WO2018060679A1 - 3c-sic igbt - Google Patents

3c-sic igbt Download PDF

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Publication number
WO2018060679A1
WO2018060679A1 PCT/GB2017/052815 GB2017052815W WO2018060679A1 WO 2018060679 A1 WO2018060679 A1 WO 2018060679A1 GB 2017052815 W GB2017052815 W GB 2017052815W WO 2018060679 A1 WO2018060679 A1 WO 2018060679A1
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Prior art keywords
region
silicon substrate
silicon
sic
conductivity type
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PCT/GB2017/052815
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French (fr)
Inventor
Peter Ward
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Anvil Semiconductors Limited
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Priority claimed from US15/282,235 external-priority patent/US20170018634A1/en
Application filed by Anvil Semiconductors Limited filed Critical Anvil Semiconductors Limited
Publication of WO2018060679A1 publication Critical patent/WO2018060679A1/en

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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof  ; Multistep manufacturing processes therefor
    • H01L29/66Types of semiconductor device ; Multistep manufacturing processes therefor
    • H01L29/68Types 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
    • H01L29/70Bipolar devices
    • H01L29/72Transistor-type devices, i.e. able to continuously respond to applied control signals
    • H01L29/739Transistor-type devices, i.e. able to continuously respond to applied control signals controlled by field-effect, e.g. bipolar static induction transistors [BSIT]
    • H01L29/7393Insulated gate bipolar mode transistors, i.e. IGBT; IGT; COMFET
    • H01L29/7395Vertical transistors, e.g. vertical IGBT
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L22/00Testing or measuring during manufacture or treatment; Reliability measurements, i.e. testing of parts without further processing to modify the parts as such; Structural arrangements therefor
    • H01L22/10Measuring as part of the manufacturing process
    • H01L22/14Measuring as part of the manufacturing process for electrical parameters, e.g. resistance, deep-levels, CV, diffusions by electrical means
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof  ; Multistep manufacturing processes therefor
    • H01L29/02Semiconductor bodies ; Multistep manufacturing processes therefor
    • H01L29/06Semiconductor 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
    • H01L29/08Semiconductor 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
    • H01L29/083Anode or cathode regions of thyristors or gated bipolar-mode devices
    • H01L29/0834Anode regions of thyristors or gated bipolar-mode devices, e.g. supplementary regions surrounding anode regions
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof  ; Multistep manufacturing processes therefor
    • H01L29/02Semiconductor bodies ; Multistep manufacturing processes therefor
    • H01L29/12Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed
    • H01L29/16Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed including, apart from doping materials or other impurities, only elements of Group IV of the Periodic System
    • H01L29/1608Silicon carbide
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof  ; Multistep manufacturing processes therefor
    • H01L29/02Semiconductor bodies ; Multistep manufacturing processes therefor
    • H01L29/12Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed
    • H01L29/16Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed including, apart from doping materials or other impurities, only elements of Group IV of the Periodic System
    • H01L29/161Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed including, apart from doping materials or other impurities, only elements of Group IV of the Periodic System including two or more of the elements provided for in group H01L29/16, e.g. alloys
    • H01L29/165Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed including, apart from doping materials or other impurities, only elements of Group IV of the Periodic System including two or more of the elements provided for in group H01L29/16, e.g. alloys in different semiconductor regions, e.g. heterojunctions
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof  ; Multistep manufacturing processes therefor
    • H01L29/02Semiconductor bodies ; Multistep manufacturing processes therefor
    • H01L29/12Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed
    • H01L29/16Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed including, apart from doping materials or other impurities, only elements of Group IV of the Periodic System
    • H01L29/167Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed including, apart from doping materials or other impurities, only elements of Group IV of the Periodic System further characterised by the doping material
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof  ; Multistep manufacturing processes therefor
    • H01L29/66Types of semiconductor device ; Multistep manufacturing processes therefor
    • H01L29/66007Multistep manufacturing processes
    • H01L29/66053Multistep manufacturing processes of devices having a semiconductor body comprising crystalline silicon carbide
    • H01L29/66068Multistep manufacturing processes of devices having a semiconductor body comprising crystalline silicon carbide the devices being controllable only by the electric current supplied or the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched, e.g. three-terminal devices
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L22/00Testing or measuring during manufacture or treatment; Reliability measurements, i.e. testing of parts without further processing to modify the parts as such; Structural arrangements therefor
    • H01L22/30Structural arrangements specially adapted for testing or measuring during manufacture or treatment, or specially adapted for reliability measurements
    • H01L22/32Additional lead-in metallisation on a device or substrate, e.g. additional pads or pad portions, lines in the scribe line, sacrificed conductors

Definitions

  • This invention relates to a 3 step cubic silicon carbide (3C SiC) based insulated gate bipolar transistor (IGBT).
  • the incumbent 4H-SiC technology fails in all three of the challenges above, it has an intrinsically high channel resistance due to traps just below the conduction band, minority carrier lifetimes are very low, and the natural n+ substrate does not allow the fabrication of a p-type injector.
  • 3C-SiC/Si technology may facilitate solutions to these problems, we know that the MOS channel traps are avoided because of the positioning of the 3C-SiC conduction band, and PN diodes from Anvil Semiconductors Ltd. have already demonstrated good conductivity modulation.
  • a p+ substrate can be used in hetero-epitaxy in place of the conventional n+ antimony (Sb) doped wafer in Anvil Semiconductor's technology, but realising a p+ substrate which is compatible with the typical 1370°C epitaxy process is problematical, as is re-engineering the epitaxy and lattice miss-match compensating processes. It has been demonstrated that to make an IGBT we can simply take a MOSFET and change the n+ Si wafer to a p+ Si wafer. In practice it may be more difficult to that.
  • SiC silicon carbide
  • IGBT insulated gate bipolar transistor
  • the silicon substrate having a principal surface, wherein the silicon substrate is of the second conductivity type
  • the principal surface of the silicon substrate may be doped using a heavy aluminium ion implant.
  • the heavily Al doped silicon region within the silicon substrate helps to avoid the use of boron in the silicon substrate and thus avoids the problems as stated above.
  • the predetermined depth of the heavily doped silicon region from the principal surface into the silicon substrate may be at least about 100 ⁇ .
  • the predetermined depth of the heavily doped silicon region from the principal surface into the silicon substrate may be at least about 150 ⁇ .
  • the predetermined temperature under which the heavily doped silicon region within the silicon substrate may be grown is at least about 1300° C.
  • the aluminium ion implant dose may be about 10 17 cnT 2 .
  • the method may further comprise: providing a masking layer on the principal surface of the silicon substrate, the masking layer having windows which expose corresponding regions of the heavily doped silicon region of the silicon substrate;
  • the masking layer may be any one of: a dielectric material; a silicon dioxide layer; a thermal oxide layer; a layer of semiconductor or conductive material; and a layer of polycrystalline silicon.
  • the masking layer may be fully consumed using a temperature of 1370°C.
  • the collector region may be formed from the monocrystalline 3C-SiC layers.
  • the polycrystalline and/or amorphous 3C SiC regions are located next to the IGBT device structure as a grid.
  • the collector region may comprise 3C-SiC material which is doped using aluminium ion implant.
  • the thickness of the collector region may be about 2 ⁇ .
  • the drift region, body region and emitter region each may comprise 3C-SiC material.
  • the thickness of the drift region may be about 8 ⁇ .
  • Each of the collector region, the drift region, the body region and the emitter region may be an epitaxial region.
  • the method may further comprise back-grinding the silicon substrate up to the silicon region.
  • the method may further comprise forming a plurality of spots of oxide formed on the collector region.
  • the method may further comprise growing polycrystalline SiC through the spots of oxide.
  • the method may further comprise diffusing aluminium ion implant through the polycrystalline SiC from a bottom to top direction to form a vertical column of aluminium-doped polycrystalline SiC.
  • a silicon carbide (SiC) based insulated gate bipolar transistor comprising: a monocrystalline silicon substrate having a principal substrate, wherein the silicon substrate is of a second conductivity type; a collector region of a first conductivity type, opposite to the second conductivity type, disposed over the principal surface of the silicon substrate, wherein the collector region comprises a material comprising 3-step cubic silicon carbide (3C-SiC); a semiconductor drift region of the second conductivity type disposed on the collector region; a body region of the first conductivity type located within the semiconductor drift region; an emitter region of the second conductivity type located within the body region; and a gate region placed above and in contact to the emitter region to form a channel region between the emitter region and the drift region through the body region; wherein the silicon substrate comprises a heavily doped silicon region of the first conductivity type near the principal surface of the silicon substrate and wherein the heavily doped silicon region within the silicon substrate comprises an aluminium ion implantation
  • the depth of the heavily doped silicon region from the principal surface into the silicon substrate may be at least about 100 ⁇ .
  • the depth of the heavily doped silicon region from the principal surface into the silicon substrate may be at least about 150 ⁇ .
  • the temperature under which the heavily doped silicon region may be grown is at least about 1300° C.
  • the dose of the aluminium ion implantation may be about 10 17 cnT 2 .
  • the collector region may form from the monocrystalline 3C-SiC layers disposed directly on the principal surface of the silicon substrate and polycrystalline and/or amorphous 3C-SiC layers between the monocrystalline 3C-SiC layers disposed directly on the principal surface of the silicon substrate.
  • the polycrystalline and/or amorphous 3C-SiC layers do not form part of the collector region but they are located adjacent the collector region.
  • the collector region may be disposed directly on the further 3C-SiC layer.
  • the collector region may comprise 3C-SiC material comprising aluminium ion implantation.
  • the thickness of the collector region may be about 2 ⁇ .
  • the drift region, body region and emitter region may each comprise 3C-SiC material.
  • the thickness of the drift region may be about 8 ⁇ .
  • Each of the collector region, the drift region, the body region and the emitter region may be an epitaxial region.
  • the IGBT may further comprise a vertical column of aluminium doped polycrystalline SiC formed on the collector region.
  • Figure 1 illustrates a 3C-SiC based IGBT
  • Figure 2 illustrates the silicon substrate of the IGBT of Figure 1 ;
  • Figure 3 illustrate a portion of the IGBT of Figure 1 ;
  • Figure 4 illustrates an alternative portion of the IGBT of Figure 1 ;
  • Figure 5 (a) to 5 (c) show the manufacturing steps of the additional 3C-SiC layer of Figure. 1 ;
  • Figure 6 illustrates a flow diagram of the method of manufacturing the IGBT of Figure 1.
  • the transistor 100 includes lightly doped n-type silicon substrate 110.
  • the doping concentration of the n- type silicon substrate 1 10 is about from 10 19 cm “3 to 10 21 cm “3 .
  • the width and/thickness of the n-type silicon substrate is about 1 mm.
  • the n-type substrate 1 10 includes a principal substrate 135.
  • a highly doped p+ silicon region 120 is epitaxially grown near the principal surface 135 of the n-type silicon substrate 110.
  • the silicon region 120 extends towards the substrate 1 10 from the principal surface.
  • the silicon region 120 is doped using aluminum (Al) ion implant.
  • the Al doped p+ silicon region 120 within the n-type silicon substrate 1 10 and near the principal surface of the n-type silicon substrate 110 is generally about 100 ⁇ .
  • the Al doped p+ silicon region 120 is generally extended from the principal surface 135 into the n-type substrate 110. It will be appreciated that the Al ion implant can use a plasma implant technique from Ion Beam Systems to great advantage in producing very high dose implants.
  • a p+ collector region 125 is epitaxially grown.
  • the p+ collector region 125 includes 3C-SiC material.
  • the p+ collector region 125 generally includes a monocrystalline 3C-SiC material.
  • the p+ collector region 125 is doped using Al and it is generally about 2 ⁇ thick. The doping concentration of the p+ collector region is about 10 21 cm "3 .
  • the collector region 125 forms part of a monocrystalline SiC layer.
  • the monocrystalline SiC layer (or the collector region 125) is spaced apart by a grid of polycrystalline SiC layers.
  • the spaced apart arrangement of the monocrystalline SiC layer (or the collector region 125) and the polycrystalline SiC layer generally helps to reduce wafer bow between the p+ silicon region 120 and p+ collector region 125.
  • a lightly-doped n-type layer 130 which provides a drift region and which is supported on the p-type silicon carbide collector layer 130.
  • P-type wells 140 at a surface 160 of the drift region 130 (or the IGBT) provide body regions 140.
  • the drift region 130 includes 3C-SiC material.
  • N-type wells 150 within the p-type wells 140 provide contact regions and provide emitters.
  • the body region 140 and the contact region (emitters) 150 can be formed using 3C-SiC material.
  • a channel 170 is formed beneath a gate 180 which is separated using a gate dielectric layer 190. Both the gate 180 and dielectric layer 190 form a gate region.
  • the IGBT shown in Figure 1 is able to support much greater breakdown voltages due to the use of 3C-SiC in the epitaxial drift region 130.
  • the on- resistance of the 3C-SiC IGBT can be significantly lower than the 4H-SiC IGBT. This is because a better channel mobility is observed in 3C-SiC (compared to 4H-SiC) and therefore the on-resistance of the channel region formed between the drift region 130 and the emitter region 150 can be significantly reduced.
  • a hetero-structure is formed between the p+ silicon region 120 within the n- type substrate 1 10 and p+ 3C-SiC layer 125.
  • FIG. 2 illustrates the silicon substrate of the IGBT of Figure 1.
  • the silicon substrate 110 includes two portions: a lowly doped n-type silicon region 1 10 and a heavily doped p+ silicon region 120.
  • the heavily doped p+ silicon region 120 is doped using Al ion implant driven in under a temperature about 1300°C.
  • the thickness of the lowly doped n-type silicon region 1 10 is about 1 mm and the thickness of the heavily doped p+ silicon region 120 is about 80 to 120 ⁇ , more preferably about 100 ⁇ .
  • Figure 3 illustrate a portion of the IGBT of Figure 1. This figure illustrates that the n- type substrate 1 10 includes a heavily doped p+ silicon region 120 which is Al ion implanted. On top of the p+ silicon region 120 an Al doped collector region 125 is grown.
  • the collector region 125 includes 3C-SiC material.
  • the thickness of the collector region 125 is generally 2 ⁇ .
  • the drift region 130 is epitaxially grown.
  • the thickness of the drift region is generally about 8 ⁇ or more.
  • Figure 4 illustrates an alternative portion of the IGBT of Figure 1.
  • small spots for example 50-100 ⁇ , of grid Si0 2 on the surface of the Si substrate 110 before epitaxy, close to the IGBT such that polySiC in these regions is grown.
  • Al diffuses through the polySiC very rapidly from bottom to top to form a vertical column 195. It is possible to add the standard p+ diffusions in the top to have a temporary top contact to the p+ region.
  • the Si wafer 1 10 is back grinded to 100 microns to reveal the p+ diffusion 120 to allow the back electrical contact provided for packaging.
  • a die assembly process called "Dice before Grind” can be employed for this. It is possible to achieve about 100 micron grooves in the top/device side of the wafer and then flip it over and grind back until the die are separated.
  • One advantage of this process is that it avoids the wafer-bowing problems that is encountered if a complete SiC/Si wafer is thinned out. It also demonstrates that -100 micron thick die are feasible in the 3C-SiC technology.
  • the "Dice before Grind” is a Disco Corporation proprietary process.
  • Figure 5 (a) to 5 (c) show the manufacturing steps of the collector region of Figure. 1.
  • silicon carbide seed layers 615 are grown between masking layers 610.
  • Figure 6 (b) at an elevated temperature of 1370°C and at a hydrogen rich atmosphere, the masking layers 610 are (fully) consumed.
  • 3C SiC layers are formed in such a way that monocrystalline 3C-SiC layers 620 are formed on the seed layer 615 and polycrystalline and/or amorphous 3C-SiC layers 625 are formed (directly) on the Al doped silicon region 120. This type of grid of monocrystalline and polycrystalline and/or amorphous SiC layers help to reduce wafer bow after the wafer is cooled down.
  • the monocrystalline 3C-SiC layer 620 then forms the collector region 125 of Figure 1.
  • the drift region 130, the body region 140, the emitter regoin 150 are subsequently formed only on the monocrystalline 3C-SiC layer 620 (but not on the polycrystalline SiC layer 625).
  • Figure 6 illustrates a flow diagram of the method of manufacturing the IGBT of Figure 1.
  • the first conductivity type refers to p type doping and the second conductivity type refers to n type doping.
  • the doping concentration can be reversed as necessary.

Abstract

We disclose herein a method of manufacturing a silicon carbide (SiC) based insulated gate bipolar transistor (IGBT), the IGBT comprising: a monocrystalline silicon substrate; a collector region of a first conductivity type disposed over the silicon substrate, wherein the collector region comprises a material comprising 3-step cubic silicon carbide (3C-SiC); a semiconductor drift region of a second conductivity type, opposite the first conductivity type, disposed on the collector region; a body region of the first conductivity type located within the semiconductor drift region; an emitter region of the second conductivity type located within the body region; a gate region placed above and in contact to the emitter region. The method comprising: providing the silicon substrate having a principal surface, wherein the silicon substrate is of the second conductivity type; doping the principal surface of the silicon substrate using an aluminium ion implant; and driving the aluminium ion implant into the silicon substrate to a predetermined depth under a predetermined temperature so that a heavily doped silicon region of the first conductivity type is formed near the principal surface within the silicon substrate.

Description

3C-SiC IGBT
FIELD OF THE INVENTION
This invention relates to a 3 step cubic silicon carbide (3C SiC) based insulated gate bipolar transistor (IGBT).
BACKGROUND TO THE INVENTION
So far there has been very little progress in any silicon carbide (SiC) technology towards building a high quality vertical 650V IGBT. There are several major challenges to be overcome, the first is to build an n-channel MOSFET with a very low channel resistance, this has to be complemented with a high minority carrier lifetime drift region to allow it to be conductivity modulated, and finally a p-type injector must be added to the "back-side" of the wafer to undertake that minority carrier injection.
The incumbent 4H-SiC technology fails in all three of the challenges above, it has an intrinsically high channel resistance due to traps just below the conduction band, minority carrier lifetimes are very low, and the natural n+ substrate does not allow the fabrication of a p-type injector. However, 3C-SiC/Si technology may facilitate solutions to these problems, we know that the MOS channel traps are avoided because of the positioning of the 3C-SiC conduction band, and PN diodes from Anvil Semiconductors Ltd. have already demonstrated good conductivity modulation.
In principle a p+ substrate can be used in hetero-epitaxy in place of the conventional n+ antimony (Sb) doped wafer in Anvil Semiconductor's technology, but realising a p+ substrate which is compatible with the typical 1370°C epitaxy process is problematical, as is re-engineering the epitaxy and lattice miss-match compensating processes. It has been demonstrated that to make an IGBT we can simply take a MOSFET and change the n+ Si wafer to a p+ Si wafer. In practice it may be more difficult to that.
The basic problem is that the normal p-type dopant in Si is Boron, but this element has a very high vapour pressure above about 1000°C, and consequently it gives problems of unwanted background doping of the epitaxy reactor even for normal Si epitaxy, here the conventional solution is to seal the back of the wafer with silicon dioxide (Si02), but that would not work at typical 3C-SiC growth temperatures. Hence Boron contamination of SiC epitaxy reactors presents a major obstacle to this device structure.
SUMMARY
According to one aspect of the present invention, there is provided a method of manufacturing a silicon carbide (SiC) based insulated gate bipolar transistor (IGBT), the IGBT comprising: a monocrystalline silicon substrate; a collector region of a first conductivity type disposed over the silicon substrate, wherein the collector region comprises a material comprising 3-step cubic silicon carbide (3C-SiC); a semiconductor drift region of a second conductivity type, opposite the first conductivity type, disposed on the collector region; a body region of the first conductivity type located within the semiconductor drift region; an emitter region of the second conductivity type the body region; a gate region placed above and in contact to the emitter region;
the method comprising:
providing the silicon substrate having a principal surface, wherein the silicon substrate is of the second conductivity type;
doping the principal surface of the silicon substrate using an aluminium ion implant; and
driving the aluminium ion implant into the silicon substrate to a predetermined depth under a predetermined temperature so that a heavily doped silicon region of the first conductivity type is formed near the principal surface within the silicon substrate.
The principal surface of the silicon substrate may be doped using a heavy aluminium ion implant. The heavily Al doped silicon region within the silicon substrate helps to avoid the use of boron in the silicon substrate and thus avoids the problems as stated above. The predetermined depth of the heavily doped silicon region from the principal surface into the silicon substrate may be at least about 100 μηι.
The predetermined depth of the heavily doped silicon region from the principal surface into the silicon substrate may be at least about 150 μηι. The predetermined temperature under which the heavily doped silicon region within the silicon substrate may be grown is at least about 1300° C.
The aluminium ion implant dose may be about 1017cnT2. The method may further comprise: providing a masking layer on the principal surface of the silicon substrate, the masking layer having windows which expose corresponding regions of the heavily doped silicon region of the silicon substrate;
forming silicon carbide seed regions on the exposed regions of the silicon substrate;
consuming the masking layer at an elevated temperature;
growing monocrystalline 3C-SiC layers on the silicon carbide seed regions; and
forming regions of polycrystalline and/or amorphous 3C-SiC between the monocrystalline 3C-SiC layers on the heavily doped silicon region of the silicon substrate.
The masking layer may be any one of: a dielectric material; a silicon dioxide layer; a thermal oxide layer; a layer of semiconductor or conductive material; and a layer of polycrystalline silicon. The masking layer may be fully consumed using a temperature of 1370°C.
The collector region may be formed from the monocrystalline 3C-SiC layers. The polycrystalline and/or amorphous 3C SiC regions are located next to the IGBT device structure as a grid.
The collector region may comprise 3C-SiC material which is doped using aluminium ion implant.
The thickness of the collector region may be about 2μηι.
The drift region, body region and emitter region each may comprise 3C-SiC material. The thickness of the drift region may be about 8 μηι.
Each of the collector region, the drift region, the body region and the emitter region may be an epitaxial region. The method may further comprise back-grinding the silicon substrate up to the silicon region.
The method may further comprise forming a plurality of spots of oxide formed on the collector region.
The method may further comprise growing polycrystalline SiC through the spots of oxide.
The method may further comprise diffusing aluminium ion implant through the polycrystalline SiC from a bottom to top direction to form a vertical column of aluminium-doped polycrystalline SiC.
According to a further aspect of the present invention, there is provided a silicon carbide (SiC) based insulated gate bipolar transistor (IGBT) comprising: a monocrystalline silicon substrate having a principal substrate, wherein the silicon substrate is of a second conductivity type; a collector region of a first conductivity type, opposite to the second conductivity type, disposed over the principal surface of the silicon substrate, wherein the collector region comprises a material comprising 3-step cubic silicon carbide (3C-SiC); a semiconductor drift region of the second conductivity type disposed on the collector region; a body region of the first conductivity type located within the semiconductor drift region; an emitter region of the second conductivity type located within the body region; and a gate region placed above and in contact to the emitter region to form a channel region between the emitter region and the drift region through the body region; wherein the silicon substrate comprises a heavily doped silicon region of the first conductivity type near the principal surface of the silicon substrate and wherein the heavily doped silicon region within the silicon substrate comprises an aluminium ion implantation.
The depth of the heavily doped silicon region from the principal surface into the silicon substrate may be at least about 100 μηι. The depth of the heavily doped silicon region from the principal surface into the silicon substrate may be at least about 150 μηι. The temperature under which the heavily doped silicon region may be grown is at least about 1300° C. The dose of the aluminium ion implantation may be about 1017cnT2.
The collector region may form from the monocrystalline 3C-SiC layers disposed directly on the principal surface of the silicon substrate and polycrystalline and/or amorphous 3C-SiC layers between the monocrystalline 3C-SiC layers disposed directly on the principal surface of the silicon substrate. The polycrystalline and/or amorphous 3C-SiC layers do not form part of the collector region but they are located adjacent the collector region.
The collector region may be disposed directly on the further 3C-SiC layer. The collector region may comprise 3C-SiC material comprising aluminium ion implantation.
The thickness of the collector region may be about 2μηι.
The drift region, body region and emitter region may each comprise 3C-SiC material.
The thickness of the drift region may be about 8 μηι. Each of the collector region, the drift region, the body region and the emitter region may be an epitaxial region.
The IGBT may further comprise a vertical column of aluminium doped polycrystalline SiC formed on the collector region.
BRIEF DESCRIPTION OF THE DRAWINGS
The present disclosure will be understood more fully from the detailed description that follows and from the accompanying drawings, which however, should not be taken to limit the invention to the specific embodiments shown, but are for explanation and understanding only.
Figure 1 illustrates a 3C-SiC based IGBT;
Figure 2 illustrates the silicon substrate of the IGBT of Figure 1 ;
Figure 3 illustrate a portion of the IGBT of Figure 1 ;
Figure 4 illustrates an alternative portion of the IGBT of Figure 1 ; Figure 5 (a) to 5 (c) show the manufacturing steps of the additional 3C-SiC layer of Figure. 1 ; and
Figure 6 illustrates a flow diagram of the method of manufacturing the IGBT of Figure 1.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
Referring to Figure 1 , an example of a vertical power semiconductor transistor 100 in the form of an insulated gate bipolar transistor (IGBT) is shown. The transistor 100 includes lightly doped n-type silicon substrate 110. The doping concentration of the n- type silicon substrate 1 10 is about from 1019 cm"3 to 1021 cm"3. The width and/thickness of the n-type silicon substrate is about 1 mm. The n-type substrate 1 10 includes a principal substrate 135. A highly doped p+ silicon region 120 is epitaxially grown near the principal surface 135 of the n-type silicon substrate 110. The silicon region 120 extends towards the substrate 1 10 from the principal surface. The silicon region 120 is doped using aluminum (Al) ion implant. Al diffuses much faster than boron, but the growth process may go up to about 1300°C. For example, a two hour diffusion can give a junction depth in excess of 150 μηι from an Al implant dose of 1017 cm"2. The Al doped p+ silicon region 120 within the n-type silicon substrate 1 10 and near the principal surface of the n-type silicon substrate 110 is generally about 100 μηι. The Al doped p+ silicon region 120 is generally extended from the principal surface 135 into the n-type substrate 110. It will be appreciated that the Al ion implant can use a plasma implant technique from Ion Beam Systems to great advantage in producing very high dose implants.
In Figure 1 , on top of the principal surface a p+ collector region 125 is epitaxially grown. The p+ collector region 125 includes 3C-SiC material. The p+ collector region 125 generally includes a monocrystalline 3C-SiC material. The p+ collector region 125 is doped using Al and it is generally about 2 μηι thick. The doping concentration of the p+ collector region is about 1021 cm"3.
In one embodiment, the collector region 125 forms part of a monocrystalline SiC layer. The monocrystalline SiC layer (or the collector region 125) is spaced apart by a grid of polycrystalline SiC layers. The spaced apart arrangement of the monocrystalline SiC layer (or the collector region 125) and the polycrystalline SiC layer generally helps to reduce wafer bow between the p+ silicon region 120 and p+ collector region 125.
In the embodiment of Figure 1 , a lightly-doped n-type layer 130 which provides a drift region and which is supported on the p-type silicon carbide collector layer 130. P-type wells 140 at a surface 160 of the drift region 130 (or the IGBT) provide body regions 140. The drift region 130 includes 3C-SiC material. N-type wells 150 within the p-type wells 140 provide contact regions and provide emitters. The body region 140 and the contact region (emitters) 150 can be formed using 3C-SiC material. A channel 170 is formed beneath a gate 180 which is separated using a gate dielectric layer 190. Both the gate 180 and dielectric layer 190 form a gate region.
The IGBT shown in Figure 1 is able to support much greater breakdown voltages due to the use of 3C-SiC in the epitaxial drift region 130. At the same time the on- resistance of the 3C-SiC IGBT can be significantly lower than the 4H-SiC IGBT. This is because a better channel mobility is observed in 3C-SiC (compared to 4H-SiC) and therefore the on-resistance of the channel region formed between the drift region 130 and the emitter region 150 can be significantly reduced. It will be appreciated that a hetero-structure is formed between the p+ silicon region 120 within the n- type substrate 1 10 and p+ 3C-SiC layer 125. The 3C-SiC material in the first epitaxial layer 125 (~2 microns) just above the SiC/Si interface 200 is very heavily defective because of the lattice miss-match between the two materials and heavily doped with Al as-grown, consequently this defective region is very conductive. In this way the heterojunction structure and consequent potential barriers can be overcome by becoming a quasi-metallic interface due to the presence of the dislocations, Al doping during epitaxial growth and Aluminium up-diffusion from the Si substrate. Figure 2 illustrates the silicon substrate of the IGBT of Figure 1. The silicon substrate 110 includes two portions: a lowly doped n-type silicon region 1 10 and a heavily doped p+ silicon region 120. The heavily doped p+ silicon region 120 is doped using Al ion implant driven in under a temperature about 1300°C. The thickness of the lowly doped n-type silicon region 1 10 is about 1 mm and the thickness of the heavily doped p+ silicon region 120 is about 80 to 120 μηι, more preferably about 100 μηι. Figure 3 illustrate a portion of the IGBT of Figure 1. This figure illustrates that the n- type substrate 1 10 includes a heavily doped p+ silicon region 120 which is Al ion implanted. On top of the p+ silicon region 120 an Al doped collector region 125 is grown. The collector region 125 includes 3C-SiC material. The thickness of the collector region 125 is generally 2 μηι. On top of the collector region 125, the drift region 130 is epitaxially grown. The thickness of the drift region is generally about 8 μηι or more. Figure 4 illustrates an alternative portion of the IGBT of Figure 1. In order to test the device at wafer level, small spots, for example 50-100 μηι, of grid Si02 on the surface of the Si substrate 110 before epitaxy, close to the IGBT such that polySiC in these regions is grown. In this case Al diffuses through the polySiC very rapidly from bottom to top to form a vertical column 195. It is possible to add the standard p+ diffusions in the top to have a temporary top contact to the p+ region.
After building the device the Si wafer 1 10 is back grinded to 100 microns to reveal the p+ diffusion 120 to allow the back electrical contact provided for packaging. A die assembly process called "Dice before Grind" can be employed for this. It is possible to achieve about 100 micron grooves in the top/device side of the wafer and then flip it over and grind back until the die are separated. One advantage of this process is that it avoids the wafer-bowing problems that is encountered if a complete SiC/Si wafer is thinned out. It also demonstrates that -100 micron thick die are feasible in the 3C-SiC technology. The "Dice before Grind" is a Disco Corporation proprietary process.
Figure 5 (a) to 5 (c) show the manufacturing steps of the collector region of Figure. 1. In Figure 5 (a), silicon carbide seed layers 615 are grown between masking layers 610. In Figure 6 (b), at an elevated temperature of 1370°C and at a hydrogen rich atmosphere, the masking layers 610 are (fully) consumed. In the step of Figure 6 (c), 3C SiC layers are formed in such a way that monocrystalline 3C-SiC layers 620 are formed on the seed layer 615 and polycrystalline and/or amorphous 3C-SiC layers 625 are formed (directly) on the Al doped silicon region 120. This type of grid of monocrystalline and polycrystalline and/or amorphous SiC layers help to reduce wafer bow after the wafer is cooled down. The monocrystalline 3C-SiC layer 620 then forms the collector region 125 of Figure 1. The drift region 130, the body region 140, the emitter regoin 150 are subsequently formed only on the monocrystalline 3C-SiC layer 620 (but not on the polycrystalline SiC layer 625). Figure 6 illustrates a flow diagram of the method of manufacturing the IGBT of Figure 1.
It will be appreciated that the first conductivity type refers to p type doping and the second conductivity type refers to n type doping. However, the doping concentration can be reversed as necessary.
Although the invention has been described in terms of preferred embodiments as set forth above, it should be understood that these embodiments are illustrative only and that the claims are not limited to those embodiments. Those skilled in the art will be able to make modifications and alternatives in view of the disclosure which are contemplated as falling within the scope of the appended claims. Each feature disclosed or illustrated in the present specification may be incorporated in the invention, whether alone or in any appropriate combination with any other feature disclosed or illustrated herein.

Claims

A method of manufacturing a silicon carbide (SiC) based insulated gate bipolar transistor (IGBT), the IGBT comprising: a monocrystalline silicon substrate; a collector region of a first conductivity type disposed over the silicon substrate, wherein the collector region comprises a material comprising 3-step cubic silicon carbide (3C-SiC); a semiconductor drift region of a second conductivity type, opposite the first conductivity type, disposed on the collector region; a body region of the first conductivity type located within the semiconductor drift region; an emitter region of the second conductivity type located within the body region; a gate region placed above and in contact to the emitter region;
the method comprising:
providing the silicon substrate having a principal surface, wherein the silicon substrate is of the second conductivity type; doping the principal surface of the silicon substrate using an aluminium ion implant; and
driving the aluminium ion implant into the silicon substrate to a predetermined depth under a predetermined temperature so that a heavily doped silicon region of the first conductivity type is formed near the principal surface within the silicon substrate.
A method according to claim 1 , wherein the principal surface of the silicon substrate is doped using a heavy aluminium ion implant.
A method according to claim 1 , wherein the predetermined depth of the heavily doped silicon region from the principal surface into the silicon substrate is at least about 100 μηι.
A method according to claim 1 , wherein the predetermined depth of the heavily doped silicon region from the principal surface into the silicon substrate is at least about 150 μηι.
5. A method according to claim 1 , wherein the predetermined temperature under which the heavily doped silicon region is grown is at least about 1300° C.
6. A method according to claim 1 , wherein the aluminium ion implant dose is about
1017cm"2.
7. A method according to any preceding claim, further comprising:
providing a masking layer on the principal surface of the silicon substrate, the masking layer having windows which expose corresponding regions of the heavily doped silicon region of the silicon substrate;
forming silicon carbide seed regions on the exposed regions of the silicon substrate;
consuming the masking layer at an elevated temperature; growing monocrystalline 3C SiC layers on the silicon carbide seed regions; and
forming regions of polycrystalline and/or amorphous 3C SiC between the monocrystalline 3C SiC layers on the heavily doped silicon region of the silicon substrate.
8. A method according to claim 7, wherein the masking layer is any one of:
a dielectric material;
a silicon dioxide layer;
a thermal oxide layer;
a layer of semiconductor or conductive material;
a layer of polycrystalline silicon.
9. A method according to claim 7, wherein the masking layer is fully consumed using a temperature of 1370°C.
10. A method according to claim 7, wherein the collector region is formed from the monocrystalline 3C SiC layers.
1 1. A method according to claim 1 , wherein the collector region comprises 3C-SiC material which is doped using aluminium ion implant.
12. A method according to claim 1 1 , wherein the thickness of the collector region is about 2μηι.
13. A method according to claim 1 , wherein the drift region, body region and emitter region each comprise 3C-SiC material.
14. A method according to claim 1 , wherein the thickness of the drift region is about 8 μηι.
15. A method according to claim 1 , wherein each of the collector region, the drift region, the body region and the emitter region is an epitaxial region.
16. A method according to claim 1 , further comprising back-grinding the silicon substrate up to the heavily doped silicon region.
17. A method according to claim 1 , further comprising forming a plurality of spots of oxide formed on the collector region.
18. A method according to claim 17, further comprising growing polycrystalline SiC through the spots of oxide.
19. A method according to claim 18, further comprising diffusing aluminium ion implant through the polycrystalline SiC from a bottom to top direction to form a vertical column of aluminium doped polycrystalline SiC.
20. A silicon carbide (SiC) based insulated gate bipolar transistor (IGBT) comprising:
a monocrystalline silicon substrate having a principal substrate, wherein the silicon substrate is of a second conductivity type;
a collector region of a first conductivity type, opposite to the second conductivity type, disposed over the principal surface of the silicon substrate, wherein the collector region comprises a material comprising 3-step cubic silicon carbide (3C-SiC);
a semiconductor drift region of the second conductivity type disposed on the collector region;
a body region of the first conductivity type located within the semiconductor drift region; an emitter region of the second conductivity type located within the body region; and
a gate region placed above and in contact to the emitter region to form a channel region between the emitter region and the drift region through the body region;
wherein the silicon substrate comprises a silicon region of the first conductivity type near the principal surface of the silicon substrate and wherein the silicon region within the silicon substrate comprises an aluminium ion implantation.
21. An IGBT according to claim 20, wherein the depth of the heavily doped silicon region from the principal surface into the silicon substrate is at least about 100 μηι.
22. An IGBT according to claim 20, wherein the depth of the heavily doped silicon region from the principal surface into the silicon substrate is at least about 150 μηι.
23. An IGBT according to claim 20, wherein the temperature under which the heavily doped silicon region is grown is at least about 1300° C.
24. An IGBT according to claim 20, wherein the dose of the aluminium ion implantation is about 1017cnT2.
25. An IGBT according to claim 20, wherein the collector region comprises monocrystalline 3C SiC layers disposed directly on the principal surface of the silicon substrate.
26. An IGBT according to claim 20, wherein the collector region comprises 3C-SiC material comprising aluminium ion implantation.
27. An IGBT according to claim 20, wherein the thickness of the collector region is about 2μηι.
28. An IGBT according to claim 20, wherein the drift region, body region and emitter region each comprise 3C-SiC material.
29. An IGBT according to claim 20, wherein the thickness of the drift region is about 8 μηι.
30. An IGBT according to claim 20, wherein each of the collector region, the drift region, the body region and the emitter region is an epitaxial region. 31. An IGBT according to claim 20, further comprising a vertical column of aluminium doped polycrystalline SiC formed on the collector region.
PCT/GB2017/052815 2016-09-30 2017-09-21 3c-sic igbt WO2018060679A1 (en)

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