate electrode 6 (terminal G1), and a voltage (for example, 0 V) at which the MOSFET 202 is turned off is input to the terminal G2 so that current flows through the collector terminal c1 and the emitter terminal 210. between. Thereby, since a small number of carriers (holes) are injected into the n-substrate 1 from the p+ type high-concentration emitter layer 7 connected to the terminal c1, the conductivity is modulated and the on-voltage is reduced. An electric signal is input to the terminal G2 from the number μs at which the terminal G1 (IGBT 201) is turned off, and the current mainly flows between the collector terminal c2 and the emitter terminal 210. Although the collector terminals c1 and c2 are commonly connected to the output terminal 209 (C), since the built-in voltage of the p-type low-concentration emitter layer 8 having a low impurity concentration is low, the electron current easily flows into the p-type low. Concentration emitter layer 8 (terminal c2). For this reason, since the minority carriers injected from the collector are reduced, the charge accumulated in the n-substrate 1 is reduced, so that the turn-off loss can be reduced. Further, since OFF operates as a low-injection IGBT, it is possible to suppress the generation of the tail current and increase the rebound voltage between the collector and the emitter.
圖3係閘極電極6(端子G1)與MOSFET202之閘極電極212(端子G2)之驅動序列。期間1係少數載子被高量注入之期間,於端子G1輸入MOS電晶體204會 ON之電壓,於端子G2輸入MOSFET202會OFF之電壓。在此期間,由於少數載子被高量注入,故導通電壓與其他的期間比較之下為小的。期間2係少數載子被低量注入之期間,從端子G1會OFF之跟前0.1~10μs在端子G2輸入ON信號。由於少數載子的注入為低的,故累積於n-基板之電荷減低,端子G1從ON切換至OFF時的損失減低。順帶一提,期間2雖累積於n-基板1之少數載子減低,而使得導通電壓增大,惟由於端子G1與G2會ON之期間(滯定時間)為短的,故全體的損失幾乎不增大。期間3係IGBT201會OFF之期間,開始時,於端子G1輸入IGBT201會OFF之電壓,於端子G2輸入MOSFET202會ON之電壓。端子G2係在端子G1輸入OFF信號之期間3中輸入OFF信號,之後僅端子G1從OFF切換至ON,轉移至期間4。期間4係與期間1相同期間,之後,重複從期間1至3的序列。在本實施形態方面,藉由如此之驅動序列可改善導通電壓與關斷損失之抵換。 3 is a driving sequence of the gate electrode 6 (terminal G1) and the gate electrode 212 (terminal G2) of the MOSFET 202. During the period 1 when a minority carrier is injected with a high amount, the MOS transistor 204 is input to the terminal G1. The voltage of ON is input to the terminal G2 and the voltage at which the MOSFET 202 is turned off. During this period, since a small number of carriers are injected at a high amount, the on-voltage is small compared with other periods. During the period 2, when a minority carrier is injected with a low amount, an ON signal is input to the terminal G2 from 0.1 to 10 μs before the terminal G1 is turned OFF. Since the injection of a small number of carriers is low, the charge accumulated in the n-substrate is reduced, and the loss when the terminal G1 is switched from ON to OFF is reduced. Incidentally, in the period 2, although the minority carriers accumulated in the n-substrate 1 are reduced, the on-voltage is increased, but since the period during which the terminals G1 and G2 are turned on (the lag time) is short, the total loss is almost Do not increase. During the period in which the IGBT 201 is turned off, the voltage at which the IGBT 201 is turned off is input to the terminal G1, and the voltage at which the MOSFET 202 is turned on is input to the terminal G2. The terminal G2 inputs an OFF signal in the period 3 during which the OFF signal is input to the terminal G1, and thereafter only the terminal G1 is switched from OFF to ON, and the process shifts to the period 4. The period 4 is the same period as the period 1, and thereafter, the sequence from the period 1 to 3 is repeated. In this embodiment, the resistance between the turn-on voltage and the turn-off loss can be improved by such a driving sequence.
圖4繪示導通電壓與關斷損失之抵換關係的一例,使反彈電壓為相同大小。於圖繪示對應於圖15之比較例、及本實施之形態1。以相同導通電壓比較之情況下,本實施之形態的關斷損失與比較例比較之下減低57%,特性大幅地改善。 FIG. 4 illustrates an example of the relationship between the on-voltage and the turn-off loss, and the bounce voltage is the same size. The comparative example corresponding to FIG. 15 and the first aspect of the present embodiment are shown in the drawing. In the case of comparison with the same on-voltage, the turn-off loss of the embodiment of the present embodiment was reduced by 57% in comparison with the comparative example, and the characteristics were greatly improved.
如以上地,在本實施之形態的IGBT方面,藉由在集極側形成p+型高濃度射極層7與p-型低濃度射極層8,並分別設置個別之電極,可一面抑制集極-射極間之 反彈電壓增大,一面改善導通電壓與關斷損失之抵換。 As described above, in the IGBT of the present embodiment, by forming the p + -type high-concentration emitter layer 7 and the p-type low-concentration emitter layer 8 on the collector side, and providing individual electrodes, it is possible to suppress the set. Polar-emitter The rebound voltage is increased to improve the resistance between the turn-on voltage and the turn-off loss.
圖5係繪示本發明之實施之形態2之IGBT的剖面構造者。在實施之形態2所示之IGBT方面,在n-基板1與p+型高濃度射極層7之間、及n-基板1與p-型低濃度射極層8之間,設置雜質濃度比n-基板1高、雜質濃度比p+型高濃度射極層7低之n緩衝層12。由於可藉n緩衝層12減低供以得到期望的崩潰電壓之n-基板1之厚度,故可改善導通電壓與崩潰電壓之抵換。 Fig. 5 is a cross-sectional structural view of an IGBT according to a second embodiment of the present invention. In the IGBT shown in the second aspect, the impurity concentration ratio is set between the n-substrate 1 and the p+ type high concentration emitter layer 7, and between the n-substrate 1 and the p-type low concentration emitter layer 8. The n-buffer layer 12 having a high n-substrate 1 and a lower impurity concentration than the p+-type high-concentration emitter layer 7. Since the thickness of the n-substrate 1 supplied with the desired breakdown voltage can be reduced by the n buffer layer 12, the resistance between the on-voltage and the breakdown voltage can be improved.
圖6係繪示本發明之實施之形態3之IGBT的剖面構造者。在實施之形態3所示之IGBT方面,在p+型高濃度射極層7與p-型低濃度射極層8之間設有雜質濃度1×1018~1×1021cm-3之高濃度n+層13。 Fig. 6 is a cross-sectional view showing the structure of an IGBT according to a third embodiment of the present invention. In the IGBT shown in the third aspect, the impurity concentration of 1×10 18 to 1×10 21 cm -3 is set between the p + -type high-concentration emitter layer 7 and the p-type low-concentration emitter layer 8 . Concentration n+ layer 13.
藉作成如此之構造,可抑制由p+型高濃度射極層7與n-基板1(或n緩衝層12)、p-型低濃度射極層8所構成之寄生pnp雙極電晶體之動作。若寄生pnp電晶體動作,則使用了外置的切換元件11之少數載子注入的調節(p+型高濃度射極層7與p-型低濃度射極層8之切換)變難,影響導通電壓與關斷損失之抵換。例如,由於若在使外置切換元件11ON時寄生電晶體動作,則少數載子從p+型高濃度射極層7被高量注入,故n-基板1的電 洞之累積量增加,關斷損失增大。 With such a structure, the action of the parasitic pnp bipolar transistor composed of the p+ type high concentration emitter layer 7 and the n-substrate 1 (or n buffer layer 12) and the p-type low concentration emitter layer 8 can be suppressed. . When the parasitic pnp transistor operates, the adjustment of the minority carrier injection using the external switching element 11 (switching of the p+ type high concentration emitter layer 7 and the p-type low concentration emitter layer 8) becomes difficult, affecting the conduction. The exchange of voltage and turn-off loss. For example, if the parasitic transistor operates when the external switching element 11 is turned on, a minority carrier is injected from the p+ type high concentration emitter layer 7 at a high amount, so that the n-substrate 1 is charged. The cumulative amount of holes increases and the turn-off loss increases.
在圖6之實施形態雖使被p+型高濃度射極層7與p-型低濃度射極層8夾住之全部的區域為高濃度n+層13,惟使被p+型高濃度射極層7與p-型低濃度射極層8夾住之一部分的區域為高濃度n+層13之構造亦可抑制寄生電晶體的動作。此外,高濃度n+層13的深度亦可為作成比p+型高濃度射極層7及p-型低濃度射極層8淺之構造。但是,若如圖7所示地使高濃度n+層13比p型高濃度射極層7及p型低濃度射極層8深,則更可抑制寄生pnp雙極電晶體之動作。 In the embodiment of Fig. 6, all of the regions sandwiched by the p+ type high-concentration emitter layer 7 and the p-type low-concentration emitter layer 8 are high-concentration n+ layers 13, but are p+-type high-concentration emitter layers. The structure in which a portion sandwiched by the p-type low-concentration emitter layer 8 is a high-concentration n+ layer 13 can also suppress the operation of the parasitic transistor. Further, the depth of the high-concentration n+ layer 13 may be made shallower than the p+-type high-concentration emitter layer 7 and the p-type low-concentration emitter layer 8. However, if the high-concentration n+ layer 13 is made deeper than the p-type high-concentration emitter layer 7 and the p-type low-concentration emitter layer 8 as shown in FIG. 7, the operation of the parasitic pnp bipolar transistor can be suppressed.
圖8繪示是本發明之實施之形態4之IGBT的剖面構造。在實施之形態4所示之IGBT方面,於p+型高濃度射極層7與p-型低濃度射極層8之間設有絕緣層14。 Fig. 8 is a cross-sectional view showing the IGBT of the fourth embodiment of the present invention. In the IGBT shown in the fourth aspect, the insulating layer 14 is provided between the p+ type high concentration emitter layer 7 and the p-type low concentration emitter layer 8.
藉作成如此之構造,可比實施之形態3更抑制寄生電晶體的動作。在實施之形態2雖藉設置高濃度n+層13而抑制寄生電晶體的動作,惟在實施之形態4係使寄生pnp電晶體之n層的一部分為絕緣層以抑制寄生電晶體的動作。在圖8雖使被p+型高濃度射極層7與p-型低濃度射極層8夾住之全部的區域為絕緣層14,惟使被p+型高濃度射極層7與p-型低濃度射極層8夾住之一部分的區域為絕緣層14之構造亦可,此外絕緣層14的深度比p+型高濃度射極層7及p-型低濃度射極層8淺亦可。此 外,若如圖9所示地使絕緣層14比p+型高濃度射極層7及p-型低濃度射極層8深,則更可抑制寄生pnp雙極電晶體之動作。 By adopting such a structure, the operation of the parasitic transistor can be suppressed more than the form 3 of the embodiment. In the second embodiment, the high-concentration n+ layer 13 is provided to suppress the operation of the parasitic transistor. However, in the fourth embodiment, a part of the n layers of the parasitic pnp transistor is made an insulating layer to suppress the operation of the parasitic transistor. In Fig. 8, the entire region sandwiched by the p+ type high-concentration emitter layer 7 and the p-type low-concentration emitter layer 8 is the insulating layer 14, but the p+ type high-concentration emitter layer 7 and the p-type are used. The region in which the low-concentration emitter layer 8 is sandwiched may be a structure of the insulating layer 14, and the depth of the insulating layer 14 may be shallower than that of the p+-type high-concentration emitter layer 7 and the p-type low-concentration emitter layer 8. this Further, when the insulating layer 14 is deeper than the p + -type high-concentration emitter layer 7 and the p-type low-concentration emitter layer 8 as shown in FIG. 9, the operation of the parasitic pnp bipolar transistor can be suppressed.
圖10係繪示是本發明之實施之形態5之IGBT的剖面構造者。在實施之形態5所示之IGBT方面,p+型高濃度射極層7與p-型低濃度射極層8之間的距離ln長於電洞的擴散距離Lp(ln>Lp)。 Fig. 10 is a cross-sectional structural view of an IGBT according to a fifth embodiment of the present invention. In the IGBT shown in the fifth aspect, the distance ln between the p + -type high-concentration emitter layer 7 and the p-type low-concentration emitter layer 8 is longer than the diffusion distance Lp (ln > Lp) of the hole.
藉作成如此之構造,可在未將高濃度n+層和絕緣層等設置於p+型高濃度射極層7與p-型低濃度射極層8之間的情況下抑制寄生pnp雙極電晶體之動作。電洞的擴散距離Lp係根據電洞的擴散係數Dp與壽命τp之積的平方根而求得,Lp長於基極區域的寬度ln之情況下,寄生電晶體動作。原因在於,從射極區域(例如p-型低濃度射極層8)所注入之電洞在基極區域(n緩衝層12或n-基板1)未再結合消滅而因擴散到達集極區域(例如p+型高濃度射極層7)。因此,由於藉Lp縮短或ln增大以使電洞在到達集極區域之前再結合消滅,故可抑制寄生電晶體的動作。p+型高濃度射極層7與p-型低濃度射極層8之間的n層(在圖10係n-基板1)之雜質濃度為1×1017cm-3以下之情況下,使ln為5μm以上最理想。 With such a configuration, the parasitic pnp bipolar transistor can be suppressed without providing a high concentration n+ layer and an insulating layer or the like between the p+ type high concentration emitter layer 7 and the p-type low concentration emitter layer 8. The action. The diffusion distance Lp of the hole is obtained from the square root of the product of the diffusion coefficient Dp of the cavity and the lifetime τp. When Lp is longer than the width ln of the base region, the parasitic transistor operates. The reason is that the hole injected from the emitter region (for example, the p-type low-concentration emitter layer 8) is not recombined in the base region (n buffer layer 12 or n-substrate 1) and is diffused to reach the collector region. (for example, p+ type high concentration emitter layer 7). Therefore, since Lp is shortened or ln is increased to cause the holes to be combined and eliminated before reaching the collector region, the operation of the parasitic transistor can be suppressed. In the case where the impurity concentration of the n layer (n-substrate 1 in FIG. 10) between the p + -type high-concentration emitter layer 7 and the p-type low-concentration emitter layer 8 is 1 × 10 17 cm -3 or less, It is most preferable that ln is 5 μm or more.
擴散距離Lp係可藉縮短壽命τp以縮短,可藉將壽命衰減元素導入集極側以控制。於使電洞再結合之 壽命衰減元素利用金和白金等之重金屬、或由於電子束等之放射線之照射損傷等;藉此,ln縮短至1μm等級仍可抑制寄生電晶體的動作。 The diffusion distance Lp can be shortened by shortening the lifetime τp, and can be controlled by introducing the life decay element into the collector side. For recombining the holes The life-attenuating element utilizes a heavy metal such as gold or platinum or an irradiation damage due to radiation such as an electron beam; thereby, the operation of the parasitic transistor can be suppressed by shortening the ln to a level of 1 μm.
圖11、12分別繪示是本發明之實施之形態6及其變化例之IGBT的剖面構造。在此等IGBT方面,在p+型高濃度射極層7與n緩衝層12(或n-基板1)之間設有n+型之電洞阻障層15。 11 and 12 respectively show cross-sectional structures of an IGBT according to a sixth embodiment of the present invention and a modified example thereof. In the case of such IGBTs, an n+ type hole barrier layer 15 is provided between the p+ type high concentration emitter layer 7 and the n buffer layer 12 (or n-substrate 1).
藉作成如此之構造,可抑制從p-型低濃度射極層8流往p+型高濃度射極層7之電洞電流,可抑制寄生pnp雙極電晶體之動作。 With such a structure, the hole current flowing from the p-type low-concentration emitter layer 8 to the p+-type high-concentration emitter layer 7 can be suppressed, and the operation of the parasitic pnp bipolar transistor can be suppressed.
圖13繪示是本發明之實施之形態之IGBT的剖面構造。 Fig. 13 is a cross-sectional view showing the IGBT of the embodiment of the present invention.
本實施之形態7之IGBT具備:n-基板1、選擇性形成於此n-基板1之表面的p型基極層2、形成於p型基極層的表面之n+型源極層3、電性連接於p型基極層2與n+型源極層3且形成於n+型源極層3的表面之射極電極4、及在被n-基板1與n+型源極層3夾住之p型基極層2的表面隔著閘極氧化膜5而設之閘極電極6。再者,在本實施形態中,於n-基板1之相反的表面,p+型高濃度射極層7與p-型低濃度射極層8與實施之形態1同樣地以 互相分離之狀態而形成,於p+型高濃度射極層7連接著集極電極20,在被p-型高濃度射極層7與p型低濃度射極層8夾住之n-基板1之表面隔著第2之閘極氧化膜17而形成第2閘極電極18。透過藉於此第2閘極電極輸入負電壓而形成之p型反轉層19,p+型高濃度射極層7與p-型低濃度射極層8被電性連接。 The IGBT of the seventh embodiment of the present invention includes an n-substrate 1, a p-type base layer 2 selectively formed on the surface of the n-substrate 1, and an n+-type source layer 3 formed on the surface of the p-type base layer. The emitter electrode 4 electrically connected to the p-type base layer 2 and the n + -type source layer 3 and formed on the surface of the n + -type source layer 3, and sandwiched by the n-substrate 1 and the n + -type source layer 3 The gate electrode 6 is provided on the surface of the p-type base layer 2 via the gate oxide film 5. Further, in the present embodiment, the p + -type high-concentration emitter layer 7 and the p-type low-concentration emitter layer 8 are formed on the opposite surface of the n-substrate 1 in the same manner as in the first embodiment. Formed in a state of being separated from each other, the collector electrode 20 is connected to the p + -type high-concentration emitter layer 7 , and the n-substrate 1 is sandwiched between the p-type high-concentration emitter layer 7 and the p-type low-concentration emitter layer 8 The second gate electrode 18 is formed on the surface via the second gate oxide film 17. The p + -type high-concentration emitter layer 7 and the p-type low-concentration emitter layer 8 are electrically connected to each other through the p-type inversion layer 19 formed by inputting a negative voltage to the second gate electrode.
藉作成如此之構造,與設有外部切換元件之情況同樣地,可改善導通電壓與關斷損失之抵換。在圖13雖使p+型高濃度射極層7與p-型低濃度射極層8之間的區域為n-基板1,惟作成插入雜質濃度比n-基板高之n型阱層(未圖示)的構造亦可。 With such a configuration, as in the case where the external switching element is provided, the resistance between the ON voltage and the turn-off loss can be improved. In Fig. 13, although the region between the p + -type high-concentration emitter layer 7 and the p-type low-concentration emitter layer 8 is the n-substrate 1, it is formed as an n-type well layer having an impurity concentration higher than that of the n-substrate (not The structure shown in the figure) is also possible.
圖16繪示是本發明之實施之形態8之二極體的剖面構造。 Fig. 16 is a cross-sectional view showing a diode of a form 8 of the embodiment of the present invention.
在本實施之形態8之二極體方面,於設有n-基板1、及形成於此n-基板1之表面之陰極側n+層21並在n+層21的表面設有陰極電極22之構造方面,在n-基板1的另一側之表面,p+型高濃度射極層7與p-型低濃度射極層8因n-基板1介入此等之間而互相分離,且於p+型高濃度射極層7與p-型低濃度射極層8分別連接著個別之電極。 In the aspect of the diode of the eighth aspect of the present invention, the n-substrate 1 and the cathode-side n+ layer 21 formed on the surface of the n-substrate 1 are provided, and the cathode electrode 22 is provided on the surface of the n+ layer 21. On the other hand, on the other side of the n-substrate 1, the p+ type high concentration emitter layer 7 and the p-type low concentration emitter layer 8 are separated from each other by the n-substrate 1 intervening, and are p+ type. The high-concentration emitter layer 7 and the p-type low-concentration emitter layer 8 are respectively connected to individual electrodes.
由於藉作成如此之構造可調節累積於n-基板1之少數載子之量,故可改善順向的電壓降與恢復損失之 抵換。 Since the amount of minority carriers accumulated in the n-substrate 1 can be adjusted by such a configuration, the forward voltage drop and recovery loss can be improved. Replace.
圖14繪示使用了藉上述之各實施之形態而說明之IGBT或二極體之電力轉換裝置的一例。 FIG. 14 shows an example of a power conversion device using an IGBT or a diode described in the above embodiments.
圖14之實施之形態9係換流器。2個的IGBT107串聯之串聯電路連接於直流端子101與102之間。此串聯電路具備交流的相數份,各串聯電路之串聯連接點連接於交流端子103、104、105。在本實施形態方面,交流的相數係3相,具備3個的串聯電路。此外,於各IGBT107反並聯地連接著二極體108。 The form of the embodiment of Fig. 14 is an inverter. A series circuit in which two IGBTs 107 are connected in series is connected between the DC terminals 101 and 102. The series circuit has a phase number of alternating current, and the series connection points of the series circuits are connected to the alternating current terminals 103, 104, and 105. In the present embodiment, the number of phases of the alternating current is three phases, and three series circuits are provided. Further, the diode 108 is connected in anti-parallel to each of the IGBTs 107.
基於各IGBT107藉閘極驅動電路106而被ON/OFF驅動,在直流端子101、102受電之直流電力轉換成交流電力,交流電力被從交流端子103、104、105輸出。 Each of the IGBTs 107 is driven by ON/OFF by the gate drive circuit 106, and DC power received at the DC terminals 101 and 102 is converted into AC power, and AC power is output from the AC terminals 103, 104, and 105.
作為IGBT107,使用上述之本實施之形態1至7的IGBT。此外,作為二極體108使用實施之形態8之二極體亦可。再者,使IGBT107為歷來的IGBT,作為二極體108使用實施之形態8之二極體亦可。 As the IGBT 107, the IGBTs of the first to seventh embodiments of the present embodiment described above are used. Further, the diode of the eighth aspect to be implemented may be used as the diode 108. Further, the IGBT 107 may be a conventional IGBT, and the diode of the eighth aspect to be implemented may be used as the diode 108.
藉將以上述之各實施之形態說明之IGBT或二極體應用於電力轉換裝置,可減低電力轉換裝置之電力損失。 By applying the IGBT or the diode described in the above embodiments to the power conversion device, the power loss of the power conversion device can be reduced.
另外,本實施之形態9雖係換流器裝置,惟對於轉換器和截波器等之其他的電力轉換裝置亦可應用依 照了本發明的IGBT及二極體,可得到同樣的效果。 Further, the ninth embodiment of the present embodiment is an inverter device, but may be applied to other power conversion devices such as a converter and a chopper. According to the IGBT and the diode of the present invention, the same effect can be obtained.
本發明之實施之形態非限定於前述之實施之形態者,在本發明之技術性思想的範圍內,不言而喻,可作種種變更。 The embodiment of the present invention is not limited to the embodiment described above, and it is needless to say that various modifications can be made without departing from the spirit and scope of the invention.
例如,射極側之閘極形狀不限於平面型,亦可為溝槽型,該閘極亦可配置成條紋狀和網狀。 For example, the shape of the gate on the emitter side is not limited to a planar type, and may be a groove type, and the gate may be configured in a stripe shape and a mesh shape.
此外,前述實施之形態雖係縱型IGBT與縱型二極體,惟亦可為橫型IGBT及橫型二極體。此外,半導體材料可為矽亦可為碳化矽。 Further, although the above-described embodiment is a vertical IGBT and a vertical diode, it may be a horizontal IGBT or a lateral diode. In addition, the semiconductor material may be tantalum or tantalum carbide.
1‧‧‧n-基板 1‧‧‧n-substrate
2‧‧‧p型基極層 2‧‧‧p-type base layer
3‧‧‧n型源極層 3‧‧‧n source layer
4‧‧‧射極電極 4‧‧ ‧ emitter electrode
5‧‧‧氧化膜 5‧‧‧Oxide film
6‧‧‧閘極電極 6‧‧‧Gate electrode
7‧‧‧p型高濃度射極層 7‧‧‧p type high concentration emitter layer
8‧‧‧p型低濃度射極層 8‧‧‧p type low concentration emitter layer
9‧‧‧連接於p型高濃度射極層之集極電極 9‧‧‧ Collector electrode connected to p-type high concentration emitter layer
10‧‧‧連接於p型低濃度射極層之集極電極 10‧‧‧ Collector electrode connected to p-type low concentration emitter layer
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