WO2022078120A1 - Insulated gate bipolar transistor and formation method therefor - Google Patents

Insulated gate bipolar transistor and formation method therefor Download PDF

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WO2022078120A1
WO2022078120A1 PCT/CN2021/117225 CN2021117225W WO2022078120A1 WO 2022078120 A1 WO2022078120 A1 WO 2022078120A1 CN 2021117225 W CN2021117225 W CN 2021117225W WO 2022078120 A1 WO2022078120 A1 WO 2022078120A1
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hydrogen
region
buffer
doped
substrate
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PCT/CN2021/117225
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French (fr)
Chinese (zh)
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王珏
陈政
戴银
徐杨
徐承福
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绍兴中芯集成电路制造股份有限公司
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor 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
    • H01L29/66Types 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
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor 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
    • H01L29/02Semiconductor 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
    • H01L29/0603Semiconductor 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
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor 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
    • H01L29/02Semiconductor 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
    • H01L29/0684Semiconductor 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 the shape, relative sizes or dispositions of the semiconductor regions or junctions between the regions
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor 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
    • H01L29/66Types of semiconductor device ; Multistep manufacturing processes therefor
    • H01L29/66007Multistep manufacturing processes
    • H01L29/66075Multistep manufacturing processes of devices having semiconductor bodies comprising group 14 or group 13/15 materials
    • H01L29/66227Multistep manufacturing processes of devices having semiconductor bodies comprising group 14 or group 13/15 materials 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
    • H01L29/66234Bipolar junction transistors [BJT]
    • H01L29/66325Bipolar junction transistors [BJT] controlled by field-effect, e.g. insulated gate bipolar transistors [IGBT]
    • H01L29/66333Vertical insulated gate bipolar transistors

Definitions

  • the present invention relates to the field of semiconductor technology, in particular to an insulated gate bipolar transistor and a method for forming the same.
  • Insulated Gate Bipolar Transistor which combines the gate voltage control characteristics of MOSFET and the low on-resistance characteristics of bipolar transistors, which improves the mutual restraint between the device's withstand voltage and on-resistance , has the advantages of high voltage, high current, high frequency, high power integration density, large input impedance, small on-resistance, and low switching loss. It has been widely used in many fields such as inverter home appliances, industrial control, electric and hybrid vehicles, new energy, and smart grids.
  • the turn-off voltage of the device tends to be larger and the turn-off time is longer.
  • a field-stop IGBT device is proposed.
  • the field-stop IGBT device is used to block the electric field by arranging an N-type buffer between the collector region and the drift region, so that the same blocking voltage can be achieved.
  • the thickness of the lower compression drift region which in turn can reduce the forward voltage drop and turn-off time.
  • the performance of the current field-stop IGBT devices is still not stable enough, and further optimization is urgently needed.
  • the purpose of the present invention is to provide a method for forming an insulated gate bipolar transistor, so as to solve the difficulty in preparing a hydrogen doped region with stable distribution by the existing forming method, which is beneficial to improve the performance stability of the formed transistor device.
  • the present invention provides a method for forming an insulated gate bipolar transistor, comprising:
  • a substrate is provided, the substrate has opposing first and second surfaces, and a gate conductive layer, a body region of a first doping type, and a second surface are formed in a portion of the substrate corresponding to the first surface Two doping types of emitter regions;
  • An ion implantation process and an annealing process are performed on the second surface of the substrate to form a buffer region of the second doping type and a collector region of the first doping type, the collector region extending from the second surface of the substrate.
  • Two surfaces extend inwardly into the substrate, the buffer zone is located on the side of the collector region proximate the body region; and,
  • An ion implantation process and a thermal annealing process are performed on the second surface of the substrate to form a hydrogen-doped region, the hydrogen-doped region is located on a side of the buffer zone close to the body region, wherein the hydrogen-doped region
  • the impurity region includes a plurality of hydrogen-doped subregions that are sequentially arranged in a direction away from the buffer zone, and ion concentration peaks of the plurality of hydrogen-doped subregions are sequentially decreased in a direction away from the buffer zone.
  • the method for forming the buffer zone includes: sequentially performing at least two ion implantation steps, and performing an annealing process, to form at least two layers of buffer subregions, the at least two layers of buffer subregions being farther away from the collector region.
  • the directions are arranged in sequence; and, the method for forming the hydrogen-doped region includes: performing multiple ion implantation steps in sequence to form the multi-layer hydrogen-doped subregion, and the multi-layer hydrogen-doped subregion is farther away from the buffer.
  • the directions of the zones are arranged in order.
  • the number of hydrogen-doped sub-regions in the hydrogen-doped region is greater than the number of buffer sub-regions in the buffer zone.
  • the ion implantation dose decreases sequentially, so as to make the ion concentration peak of the formed at least two buffer zones. It decreases sequentially in the direction away from the collector region.
  • the ion implantation dose is sequentially decreased, so that the ions of the formed multilayer hydrogen doped region are reduced.
  • concentration peaks decrease successively in the direction away from the buffer zone.
  • the buffer zone includes two layers of buffer zones, the peak ion concentrations of the buffer zones in the two layers are both between 1E16 atoms/cm 3 and 1E17 atoms/cm 3 , and the widths of the buffer zones in the two layers are both 1E16 atoms/cm 3 and 1E17 atoms/cm 3 0.4 ⁇ m ⁇ 0.7 ⁇ m.
  • the hydrogen-doped region includes four hydrogen-doped subregions, wherein the peak ion concentrations of the two hydrogen-doped subregions closest to the buffer zone are both between 1E12 atoms/cm 3 to 1E14 atoms/cm 3 , and the ion concentration peaks of the two hydrogen-doped partitions farthest from the buffer zone are all between 1E12 atoms/cm 3 and 1E13 atoms/cm 3 , and the widths of the four hydrogen-doped partitions are all 6 ⁇ m to 8 ⁇ m .
  • the doping ions in the buffer zone include phosphorus, and a laser annealing process is used in the annealing process for forming the buffer zone, and the annealing temperature is set to be greater than or equal to 600°C.
  • the annealing temperature is 350°C to 450°C.
  • the present invention also provides an insulated gate bipolar transistor, comprising:
  • a substrate having opposing first and second surfaces, and having a gate conductive layer, a body region of a first doping type, and a second formed in a portion of the substrate corresponding to the first surface Doping type of emitter region;
  • collector region of the first doping type extending inwardly into the substrate from the second surface of the substrate;
  • a buffer area of a second doping type is formed on the side of the collector region adjacent to the body region, and,
  • a hydrogen-doped region is formed on a side of the buffer zone close to the body region, and the hydrogen-doped region includes a plurality of hydrogen-doped subregions arranged in sequence in a direction away from the buffer zone, the multiple The ion concentration peaks of each of the hydrogen-doped subregions decrease sequentially in the direction away from the buffer zone.
  • the thickness of the hydrogen doped region is greater than the thickness of the buffer zone.
  • the buffer zone includes at least two buffer zones arranged in sequence away from the collector region, and the number of hydrogen-doped zones in the hydrogen-doped zone is greater than the number of buffer zones in the buffer zone .
  • the ion concentration peaks of the at least two buffer zones in a direction away from the collector zone decrease sequentially.
  • the buffer zone includes two layers of buffer zones, the peak ion concentrations of the buffer zones in the two layers are both between 1E16 atoms/cm 3 and 1E17 atoms/cm 3 , and the widths of the buffer zones in the two layers are both 1E16 atoms/cm 3 and 1E17 atoms/cm 3 0.4 ⁇ m ⁇ 0.7 ⁇ m.
  • the hydrogen-doped region includes four hydrogen-doped subregions, wherein the peak ion concentrations of the two hydrogen-doped subregions closest to the buffer zone are both between 1E12 atoms/cm 3 to 1E14 atoms/cm 3 , and the ion concentration peaks of the two hydrogen-doped partitions farthest from the buffer zone are all between 1E12 atoms/cm 3 and 1E13 atoms/cm 3 , and the widths of the four hydrogen-doped partitions are all 6 ⁇ m to 8 ⁇ m .
  • the hydrogen-doped subregion with the largest ion concentration peak in the hydrogen-doped region is adjacent to the buffer subregion with the smallest ion concentration peak in the buffer zone, and the hydrogen-doped subregion with the largest ion concentration peak is The peak ion concentration is still smaller than the peak ion concentration of the buffer partition with the smallest peak ion concentration.
  • the hydrogen doped region is prepared after the buffer zone of the second doping type is formed, so that the formed hydrogen doped region can be prevented from being buffered
  • the method provided by the present invention effectively avoids that the hydrogen in the hydrogen-doped region is recombined during the annealing process of the buffer zone, resulting in the ion concentration of the hydrogen-doped region. Problems where the distribution is unstable and cannot be precisely controlled.
  • the method provided by the present invention it is possible to effectively control the concentration distribution of each hydrogen-doped sub-area in the hydrogen-doped region, and further, a plurality of hydrogen-doped regions with the peak ion concentration decreasing in turn in the direction away from the buffer zone can be prepared.
  • the stray partition is beneficial to improve the performance of the device. For example, the voltage change (dV/dt) between the collector and the emitter when the device is turned off can be more gentle.
  • FIG. 1 is a schematic flowchart of a method for forming an insulated gate bipolar transistor according to an embodiment of the present invention
  • 2 to 12 are schematic structural diagrams of an insulated gate bipolar transistor in an embodiment of the present invention during its fabrication
  • FIG. 13 is a concentration profile of a part of the doped region of the insulated gate bipolar transistor according to an embodiment of the present invention.
  • the core idea of the present invention is to provide a method for forming an insulated gate bipolar transistor, which is beneficial to improve the preparation precision of the buffer layer in the device.
  • the method for forming the insulated gate bipolar transistor may include:
  • Step S100 a substrate is provided, the substrate has a first surface and a second surface opposite to each other, and a gate conductive layer, a body of a first doping type are formed in a portion of the substrate corresponding to the first surface region and an emitter region of the second doping type;
  • Step S200 performing an ion implantation process and an annealing process on the second surface of the substrate to form a buffer region of the second doping type and a collector region of the first doping type;
  • Step S300 performing an ion implantation process on the second surface of the substrate to form a hydrogen-doped hydrogen-doped region, where the hydrogen-doped region is located on a side of the buffer zone close to the body region, wherein the The hydrogen-doped region includes a plurality of hydrogen-doped subregions that are sequentially arranged in a direction away from the buffer zone, and ion concentration peaks of the plurality of hydrogen-doped subregions are sequentially decreased in a direction away from the buffer zone.
  • an ion implantation process is performed to form a hydrogen doped region having a plurality of hydrogen doping subregions Miscellaneous area.
  • the formation of the hydrogen doped region can be prevented from being affected by the preparation process of the buffer region and the collector region, and the hydrogen ions implanted in the hydrogen doped region can be prevented from being recombined at high temperature, so as to ensure the safety of the hydrogen doped region.
  • the stability of the ion concentration distribution is beneficial to the formation of a plurality of hydrogen doping partitions with a gradient in the peak value of the ion concentration.
  • a substrate 100N is provided, the substrate 100N has a first surface A1 and a second surface A2 opposite to each other, and the substrate 100N corresponds to the first surface A gate conductive layer 220 , a body region 300P of a first doping type and an emitter region 400N of a second doping type are formed in the portion of .
  • the substrate 100N is, for example, a substrate 100N of the second doping type, and a part of the substrate 100N may constitute the drift region of the second doping type of the insulated gate bipolar transistor.
  • the second doping type is N-type, that is, the substrate 100N is an N-type substrate and is used to form an N-type drift region.
  • the preparation steps of the gate conductive layer 220 , the body region 300P and the emitter region 400N can be adjusted according to actual conditions.
  • the gate conductive layer 220 may be preferentially formed in the substrate 100N, and then the body region 300P and the emitter region 400N may be sequentially prepared; or, the body region 300P may be preferentially formed and then prepared
  • the gate conductive layer 220 is preferentially formed as an example for explanation.
  • the gate conductive layer 220 is formed in the gate trench 200a in the substrate 100N. Specifically, by etching the first surface A1 of the substrate 100N, a gate trench 200a extending inward from the first surface A1 of the substrate 100N is formed, wherein the gate trench
  • the trench depth of 200a is, for example, 1 ⁇ m ⁇ 6 ⁇ m, and the sidewalls of the gate trenches 200a may be slightly inclined inclined sidewalls, and the inclined sidewalls of the gate trenches 200a have an acute angle with respect to the horizontal direction. ⁇ is, for example, 85° to 90°.
  • the method further includes: forming a gate dielectric layer 210 on the bottom wall and sidewall of the gate trench 200a.
  • the gate dielectric layer 210 can cover the entire trench sidewall of the gate trench 200a, so that the top of the gate dielectric layer 210 is not lower than the top of the gate trench 200a.
  • the gate conductive layer 220 is filled in the gate trench 200a.
  • the method for forming the gate conductive layer 220 includes: filling the gate conductive material layer in the gate trench 200a, and etching back the gate conductive material layer, so that the top surface is lower than the lining material layer.
  • the height difference between the top surface of the gate conductive layer 220 and the first surface A1 of the substrate is, for example, less than or equal to 1 ⁇ m.
  • the gate dielectric layer 210 covers the entire trench sidewall of the gate trench. Therefore, when an etch-back process is performed to reduce the top surface of the gate conductive layer 220, the Under the protection of the gate dielectric layer 210 , damage to the sidewall of the trench higher than the gate conductive layer 220 is avoided.
  • one or more gate conductive layers 220 may be formed on the substrate 100N.
  • at least two gate conductive layers 220 are formed on the substrate 100N to form at least two transistor cells.
  • an ion implantation process and an annealing process are performed on the first surface A1 of the substrate 100N to sequentially form the body region 300P of the first doping type and the emitter of the second doping type District 400N.
  • the body region 300P is a P-type doped region
  • the emitter region 400N is an N-type doped region.
  • the method for forming the body region 300P includes: performing an ion implantation process and an annealing process to form a body region 300P extending into the substrate, and the bottom boundary of the body region 300P is extended to be lower than
  • the depth position of the top of the gate conductive layer 220 is such that the body region 300P at least partially overlaps the gate conductive layer 220 in a lateral space.
  • the annealing temperature of the annealing process for forming the body region 300P is, for example, 1000° C. ⁇ 1200° C.
  • the extension depth of the body region 300P in the substrate 100N is, for example, 2 ⁇ m ⁇ 4 ⁇ m, which ensures that the body The region 300P can laterally overlap with the gate conductive layer 220 .
  • the emitter region 400N can also be formed by an ion implantation process and an annealing process, so that the emitter region 400N extends inward from the first surface A1 of the substrate to the body region 300P .
  • the bottom boundary of the emitter region 400N also extends to a depth lower than the top of the gate conductive layer 220 , and the bottom boundary of the emitter region 400N is also higher than the bottom boundary of the body region 300P , so as to utilize the portion of the body region 300P below the emitter region 400N to form a conductive channel region.
  • the extension depth of the emitter region 400N in the substrate 100N is, for example, 0.2 ⁇ m ⁇ 1 ⁇ m.
  • the method further includes: forming a contact electrode on the first surface A1 of the substrate 100N for electrically extracting the emitter region 400N and the body region 300P.
  • the method for forming the contact electrode 620 may include the following steps.
  • the first step forms an insulating layer 500 on the first surface of the substrate 100N, and the insulating layer 500 also fills the space above the gate conductive layer 220 in the gate trench, The gate conductive layer 220 and the emitter region 400N are covered by the insulating layer 500 .
  • the second step is to etch the insulating layer 500 to the substrate above the emitter region 400N to sequentially expose the emitter region 400N and the body region 300P, and form contacts hole 600a.
  • the contact hole 600 a is used to accommodate the contact electrode 620 .
  • the insulating layer 500 and the substrate 100N are sequentially etched, so that the contact hole 600a penetrates through the emitter region 400N and extends into the body region 300P.
  • a contact electrode formed in the contact hole 600a electrically connects the emitter region 400N and the body region 300P
  • the method before filling the contact electrode 620 into the contact hole 600a, the method further includes: implanting dopant ions of the first doping type through the contact hole 600a to A heavily doped region 610P is formed at the bottom of the contact hole 600a.
  • the heavily doped region 610P is a P-type doped region, and the doping concentration of the heavily doped region 610P is higher than that of the body region 300P.
  • the heavily doped region 610P is provided at the bottom of the contact hole 600a (after the contact electrode is subsequently formed, the heavily doped region 610P is provided at the bottom of the contact electrode), thereby The parasitic NPN transistors described above can be shorted to improve the hold-up effect of the device.
  • the contact resistance between the contact electrode and the body region 300P can also be effectively reduced.
  • a contact electrode 620 is formed in the contact hole 600a.
  • the method for forming the contact electrode 620 includes: forming a metal diffusion barrier layer 621 on the bottom wall and sidewall of the contact hole 600a, and filling the contact hole 600a with a metal layer 622 to form the contact electrode 620. Specifically, a planarization process may be used to make the top surface of the contact electrode 620 flush with the top surface of the insulating layer 500 .
  • the metal diffusion barrier layer 621 is surrounded on the periphery of the metal layer 622 to prevent the metal in the metal layer 622 from diffusing into the substrate 100N, thereby improving the leakage current phenomenon of the device.
  • the material of the metal diffusion barrier layer 621 includes, for example, at least one of titanium (Ti) and titanium nitride (TiN), and the thickness of the metal diffusion barrier layer 621 is, for example, 500A ⁇ 2000A.
  • the material of the metal layer 622 includes, for example, tungsten.
  • the method further includes: forming an electrode lead layer 630 to electrically connect the contact electrodes 620 .
  • the electrode lead layer 630 covers the insulating layer 500 and the contact electrode 620 .
  • the material of the electrode lead layer 630 includes, for example, aluminum, copper, aluminum-silicon alloy, or aluminum-silicon-copper alloy.
  • At least two gate conductive layers 220 are formed in the substrate 100N of this embodiment, and the body region 300P and the emitter region are correspondingly formed on the sides of each gate conductive layer 220 400N.
  • at least two contact electrodes 620 are formed correspondingly to connect the corresponding body regions 300P and the emitter regions 400N in a one-to-one correspondence, and the at least two contact electrodes 620 can be electrically connected to the electrode lead layer. 630.
  • step S200 referring specifically to FIG. 10, an ion implantation process and an annealing process are performed on the second surface A2 of the substrate 100N to form a buffer zone 700N of the second doping type and a set of the first doping type Electrode area 800P.
  • the buffer region 700N is an N-type doped region
  • the collector region 800P is a P-type doped region.
  • the buffer area 700N is located on the side of the collector area 800P close to the body area 300P, and the buffer area 700N includes at least two buffer areas arranged in sequence away from the collector area 800P (this In an embodiment, a first buffer partition 710N and a second buffer partition 720N are included.
  • the method before the ion implantation process is performed on the second surface A2 of the substrate 100N, the method further includes: thinning the substrate 100N from the second surface of the substrate 100N, so that the thinned The thickness of the substrate 100N satisfies predetermined requirements.
  • the formation method provided in this embodiment is conducive to further reducing the thickness of the drift region of the device, so when the substrate 100N is thinned, the substrate 100N can be correspondingly reduced to a thinner thickness , in order to improve the emission efficiency of the device.
  • the thickness of the thinned substrate 100N is 40 ⁇ m ⁇ 150 ⁇ m.
  • an ion implantation process can be performed on the thinned substrate 100N to form the buffer region 700N and the collector region 800P.
  • the buffer region 700N can be formed by the ion implantation process first, and then the collector region 800P can be formed by performing the ion implantation process again; And the ion implantation process is performed again to form the buffer zone 700N.
  • At least two ion implantation steps and an annealing process can be performed in sequence to form at least two layers of the second dopant in the substrate 100N.
  • Miscellaneous buffer partitions in this embodiment, including: a first buffer partition 710N and a second buffer partition 720N
  • at least two layers of buffer partitions are sequentially arranged along the thickness direction of the substrate 100N, and the buffer partitions
  • the ion concentration peaks of the at least two-layer buffer partitions in 700N successively decrease in the direction away from the second surface A2 of the substrate. That is, in this embodiment, the peak value of the ion concentration of the first buffer zone 710N is lower than the peak value of the ion concentration of the second buffer zone 720N.
  • the ion implantation energy of the ion implantation step can be adjusted to further adjust the depth position of each buffer subregion implanted into the substrate 100N, and the ion implantation dose of the ion implantation step can be adjusted to further adjust the formed buffer subregions. ion concentration.
  • the ion implantation dose decreases sequentially, so that the formed at least two ion implantation steps are The ion concentration peaks in the buffer zone decreased sequentially.
  • two buffer partitions are formed by sequentially performing two ion implantation steps as an example for explanation.
  • a first ion implantation step is performed to form a first buffer region 710N in a deeper position of the substrate 100N.
  • the ion implantation energy of the first ion implantation step is, for example, 1Me ⁇ 2Me, and the deepest boundary of the first buffer subregion 710N can reach a depth position of 1.6 ⁇ m ⁇ 1.9 ⁇ m from the second surface of the substrate , and the width dimension of the first buffer subregion 710N along the thickness direction of the substrate is, for example, 0.4 ⁇ m ⁇ 0.7 ⁇ m.
  • the ion concentration distribution of the first buffer subregion 710N presents a Gaussian distribution
  • the ion concentration peak value of the first buffer subregion 710 is, for example, 1E16 atoms/cm 3 to 1E17 atoms/cm 3 .
  • a second ion implantation step is performed to form a second buffer region 720N in a shallower position of the substrate 100N.
  • the ion implantation energy of the second ion implantation step is lower than the ion implantation energy of the first ion implantation step.
  • the ion implantation energy of the second ion implantation step is, for example, 200kev ⁇ 700kev, and the distance from the deepest boundary of the formed second buffer region 720N to the second surface of the substrate is 0.3 ⁇ m ⁇ 1.0 ⁇ m, and the width dimension of the second buffer region 720N may be the same as or approximately the same as the width dimension of the first buffer region 710N.
  • the ion concentration distribution in the second buffer zone 720 also presents a Gaussian distribution.
  • the ion concentration peak value of the second buffer zone 720 is, for example, between 1E16 atoms/cm 3 to 1E17 atoms/cm 3 . within the range.
  • the ion concentration peaks of the first buffer subregion 710N and the second buffer subregion 720N are both within the same numerical range, the ion implantation doses of the two can still be adjusted within the same numerical range, so that the peak value of the ion concentration of the first buffer zone 710N is lower than the peak value of the ion concentration of the second buffer zone 720N.
  • the first ion implantation step and the second ion implantation step are, for example, phosphorus ion implantation, arsenic ion implantation or antimony ion implantation, so as to form the N-type first buffer region 710N and the second ion implantation.
  • the ion implantation may be performed at a slightly inclined angle with respect to the second surface A2 of the substrate 100N, for example, the ion implantation may be performed at an inclined angle. Ion implantation is performed on the second surface of the substrate 100N in the direction of 0° ⁇ 7°.
  • an annealing process is performed to activate the implanted ions in each buffer region in the buffer region 700N.
  • a laser annealing process is usually used, and a higher annealing temperature is required, for example, the annealing temperature of the annealing process can be greater than or equal to 600°C.
  • an ion implantation process and an annealing process are also used to form a collector region 800P of a first doping type, the collector region 800P extending from the substrate 100N
  • the second surface A2 of A2 extends inward to the buffer area 700N so that the buffer area 700N and the collector region 800P abut.
  • the thickness of the collector region 800P is, for example, less than or equal to 0.5 ⁇ m, that is, the depth of the inward extension of the collector region 800P from the second surface A2 of the substrate 100N is less than or equal to 0.5 ⁇ m.
  • the ion implantation process for forming the collector region 800P is specifically: an ion implantation process of boron ions to form the P-type collector region 800P.
  • the ion doping concentration of the collector region 800P may be 1E16 atoms/cm 3 to 1E18 atoms/cm 3 .
  • step S300 referring specifically to FIG. 11 , an ion implantation process and an annealing process are performed on the second surface of the substrate 100N to form a hydrogen-doped region 900H, and the hydrogen-doped region 900H is located in the buffer zone 700N is close to one side of the body region 300P.
  • the hydrogen-doped region 900H is formed after the buffer region 700N and the collector region 800P are formed.
  • the annealing process during the preparation of the buffer region 700N and the collector region 800P can effectively avoid the influence on the hydrogen doped region 900H.
  • the dopant ions in the buffer zone 700N include phosphorus ions
  • a higher annealing temperature is usually required to activate the phosphorus ions
  • the annealing temperature for activating the phosphorus ions is, for example, higher than 600°C.
  • the environment is particularly prone to cause hydrogen ions in the substrate to be recombined.
  • the hydrogen in the hydrogen doped region 900H is prevented from being recombined at high temperature, which would cause the hydrogen doped region 900H to be recombined.
  • the ion doping concentration cannot be precisely controlled.
  • the prepared hydrogen-doped region 900H includes a plurality of hydrogen-doped sub-regions (in this embodiment, including: the first hydrogen-doped sub-region 910H, the second hydrogen-doped sub-region 910H, the second The hydrogen-doped subregions 920H, the third hydrogen-doped subregions 930H, and the fourth hydrogen-doped subregions 940H), and the ion concentration peaks of the plurality of hydrogen-doped subregions gradually decrease in the direction away from the buffer zone.
  • the hydrogen-doped partitions closer to the surface of the substrate are more affected by the temperature, which is likely to cause The concentration of the hydrogen doped partition is lower.
  • the substrate formed with a plurality of hydrogen-doped subregions is placed under a high temperature condition to complete the high-temperature annealing process, it will be disadvantageous to form a plurality of hydrogen-doped subregions whose concentration peaks decrease sequentially from the substrate surface inward.
  • the hydrogen doped region 900H is formed after the collector region electricity 800P and the buffer region 700N are prepared, so the hydrogen doped region 900H will not be affected by the collector region electricity 800P and the buffer region 700N.
  • the hydrogen concentration is unstable due to the preparation process of the buffer zone 700N, so that the hydrogen concentration in the formed hydrogen-doped region 900H can be controlled more precisely, so that it is easier to prepare the ion concentration peaks that decrease sequentially from the substrate surface inward. of multiple hydrogen-doped partitions.
  • the hydrogen-doped region 900H includes a fourth hydrogen-doped subregion 940H, a third hydrogen-doped subregion 930H, a second hydrogen-doped subregion 920H and The first hydrogen doped partition 910H.
  • the ion concentration distributions of the fourth hydrogen-doped subregion 940H, the third hydrogen-doped subregion 930H, the second hydrogen-doped subregion 920H, and the first hydrogen-doped subregion 910H are all Gaussian distributions, and the fourth hydrogen-doped subregion 910H has a Gaussian distribution.
  • the ion concentration peaks of the doping subregion 940H, the third hydrogen doping subregion 930H, the second hydrogen doping subregion 920H and the first hydrogen doping subregion 910H decrease sequentially. That is, the fourth hydrogen-doped subregion 940H is closest to the second surface A2 of the substrate 100N and has the largest ion concentration peak, and the first hydrogen-doped subregion 910H is farthest from the substrate 100N The second surface, A2, has the smallest peak ion concentration.
  • the width of the hydrogen-doped region 900H is larger than the width of the buffer zone 700N, so that the hydrogen-doped region 900H can be used to greatly weaken the electric field, so as to realize the electric field cut-off to a greater extent, and can even be based on
  • the hydrogen-doped region 900H directly realizes the electric field cut-off, so that the electric field strength reaching the buffer zone 700N is greatly reduced, and the voltage withstand performance of the device is effectively guaranteed.
  • the hydrogen-doped region 900H includes multiple layers of hydrogen-doped subregions
  • the buffer region 700N includes at least two layers of buffer subregions
  • the hydrogen-doped subregions in the hydrogen-doped region 900H can be The number is greater than the number of buffer partitions in the buffer 700N. In this way, on the one hand, the width of the formed hydrogen doped region 900H is guaranteed to be greater than that of the buffer zone 700N;
  • the multi-layer hydrogen-doped subregions in the hydrogen-doped region 900H may be formed separately by multiple ion implantation steps. 11 and FIG. 13 , first, a first ion implantation step is performed to form a first hydrogen-doped subregion 910H; then, a second ion implantation step is performed to form a second hydrogen-doped subregion 920H; Next, a third ion implantation step is performed to form a third hydrogen-doped subregion 930H; then, a fourth ion implantation step is performed to form a fourth hydrogen-doped subregion 940H. And, after performing the multi-pass ion implantation steps as described above, an annealing process is performed. Wherein, for the hydrogen-doped region 900H, a thermal annealing process can be used, and the annealing temperature is, for example, 350°C to 450°C.
  • the process parameters of the four ion implantation steps for forming the hydrogen-doped region 900H and the ion distribution of the formed four-layer hydrogen-doped partition can be referred to, for example, as shown in Table 1.
  • the implant doses of the four hydrogen-doped subregions have overlapping value ranges, however, it should be recognized that the values shown above may still be within the range of the values shown above during the actual ion implantation.
  • the implantation dose of each hydrogen-doped subregion is adjusted within the range, so that the ion concentration peaks of a plurality of hydrogen-doped subregions from deep to shallow increase step by step. In this way, the electric field can be gradually weakened by using a plurality of hydrogen-doped subregions with gradually increasing ion concentrations.
  • the hydrogen-doped subregion (ie, the fourth hydrogen-doped subregion 940H) with the largest ion concentration peak in the hydrogen doping region 900H is adjacent to the buffer with the smallest ion concentration peak in the buffer region 700N partition (ie, the first buffer partition 710N), and the ion concentration peak of the hydrogen-doped partition with the largest ion concentration peak (ie, the fourth hydrogen-doped partition 940H) is still smaller than the buffer with the smallest ion concentration peak The peak ion concentration of the partition (ie, the first buffer partition 710N).
  • the ion concentration of the multi-layer doped region formed by the hydrogen doped region 900H and the buffer region 700N is generally increased from deep to shallow, so that the electric field can be weakened step by step.
  • the ion concentration of the doped region closest to the collector region 800P is the highest, which ensures that the electric field can be completely cut off in the doped region before the collector region 800P, and is beneficial to improve the leakage phenomenon of the device.
  • the hydrogen-doped region 900H after forming the hydrogen-doped region 900H, it further includes: forming an ohmic electrode 810 on the second surface A2 of the substrate 100N, the ohmic electrode 810 and the The collector region 800P contacts.
  • the method for forming the ohmic electrode 810 includes, for example: first, depositing a metal layer on the second surface of the substrate 100N, where the material of the metal layer includes, for example, at least one of aluminum, titanium, nickel and gold Next, an alloying process is performed, so that the metal in the metal layer and the silicon in the substrate 100N realize metal-silicon alloying on the contact surface of the two, so as to reduce the ohmic electrode 810 and the silicon in the substrate 100N. Contact resistance between collector regions 800P.
  • the insulated gate bipolar transistor includes:
  • a second conductivity type substrate 100N having opposing first and second surfaces
  • the gate conductive layer 220 is formed in the substrate 100N;
  • the body region 300P of the first doping type extends inward from the first surface of the substrate 100N into the substrate 100N, so that the body region 300P at least partially overlaps the gate conductive layer 220 laterally ;
  • the emitter region 400N of the second doping type extends inward from the first surface of the substrate 100N into the body region 300P, and the bottom boundary of the emitter region 400N is between the gate conductive layer between the top boundary of 220 and the bottom boundary of the body region 300P;
  • the collector region 800P of the first doping type extends inward from the second surface of the substrate 100N into the substrate 100N;
  • a buffer zone 700N of the second doping type is formed on the side of the collector region 800P close to the body region 300P, and,
  • the hydrogen-doped region 900H is formed on the side of the buffer zone 700N close to the body region 300P, and the hydrogen-doped region 900H includes a plurality of hydrogen-doped subregions arranged in sequence away from the buffer zone , the ion concentration peaks of the plurality of hydrogen-doped subregions decrease sequentially in the direction away from the buffer zone. That is, the hydrogen-doped sub-region closest to the second surface of the substrate 100N among the plurality of hydrogen-doped sub-regions has the highest ion concentration peak.
  • the temperature of the substrate surface is generally the highest, that is, the temperature inside the substrate is usually lower than the temperature of the substrate surface.
  • the temperature of the substrate surface is generally the highest, that is, the temperature inside the substrate is usually lower than the temperature of the substrate surface.
  • the preparation step of the hydrogen-doped region is creatively adjusted to be after the preparation step of the buffer zone, so as to avoid the adverse effect of the preparation process of the buffer zone on the hydrogen-doped region, and improve the efficiency of the buffer zone.
  • the control accuracy of the ion concentration distribution in the formed hydrogen doped region can further prepare a plurality of hydrogen doped subregions with the peak hydrogen ion concentration decreasing in turn in the direction away from the buffer zone, and improve the stability of the prepared device.

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Abstract

Provided is an insulated gate bipolar transistor and a formation method therefor. In the formation method, a hydrogen doped region is formed after forming a collector region of a first doping type and a buffer region of a second doping type, and thereby the hydrogen doped region being affected by a processing technique of another doping region can be prevented, improvement of control precision of a preparation technique of the hydrogen doping region is facilitated, and it is easier to form a plurality of hydrogen doped sub-regions having sequentially reduced ion concentration peaks along a direction away from a substrate surface. At this point, on the basis of the formed buffer region and the hydrogen doped region having a precisely controllable concentration distribution, a transistor device at turn-off can be made to achieve a highly efficient electric field stop, and performance of the transistor device is improved.

Description

绝缘栅双极型晶体管及其形成方法Insulated gate bipolar transistor and method of forming the same 技术领域technical field
本发明涉及半导体技术领域,特别涉及一种绝缘栅双极型晶体管及其形成方法。The present invention relates to the field of semiconductor technology, in particular to an insulated gate bipolar transistor and a method for forming the same.
背景技术Background technique
绝缘栅双极晶体管(IGBT,Insulated Gate Bipolar Transistor),其集MOSFET的栅极电压控制特性和双极型晶体管的低导通电阻特性于一身,改善了器件耐压和导通电阻相互牵制的情况,具有高电压、大电流、高频率、功率集成密度高、输入阻抗大、导通电阻小、开关损耗低等优点。在变频家电、工业控制、电动及混合动力汽车、新能源、智能电网等诸多领域获得了广泛的应用空间。Insulated Gate Bipolar Transistor (IGBT, Insulated Gate Bipolar Transistor), which combines the gate voltage control characteristics of MOSFET and the low on-resistance characteristics of bipolar transistors, which improves the mutual restraint between the device's withstand voltage and on-resistance , has the advantages of high voltage, high current, high frequency, high power integration density, large input impedance, small on-resistance, and low switching loss. It has been widely used in many fields such as inverter home appliances, industrial control, electric and hybrid vehicles, new energy, and smart grids.
通常而言,随着绝缘栅双极型晶体管其基底厚度(即,漂移区的厚度)的增加,往往会导致器件的关断电压也越大、关断时间较长。为此,一种场截止型IGBT器件被提出,该场截止型IGBT器件是通过在集电极区与漂移区之间设置N型缓冲区,以用于阻挡电场,从而可以在相同的阻断电压下压缩漂移区的厚度,进而可以降低正向导通压降和关断时间。然而,目前的场截止型IGBT器件其性能仍然不够稳定,亟需进一步优化。Generally speaking, with the increase of the substrate thickness (ie, the thickness of the drift region) of the insulated gate bipolar transistor, the turn-off voltage of the device tends to be larger and the turn-off time is longer. To this end, a field-stop IGBT device is proposed. The field-stop IGBT device is used to block the electric field by arranging an N-type buffer between the collector region and the drift region, so that the same blocking voltage can be achieved. The thickness of the lower compression drift region, which in turn can reduce the forward voltage drop and turn-off time. However, the performance of the current field-stop IGBT devices is still not stable enough, and further optimization is urgently needed.
发明内容SUMMARY OF THE INVENTION
本发明的目的在于提供一种绝缘栅双极型晶体管的形成方法,以解决现有的形成方法难以制备出分布稳定的氢掺杂区,有利于提高所形成的晶体管器件的性能稳定性。The purpose of the present invention is to provide a method for forming an insulated gate bipolar transistor, so as to solve the difficulty in preparing a hydrogen doped region with stable distribution by the existing forming method, which is beneficial to improve the performance stability of the formed transistor device.
为此,本发明提供了一种绝缘栅双极型晶体管的形成方法,包括:To this end, the present invention provides a method for forming an insulated gate bipolar transistor, comprising:
提供衬底,所述衬底具有相对的第一表面和第二表面,以及在所述衬底对应于第一表面的部分中形成有栅极导电层、第一掺杂类型的体区和第二掺杂类型的发射极区;A substrate is provided, the substrate has opposing first and second surfaces, and a gate conductive layer, a body region of a first doping type, and a second surface are formed in a portion of the substrate corresponding to the first surface Two doping types of emitter regions;
对所述衬底的第二表面执行离子注入工艺和退火工艺,以形成第二掺杂 类型的缓冲区和第一掺杂类型的集电极区,所述集电极区从所述衬底的第二表面向内扩展至所述衬底中,所述缓冲区位于所述集电极区靠近所述体区的一侧;以及,An ion implantation process and an annealing process are performed on the second surface of the substrate to form a buffer region of the second doping type and a collector region of the first doping type, the collector region extending from the second surface of the substrate. Two surfaces extend inwardly into the substrate, the buffer zone is located on the side of the collector region proximate the body region; and,
对所述衬底的第二表面执行离子注入工艺和热退火工艺,以形成氢掺杂区,所述氢掺杂区位于所述缓冲区靠近所述体区的一侧,其中所述氢掺杂区包括往远离所述缓冲区的方向依次排布的多个氢掺杂分区,所述多个氢掺杂分区的离子浓度峰值往远离所述缓冲区的方向依次降低。An ion implantation process and a thermal annealing process are performed on the second surface of the substrate to form a hydrogen-doped region, the hydrogen-doped region is located on a side of the buffer zone close to the body region, wherein the hydrogen-doped region The impurity region includes a plurality of hydrogen-doped subregions that are sequentially arranged in a direction away from the buffer zone, and ion concentration peaks of the plurality of hydrogen-doped subregions are sequentially decreased in a direction away from the buffer zone.
可选的,所述缓冲区的形成方法包括:依次执行至少两道离子注入步骤,以及执行退火工艺,以形成至少两层缓冲分区,所述至少两层缓冲分区往远离所述集电极区的方向依次排布;以及,所述氢掺杂区的形成方法包括:依次执行多道离子注入步骤,以形成所述多层氢掺杂分区,所述多层氢掺杂分区往远离所述缓冲区的方向依次排布。Optionally, the method for forming the buffer zone includes: sequentially performing at least two ion implantation steps, and performing an annealing process, to form at least two layers of buffer subregions, the at least two layers of buffer subregions being farther away from the collector region. The directions are arranged in sequence; and, the method for forming the hydrogen-doped region includes: performing multiple ion implantation steps in sequence to form the multi-layer hydrogen-doped subregion, and the multi-layer hydrogen-doped subregion is farther away from the buffer. The directions of the zones are arranged in order.
可选的,所述氢掺杂区中氢掺杂分区的数量大于所述缓冲区中缓冲分区的数量。Optionally, the number of hydrogen-doped sub-regions in the hydrogen-doped region is greater than the number of buffer sub-regions in the buffer zone.
可选的,在形成所述缓冲区的所述至少两道离子注入步骤中,随着离子注入能量的增加,离子注入剂量依次减小,以使所形成的至少两层缓冲分区的离子浓度峰值往远离所述集电极区的方向依次降低。Optionally, in the at least two ion implantation steps of forming the buffer zone, as the ion implantation energy increases, the ion implantation dose decreases sequentially, so as to make the ion concentration peak of the formed at least two buffer zones. It decreases sequentially in the direction away from the collector region.
可选的,在形成所述氢掺杂区的所述多道离子注入步骤中,随着离子注入能量的增加,离子注入剂量依次减小,以使所形成的多层氢掺杂分区的离子浓度峰值往远离所述缓冲区的方向依次降低。Optionally, in the multi-channel ion implantation step of forming the hydrogen doped region, as the ion implantation energy increases, the ion implantation dose is sequentially decreased, so that the ions of the formed multilayer hydrogen doped region are reduced. The concentration peaks decrease successively in the direction away from the buffer zone.
可选的,所述缓冲区包括两层缓冲分区,两层所述缓冲分区的离子浓度峰值均介于1E16atoms/cm 3~1E17atoms/cm 3之间,并且两层所述缓冲分区的宽度均为0.4μm~0.7μm。 Optionally, the buffer zone includes two layers of buffer zones, the peak ion concentrations of the buffer zones in the two layers are both between 1E16 atoms/cm 3 and 1E17 atoms/cm 3 , and the widths of the buffer zones in the two layers are both 1E16 atoms/cm 3 and 1E17 atoms/cm 3 0.4μm~0.7μm.
可选的,所述氢掺杂区包括四个氢掺杂分区,其中最靠近所述缓冲区的两个氢掺杂分区的离子浓度峰值均介于1E12atoms/cm 3~1E14atoms/cm 3之间,以及最远离所述缓冲区的两个氢掺杂分区的离子浓度峰值均介于1E12atoms/cm 3~1E13atoms/cm 3之间,并且所述四个氢掺杂分区的宽度均为6μm~8μm。 Optionally, the hydrogen-doped region includes four hydrogen-doped subregions, wherein the peak ion concentrations of the two hydrogen-doped subregions closest to the buffer zone are both between 1E12 atoms/cm 3 to 1E14 atoms/cm 3 , and the ion concentration peaks of the two hydrogen-doped partitions farthest from the buffer zone are all between 1E12 atoms/cm 3 and 1E13 atoms/cm 3 , and the widths of the four hydrogen-doped partitions are all 6 μm to 8 μm .
可选的,所述缓冲区中的掺杂离子包括磷,以及在形成所述缓冲区的退 火工艺中采用激光退火工艺,并使退火温度大于等于600℃。Optionally, the doping ions in the buffer zone include phosphorus, and a laser annealing process is used in the annealing process for forming the buffer zone, and the annealing temperature is set to be greater than or equal to 600°C.
可选的,在形成所述氢掺杂区的热退火工艺中其退火温度为350℃~450℃。Optionally, in the thermal annealing process for forming the hydrogen doped region, the annealing temperature is 350°C to 450°C.
本发明还提供了一种绝缘栅双极型晶体管,包括:The present invention also provides an insulated gate bipolar transistor, comprising:
衬底,所述衬底具有相对的第一表面和第二表面,以及在所述衬底对应于第一表面的部分中形成有栅极导电层、第一掺杂类型的体区和第二掺杂类型的发射极区;a substrate having opposing first and second surfaces, and having a gate conductive layer, a body region of a first doping type, and a second formed in a portion of the substrate corresponding to the first surface Doping type of emitter region;
第一掺杂类型的集电极区,由所述衬底的第二表面向内扩展至所述衬底中;a collector region of the first doping type extending inwardly into the substrate from the second surface of the substrate;
第二掺杂类型的缓冲区,形成在所述集电极区靠近所述体区的一侧,以及,A buffer area of a second doping type is formed on the side of the collector region adjacent to the body region, and,
氢掺杂区,形成在所述缓冲区靠近所述体区的一侧,并且所述氢掺杂区包括往远离所述缓冲区的方向依次排布的多个氢掺杂分区,所述多个氢掺杂分区的离子浓度峰值往远离所述缓冲区的方向依次降低。A hydrogen-doped region is formed on a side of the buffer zone close to the body region, and the hydrogen-doped region includes a plurality of hydrogen-doped subregions arranged in sequence in a direction away from the buffer zone, the multiple The ion concentration peaks of each of the hydrogen-doped subregions decrease sequentially in the direction away from the buffer zone.
可选的,所述氢掺杂区的厚度大于所述缓冲区的厚度。Optionally, the thickness of the hydrogen doped region is greater than the thickness of the buffer zone.
可选的,所述缓冲区包括往远离所述集电极区依次排布的至少两个缓冲分区,以及所述氢掺杂区中氢掺杂分区的数量大于所述缓冲区中缓冲分区的数量。Optionally, the buffer zone includes at least two buffer zones arranged in sequence away from the collector region, and the number of hydrogen-doped zones in the hydrogen-doped zone is greater than the number of buffer zones in the buffer zone .
可选的,在所述缓冲区中,沿着远离所述集电极区的方向所述至少两个缓冲分区的离子浓度峰值依次降低。Optionally, in the buffer zone, the ion concentration peaks of the at least two buffer zones in a direction away from the collector zone decrease sequentially.
可选的,所述缓冲区包括两层缓冲分区,两层所述缓冲分区的离子浓度峰值均介于1E16atoms/cm 3~1E17atoms/cm 3之间,并且两层所述缓冲分区的宽度均为0.4μm~0.7μm。 Optionally, the buffer zone includes two layers of buffer zones, the peak ion concentrations of the buffer zones in the two layers are both between 1E16 atoms/cm 3 and 1E17 atoms/cm 3 , and the widths of the buffer zones in the two layers are both 1E16 atoms/cm 3 and 1E17 atoms/cm 3 0.4μm~0.7μm.
可选的,所述氢掺杂区包括四个氢掺杂分区,其中最靠近所述缓冲区的两个氢掺杂分区的离子浓度峰值均介于1E12atoms/cm 3~1E14atoms/cm 3之间,以及最远离所述缓冲区的两个氢掺杂分区的离子浓度峰值均介于1E12atoms/cm 3~1E13atoms/cm 3之间,并且所述四个氢掺杂分区的宽度均为6μm~8μm。 Optionally, the hydrogen-doped region includes four hydrogen-doped subregions, wherein the peak ion concentrations of the two hydrogen-doped subregions closest to the buffer zone are both between 1E12 atoms/cm 3 to 1E14 atoms/cm 3 , and the ion concentration peaks of the two hydrogen-doped partitions farthest from the buffer zone are all between 1E12 atoms/cm 3 and 1E13 atoms/cm 3 , and the widths of the four hydrogen-doped partitions are all 6 μm to 8 μm .
可选的,所述氢掺杂区中具有最大离子浓度峰值的氢掺杂分区邻接所述 缓冲区中具有最小离子浓度峰值的缓冲分区,并且所述具有最大离子浓度峰值的氢掺杂分区的离子浓度峰值仍小于所述具有最小离子浓度峰值的缓冲分区的离子浓度峰值。Optionally, the hydrogen-doped subregion with the largest ion concentration peak in the hydrogen-doped region is adjacent to the buffer subregion with the smallest ion concentration peak in the buffer zone, and the hydrogen-doped subregion with the largest ion concentration peak is The peak ion concentration is still smaller than the peak ion concentration of the buffer partition with the smallest peak ion concentration.
在本发明提供的绝缘栅双极型晶体管的形成方法中,是在形成第二掺杂类型的缓冲区之后,再制备氢掺杂区,如此,即可避免所形成的氢掺杂区受到缓冲区的制备工艺的影响。可见,与先制备氢掺杂区再形成缓冲区相比,本发明提供的方法,有效避免了氢掺杂区中的氢在缓冲区的退火工艺中被复合而导致氢掺杂区的离子浓度分布不稳定而无法精确控制的问题。即,根据本发明提供的方法,可以实现对氢掺杂区中的各个氢掺杂分区的浓度分布的有效控制,进而可以制备出离子浓度峰值往远离缓冲区的方向依次降低的多个氢掺杂分区,有利于提高器件的性能,例如,可以实现器件在关断时集电极和发射极之间的电压变化(dV/dt)更为平缓。In the method for forming an insulated gate bipolar transistor provided by the present invention, the hydrogen doped region is prepared after the buffer zone of the second doping type is formed, so that the formed hydrogen doped region can be prevented from being buffered The influence of the preparation process of the area. It can be seen that, compared with first preparing the hydrogen-doped region and then forming the buffer zone, the method provided by the present invention effectively avoids that the hydrogen in the hydrogen-doped region is recombined during the annealing process of the buffer zone, resulting in the ion concentration of the hydrogen-doped region. Problems where the distribution is unstable and cannot be precisely controlled. That is, according to the method provided by the present invention, it is possible to effectively control the concentration distribution of each hydrogen-doped sub-area in the hydrogen-doped region, and further, a plurality of hydrogen-doped regions with the peak ion concentration decreasing in turn in the direction away from the buffer zone can be prepared. The stray partition is beneficial to improve the performance of the device. For example, the voltage change (dV/dt) between the collector and the emitter when the device is turned off can be more gentle.
附图说明Description of drawings
图1是本发明一实施例中的绝缘栅双极型晶体管的形成方法的流程示意图;1 is a schematic flowchart of a method for forming an insulated gate bipolar transistor according to an embodiment of the present invention;
图2~图12是本发明一实施例中的绝缘栅双极型晶体管在其制备过程中的结构示意图;2 to 12 are schematic structural diagrams of an insulated gate bipolar transistor in an embodiment of the present invention during its fabrication;
图13是本发明一实施例中的绝缘栅双极型晶体管其部分掺杂区的浓度分布曲线。FIG. 13 is a concentration profile of a part of the doped region of the insulated gate bipolar transistor according to an embodiment of the present invention.
其中,附图标记如下:Among them, the reference numerals are as follows:
100N-衬底;100N-substrate;
200a-栅极沟槽;200a-gate trench;
210-栅极介质层;210-gate dielectric layer;
220-栅极导电层;220-gate conductive layer;
300P-体区;300P-body area;
400N-发射极区;400N-emitter region;
500-绝缘层;500-insulation layer;
600a-接触孔;600a-contact hole;
610P-重掺杂区;610P-heavy doped region;
620-接触电极;620 - Contact electrode;
621-金属扩散阻挡层;621 - metal diffusion barrier;
622-金属层;622 - metal layer;
630-电极引线层;630 - electrode lead layer;
700N-缓冲区;700N-buffer;
710N-第一缓冲分区;710N - the first buffer partition;
720N-第二缓冲分区;720N - the second buffer partition;
800P-集电极区;800P-collector area;
810-欧姆电极;810-ohm electrode;
900H-氢掺杂区;900H-Hydrogen doped region;
910H-第一氢掺杂分区;910H-the first hydrogen-doped partition;
920H-第二氢掺杂分区;920H-second hydrogen doping partition;
930H-第三氢掺杂分区;930H-the third hydrogen doped partition;
940H-第四氢掺杂分区;940H-the fourth hydrogen-doped partition;
A1-第一表面;A1 - the first surface;
A2-第二表面。A2 - Second surface.
具体实施方式Detailed ways
本发明的核心思路在于提供一种绝缘栅双极型晶体管的形成方法,该形成方法有利于提高对器件中的缓冲层的制备精度。The core idea of the present invention is to provide a method for forming an insulated gate bipolar transistor, which is beneficial to improve the preparation precision of the buffer layer in the device.
具体参考图1所示,所述绝缘栅双极型晶体管的形成方法可包括:Referring specifically to FIG. 1 , the method for forming the insulated gate bipolar transistor may include:
步骤S100,提供衬底,所述衬底具有相对的第一表面和第二表面,以及在所述衬底对应于第一表面的部分中形成有栅极导电层、第一掺杂类型的体区和第二掺杂类型的发射极区;Step S100, a substrate is provided, the substrate has a first surface and a second surface opposite to each other, and a gate conductive layer, a body of a first doping type are formed in a portion of the substrate corresponding to the first surface region and an emitter region of the second doping type;
步骤S200,对所述衬底的第二表面执行离子注入工艺和退火工艺,以形成第二掺杂类型的缓冲区和第一掺杂类型的集电极区;Step S200, performing an ion implantation process and an annealing process on the second surface of the substrate to form a buffer region of the second doping type and a collector region of the first doping type;
步骤S300,对所述衬底的第二表面执行离子注入工艺,以形成氢掺杂的氢掺杂区,所述氢掺杂区位于所述缓冲区靠近所述体区的一侧,其中所述氢掺 杂区包括往远离所述缓冲区的方向依次排布的多个氢掺杂分区,所述多个氢掺杂分区的离子浓度峰值往远离所述缓冲区的方向依次降低。Step S300, performing an ion implantation process on the second surface of the substrate to form a hydrogen-doped hydrogen-doped region, where the hydrogen-doped region is located on a side of the buffer zone close to the body region, wherein the The hydrogen-doped region includes a plurality of hydrogen-doped subregions that are sequentially arranged in a direction away from the buffer zone, and ion concentration peaks of the plurality of hydrogen-doped subregions are sequentially decreased in a direction away from the buffer zone.
即,本发明提供的形成方法中,是在形成第二掺杂类型的缓冲区和第一掺杂类型的集电极区之后,再执行离子注入工艺以形成具有多个氢掺杂分区的氢掺杂区。此时,即可避免所形成的氢掺杂区受到缓冲区和集电极区的制备工艺的影响,防止氢掺杂区中注入的氢离子在高温下被复合,保障了氢掺杂区中的离子浓度分布的稳定性,有利于形成离子浓度峰值呈梯度变化的多个氢掺杂分区。That is, in the formation method provided by the present invention, after forming the buffer region of the second doping type and the collector region of the first doping type, an ion implantation process is performed to form a hydrogen doped region having a plurality of hydrogen doping subregions Miscellaneous area. At this time, the formation of the hydrogen doped region can be prevented from being affected by the preparation process of the buffer region and the collector region, and the hydrogen ions implanted in the hydrogen doped region can be prevented from being recombined at high temperature, so as to ensure the safety of the hydrogen doped region. The stability of the ion concentration distribution is beneficial to the formation of a plurality of hydrogen doping partitions with a gradient in the peak value of the ion concentration.
以下结合附图和具体实施例对本发明提出的绝缘栅双极型晶体管及其形成方法作进一步详细说明。根据下面说明,本发明的优点和特征将更清楚。需说明的是,附图均采用非常简化的形式且均使用非精准的比例,仅用以方便、明晰地辅助说明本发明实施例的目的。The insulated gate bipolar transistor and its formation method proposed by the present invention will be further described in detail below with reference to the accompanying drawings and specific embodiments. The advantages and features of the present invention will become more apparent from the following description. It should be noted that, the accompanying drawings are all in a very simplified form and in inaccurate scales, and are only used to facilitate and clearly assist the purpose of explaining the embodiments of the present invention.
在步骤S100中,具体参考图2~图12所示,提供衬底100N,所述衬底100N具有相对的第一表面A1和第二表面A2,以及在所述衬底100N对应于第一表面的部分中形成有栅极导电层220、第一掺杂类型的体区300P和第二掺杂类型的发射极区400N。In step S100 , referring specifically to FIGS. 2 to 12 , a substrate 100N is provided, the substrate 100N has a first surface A1 and a second surface A2 opposite to each other, and the substrate 100N corresponds to the first surface A gate conductive layer 220 , a body region 300P of a first doping type and an emitter region 400N of a second doping type are formed in the portion of .
其中,所述衬底100N例如为第二掺杂类型的衬底100N,并可以由部分衬底100N构成绝缘栅双极型晶体管其第二掺杂类型的漂移区。本实施例中,所述第二掺杂类型为N型,即所述衬底100N为N型衬底,并用于构成N型漂移区。The substrate 100N is, for example, a substrate 100N of the second doping type, and a part of the substrate 100N may constitute the drift region of the second doping type of the insulated gate bipolar transistor. In this embodiment, the second doping type is N-type, that is, the substrate 100N is an N-type substrate and is used to form an N-type drift region.
以及,所述栅极导电层220、所述体区300P和所述发射极区400N的制备步骤可以根据实际情况调整。例如,可以优先在所述衬底100N中形成栅极导电层220,之后再依次制备所述体区300P和所述发射极区400N;或者,也可以优先形成所述体区300P,之后再制备所述栅极导电层220和所述发射极区400N等。本实施例中,以优先形成所述栅极导电层220为例进行解释说明。And, the preparation steps of the gate conductive layer 220 , the body region 300P and the emitter region 400N can be adjusted according to actual conditions. For example, the gate conductive layer 220 may be preferentially formed in the substrate 100N, and then the body region 300P and the emitter region 400N may be sequentially prepared; or, the body region 300P may be preferentially formed and then prepared The gate conductive layer 220 and the emitter region 400N, etc. In this embodiment, the gate conductive layer 220 is preferentially formed as an example for explanation.
继续参考图3所示,所述栅极导电层220形成在所述衬底100N内的栅极沟槽200a中。具体的,通过对所述衬底100N的第一表面A1进行刻蚀,以形成从所述衬底100N的第一表面A1向内延伸的栅极沟槽200a,其中,所述栅极沟槽200a的沟槽深度例如为1μm~6μm,以及所述栅极沟槽200a的侧壁可 以为略微倾斜的倾斜侧壁,所述栅极沟槽200a的倾斜侧壁相对于水平方向的锐角夹角α例如为85°~90°。Continuing to refer to FIG. 3 , the gate conductive layer 220 is formed in the gate trench 200a in the substrate 100N. Specifically, by etching the first surface A1 of the substrate 100N, a gate trench 200a extending inward from the first surface A1 of the substrate 100N is formed, wherein the gate trench The trench depth of 200a is, for example, 1 μm˜6 μm, and the sidewalls of the gate trenches 200a may be slightly inclined inclined sidewalls, and the inclined sidewalls of the gate trenches 200a have an acute angle with respect to the horizontal direction. α is, for example, 85° to 90°.
进一步的,在所述栅极沟槽200a中形成所述栅极导电层220之前,还包括:在所述栅极沟槽200a的底壁和侧壁上形成栅极介质层210。所述栅极介质层210可覆盖所述栅极沟槽200a的整个沟槽侧壁,以使所述栅极介质层210的顶部不低于所述栅极沟槽200a的顶部。Further, before forming the gate conductive layer 220 in the gate trench 200a, the method further includes: forming a gate dielectric layer 210 on the bottom wall and sidewall of the gate trench 200a. The gate dielectric layer 210 can cover the entire trench sidewall of the gate trench 200a, so that the top of the gate dielectric layer 210 is not lower than the top of the gate trench 200a.
在形成所述栅极介质层210后,即填充所述栅极导电层220在所述栅极沟槽200a中。具体的,所述栅极导电层220的形成方法包括:在所述栅极沟槽200a中填充栅极导电材料层,并回刻蚀所述栅极导电材料层,从而形成顶表面低于衬底100N的第一表面的栅极导电层220。其中,所述栅极导电层220的顶表面相对于所述衬底的第一表面A1的高度差例如小于等于1μm。After the gate dielectric layer 210 is formed, the gate conductive layer 220 is filled in the gate trench 200a. Specifically, the method for forming the gate conductive layer 220 includes: filling the gate conductive material layer in the gate trench 200a, and etching back the gate conductive material layer, so that the top surface is lower than the lining material layer. The gate conductive layer 220 on the first surface of the bottom 100N. Wherein, the height difference between the top surface of the gate conductive layer 220 and the first surface A1 of the substrate is, for example, less than or equal to 1 μm.
本实施例中,所述栅极介质层210覆盖所述栅极沟槽的整个沟槽侧壁,因此在执行回刻蚀工艺以降低所述栅极导电层220的顶表面时,即可在所述栅极介质层210的保护下,避免对高于栅极导电层220的沟槽侧壁造成损伤。In this embodiment, the gate dielectric layer 210 covers the entire trench sidewall of the gate trench. Therefore, when an etch-back process is performed to reduce the top surface of the gate conductive layer 220, the Under the protection of the gate dielectric layer 210 , damage to the sidewall of the trench higher than the gate conductive layer 220 is avoided.
此外,在所述衬底100N上可以形成有一个或多个栅极导电层220。本实施例中,即在所述衬底100N上形成有至少两个栅极导电层220,以用于构成至少两个晶体管元胞。In addition, one or more gate conductive layers 220 may be formed on the substrate 100N. In this embodiment, at least two gate conductive layers 220 are formed on the substrate 100N to form at least two transistor cells.
继续参考图4和图5所示,对所述衬底100N的第一表面A1执行离子注入工艺和退火工艺,以依次形成第一掺杂类型的体区300P和第二掺杂类型的发射极区400N。本实施例中,所述体区300P为P型掺杂区,所述发射极区400N为N型掺杂区。Continuing to refer to FIG. 4 and FIG. 5 , an ion implantation process and an annealing process are performed on the first surface A1 of the substrate 100N to sequentially form the body region 300P of the first doping type and the emitter of the second doping type District 400N. In this embodiment, the body region 300P is a P-type doped region, and the emitter region 400N is an N-type doped region.
重点参考图4所示,所述体区300P的形成方法包括:执行离子注入工艺和退火工艺,以形成扩展至衬底中的体区300P,并且所述体区300P的底部边界扩展至低于所述栅极导电层220的顶部的深度位置,以使所述体区300P至少部分和所述栅极导电层220横向空间重叠。本实施例中,形成所述体区300P的退火工艺的退火温度例如为1000℃~1200℃,以及所述体区300P在衬底100N中的扩展深度例如为2μm~4μm,保证了所述体区300P能够和所述栅极导电层220横向空间重叠。4 , the method for forming the body region 300P includes: performing an ion implantation process and an annealing process to form a body region 300P extending into the substrate, and the bottom boundary of the body region 300P is extended to be lower than The depth position of the top of the gate conductive layer 220 is such that the body region 300P at least partially overlaps the gate conductive layer 220 in a lateral space. In this embodiment, the annealing temperature of the annealing process for forming the body region 300P is, for example, 1000° C.˜1200° C., and the extension depth of the body region 300P in the substrate 100N is, for example, 2 μm˜4 μm, which ensures that the body The region 300P can laterally overlap with the gate conductive layer 220 .
接着参考图5所示,同样可以利用离子注入工艺和退火工艺,形成所述 发射极区400N,以使所述发射极区400N从衬底的第一表面A1向内扩展至所述体区300P。其中,所述发射极区400N的底部边界也扩展至低于所述栅极导电层220的顶部的深度位置,并且所述发射极区400N的底部边界还高于所述体区300P的底部边界,以利用所述体区300P中位于所述发射极区400N下方的部分构成导电沟道区。本实施例中,所述发射极区400N在衬底100N中的扩展深度例如为0.2μm~1μm。Next, as shown in FIG. 5 , the emitter region 400N can also be formed by an ion implantation process and an annealing process, so that the emitter region 400N extends inward from the first surface A1 of the substrate to the body region 300P . The bottom boundary of the emitter region 400N also extends to a depth lower than the top of the gate conductive layer 220 , and the bottom boundary of the emitter region 400N is also higher than the bottom boundary of the body region 300P , so as to utilize the portion of the body region 300P below the emitter region 400N to form a conductive channel region. In this embodiment, the extension depth of the emitter region 400N in the substrate 100N is, for example, 0.2 μm˜1 μm.
进一步的,在形成所述发射极区400N之后,还包括:在所述衬底100N的第一表面A1上形成接触电极,以用于电性引出所述发射极区400N和体区300P。Further, after forming the emitter region 400N, the method further includes: forming a contact electrode on the first surface A1 of the substrate 100N for electrically extracting the emitter region 400N and the body region 300P.
具体参考图6~图8所示,所述接触电极620的形成方法可包括如下步骤。Referring specifically to FIGS. 6 to 8 , the method for forming the contact electrode 620 may include the following steps.
第一步骤,具体参考图6所示,在所述衬底100N的第一表面上形成绝缘层500,所述绝缘层500还填充所述栅极沟槽高于栅极导电层220的空间,以利用所述绝缘层500覆盖所述栅极导电层220和所述发射极区400N。The first step, specifically referring to FIG. 6 , forms an insulating layer 500 on the first surface of the substrate 100N, and the insulating layer 500 also fills the space above the gate conductive layer 220 in the gate trench, The gate conductive layer 220 and the emitter region 400N are covered by the insulating layer 500 .
第二步骤,具体参考图7所示,在所述发射极区400N的上方刻蚀所述绝缘层500至衬底以依次暴露出所述发射极区400N和所述体区300P,并形成接触孔600a。所述接触孔600a即用于容纳所述接触电极620。The second step, specifically referring to FIG. 7 , is to etch the insulating layer 500 to the substrate above the emitter region 400N to sequentially expose the emitter region 400N and the body region 300P, and form contacts hole 600a. The contact hole 600 a is used to accommodate the contact electrode 620 .
本实施例中,依次刻蚀所述绝缘层500和所述衬底100N,以使所述接触孔600a贯穿所述发射极区400N,并延伸至所述体区300P中,如此,以利用后续形成在所述接触孔600a中的接触电极电性连接所述发射极区400N和所述体区300PIn this embodiment, the insulating layer 500 and the substrate 100N are sequentially etched, so that the contact hole 600a penetrates through the emitter region 400N and extends into the body region 300P. A contact electrode formed in the contact hole 600a electrically connects the emitter region 400N and the body region 300P
进一步的方案中,继续参考图7所示,在填充所述接触电极620至所述接触孔600a内之前,还包括:通过所述接触孔600a注入第一掺杂类型的掺杂离子,以在所述接触孔600a的底部形成重掺杂区610P。本实施例中,所述重掺杂区610P即为P型掺杂区,并且所述重掺杂区610P的掺杂浓度高于所述体区300P的掺杂浓度。In a further solution, as shown in FIG. 7 , before filling the contact electrode 620 into the contact hole 600a, the method further includes: implanting dopant ions of the first doping type through the contact hole 600a to A heavily doped region 610P is formed at the bottom of the contact hole 600a. In this embodiment, the heavily doped region 610P is a P-type doped region, and the doping concentration of the heavily doped region 610P is higher than that of the body region 300P.
需要说明的是,在不设置所述重掺杂区610P的情况下,则在器件的关断过程中,集电极区和发射极区之间的电压会瞬间抬升,从而容易导致由发射极区-体区和漂移区所构成的寄生NPN晶体管导通,产生擎住效应,进而会导致器件失效。为此,本实施例中,通过在接触孔600a的底部设置所述重掺杂 区610P(在后续形成接触电极之后,所述重掺杂区610P即设置在所述接触电极的底部),从而可以将如上所述的寄生NPN晶体管短路,改善器件的擎住效应。此外,通过设置所述重掺杂区610P,还可以有效降低所述接触电极和所述体区300P之间的接触电阻。It should be noted that, in the case where the heavily doped region 610P is not provided, the voltage between the collector region and the emitter region will rise instantaneously during the turn-off process of the device, which may easily lead to - The parasitic NPN transistor formed by the body region and the drift region is turned on, resulting in a hold-up effect, which will lead to device failure. To this end, in this embodiment, the heavily doped region 610P is provided at the bottom of the contact hole 600a (after the contact electrode is subsequently formed, the heavily doped region 610P is provided at the bottom of the contact electrode), thereby The parasitic NPN transistors described above can be shorted to improve the hold-up effect of the device. In addition, by arranging the heavily doped region 610P, the contact resistance between the contact electrode and the body region 300P can also be effectively reduced.
第三步骤,具体参考图8所示,在所述接触孔600a中形成接触电极620。In the third step, as shown in FIG. 8 , a contact electrode 620 is formed in the contact hole 600a.
其中,所述接触电极620的形成方法包括:在所述接触孔600a的底壁和侧壁上形成金属扩散阻挡层621,以及在所述接触孔600a中填充金属层622,以构成所述接触电极620。具体的,可以利用平坦化工艺,使所述接触电极620的顶表面和所述绝缘层500的顶表面齐平。The method for forming the contact electrode 620 includes: forming a metal diffusion barrier layer 621 on the bottom wall and sidewall of the contact hole 600a, and filling the contact hole 600a with a metal layer 622 to form the contact electrode 620. Specifically, a planarization process may be used to make the top surface of the contact electrode 620 flush with the top surface of the insulating layer 500 .
本实施例中,通过在所述金属层622的外围围设所述金属扩散阻挡层621,以阻挡所述金属层622中的金属扩散至衬底100N中,改善器件的漏电流现象。其中,所述金属扩散阻挡层621的材料例如包括钛(Ti)和氮化钛(TiN)中的至少一种,所述金属扩散阻挡层621的厚度例如为500A~2000A。以及,所述金属层622的材料例如包括钨。In this embodiment, the metal diffusion barrier layer 621 is surrounded on the periphery of the metal layer 622 to prevent the metal in the metal layer 622 from diffusing into the substrate 100N, thereby improving the leakage current phenomenon of the device. The material of the metal diffusion barrier layer 621 includes, for example, at least one of titanium (Ti) and titanium nitride (TiN), and the thickness of the metal diffusion barrier layer 621 is, for example, 500A˜2000A. And, the material of the metal layer 622 includes, for example, tungsten.
可选的方案中,具体参考图9所示,在形成所述接触电极620之后,还包括:形成电极引线层630,以电性连接所述接触电极620。具体的,所述电极引线层630覆盖所述绝缘层500和所述接触电极620。其中,所述电极引线层630的材料例如包括铝、铜、铝硅合金或铝硅铜合金等。In an optional solution, specifically referring to FIG. 9 , after forming the contact electrodes 620 , the method further includes: forming an electrode lead layer 630 to electrically connect the contact electrodes 620 . Specifically, the electrode lead layer 630 covers the insulating layer 500 and the contact electrode 620 . The material of the electrode lead layer 630 includes, for example, aluminum, copper, aluminum-silicon alloy, or aluminum-silicon-copper alloy.
如上所述,本实施例的衬底100N中形成有至少两个栅极导电层220,相应的在每一栅极导电层220的侧边均形成有所述体区300P和所述发射极区400N。此时,即对应形成有至少两个接触电极620,以一一对应连接相应的体区300P和发射极区400N,以及所述至少两个接触电极620可均电性连接至所述电极引线层630。As described above, at least two gate conductive layers 220 are formed in the substrate 100N of this embodiment, and the body region 300P and the emitter region are correspondingly formed on the sides of each gate conductive layer 220 400N. At this time, at least two contact electrodes 620 are formed correspondingly to connect the corresponding body regions 300P and the emitter regions 400N in a one-to-one correspondence, and the at least two contact electrodes 620 can be electrically connected to the electrode lead layer. 630.
在步骤S200中,具体参考图10所示,对所述衬底100N的第二表面A2执行离子注入工艺和退火工艺,以形成第二掺杂类型的缓冲区700N和第一掺杂类型的集电极区800P。本实施例中,所述缓冲区700N为N型掺杂区,所述集电极区800P为P型掺杂区。In step S200, referring specifically to FIG. 10, an ion implantation process and an annealing process are performed on the second surface A2 of the substrate 100N to form a buffer zone 700N of the second doping type and a set of the first doping type Electrode area 800P. In this embodiment, the buffer region 700N is an N-type doped region, and the collector region 800P is a P-type doped region.
其中,所述缓冲区700N位于所述集电极区800P靠近所述体区300P的一侧,并且所述缓冲区700N包括往远离所述集电极区800P依次排布的至少两 个缓冲分区(本实施例中,包括第一缓冲分区710N和第二缓冲分区720N)。The buffer area 700N is located on the side of the collector area 800P close to the body area 300P, and the buffer area 700N includes at least two buffer areas arranged in sequence away from the collector area 800P (this In an embodiment, a first buffer partition 710N and a second buffer partition 720N are included.
具体的方案中,在对所述衬底100N的第二表面A2执行离子注入工艺之前,还包括:从所述衬底100N的第二表面减薄所述衬底100N,以使减薄后的衬底100N的厚度满足预定要求。In a specific solution, before the ion implantation process is performed on the second surface A2 of the substrate 100N, the method further includes: thinning the substrate 100N from the second surface of the substrate 100N, so that the thinned The thickness of the substrate 100N satisfies predetermined requirements.
应当认识到,本实施例提供的形成方法,有利于进一步降低器件的漂移区的厚度,因此在减薄所述衬底100N时,即相应的可以将所述衬底100N降低至更薄的厚度,以利于提高器件的发射效率。例如,减薄后的衬底100N的厚度为40μm~150μm。It should be recognized that the formation method provided in this embodiment is conducive to further reducing the thickness of the drift region of the device, so when the substrate 100N is thinned, the substrate 100N can be correspondingly reduced to a thinner thickness , in order to improve the emission efficiency of the device. For example, the thickness of the thinned substrate 100N is 40 μm˜150 μm.
以及,在减薄所述衬底100N后,即可对减薄后的衬底100N执行离子注入工艺,以形成所述缓冲区700N和所述集电极区800P。可选的方案中,可以先利用离子注入工艺形成缓冲区700N,并再次执行离子注入工艺形成集电极区800P;或者,在其他的方案中,也可以先利用离子注入工艺形成集电极区800P,并再次执行离子注入工艺以形成缓冲区700N。And, after the substrate 100N is thinned, an ion implantation process can be performed on the thinned substrate 100N to form the buffer region 700N and the collector region 800P. In an optional solution, the buffer region 700N can be formed by the ion implantation process first, and then the collector region 800P can be formed by performing the ion implantation process again; And the ion implantation process is performed again to form the buffer zone 700N.
具体可结合图10和图12所示,在制备所述缓冲区700N时,可通过依次执行至少两道离子注入步骤以及执行退火工艺,以在所述衬底100N中形成至少两层第二掺杂类型的缓冲分区(本实施例中,包括:第一缓冲分区710N和第二缓冲分区720N),并使至少两层缓冲分区沿着衬底100N的厚度方向依次排布,以及所述缓冲区700N中的至少两层缓冲分区的离子浓度峰值往远离衬底的第二表面A2的方向依次降低。即,本实施例中,所述第一缓冲分区710N的离子浓度峰值低于所述第二缓冲分区720N的离子浓度峰值。Specifically, as shown in FIG. 10 and FIG. 12 , when preparing the buffer zone 700N, at least two ion implantation steps and an annealing process can be performed in sequence to form at least two layers of the second dopant in the substrate 100N. Miscellaneous buffer partitions (in this embodiment, including: a first buffer partition 710N and a second buffer partition 720N), and at least two layers of buffer partitions are sequentially arranged along the thickness direction of the substrate 100N, and the buffer partitions The ion concentration peaks of the at least two-layer buffer partitions in 700N successively decrease in the direction away from the second surface A2 of the substrate. That is, in this embodiment, the peak value of the ion concentration of the first buffer zone 710N is lower than the peak value of the ion concentration of the second buffer zone 720N.
其中,可通过调整离子注入步骤的离子注入能量,以进一步调整注入至衬底100N中的各个缓冲分区的深度位置,并通过调整离子注入步骤的离子注入剂量,以进一步调整所形成的各个缓冲分区的离子浓度。基于此,本实施例中,在形成所述缓冲区700N时所执行的至少两道离子注入步骤,即随着离子注入能量的增加,离子注入剂量依次减小,以使所形成的至少两个缓冲分区的离子浓度峰值依次降低。The ion implantation energy of the ion implantation step can be adjusted to further adjust the depth position of each buffer subregion implanted into the substrate 100N, and the ion implantation dose of the ion implantation step can be adjusted to further adjust the formed buffer subregions. ion concentration. Based on this, in this embodiment, in the at least two ion implantation steps performed when the buffer zone 700N is formed, that is, as the ion implantation energy increases, the ion implantation dose decreases sequentially, so that the formed at least two ion implantation steps are The ion concentration peaks in the buffer zone decreased sequentially.
本实施例中,以依次执行两道离子注入步骤分别形成两道缓冲分区为例进行解释说明。In this embodiment, two buffer partitions are formed by sequentially performing two ion implantation steps as an example for explanation.
首先,执行第一道离子注入步骤,以在所述衬底100N的较深位置中形成 第一缓冲分区710N。其中,所述第一道离子注入步骤的离子注入能量例如为1Me~2Me,并可使所述第一缓冲分区710N的最深边界抵达至距离衬底的第二表面1.6μm~1.9μm的深度位置,以及所述第一缓冲分区710N沿着衬底的厚度方向上的宽度尺寸例如为0.4μm~0.7μm。进一步的,所述第一缓冲分区710N的离子浓度分布呈现为高斯分布,所述第一缓冲分区710的离子浓度峰值例如为1E16atoms/cm 3~1E17atoms/cm 3First, a first ion implantation step is performed to form a first buffer region 710N in a deeper position of the substrate 100N. Wherein, the ion implantation energy of the first ion implantation step is, for example, 1Me˜2Me, and the deepest boundary of the first buffer subregion 710N can reach a depth position of 1.6 μm˜1.9 μm from the second surface of the substrate , and the width dimension of the first buffer subregion 710N along the thickness direction of the substrate is, for example, 0.4 μm˜0.7 μm. Further, the ion concentration distribution of the first buffer subregion 710N presents a Gaussian distribution, and the ion concentration peak value of the first buffer subregion 710 is, for example, 1E16 atoms/cm 3 to 1E17 atoms/cm 3 .
接着,执行第二道离子注入步骤,以在所述衬底100N的较浅位置中形成第二缓冲分区720N。其中,所述第二道离子注入步骤的离子注入能量低于所述第一道离子注入步骤的离子注入能量。本实施例中,所述第二道离子注入步骤的离子注入能量例如为200kev~700kev,并使所形成的第二缓冲分区720N的最深边界至所述衬底的第二表面的距离为0.3μm~1.0μm,以及所述第二缓冲分区720N的宽度尺寸可以和所述第一缓冲分区710N的宽度尺寸相同或大致相同。同样的,所述第二缓冲分区720中的离子浓度分布也呈现为高斯分布,具体的,所述第二缓冲分区720的离子浓度峰值例如介于1E16atoms/cm 3~1E17atoms/cm 3的这一范围内。 Next, a second ion implantation step is performed to form a second buffer region 720N in a shallower position of the substrate 100N. Wherein, the ion implantation energy of the second ion implantation step is lower than the ion implantation energy of the first ion implantation step. In this embodiment, the ion implantation energy of the second ion implantation step is, for example, 200kev˜700kev, and the distance from the deepest boundary of the formed second buffer region 720N to the second surface of the substrate is 0.3 μm ~1.0 μm, and the width dimension of the second buffer region 720N may be the same as or approximately the same as the width dimension of the first buffer region 710N. Similarly, the ion concentration distribution in the second buffer zone 720 also presents a Gaussian distribution. Specifically, the ion concentration peak value of the second buffer zone 720 is, for example, between 1E16 atoms/cm 3 to 1E17 atoms/cm 3 . within the range.
需要说明的是,本实施例中,虽然第一缓冲分区710N和第二缓冲分区720N的离子浓度峰值均介于同一数值范围内,但仍可以在同一数值范围内调整两者的离子注入剂量,以使得第一缓冲分区710N的离子浓度峰值低于第二缓冲分区720N的离子浓度峰值。It should be noted that, in this embodiment, although the ion concentration peaks of the first buffer subregion 710N and the second buffer subregion 720N are both within the same numerical range, the ion implantation doses of the two can still be adjusted within the same numerical range, so that the peak value of the ion concentration of the first buffer zone 710N is lower than the peak value of the ion concentration of the second buffer zone 720N.
具体的实施例中,所述第一道离子注入步骤和所述第二道离子注入步骤例如均为磷离子注入、砷离子注入或锑离子注入,以形成N型的第一缓冲分区710N和第二缓冲分区720N。以及,在执行所述第一道离子注入步骤和所述第二道离子注入步骤时,可均以相对于衬底100N的第二表面A2轻度倾斜的角度执行离子注入,例如,可以以倾斜0°~7°的方向对所述衬底100N的第二表面进行离子注入。In a specific embodiment, the first ion implantation step and the second ion implantation step are, for example, phosphorus ion implantation, arsenic ion implantation or antimony ion implantation, so as to form the N-type first buffer region 710N and the second ion implantation. Two buffer partitions 720N. And, when the first ion implantation step and the second ion implantation step are performed, the ion implantation may be performed at a slightly inclined angle with respect to the second surface A2 of the substrate 100N, for example, the ion implantation may be performed at an inclined angle. Ion implantation is performed on the second surface of the substrate 100N in the direction of 0°˜7°.
进一步的,在执行如上所述的至少两道离子注入步骤之后,执行退火工艺,以激活所述缓冲区700N中的各个缓冲分区的注入离子。其中,针对N型离子的激活(例如,磷离子的激活),通常可采用激光退火工艺,以及其需要较高的退火温度,例如所述退火工艺的退火温度可大于等于600℃。Further, after performing the above-mentioned at least two ion implantation steps, an annealing process is performed to activate the implanted ions in each buffer region in the buffer region 700N. Wherein, for the activation of N-type ions (for example, activation of phosphorus ions), a laser annealing process is usually used, and a higher annealing temperature is required, for example, the annealing temperature of the annealing process can be greater than or equal to 600°C.
继续参考图10所示,在形成所述缓冲区700N之后或之前,也利用离子注入工艺和退火工艺,以形成第一掺杂类型的集电极区800P,所述集电极区800P从衬底100N的第二表面A2向内扩展至所述缓冲区700N,以使所述缓冲区700N和所述集电极区800P邻接。具体的,所述集电极区800P的厚度例如小于等于0.5μm,即所述集电极区800P从衬底100N的第二表面A2向内扩展的深度小于等于0.5μm。Continuing to refer to FIG. 10 , after or before the formation of the buffer zone 700N, an ion implantation process and an annealing process are also used to form a collector region 800P of a first doping type, the collector region 800P extending from the substrate 100N The second surface A2 of A2 extends inward to the buffer area 700N so that the buffer area 700N and the collector region 800P abut. Specifically, the thickness of the collector region 800P is, for example, less than or equal to 0.5 μm, that is, the depth of the inward extension of the collector region 800P from the second surface A2 of the substrate 100N is less than or equal to 0.5 μm.
本实施例中,形成所述集电极区800P的离子注入工艺具体为:硼离子的离子注入工艺,以形成P型的集电极区800P。以及,所述集电极区800P的离子掺杂浓度可以为1E16atoms/cm 3~1E18atoms/cm 3In this embodiment, the ion implantation process for forming the collector region 800P is specifically: an ion implantation process of boron ions to form the P-type collector region 800P. And, the ion doping concentration of the collector region 800P may be 1E16 atoms/cm 3 to 1E18 atoms/cm 3 .
在步骤S300中,具体参考图11所示,对所述衬底100N的第二表面执行离子注入工艺和退火工艺,以形成氢掺杂区900H,所述氢掺杂区900H位于所述缓冲区700N靠近所述体区300P的一侧。In step S300 , referring specifically to FIG. 11 , an ion implantation process and an annealing process are performed on the second surface of the substrate 100N to form a hydrogen-doped region 900H, and the hydrogen-doped region 900H is located in the buffer zone 700N is close to one side of the body region 300P.
需要说明的是,本实施例中,是在形成所述缓冲区700N和集电极区800P之后,形成所述氢掺杂区900H。如此,即可以有效避免在制备缓冲区700N和集电极区800P时的退火工艺对氢掺杂区900H造成影响。特别是,当所述缓冲区700N中的掺杂离子包括磷离子时,则通常需要较高的退火温度以激活磷离子,用于激活磷离子的退火温度例如高于600℃,在如此高温的环境中尤其容易导致衬底中的氢离子被复合。而本实施例中,通过将氢掺杂区900H的制备步骤调整至缓冲区700N的制备步骤之后,进而避免了氢掺杂区900H中的氢在高温下被复合而导致氢掺杂区900H中的离子掺杂浓度无法精确控制。It should be noted that, in this embodiment, the hydrogen-doped region 900H is formed after the buffer region 700N and the collector region 800P are formed. In this way, the annealing process during the preparation of the buffer region 700N and the collector region 800P can effectively avoid the influence on the hydrogen doped region 900H. In particular, when the dopant ions in the buffer zone 700N include phosphorus ions, a higher annealing temperature is usually required to activate the phosphorus ions, and the annealing temperature for activating the phosphorus ions is, for example, higher than 600°C. The environment is particularly prone to cause hydrogen ions in the substrate to be recombined. In this embodiment, by adjusting the preparation steps of the hydrogen doped region 900H to be after the preparation steps of the buffer zone 700N, the hydrogen in the hydrogen doped region 900H is prevented from being recombined at high temperature, which would cause the hydrogen doped region 900H to be recombined. The ion doping concentration cannot be precisely controlled.
尤其是,当所制备的氢掺杂区900H包括了往远离所述缓冲区700N的方向依次排布的多个氢掺杂分区(本实施例中,包括:第一氢掺杂分区910H、第二氢掺杂分区920H、第三氢掺杂分区930H和第四氢掺杂分区940H),并且所述多个氢掺杂分区的离子浓度峰值往远离所述缓冲区的方向依次降低。此时,若将形成有多个氢掺杂分区的衬底置于高温条件下时,则越靠近衬底表面的氢掺杂分区其受到温度的影响更大,容易导致越靠近衬底表面的氢掺杂分区的浓度越低。换言之,在将形成有多个氢掺杂分区的衬底置于高温条件下以完成高温退火工艺时,将不利于形成浓度峰值由衬底表面向内依次降低的多个氢掺杂分区。In particular, when the prepared hydrogen-doped region 900H includes a plurality of hydrogen-doped sub-regions (in this embodiment, including: the first hydrogen-doped sub-region 910H, the second hydrogen-doped sub-region 910H, the second The hydrogen-doped subregions 920H, the third hydrogen-doped subregions 930H, and the fourth hydrogen-doped subregions 940H), and the ion concentration peaks of the plurality of hydrogen-doped subregions gradually decrease in the direction away from the buffer zone. At this time, if the substrate formed with a plurality of hydrogen-doped partitions is placed under high temperature conditions, the hydrogen-doped partitions closer to the surface of the substrate are more affected by the temperature, which is likely to cause The concentration of the hydrogen doped partition is lower. In other words, when the substrate formed with a plurality of hydrogen-doped subregions is placed under a high temperature condition to complete the high-temperature annealing process, it will be disadvantageous to form a plurality of hydrogen-doped subregions whose concentration peaks decrease sequentially from the substrate surface inward.
然而,本实施例中,是在集电极区电800P和缓冲区700N制备完成后,再形成所述氢掺杂区900H,因此所述氢掺杂区900H并不会由于集电极区电800P和缓冲区700N的制备工艺而导致氢浓度不稳定,实现了所形成的氢掺杂区900H中的氢浓度可以更为精确的控制,从而更易于制备出离子浓度峰值由衬底表面向内依次降低的多个氢掺杂分区。However, in this embodiment, the hydrogen doped region 900H is formed after the collector region electricity 800P and the buffer region 700N are prepared, so the hydrogen doped region 900H will not be affected by the collector region electricity 800P and the buffer region 700N. The hydrogen concentration is unstable due to the preparation process of the buffer zone 700N, so that the hydrogen concentration in the formed hydrogen-doped region 900H can be controlled more precisely, so that it is easier to prepare the ion concentration peaks that decrease sequentially from the substrate surface inward. of multiple hydrogen-doped partitions.
本实施例中,所述氢掺杂区900H包括往远离所述缓冲区700N的方向依次排布的第四氢掺杂分区940H、第三氢掺杂分区930H、第二氢掺杂分区920H和第一氢掺杂分区910H。以及,所述第四氢掺杂分区940H、第三氢掺杂分区930H、第二氢掺杂分区920H和第一氢掺杂分区910H的离子浓度分布均为高斯分布,并且所述第四氢掺杂分区940H、第三氢掺杂分区930H、第二氢掺杂分区920H和第一氢掺杂分区910H的离子浓度峰值依次降低。即,所述第四氢掺杂分区940H最靠近所述衬底100N的第二表面A2,并具有最大的离子浓度峰值,以及所述第一氢掺杂分区910H最远离所述衬底100N的第二表面A2,并具有最小的离子浓度峰值。In this embodiment, the hydrogen-doped region 900H includes a fourth hydrogen-doped subregion 940H, a third hydrogen-doped subregion 930H, a second hydrogen-doped subregion 920H and The first hydrogen doped partition 910H. And, the ion concentration distributions of the fourth hydrogen-doped subregion 940H, the third hydrogen-doped subregion 930H, the second hydrogen-doped subregion 920H, and the first hydrogen-doped subregion 910H are all Gaussian distributions, and the fourth hydrogen-doped subregion 910H has a Gaussian distribution. The ion concentration peaks of the doping subregion 940H, the third hydrogen doping subregion 930H, the second hydrogen doping subregion 920H and the first hydrogen doping subregion 910H decrease sequentially. That is, the fourth hydrogen-doped subregion 940H is closest to the second surface A2 of the substrate 100N and has the largest ion concentration peak, and the first hydrogen-doped subregion 910H is farthest from the substrate 100N The second surface, A2, has the smallest peak ion concentration.
继续参考图11所示,所述氢掺杂区900H的宽度大于所述缓冲区700N的宽度,以利用所述氢掺杂区900H大量削弱电场,以较大程度的实现电场截止,甚至可以基于氢掺杂区900H直接实现电场截止,从而使得抵达至缓冲区700N的电场强度大大降低,有效保障了器件的耐压性能。Continuing to refer to FIG. 11 , the width of the hydrogen-doped region 900H is larger than the width of the buffer zone 700N, so that the hydrogen-doped region 900H can be used to greatly weaken the electric field, so as to realize the electric field cut-off to a greater extent, and can even be based on The hydrogen-doped region 900H directly realizes the electric field cut-off, so that the electric field strength reaching the buffer zone 700N is greatly reduced, and the voltage withstand performance of the device is effectively guaranteed.
本实施例中,所述氢掺杂区900H包括多层氢掺杂分区,以及所述缓冲区700N包括至少两层缓冲分区,并且可使所述氢掺杂区900H中的氢掺杂分区的数量大于所述缓冲区700N中的缓冲分区的数量。如此,一方面保证了所构成的氢掺杂区900H的宽度能够大于缓冲区700N的宽度;另一方面,有利于实现对氢掺杂区900H在不同深度位置的离子浓度分布的设置。In this embodiment, the hydrogen-doped region 900H includes multiple layers of hydrogen-doped subregions, and the buffer region 700N includes at least two layers of buffer subregions, and the hydrogen-doped subregions in the hydrogen-doped region 900H can be The number is greater than the number of buffer partitions in the buffer 700N. In this way, on the one hand, the width of the formed hydrogen doped region 900H is guaranteed to be greater than that of the buffer zone 700N;
进一步的,所述氢掺杂区900H中的多层氢掺杂分区可利用多次离子注入步骤分别形成。具体参考图11和图13所示,首先,执行第一道离子注入步骤,以形成第一氢掺杂分区910H;接着,执行第二道离子注入步骤,以形成第二氢掺杂分区920H;接着,执行第三道离子注入步骤,以形成第三氢掺杂分区930H;接着,执行第四道离子注入步骤,以形成第四氢掺杂分区940H。以及,在执行如上所述的多道离子注入步骤之后,执行退火工艺。其中,针 对氢掺杂区900H,可采用热退火工艺,其退火温度例如为350℃~450℃。Further, the multi-layer hydrogen-doped subregions in the hydrogen-doped region 900H may be formed separately by multiple ion implantation steps. 11 and FIG. 13 , first, a first ion implantation step is performed to form a first hydrogen-doped subregion 910H; then, a second ion implantation step is performed to form a second hydrogen-doped subregion 920H; Next, a third ion implantation step is performed to form a third hydrogen-doped subregion 930H; then, a fourth ion implantation step is performed to form a fourth hydrogen-doped subregion 940H. And, after performing the multi-pass ion implantation steps as described above, an annealing process is performed. Wherein, for the hydrogen-doped region 900H, a thermal annealing process can be used, and the annealing temperature is, for example, 350°C to 450°C.
具体的实施例中,形成所述氢掺杂区900H的四道离子注入步骤的工艺参数以及所形成的四层氢掺杂分区的离子分布状况例如可参考表1所示。In a specific embodiment, the process parameters of the four ion implantation steps for forming the hydrogen-doped region 900H and the ion distribution of the formed four-layer hydrogen-doped partition can be referred to, for example, as shown in Table 1.
Figure PCTCN2021117225-appb-000001
Figure PCTCN2021117225-appb-000001
表1Table 1
如表1所示,在一个具体的示例中,四个氢掺杂分区的注入剂量具有交叠的数值范围,然而应当认识到,在实际执行离子注入的过程中仍可以在如上所示的数值范围内调整各个氢掺杂分区的注入剂量,以使得由深至浅的多个氢掺杂分区的离子浓度峰值逐级递增。如此,即可利用离子浓度逐步增加的多个氢掺杂分区逐渐削弱电场。As shown in Table 1, in a specific example, the implant doses of the four hydrogen-doped subregions have overlapping value ranges, however, it should be recognized that the values shown above may still be within the range of the values shown above during the actual ion implantation. The implantation dose of each hydrogen-doped subregion is adjusted within the range, so that the ion concentration peaks of a plurality of hydrogen-doped subregions from deep to shallow increase step by step. In this way, the electric field can be gradually weakened by using a plurality of hydrogen-doped subregions with gradually increasing ion concentrations.
此外,本实施例中,所述氢掺杂区900H中具有最大离子浓度峰值的氢掺杂分区(即,第四氢掺杂分区940H)邻接所述缓冲区700N中具有最小离子浓度峰值的缓冲分区(即,第一缓冲分区710N),并且所述具有最大离子浓度峰值的氢掺杂分区(即,第四氢掺杂分区940H)的离子浓度峰值仍小于所述具有最小离子浓度峰值的缓冲分区(即,第一缓冲分区710N)的离子浓度峰值。In addition, in this embodiment, the hydrogen-doped subregion (ie, the fourth hydrogen-doped subregion 940H) with the largest ion concentration peak in the hydrogen doping region 900H is adjacent to the buffer with the smallest ion concentration peak in the buffer region 700N partition (ie, the first buffer partition 710N), and the ion concentration peak of the hydrogen-doped partition with the largest ion concentration peak (ie, the fourth hydrogen-doped partition 940H) is still smaller than the buffer with the smallest ion concentration peak The peak ion concentration of the partition (ie, the first buffer partition 710N).
即,本实施例中,由氢掺杂区900H和缓冲区700N所构成的多层掺杂区的离子浓度整体上是由深至浅逐级递增,从而可以逐级削弱电场。同时,最靠近集电极区800P的掺杂区的离子浓度最高,保证了电场在集电极区800P之前掺杂区中可以完全被截止,并有利于改善器件的漏电现象。That is, in this embodiment, the ion concentration of the multi-layer doped region formed by the hydrogen doped region 900H and the buffer region 700N is generally increased from deep to shallow, so that the electric field can be weakened step by step. At the same time, the ion concentration of the doped region closest to the collector region 800P is the highest, which ensures that the electric field can be completely cut off in the doped region before the collector region 800P, and is beneficial to improve the leakage phenomenon of the device.
进一步的方案中,具体参考图12所示,在形成所述氢掺杂区900H后,还包括:在所述衬底100N的第二表面A2上形成欧姆电极810,所述欧姆电极810和所述集电极区800P接触。In a further solution, referring specifically to FIG. 12 , after forming the hydrogen-doped region 900H, it further includes: forming an ohmic electrode 810 on the second surface A2 of the substrate 100N, the ohmic electrode 810 and the The collector region 800P contacts.
具体的,所述欧姆电极810的形成方法例如包括:首先,在所述衬底100N的第二表面上沉积金属层,所述金属层的材料例如包括铝、钛、镍和金中的至少一种;接着,执行合金化处理,以使所述金属层中的金属和所述衬底100N中的硅在两者的接触面上实现金属硅合金化,以降低所述欧姆电极810和所述集电极区800P之间的接触电阻。Specifically, the method for forming the ohmic electrode 810 includes, for example: first, depositing a metal layer on the second surface of the substrate 100N, where the material of the metal layer includes, for example, at least one of aluminum, titanium, nickel and gold Next, an alloying process is performed, so that the metal in the metal layer and the silicon in the substrate 100N realize metal-silicon alloying on the contact surface of the two, so as to reduce the ohmic electrode 810 and the silicon in the substrate 100N. Contact resistance between collector regions 800P.
基于如上所述的形成方法,以下对所形成的绝缘栅双极型晶体管的结构进行说明。具体可参考图12和图13所示,所述绝缘栅双极型晶体管包括:Based on the above-described formation method, the structure of the formed insulated gate bipolar transistor will be described below. 12 and 13, the insulated gate bipolar transistor includes:
第二导电类型的衬底100N,所述衬底100N具有相对的第一表面和第二表面;a second conductivity type substrate 100N, the substrate 100N having opposing first and second surfaces;
栅极导电层220,形成在所述衬底100N中;The gate conductive layer 220 is formed in the substrate 100N;
第一掺杂类型的体区300P,由所述衬底100N的第一表面向内扩展至所述衬底100N中,以使所述体区300P至少部分和所述栅极导电层220横向重叠;The body region 300P of the first doping type extends inward from the first surface of the substrate 100N into the substrate 100N, so that the body region 300P at least partially overlaps the gate conductive layer 220 laterally ;
第二掺杂类型的发射极区400N,由所述衬底100N的第一表面向内扩展至所述体区300P中,并且所述发射极区400N的底部边界介于所述栅极导电层220的顶部边界和所述体区300P的底部边界之间;The emitter region 400N of the second doping type extends inward from the first surface of the substrate 100N into the body region 300P, and the bottom boundary of the emitter region 400N is between the gate conductive layer between the top boundary of 220 and the bottom boundary of the body region 300P;
第一掺杂类型的集电极区800P,由所述衬底100N的第二表面向内扩展至所述衬底100N中;The collector region 800P of the first doping type extends inward from the second surface of the substrate 100N into the substrate 100N;
第二掺杂类型的缓冲区700N,形成在所述集电极区800P靠近所述体区300P的一侧,以及,A buffer zone 700N of the second doping type is formed on the side of the collector region 800P close to the body region 300P, and,
氢掺杂区900H,形成在所述缓冲区700N靠近所述体区300P的一侧,并且所述氢掺杂区900H包括往远离所述缓冲区的方向依次排布的多个氢掺杂分区,所述多个氢掺杂分区的离子浓度峰值往远离所述缓冲区的方向依次降低。即,所述多个氢掺杂分区中最靠近衬底100N的第二表面的氢掺杂分区的离子浓度峰值最高。The hydrogen-doped region 900H is formed on the side of the buffer zone 700N close to the body region 300P, and the hydrogen-doped region 900H includes a plurality of hydrogen-doped subregions arranged in sequence away from the buffer zone , the ion concentration peaks of the plurality of hydrogen-doped subregions decrease sequentially in the direction away from the buffer zone. That is, the hydrogen-doped sub-region closest to the second surface of the substrate 100N among the plurality of hydrogen-doped sub-regions has the highest ion concentration peak.
需要说明的是,在对衬底结构进行热处理时(例如,退火工艺),则衬底 表面的温度一般是最高的,即衬底内部的温度通常会低于衬底表面的温度。此时,若衬底中已经形成有氢掺杂区时,则容易导致氢掺杂区中最靠近衬底表面的部分更容易受到高温复合,进而使得氢掺杂区中最靠近衬底表面的部分的离子浓度较低。It should be noted that when the substrate structure is heat treated (for example, annealing process), the temperature of the substrate surface is generally the highest, that is, the temperature inside the substrate is usually lower than the temperature of the substrate surface. At this time, if a hydrogen doped region has been formed in the substrate, it is easy to cause the part of the hydrogen doped region closest to the substrate surface to be more susceptible to high temperature recombination, thereby making the hydrogen doped region closest to the substrate surface. Some have lower ion concentrations.
然而,与传统工艺不同的是,本实施例中创造性的将氢掺杂区的制备步骤调整至缓冲区的制备步骤之后,以避免缓冲区的制备工艺对氢掺杂区造成不利影响,提高对所形成的氢掺杂区中的离子浓度分布的控制精度,进而能够制备出氢离子浓度峰值往远离缓冲区的方向依次降低的多个氢掺杂分区,提高所制备出的器件的稳定性。However, different from the traditional process, in this embodiment, the preparation step of the hydrogen-doped region is creatively adjusted to be after the preparation step of the buffer zone, so as to avoid the adverse effect of the preparation process of the buffer zone on the hydrogen-doped region, and improve the efficiency of the buffer zone. The control accuracy of the ion concentration distribution in the formed hydrogen doped region can further prepare a plurality of hydrogen doped subregions with the peak hydrogen ion concentration decreasing in turn in the direction away from the buffer zone, and improve the stability of the prepared device.
虽然本发明已以较佳实施例披露如上,然而上述实施例并非用以限定本发明。对于任何熟悉本领域的技术人员而言,在不脱离本发明技术方案范围情况下,都可利用上述揭示的技术内容对本发明技术方案作出许多可能的变动和修饰,或修改为等同变化的等效实施例。因此,凡是未脱离本发明技术方案的内容,依据本发明的技术实质对以上实施例所做的任何简单修改、等同变化及修饰,均仍属于本发明技术方案保护的范围。Although the present invention has been disclosed above with preferred embodiments, the above embodiments are not intended to limit the present invention. For any person skilled in the art, without departing from the scope of the technical solution of the present invention, many possible changes and modifications can be made to the technical solution of the present invention by using the technical content disclosed above, or modified into equivalents of equivalent changes Example. Therefore, any simple modifications, equivalent changes and modifications made to the above embodiments according to the technical essence of the present invention without departing from the content of the technical solutions of the present invention still fall within the protection scope of the technical solutions of the present invention.
还应当理解的是,除非特别说明或者指出,否则说明书中的术语“第一”、“第二”、“第三”等描述仅仅用于区分说明书中的各个组件、元素、步骤等,而不是用于表示各个组件、元素、步骤之间的逻辑关系或者顺序关系等。It should also be understood that unless otherwise specified or indicated, the terms "first", "second", "third" and other descriptions in the specification are only used to distinguish various components, elements, steps, etc. in the specification, rather than It is used to represent the logical relationship or sequence relationship among various components, elements, steps, etc.
此外还应该认识到,此处描述的术语仅仅用来描述特定实施例,而不是用来限制本发明的范围。必须注意的是,此处的以及所附权利要求中使用的单数形式“一个”和“一种”包括复数基准,除非上下文明确表示相反意思。例如,对“一个步骤”或“一个装置”的引述意味着对一个或多个步骤或装置的引述,并且可能包括次级步骤以及次级装置。应该以最广义的含义来理解使用的所有连词。以及,词语“或”应该被理解为具有逻辑“或”的定义,而不是逻辑“异或”的定义,除非上下文明确表示相反意思。此外,本发明实施例中的方法和/或设备的实现可包括手动、自动或组合地执行所选任务。Also, it should be appreciated that the terminology described herein is used to describe particular embodiments only, and not to limit the scope of the present invention. It must be noted that, as used herein and in the appended claims, the singular forms "a" and "an" include plural references unless the context clearly dictates otherwise. For example, reference to "a step" or "a means" means a reference to one or more steps or means, and may include sub-steps as well as sub-means. All conjunctions used should be understood in their broadest sense. Also, the word "or" should be understood to have the definition of a logical "or" rather than a logical "exclusive or" unless the context clearly dictates otherwise. Furthermore, implementation of methods and/or apparatuses in embodiments of the present invention may include performing selected tasks manually, automatically, or a combination.

Claims (16)

  1. 一种绝缘栅双极型晶体管的形成方法,其特征在于,包括:A method for forming an insulated gate bipolar transistor, comprising:
    提供衬底,所述衬底具有相对的第一表面和第二表面,以及在所述衬底对应于所述第一表面的部分中形成有栅极导电层、第一掺杂类型的体区和第二掺杂类型的发射极区;A substrate is provided, the substrate has opposing first and second surfaces, and a gate conductive layer, a body region of a first doping type are formed in a portion of the substrate corresponding to the first surface and an emitter region of the second doping type;
    对所述衬底的第二表面执行离子注入工艺和退火工艺,以形成第二掺杂类型的缓冲区和第一掺杂类型的集电极区,所述集电极区从所述衬底的所述第二表面向内扩展至所述衬底中,所述缓冲区位于所述集电极区靠近所述体区的一侧;以及,An ion implantation process and an annealing process are performed on the second surface of the substrate to form a buffer region of the second doping type and a collector region of the first doping type, the collector region extending from all of the substrate. the second surface extends inwardly into the substrate, the buffer zone is located on a side of the collector region proximate the body region; and,
    对所述衬底的第二表面执行离子注入工艺和热退火工艺,以形成氢掺杂区,所述氢掺杂区位于所述缓冲区靠近所述体区的一侧,其中所述氢掺杂区包括往远离所述缓冲区的方向依次排布的多个氢掺杂分区,所述多个氢掺杂分区的离子浓度峰值往远离所述缓冲区的方向依次降低。An ion implantation process and a thermal annealing process are performed on the second surface of the substrate to form a hydrogen-doped region, the hydrogen-doped region is located on a side of the buffer zone close to the body region, wherein the hydrogen-doped region The impurity region includes a plurality of hydrogen-doped subregions that are sequentially arranged in a direction away from the buffer zone, and ion concentration peaks of the plurality of hydrogen-doped subregions are sequentially decreased in a direction away from the buffer zone.
  2. 如权利要求1所述的绝缘栅双极型晶体管的形成方法,其特征在于,所述缓冲区的形成方法包括:依次执行至少两道离子注入步骤,以及执行退火工艺,以形成至少两层缓冲分区,所述至少两层缓冲分区往远离所述集电极区的方向依次排布;The method for forming an insulated gate bipolar transistor according to claim 1, wherein the method for forming the buffer area comprises: sequentially performing at least two ion implantation steps and performing an annealing process to form at least two buffer layers partitions, the at least two buffer partitions are sequentially arranged in a direction away from the collector region;
    以及,所述氢掺杂区的形成方法包括:依次执行多道离子注入步骤,以形成所述多层氢掺杂分区,所述多层氢掺杂分区往远离所述缓冲区的方向依次排布。And, the method for forming the hydrogen-doped region includes: sequentially performing multiple ion implantation steps to form the multi-layer hydrogen-doped sub-regions, and the multi-layer hydrogen-doped sub-regions are sequentially arranged in a direction away from the buffer zone cloth.
  3. 如权利要求2所述的绝缘栅双极型晶体管的形成方法,其特征在于,所述氢掺杂区中氢掺杂分区的数量大于所述缓冲区中缓冲分区的数量。3. The method for forming an insulated gate bipolar transistor according to claim 2, wherein the number of hydrogen-doped subregions in the hydrogen-doped region is greater than the number of buffer subregions in the buffer region.
  4. 如权利要求2所述的绝缘栅双极型晶体管的形成方法,其特征在于,在形成所述缓冲区的所述至少两道离子注入步骤中,随着离子注入能量的增加,离子注入剂量依次减小,以使所形成的至少两层缓冲分区的离子浓度峰值往远离所述集电极区的方向依次降低。The method for forming an insulated gate bipolar transistor according to claim 2, wherein in the at least two ion implantation steps of forming the buffer zone, with the increase of ion implantation energy, the ion implantation dose is sequentially decrease, so that the peak values of ion concentrations of the formed at least two-layer buffer regions are successively decreased in the direction away from the collector region.
  5. 如权利要求2所述的绝缘栅双极型晶体管的形成方法,其特征在于,在形成所述氢掺杂区的所述多道离子注入步骤中,随着离子注入能量的增加, 离子注入剂量依次减小,以使所形成的多层氢掺杂分区的离子浓度峰值往远离所述缓冲区的方向依次降低。The method for forming an insulated gate bipolar transistor according to claim 2, wherein in the multi-channel ion implantation step of forming the hydrogen doped region, as the ion implantation energy increases, the ion implantation dose decreasing in sequence, so that the peak value of the ion concentration of the formed multilayer hydrogen-doped subregion decreases in sequence in the direction away from the buffer zone.
  6. 如权利要求2所述的绝缘栅双极型晶体管的形成方法,其特征在于,所述缓冲区包括两层缓冲分区,两层所述缓冲分区的离子浓度峰值均介于1E16atoms/cm 3~1E17atoms/cm 3之间,并且两层所述缓冲分区的宽度均为0.4μm~0.7μm。 The method for forming an insulated gate bipolar transistor according to claim 2, wherein the buffer zone comprises two layers of buffer zones, and the peak ion concentrations of the two layers of the buffer zones are both between 1E16 atoms/cm 3 to 1E17 atoms /cm 3 , and the widths of the buffer partitions of the two layers are both 0.4 μm to 0.7 μm.
  7. 如权利要求6所述的绝缘栅双极型晶体管的形成方法,其特征在于,所述氢掺杂区包括四个氢掺杂分区,其中最靠近所述缓冲区的两个氢掺杂分区的离子浓度峰值均介于1E12atoms/cm 3~1E14atoms/cm 3之间,以及最远离所述缓冲区的两个氢掺杂分区的离子浓度峰值均介于1E12atoms/cm 3~1E13atoms/cm 3之间,并且所述四个氢掺杂分区的宽度均为6μm~8μm。 The method for forming an insulated gate bipolar transistor according to claim 6, wherein the hydrogen-doped region comprises four hydrogen-doped subregions, wherein two hydrogen-doped subregions closest to the buffer zone are The ion concentration peaks are all between 1E12atoms/cm 3 to 1E14 atoms/cm 3 , and the ion concentration peaks of the two hydrogen-doped partitions farthest from the buffer zone are all between 1E12 atoms/cm 3 to 1E13 atoms/cm 3 , and the widths of the four hydrogen-doped partitions are all 6 μm˜8 μm.
  8. 如权利要求1所述的绝缘栅双极型晶体管的形成方法,其特征在于,所述缓冲区中的掺杂离子包括磷,以及在形成所述缓冲区的退火工艺中采用激光退火工艺,并使退火温度大于等于600℃。The method for forming an insulated gate bipolar transistor according to claim 1, wherein the doping ions in the buffer zone comprise phosphorus, and a laser annealing process is used in the annealing process for forming the buffer zone, and Make the annealing temperature equal to or higher than 600°C.
  9. 如权利要求1所述的绝缘栅双极型晶体管的形成方法,其特征在于,在形成所述氢掺杂区的热退火工艺中其退火温度为350℃~450℃。The method for forming an insulated gate bipolar transistor according to claim 1, wherein in the thermal annealing process for forming the hydrogen doped region, the annealing temperature is 350°C˜450°C.
  10. 一种绝缘栅双极型晶体管,其特征在于,包括:An insulated gate bipolar transistor, comprising:
    衬底,所述衬底具有相对的第一表面和第二表面,以及在所述衬底对应于所述第一表面的部分中形成有栅极导电层、第一掺杂类型的体区和第二掺杂类型的发射极区;a substrate having opposing first and second surfaces, and a gate conductive layer, a body region of a first doping type, and a portion of the substrate corresponding to the first surface are formed an emitter region of the second doping type;
    第一掺杂类型的集电极区,由所述衬底的所述第二表面向内扩展至所述衬底中;a collector region of a first doping type extending inwardly into the substrate from the second surface of the substrate;
    第二掺杂类型的缓冲区,形成在所述集电极区靠近所述体区的一侧,以及,A buffer area of a second doping type is formed on the side of the collector region adjacent to the body region, and,
    氢掺杂区,形成在所述缓冲区靠近所述体区的一侧,并且所述氢掺杂区包括往远离所述缓冲区的方向依次排布的多个氢掺杂分区,所述多个氢掺杂分区的离子浓度峰值往远离所述缓冲区的方向依次降低。A hydrogen-doped region is formed on a side of the buffer zone close to the body region, and the hydrogen-doped region includes a plurality of hydrogen-doped subregions arranged in sequence in a direction away from the buffer zone, the multiple The ion concentration peaks of each of the hydrogen-doped subregions decrease sequentially in the direction away from the buffer zone.
  11. 如权利要求10所述的绝缘栅双极型晶体管,其特征在于,所述氢掺 杂区的厚度大于所述缓冲区的厚度。The insulated gate bipolar transistor of claim 10, wherein the thickness of the hydrogen-doped region is greater than the thickness of the buffer region.
  12. 如权利要求10所述的绝缘栅双极型晶体管,其特征在于,所述缓冲区包括往远离所述集电极区依次排布的至少两个缓冲分区,以及所述氢掺杂区中氢掺杂分区的数量大于所述缓冲区中缓冲分区的数量。11. The insulated gate bipolar transistor of claim 10, wherein the buffer area comprises at least two buffer areas arranged in sequence away from the collector area, and the hydrogen doped area in the hydrogen doped area The number of miscellaneous partitions is greater than the number of buffer partitions in the buffer.
  13. 如权利要求12所述的绝缘栅双极型晶体管,其特征在于,在所述缓冲区中,沿着远离所述集电极区的方向所述至少两个缓冲分区的离子浓度峰值依次降低。13. The insulated gate bipolar transistor of claim 12, wherein, in the buffer region, the ion concentration peaks of the at least two buffer regions in a direction away from the collector region decrease sequentially.
  14. 如权利要求13所述的绝缘栅双极型晶体管,其特征在于,所述缓冲区包括两层缓冲分区,两层所述缓冲分区的离子浓度峰值均介于1E16atoms/cm 3~1E17atoms/cm 3之间,并且两层所述缓冲分区的宽度均为0.4μm~0.7μm。 14. The insulated gate bipolar transistor of claim 13, wherein the buffer zone comprises two layers of buffer zones, and the peak ion concentrations of the two layers of the buffer zones are both between 1E16 atoms/cm 3 to 1E17 atoms/cm 3 between, and the widths of the buffer partitions of the two layers are both 0.4 μm˜0.7 μm.
  15. 如权利要求14所述的绝缘栅双极型晶体管,其特征在于,所述氢掺杂区包括四个氢掺杂分区,其中最靠近所述缓冲区的两个氢掺杂分区的离子浓度峰值均介于1E12atoms/cm 3~1E14atoms/cm 3之间,以及最远离所述缓冲区的两个氢掺杂分区的离子浓度峰值均介于1E12atoms/cm 3~1E13atoms/cm 3之间,并且所述四个氢掺杂分区的宽度均为6μm~8μm。 15. The insulated gate bipolar transistor of claim 14, wherein the hydrogen-doped region comprises four hydrogen-doped subregions, wherein two hydrogen-doped subregions closest to the buffer zone have peak ion concentrations Both are between 1E12atoms/cm 3 to 1E14 atoms/cm 3 , and the peak ion concentrations of the two hydrogen-doped partitions farthest from the buffer zone are both between 1E12 atoms/cm 3 to 1E13 atoms/cm 3 , and all The widths of the four hydrogen-doped partitions are all 6 μm˜8 μm.
  16. 如权利要求12所述的绝缘栅双极型晶体管,其特征在于,所述氢掺杂区中具有最大离子浓度峰值的氢掺杂分区邻接所述缓冲区中具有最小离子浓度峰值的缓冲分区,并且所述具有最大离子浓度峰值的氢掺杂分区的离子浓度峰值仍小于所述具有最小离子浓度峰值的缓冲分区的离子浓度峰值。13. The insulated gate bipolar transistor of claim 12, wherein the hydrogen-doped subregion with the largest ion concentration peak in the hydrogen-doped region is adjacent to the buffer subregion with the smallest ion concentration peak in the buffer region, And the ion concentration peak value of the hydrogen-doped subregion with the largest ion concentration peak value is still smaller than the ion concentration peak value of the buffer subregion with the smallest ion concentration peak value.
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