WO2006054394A1 - 炭化ケイ素mos電界効果トランジスタおよびその製造方法 - Google Patents
炭化ケイ素mos電界効果トランジスタおよびその製造方法 Download PDFInfo
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- WO2006054394A1 WO2006054394A1 PCT/JP2005/018104 JP2005018104W WO2006054394A1 WO 2006054394 A1 WO2006054394 A1 WO 2006054394A1 JP 2005018104 W JP2005018104 W JP 2005018104W WO 2006054394 A1 WO2006054394 A1 WO 2006054394A1
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- 238000000034 method Methods 0.000 title claims description 9
- HBMJWWWQQXIZIP-UHFFFAOYSA-N silicon carbide Chemical compound [Si+]#[C-] HBMJWWWQQXIZIP-UHFFFAOYSA-N 0.000 title description 43
- 229910010271 silicon carbide Inorganic materials 0.000 title description 42
- 230000005669 field effect Effects 0.000 title description 2
- 230000008021 deposition Effects 0.000 claims abstract description 20
- 238000005468 ion implantation Methods 0.000 claims description 44
- 239000012535 impurity Substances 0.000 claims description 31
- 238000004519 manufacturing process Methods 0.000 claims description 23
- 239000004065 semiconductor Substances 0.000 claims description 19
- 239000000758 substrate Substances 0.000 claims description 19
- 238000000151 deposition Methods 0.000 claims description 15
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 claims description 3
- 229910052799 carbon Inorganic materials 0.000 claims description 3
- 150000002500 ions Chemical class 0.000 claims description 3
- 230000002093 peripheral effect Effects 0.000 claims description 2
- 230000015556 catabolic process Effects 0.000 abstract description 21
- 238000002347 injection Methods 0.000 abstract description 7
- 239000007924 injection Substances 0.000 abstract description 7
- 239000010410 layer Substances 0.000 description 166
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 20
- 210000004027 cell Anatomy 0.000 description 20
- 239000013078 crystal Substances 0.000 description 13
- 229910052782 aluminium Inorganic materials 0.000 description 11
- 229910052757 nitrogen Inorganic materials 0.000 description 11
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 9
- 230000005684 electric field Effects 0.000 description 9
- 230000001133 acceleration Effects 0.000 description 8
- 230000000903 blocking effect Effects 0.000 description 8
- 239000011229 interlayer Substances 0.000 description 7
- -1 aluminum ions Chemical class 0.000 description 6
- 230000000694 effects Effects 0.000 description 6
- 238000009792 diffusion process Methods 0.000 description 3
- BHEPBYXIRTUNPN-UHFFFAOYSA-N hydridophosphorus(.) (triplet) Chemical compound [PH] BHEPBYXIRTUNPN-UHFFFAOYSA-N 0.000 description 3
- 239000002344 surface layer Substances 0.000 description 3
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 2
- 239000012300 argon atmosphere Substances 0.000 description 2
- 239000002772 conduction electron Substances 0.000 description 2
- 230000007547 defect Effects 0.000 description 2
- 230000001771 impaired effect Effects 0.000 description 2
- 238000002513 implantation Methods 0.000 description 2
- 238000009413 insulation Methods 0.000 description 2
- 238000004518 low pressure chemical vapour deposition Methods 0.000 description 2
- 230000003647 oxidation Effects 0.000 description 2
- 238000007254 oxidation reaction Methods 0.000 description 2
- 229910052698 phosphorus Inorganic materials 0.000 description 2
- 239000011574 phosphorus Substances 0.000 description 2
- 238000000206 photolithography Methods 0.000 description 2
- 230000000704 physical effect Effects 0.000 description 2
- 239000002994 raw material Substances 0.000 description 2
- 229910052710 silicon Inorganic materials 0.000 description 2
- 239000010703 silicon Substances 0.000 description 2
- 229910018540 Si C Inorganic materials 0.000 description 1
- 238000000137 annealing Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000005530 etching Methods 0.000 description 1
- 229910021420 polycrystalline silicon Inorganic materials 0.000 description 1
- 230000002040 relaxant effect Effects 0.000 description 1
- 239000007858 starting material Substances 0.000 description 1
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- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/04—Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer
- H01L21/0445—Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising crystalline silicon carbide
- H01L21/0455—Making n or p doped regions or layers, e.g. using diffusion
- H01L21/046—Making n or p doped regions or layers, e.g. using diffusion using ion implantation
- H01L21/0465—Making n or p doped regions or layers, e.g. using diffusion using ion implantation using masks
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- H01L29/0615—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 for preventing surface leakage or controlling electric field concentration for increasing or controlling the breakdown voltage of reverse biased devices by the doping profile or the shape or the arrangement of the PN junction, or with supplementary regions, e.g. junction termination extension [JTE]
- H01L29/0619—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 for preventing surface leakage or controlling electric field concentration for increasing or controlling the breakdown voltage of reverse biased devices by the doping profile or the shape or the arrangement of the PN junction, or with supplementary regions, e.g. junction termination extension [JTE] with a supplementary region doped oppositely to or in rectifying contact with the semiconductor containing or contacting region, e.g. guard rings with PN or Schottky junction
- H01L29/0623—Buried supplementary region, e.g. buried guard ring
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- H01L29/1095—Body region, i.e. base region, of DMOS transistors or IGBTs
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- H01L29/02—Semiconductor bodies ; Multistep manufacturing processes therefor
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- H01L29/16—Semiconductor 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 Table
- H01L29/1608—Silicon carbide
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- H01L29/66—Types of semiconductor device ; Multistep manufacturing processes therefor
- H01L29/66007—Multistep manufacturing processes
- H01L29/66053—Multistep manufacturing processes of devices having a semiconductor body comprising crystalline silicon carbide
- H01L29/66068—Multistep 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
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- H01L29/78—Field effect transistors with field effect produced by an insulated gate
- H01L29/7801—DMOS transistors, i.e. MISFETs with a channel accommodating body or base region adjoining a drain drift region
- H01L29/7802—Vertical DMOS transistors, i.e. VDMOS transistors
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- H01L29/78—Field effect transistors with field effect produced by an insulated gate
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- H01L29/7828—Vertical transistors without inversion channel, e.g. vertical ACCUFETs, normally-on vertical MISFETs
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- H01L29/0642—Isolation within the component, i.e. internal isolation
- H01L29/0649—Dielectric regions, e.g. SiO2 regions, air gaps
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Definitions
- the present invention relates to a structure of a low on-resistance, high voltage vertical MOSFET made of silicon carbide and a manufacturing method.
- SiC single crystals have superior physical properties compared to silicon (Si) single crystals, such as a wide band gap, high dielectric breakdown strength, and high electron saturation drift velocity. Therefore, by using SiC as a starting material, it is possible to fabricate a power semiconductor device with high breakdown voltage and low resistance that exceeds the limit of Si. In addition, SiC has a feature that an insulating layer can be formed by thermal oxidation like Si. From these facts, it is considered that a vertical MOSFET with high breakdown voltage and low on-resistance can be realized by using SiC single crystal as a raw material.
- the Si C vertical MOSFET fabricated by the double ion implantation method has a channel mobility of 5 cm 2 / Vs or less, which is much smaller than the Si D—MOSFET of about 500 cm 2 / Vs. As a result, the on-resistance is much higher than the theoretical value.
- FIG. 7 is a sectional view of the unit senor.
- a low-concentration n-type drift layer 2 is deposited on a high-concentration n-type substrate 1, and a high-concentration p-type gate layer 31 is formed on the surface of the n-type drift layer 2 by ion implantation.
- a low concentration P-type layer 32 is deposited.
- the surface portion of the low-concentration p-type layer 32 is selectively ion-implanted with an n-type source layer 5, a gate electrode 7 via a gate oxide film 6, and a source electrode via an interlayer insulating film 8. 9 is formed, and a channel region 11 is formed in the low-concentration p-type deposition layer 32 immediately below the gate oxide film 6.
- the n-type base layer 4 that penetrates the low-concentration p-type deposited layer 32 and reaches the n-type drift layer 2 is selectively formed by n-type impurity ion implantation from the surface (
- this n-type base layer 4 is also referred to as a “back layer”.
- the channel region 11 is formed in a low-concentration P-type deposited layer that is not ion-implanted, so that high conduction electron mobility and mobility can be obtained, and a vertical MOSFET with low on-resistance is fabricated. be able to.
- the high-concentration P-type gate layer 31 force is also low in the vertical channel portion 24 by the depletion layer extending laterally in the low-concentration n-type drift layer 2, and is completely pinched off by the voltage, so near the channel region 11 It has a special feature that it can prevent the leakage of electric field to the gate oxide film and increase the source / drain withstand voltage.
- the depletion layer is in the above-described state until the vertical channel portion 24 is completely pinched off by the depletion layer extending laterally from the high-concentration p-type gate layer 31 to the low-concentration n-type drift layer 2.
- the n-type base layer 4 (back layer) also extends upward.
- the depletion layer reaches the interface with the gate oxide film 6 before the vertical channel portion is completely pinched off, and the gate electrode 7 and the n-type A strong electric field is applied to the gate oxide film interposed between the base layers 4 to cause dielectric breakdown.
- the electric field becomes stronger as the voltage increases, and the breakdown voltage between the source and the drain is limited by the dielectric breakdown of the gate oxide film in this part. .
- the electron mobility in the channel should be a large value, but actually it is as large as expected for the following reason. Don't be. That is, the low-concentration p-type deposited film 32 is directly formed on the p-type gate layer 31 ion-implanted at a high concentration, but the physical properties of the deposited film on the high-concentration implanted layer as a single crystal film are significantly impaired. In particular, when the deposited film is thin, The electron mobility in the film is not increased due to the influence. As a result, there is a problem that the on-resistance is not as small as expected.
- the channel region is provided in the low-concentration p-type deposited film, and the portion of the deposited film is returned to the n-type by selective ion implantation to form the electron path.
- the problem of obstructing the high breakdown voltage and low on-resistance of the vertical MOSFET is considered to be avoided if the low-concentration P-type deposited film 32 is thickened to some extent. If the deposited film is thickened, the thick n base layer 4 can reduce the electric field exerted on the gate oxide film, and the channel region can be formed in a high quality deposited film farther from the high injection layer. It is the power that can be achieved.
- the above-described low-concentration p-type deposited film cannot be formed thick due to process restrictions when manufacturing it. . That is, as described in [0004], in the method of manufacturing a vertical MOSFET having a conventional structure, the n-type base layer 4 is formed by ion implantation of n-type impurities until it penetrates the low-concentration p-type deposited film 32 from the surface. Therefore, it is formed by flipping (turning back) from p-type to n-type. However, there is a limit to the thickness of the film that can be overcome by ion implantation.
- the depth at which ions are implanted depends on the acceleration voltage of the ions, but at the normal acceleration voltage (several lOOkeV to 1000 keV), it is about 1 / z m at most. For this reason, the thickness of the striking layer (that is, corresponding to the thickness of the P-type deposited film) is usually limited to about 0.5 to 0.7 m, and it is difficult to make it thicker.
- the SiC vertical MOSFET has a problem that the channel mobility is small and the on-resistance is not lowered compared to the Si-MOSFET.
- a vertical MOSFET with a channel region formed of a low-concentration p-type deposited film is expected to be effective in reducing on-resistance because channel mobility is improved.
- the structure proposed so far is a structure in which the p-type force is returned to the n-type by ion implantation of the conductivity type of the low-concentration p-type deposited film.
- the thickness of the deposited film that can be beaten is limited to be thin, and the crystal quality of the channel region is sufficiently high, and the deposited film cannot be thick enough to relax the electric field in the voltage blocking state. . So As a result, there was a problem that the high voltage blocking capability could not be maintained and a problem that the on-resistance did not decrease as expected! /, And! /.
- an object of the present invention is to provide a SiC vertical MOSFE having a low on-resistance and a high breakdown voltage.
- T is to provide a new structure of a SiC vertical MOSFET having a channel region formed by a low-concentration p-type deposited film.
- Another object of the present invention is to provide a method for manufacturing a high breakdown voltage SiC vertical MOSFET having a channel region formed by a low concentration p-type deposition layer.
- Another object of the present invention is to provide a structure and a manufacturing method capable of manufacturing a high breakdown voltage SiC vertical MOSFET having a channel region formed by a low-concentration p-type deposition layer with a high yield.
- the present invention provides the low concentration as a means for increasing the breakdown voltage and reducing the on-resistance of a SiC vertical MOSFET having a low concentration channel region formed in a low concentration p-type deposition layer.
- a high-concentration p-type layer and a low-concentration n-type deposition layer are interposed between the P-type deposition layer and the n-type drift layer.
- the low-concentration n-type deposition layer is in direct contact with the high-concentration p-type layer and the high-concentration p-type layer.
- the concentration p-type layer has a structure in direct contact with the n-type drift layer in the part lacking portion.
- the SiC vertical MOSFET having the above-described structure is characterized in that it is formed by two deposited films in which the low-concentration p-type deposition layer and the low-concentration n-type stack are laminated.
- selective low-concentration n-type impurity ion implantation is performed so as to penetrate the low-concentration p-type deposition film and reach the low-concentration n-type deposition film.
- a step of forming the n-type base region by inverting (turning back) the part to n-type is provided.
- the low-concentration P-type deposited film needs to be penetrated by ion implantation and returned to the n-type. Therefore, the low-concentration n-type layer interposed between the low-concentration p-type deposited film and the high-concentration P-type layer and the n-type drift layer in the part lacking portion.
- the depletion layer reaches the interface with the gate oxide film 6 before the vertical channel portion is completely pinched off, and the gate oxide film interposed between the gate electrode 7 and the n-type base region 4 is formed. If a strong electric field is applied to cause breakdown (problem described in [0005]), or if the thickness of the deposited film is thin, the influence of the substrate must be significantly affected to increase the electron mobility in the film! The above problem (the problem described in [0006]) can be solved.
- the present invention has the following effects.
- a deposited film having a low-concentration channel region formed in the low-concentration p-type deposition layer and a relatively thick film between the gate oxide film and the high-concentration gate layer By interposing this, it has become possible to realize a SiC vertical MOSFET with low on-resistance and high breakdown voltage. If the impurity concentration and thickness of the intervening n-type deposited layer (33) are selected appropriately, a high breakdown voltage vertical MOSFET of 150 OV or more can be realized.
- the second-conductivity type high-concentration gate layer can be formed with high accuracy, cell miniaturization is facilitated, and the SiC vertical MOSFET has a high breakdown voltage and low loss. I was able to hesitate.
- a SiC vertical MOSFET having a high breakdown voltage and a low on-resistance can be easily manufactured.
- the uniformity of the current flowing at the time of ON is improved, and the cell size can be reduced to about 15 ⁇ m by the effect of a kind of cell filament action.
- the on-resistance can be greatly reduced.
- a high breakdown voltage SiC vertical MOSFET with reduced leakage current can be realized by removing the leakage path of the off-state current.
- a SiC vertical MOSFET having a small on-state resistance and a high withstand voltage can be realized.
- FIG. 1 is a cross-sectional view of a unit cell of a SiC vertical MOSFET according to a first embodiment of the present invention.
- FIG. 2a] ( a ) to (l) are cross-sectional views of cells in the manufacturing process of the SiC vertical MOSFET of the first embodiment of the present invention
- FIG. 2b] (g) to (k) are cross-sectional views of the manufacturing process of the SiC vertical MOSFET according to the first embodiment of the present invention.
- FIG. 3 is a sectional view of a unit cell of a SiC vertical MOSFET according to a second embodiment of the present invention.
- FIG. 4 is a sectional view of a unit cell of a SiC vertical MOSFET according to a third embodiment of the present invention.
- FIG. 5] (d) to (l) are cross-sectional views of a part of the manufacturing process of the SiC vertical MOSFET according to the third embodiment of the present invention.
- FIG. 6 is a sectional view of a unit cell of a SiC vertical MOSFET according to a fourth embodiment of the present invention.
- FIG. 1 is a sectional view of a unit cell of a SiC vertical MO SFET according to the first embodiment of the present invention.
- Layer 2 is deposited.
- the ⁇ -type layer 31 doped with 2xl0 18 cm- 3 of aluminum is formed over a depth of 0.5 ⁇ m, and the p-type layer 31 is provided with a partial lacking portion 24 having a width of about 2.0 m.
- the portion of the p-type layer 32 projected in the thickness direction of the portion lacking portion 24 is doped with lxl0 16 cm ⁇ 3 or more of nitrogen by ion implantation, and a ⁇ -type base with a depth of about 0.7 ⁇ m. Formed to a depth where region 4 penetrates ⁇ -type layer 32 and reaches ⁇ -type layer 33 It ’s done! A channel region 11 is formed in the surface layer of the p-type layer 32 in the middle of the n-type base region 4 and the n-type source layer 5.
- a gate electrode 7 is provided on the channel region 11, on the surface of the n-type base region 4 and the n-type source layer 5 via a gate insulating film 6, and on the gate electrode 7 via an interlayer insulating film 8.
- a source electrode 9 having a low resistance connection is formed on the surface of the n-type source layer 5. Further, the source electrode 9, the Configure the pn junction between the n-type layer, and said p-type layer 32 the p-type layer 31 Niwata connexion formed l X 10 19 cm- 3 of about A low resistance connection is also made to the surface of the P + layer 34 doped with aluminum at a high concentration.
- a drain electrode 10 is formed on the back surface of the high-concentration n-type substrate 1 with a low resistance connection.
- the gate oxide film 6 and the gate electrode 7 formed on the surface of the n-type base region 4 may be deleted.
- this SiC vertical MOSFET is basically the same as that of a general Si vertical MOSFET. That is, in the ON state, when a gate voltage higher than the threshold voltage is applied to the gate electrode 7, electrons are induced on the surface of the p-type layer 32, and the channel region 11 is formed. As a result, the n-type source layer 5 and the n-type drift layer 2 are connected by a current path of electrons passing through the channel region 11, the n-type base region 4, the n-type layer 33, and the partial missing portion 24, and the source from the drain electrode 10 Current flows to electrode 9.
- the channel region 11 is formed in a low-concentration p-type deposited film of 5xl0 15 cm- 3 , and is deposited to a thickness of 1.0 m between the high-concentration p-type layer 31 and the n-type layer.
- a p-type layer 32 deposited to a thickness of 33 and 0.5 m is formed on the surface layer separated from the p-type layer 31 by 1 or more. Therefore, even if the p-type layer 31 is formed by high-concentration ion implantation and contains many crystal defects, the thickly deposited portion of the film has a sufficiently high crystal quality of several 10 cm. A high channel mobility of 2 / V S was obtained, and the on-resistance could be reduced.
- the applied voltage between the drain and source electrodes is blocked by the pn junction formed between the high-concentration p-type layer 31 and the n-type drift layer 2, but the p-type layer 31
- the voltage is blocked by the lateral MOSFET part.
- the p-type layer 31 has a partial missing portion 24 having a width of 2 ⁇ m
- the n-type drift layer 2 has a doping concentration of 5xl0 15 cm— 3.
- the lateral MOSFET part can withstand a powerful low voltage. Even after the pinch-off at the partial missing portion 24 is over, when a higher voltage is applied, the gate oxide film of the lateral MOSFET causes dielectric breakdown due to the leakage electric field.
- the n-type layer 33 interposed between the partial missing portion 24 and the n-type base region 4 can solve the problem by relaxing the electric field, and in this embodiment, a blocking voltage of 1500 V can be obtained.
- the impurity concentration and thickness of the n-type layer 33 can be adjusted in any way by the blocking voltage of the designed SiC vertical MOSFET without being limited to the values of the present embodiment.
- FIG. 2a and (g) to (k) in FIG. 2b are views showing a manufacturing process of the SiC vertical MOSFET according to the first embodiment of the present invention.
- a cross-sectional view of each unit cell is shown.
- a low-concentration n-type drift layer 2 doped with 5xl0 15 cm- 3 nitrogen is deposited on a high-concentration n-type substrate 1 to a thickness of 15 m (a).
- p-type impurity ion implantation 3a using the mask 15 is performed (b).
- the mask 15 was formed by pattern scanning by photolithography of a 1 ⁇ m thick SiO film deposited on the surface by a low pressure CVD method.
- Object ion implantation 3a uses aluminum ions at a substrate temperature of 500. C, acceleration energy 40 keV to 250 keV, injection amount 2xl0 18 cm- 3 . After removing the mask, a lightly doped n-type layer 33 doped with lxlO 16 cm “ 3 phosphorous is deposited on the surface to a thickness of 1.0 m, followed by a lightly doped p-type doped with 5x10 15 cm- 3 aluminum Layer 32 is deposited to a thickness of 0.5 m (c), and then n-type impurity ion implantation 4a is performed using mask 13 to form n-type source region 5 (d).
- Phosphorus ions were used at a substrate temperature of 500 C, acceleration energy of 40 keV to 250 keV, and an implantation amount of 2xl0 2 ° cm— 3 .
- the mask was formed to form the n-type base region 4.
- the active anneal was performed at 1500 ° C for 30 minutes in an argon atmosphere. This forms the p-type layer 32, the n + base layer 4 and the n-type source layer 5.
- the groove 50 reaching the p-type layer 31 from the n-type source layer 5 is dry-etched.
- p-type impurity ion implantation is performed using the mask 16.
- the p-type impurity ion implantation 6a uses aluminum ions at a substrate temperature of 500 ° C and acceleration energy. The test was carried out with a rugie of 40 keV to 250 keV and an injection amount of 2x10 cm. As a result, a P + layer 34 doped with aluminum at a high concentration of about 1 ⁇ 10 cm _ 3 is formed (h).
- a 40-nm-thick gate insulating film 6 is formed by thermal oxidation at 1200 ° C for 140 minutes, and 0.3 ⁇ m polycrystalline silicon deposited by low-pressure C VD method is formed on it by photolithography.
- Form pattern gate electrode 7 (0.
- 0.5 / zm of interlayer insulating film 8 is deposited on the surface by low pressure CVD, and a window is opened in the interlayer insulating film 8 (j).
- a common source electrode 9 is formed on the source layer 5 and the high-concentration p + layer 3 4 to complete the device.
- FIG. 3 is a sectional view of a unit cell of the SiC vertical MOSFET according to the second embodiment of the present invention.
- an n-type drift layer 2 having a thickness of 15 / zm doped with 5 ⁇ 10 15 cm— 3 nitrogen on a substrate 1 having a thickness of about 300 m doped with 5xl0 18 cm— 3 nitrogen. Is deposited.
- a 0.5 ⁇ m thick ⁇ -type layer 31 doped with 2xl0 18 cm— 3 aluminum is deposited on the surface, and the ⁇ -type layer 31 is provided with a partial lacking portion 24 having a width of about 2.0 m. .
- a ⁇ -type layer 33 On the surface of the p-type layer 31 and the surface of the n-type drift layer 2 of the partial lacking portion 24 is deposited a ⁇ -type layer 33 having a thickness of 1.0 ⁇ m doped with lxl0 16 cm- 3 nitrogen.
- a 0.5 m thick p-type layer 32 doped with 5xl0 15 cm- 3 aluminum is deposited on the surface.
- an n-type source layer 5 selectively doped with about lxl0 2Q cm- 3 phosphorous is formed.
- the portion of the p-type layer 32 projected in the thickness direction of the partial lacking portion 24 has a depth of about 0.7 ⁇ m doped with nitrogen of 1 ⁇ 10 16 cm ⁇ 3 or more by ion implantation.
- the n- type base region 4 is formed to a depth that reaches the n-type layer 33 through the p-type layer 32.
- a channel region 11 is formed on the surface layer of the p-type layer 32 in the middle of the n-type base region 4 and the n-type source layer 5.
- a gate electrode 7 is provided on the channel region 11, on the surface of the n-type base region 4 and the n-type source layer 5 via a gate insulating film 6, and on the gate electrode 7 via an interlayer insulating film 8.
- a source electrode 9 having a low resistance connection is formed on the surface of the n-type source layer 5.
- the source electrode 9 forms a pn junction with the n-type layer, and aluminum is formed at a high concentration of about lxl0 19 cnf 3 formed over the P-type layer and the P-type layer.
- a low resistance connection is also made to the surface of the doped p + layer 34.
- a drain electrode 10 is formed on the back surface of the high-concentration n-type substrate 1 with a low resistance connection.
- the n-type base region 4 The gate oxide film 6 and the gate electrode 7 formed on the surface may be deleted.
- the p-type layer 31 is formed by ion implantation in the n-type drift layer 2, and therefore the n-type drift layer 2 In other words, a part lacking part 24 is provided by removing a part of the p-type layer 31 by etching. Since the p-type layer 31 is formed by a deposited film such as epitaxial growth that is not performed by ion implantation, the quality of the crystal film of the n-type layer 33 and the p-type layer 32 deposited thereon is not significantly impaired. Therefore, there are advantages in that it is higher than that of the second embodiment and the electron mobility can be easily obtained.
- FIG. 4 is a cross-sectional view of a SiC vertical MOSFET according to a third embodiment of the present invention.
- the same reference numerals as those in FIG. 1 indicate the same parts, and the basic structure is the same as in the first embodiment except that high-concentration n-type layers 41 on both sides of the n-type base region 4 are added.
- the high-concentration n-type layer 41 is formed at the same time as the n-type source layer 5 and has the same impurity concentration and depth from the surface, and has a length almost equal to that of the partial lacking portion 24.
- the lengths of the two channel regions 11 in the unit cell can be made equal, and the relative positions thereof can be in a predetermined relationship. This is effective in preventing current concentration. This effect will be better understood by the manufacturing method described below.
- FIGS. 2b to (g) to (k) are diagrams showing a part of the manufacturing process of the SiC vertical MOSFET according to the third embodiment of the present invention, (a) to (£) of FIG.
- the steps (d) and (!) are the same, and the other steps are the same, that is, the n-type source region 5 is formed by the n-type impurity ion implantation 4a in the step (d)!
- a mask window 40 is opened in the mask 13 for performing the ion implantation at a position in the vicinity of the vertical projection of the partial lacking portion 24 of the p-type layer 31 so as to have a width substantially equal to the partial lacking portion 24.
- N-type impurity ion implantation 4a was carried out with phosphorus ions at a substrate temperature of 500.
- C acceleration energy of 40 keV to 250 keV, implantation amount of 2xl0 2 ° cm— 3.
- n-type base Shape area 4 is performed using mask 14 (e).
- the two channel regions 11 in the unit cell formed between the two layers have the length. (Corresponding to the so-called gate length) and their relative positional relationships can be formed as designed in advance. Therefore, the uniformity of the current that flows when the transistor is on is improved, and the cell can be miniaturized by the effect of a kind of cell filament operation, so that the on-resistance of the vertical MOSFET can be reduced.
- FIG. 6 is a cross-sectional view of a SiC vertical MOSFET according to a fourth embodiment of the present invention.
- the basic structure of the cell is the same as that of Embodiment 1 in FIG. Embodiment 1 differs constitute a pn junction between the n-type layer 33 in FIG. 1, the force one p-type layer 32 and the p-type layer 31 Niwata connexion formed lxl0 19 cm- 3 as high
- the insulating film 51 is interposed between the n-type layer 33 and the force sword electrode 9 in place of the p + layer 34 doped with aluminum in concentration. This prevents a short circuit between the n-type layer and the force sword electrode and eliminates a current leakage path in the voltage blocking state.
- This structure can also be applied to the cell structures of the second and third embodiments.
- the source electrode 9 is spanned between the gate electrode 7 and the cell surface via the interlayer insulating film 8.
- the present invention is not limited to this, as long as the source electrode is in low resistance contact with the surface exposed portions of the source layer 5, p-type layer 32, and p-type layer 31.
- the gate oxide film 6 and the gate electrode 7 are ion-implanted.
- the p-type force is shown to cover the entire surface of the n-type base region 4 formed by reversing the n-type. However, this part of the gate oxide film and the gate electrode are partially or entirely covered.
- the present invention can also be applied to a MOSFET having a so-called buried channel structure in which channel conductivity is improved by ion-implanting thin n-type impurities into the surface of the P-type layer 32 serving as the channel region 11.
- the orientation of the crystal plane of the SiC crystal substrate 1 is normally specified, but is generally widely applied.
- ⁇ 000JJ plane Substrate (called silicon face), ⁇ 110 ⁇ face board, or ⁇ 000JJ face (called carbon face) board, and a board with a surface parallel to the face with a slight off-angle on these faces
- Applying a force ⁇ 000 ⁇ ⁇ ⁇ plane (carbon plane) substrate and a surface substrate parallel to a plane with a slight off angle on this plane will increase the breakdown electric field strength near the voltage blocking junction. It has a high electron mobility in the channel region, and is most excellent for obtaining a vertical MOSFET with high voltage and low on-resistance.
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Abstract
Description
Claims
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
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EP05788237A EP1814162A4 (en) | 2004-11-18 | 2005-09-30 | SILICON CARBIDE MOS FIELD EFFECT TRANSISTOR AND PROCESS FOR ITS MANUFACTURE |
KR1020077009697A KR101057199B1 (ko) | 2004-11-18 | 2005-09-30 | 탄화규소 mos 전계 효과 트랜지스터 및 그 제조 방법 |
US11/718,036 US20090134402A1 (en) | 2004-11-18 | 2005-09-30 | Silicon carbide mos field-effect transistor and process for producing the same |
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JP2004-334920 | 2004-11-18 | ||
JP2004334920A JP4604241B2 (ja) | 2004-11-18 | 2004-11-18 | 炭化ケイ素mos電界効果トランジスタおよびその製造方法 |
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US (1) | US20090134402A1 (ja) |
EP (1) | EP1814162A4 (ja) |
JP (1) | JP4604241B2 (ja) |
KR (1) | KR101057199B1 (ja) |
CN (1) | CN100536165C (ja) |
WO (1) | WO2006054394A1 (ja) |
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WO2012177699A1 (en) * | 2011-06-20 | 2012-12-27 | The Regents Of The University Of California | Current aperture vertical electron transistors |
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JP6965499B2 (ja) * | 2016-03-16 | 2021-11-10 | 富士電機株式会社 | 炭化珪素半導体装置および炭化珪素半導体装置の製造方法 |
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- 2005-09-30 KR KR1020077009697A patent/KR101057199B1/ko not_active IP Right Cessation
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Also Published As
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EP1814162A1 (en) | 2007-08-01 |
KR20070083844A (ko) | 2007-08-24 |
CN100536165C (zh) | 2009-09-02 |
KR101057199B1 (ko) | 2011-08-16 |
US20090134402A1 (en) | 2009-05-28 |
EP1814162A4 (en) | 2008-12-03 |
JP4604241B2 (ja) | 2011-01-05 |
CN101065847A (zh) | 2007-10-31 |
JP2006147789A (ja) | 2006-06-08 |
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