CN109087954A - A kind of silicon carbide drift step recovery diode - Google Patents

A kind of silicon carbide drift step recovery diode Download PDF

Info

Publication number
CN109087954A
CN109087954A CN201810961593.6A CN201810961593A CN109087954A CN 109087954 A CN109087954 A CN 109087954A CN 201810961593 A CN201810961593 A CN 201810961593A CN 109087954 A CN109087954 A CN 109087954A
Authority
CN
China
Prior art keywords
type
silicon carbide
base area
recovery diode
step recovery
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
CN201810961593.6A
Other languages
Chinese (zh)
Inventor
陈万军
高吴昊
谯彬
左慧玲
邓操
夏云
刘超
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
University of Electronic Science and Technology of China
Original Assignee
University of Electronic Science and Technology of China
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by University of Electronic Science and Technology of China filed Critical University of Electronic Science and Technology of China
Priority to CN201810961593.6A priority Critical patent/CN109087954A/en
Publication of CN109087954A publication Critical patent/CN109087954A/en
Pending legal-status Critical Current

Links

Classifications

    • 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
    • H01L29/86Types of semiconductor device ; Multistep manufacturing processes therefor controllable only by variation of the electric current supplied, or only the electric potential applied, to one or more of the electrodes carrying the current to be rectified, amplified, oscillated or switched
    • H01L29/861Diodes
    • 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

Landscapes

  • Engineering & Computer Science (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Power Engineering (AREA)
  • Physics & Mathematics (AREA)
  • Ceramic Engineering (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Computer Hardware Design (AREA)
  • Bipolar Transistors (AREA)

Abstract

The present invention relates to power semiconductor technologies, in particular to a kind of silicon carbide drift step recovery diode.The present invention is to conventional p+‑p‑n0‑n+The n of silicon carbide drift step recovery diode0Base area is transformed, by by the n of Uniform Doped0N-type staged varying doping base area 3 is changed into base area, it is built in field from bottom to top to introduce direction in N-type base area, drift step recovery diode pulsed discharge the backward pumping stage, so that the minority carrier hole in N-type base area is extracted faster, and earlier be accelerated to saturated velocity, so that the time in backward pumping stage reduces, so that the voltage change ratio in the voltage pulse forward position formed in the load in pulse discharge loop is bigger, the time is shorter.

Description

A kind of silicon carbide drift step recovery diode
Technical field
The present invention relates to a kind of semiconductor switch diode, in particular to a kind of silicon carbide drift step recovery diode.
Background technique
Drift step recovery diode (Drift step recovery diodes, abbreviation DSRD) is that a kind of semiconductor is opened Diode is closed, is proposed by Russian Ioffe physical technique research institute, ultra wide band (Ultra Wide Band, letter are generally used for Claim UWB) pulse signal source, it can achieve the nanosecond even switch time of picosecond, have high efficiency, high reliability, structure tight The features such as gathering and be light-weight, therefore used in a variety of pulse signal sources as Primary Component.
In several kilovolts even tens kilovolts of nanosecond pulse system, for single silicon substrate DSRD device, due to drift It is very big to move area's thickness, has been unable to satisfy the time requirement of pulse front edge, multiple devices in series is needed to use, this greatly increases The volume of system.Broad stopband carbofrax material has the forbidden bandwidth higher than silicon materials, saturation carrier velocity, thermal conductivity and faces Boundary's breakdown electric field, so that the performance of silicon carbide DSRD device is significantly better than silicon DSRD, thus in same voltage class and pulse Between in desired pulse system, the serial number of silicon carbide DSRD is much smaller than silicon DSRD, is greatly saved the volume of system.But It is that, due to the limitation of the state of the art, the carrier mobility and carrier lifetime of carbofrax material are lower, so that often Non- speed saturation stage of the silicon carbide DSRD device of rule in the backward pumping stage of pulsed discharge, the pumping in minority carrier hole Take speed slower, so as to cause voltage pulse leading edge time is long, voltage pulse peak value is low, silicon carbide DSRD power consumption is big, it is difficult to fill The advantage of carbofrax material is waved in distribution, limits the raising of the performance of device.
Summary of the invention
The technical problem to be solved by the present invention is to pass through the internal structure for changing silicon carbide drift step recovery diode, with Solve the problems, such as that voltage pulse leading edge time is long, voltage pulse peak value is low, silicon carbide drift step recovery diode power consumption is big.
Technical solution of the present invention: a kind of silicon carbide drift step recovery diode, as shown in Fig. 2, a kind of silicon carbide floats Move step-recovery diode, structure cell from bottom to top be respectively including N-type Ohm contact electrode 1, N-type silicon carbide substrates 2, N-type staged varying doping base area 3, p-type plasma accumulation layer 4, p-type heavy doping anode 5, p-type Ohm contact electrode 6;
The N-type silicon carbide substrates 2 include N+ substrate layer 21 and N+buffer layer 22;
The N-type staged varying doping base area 3 includes the N-type silicon carbide epitaxial layers of n-layer (n >=2) different levels of doping, often The doping concentration changing rule of layer N-type epitaxy layer is successively to successively decrease from bottom to top, shows as stepped concentration distribution;
The solution of the present invention, compared to conventional p+-p-n0-n+Silicon carbide drift step recovery diode, carbon of the invention The n of SiClx drift step recovery diode0Base area uses the staged varying doping base that doping concentration gradually decreases from bottom to top Area.
Beneficial effects of the present invention are that the present invention is to conventional p+-p-n0-n+The n of silicon carbide drift step recovery diode0 Base area is transformed, by by the n of Uniform Doped0N-type staged varying doping base area 3 is changed into base area, thus in N-type base area Inside introducing direction is built in field from bottom to top, drift step recovery diode pulsed discharge backward pumping rank Section is accelerated to saturated velocity so that the minority carrier hole in N-type base area is extracted faster, and earlier, so that instead It is reduced to the time in pumping stage, so that the voltage in the voltage pulse forward position formed in the load in pulse discharge loop becomes Rate is bigger, the time is shorter.N-type staged varying doping base region structure of the invention uses conventional silicon carbide epitaxy technique, with Conventional p+-p-n0-n+The fabrication processing of silicon carbide drift step recovery diode is compared, and mixing of being delayed outside need to be only changed Miscellaneous condition, without additionally developing new process.
Detailed description of the invention
Fig. 1 is conventional silicon carbide DSRD structure cell schematic diagram;
Fig. 2 is DSRD structure cell schematic diagram of the invention;
Fig. 3 is DSRD pulse-generating circuit schematic diagram;
Fig. 4 is the device inside cavity speed comparison diagram of conventional DSRD and DSRD of the present invention at initial stage in backward pumping stage;
Fig. 5 is the device inside hole concentration comparison diagram of conventional DSRD and DSRD of the present invention at initial stage in backward pumping stage;
Fig. 6 is that conventional DSRD and DSRD of the present invention are compared by the voltage pulse waveforms that pulse-generating circuit exports.
Specific embodiment
The present invention is described in detail with reference to the accompanying drawing
As shown in Fig. 2, silicon carbide drift step recovery diode of the invention, structure cell is respectively to wrap from bottom to top Include N-type Ohm contact electrode 1, N-type silicon carbide substrates 2, N-type staged varying doping base area 3, p-type plasma accumulation layer 4, p-type weight Adulterate anode 5, p-type Ohm contact electrode 6;The N-type silicon carbide substrates 2 include N+ substrate layer 21 and N+buffer layer 22;Institute State the N-type silicon carbide epitaxial layers that N-type staged varying doping base area 3 includes n-layer (n >=2) different levels of doping, every layer of N-type extension The doping concentration changing rule of layer is successively to successively decrease from bottom to top, shows as stepped concentration distribution;It is characterized in that, comparing In conventional p+-p-n0-n+Silicon carbide drift step recovery diode, silicon carbide drift step recovery diode of the invention n0Base area uses the staged varying doping base area that doping concentration gradually decreases from bottom to top.
As shown in Figure 1, for conventional p+-p-n0-n+Silicon carbide drift step recovery diode.As shown in Fig. 2, being this hair Bright silicon carbide drift step recovery diode.The present invention and conventional p+-p-n0-n+Silicon carbide drift step recovery diode The different place of structure is that the present invention is to n0Base area is transformed, by by the n of Uniform Doped0N-type rank is changed into base area Ladder type varying doping base area 3, so that introducing direction in N-type base area is built in field from bottom to top, in drift step recovery Diode is in the backward pumping stage of pulsed discharge, so that the minority carrier hole in N-type base area is extracted faster, and more Early is accelerated to saturated velocity, so that the time in backward pumping stage reduces, so that the load in pulse discharge loop The voltage change ratio in the voltage pulse forward position of upper formation is bigger, the time is shorter.N-type staged varying doping base region structure of the invention Using conventional silicon carbide epitaxy technique, with conventional p+-p-n0-n+The manufacture craft of silicon carbide drift step recovery diode Process is compared, and only need to change the doping condition being delayed outside, without additionally developing new process.
Silicon carbide drift step recovery diode provided by the invention, its working principles are as follows:
In structure cell as shown in Figure 2, when silicon carbide DSRD device is in the forward pumping stage of pulsed discharge, just It is respectively stored in p-type carrier accumulation layer 4 and N-type base area 3 to the carrier inside current injection device;Work as silicon carbide When DSRD device is in the backward pumping stage of pulsed discharge, the minority carrier stored in silicon carbide DSRD device is extracted, Reverse current is formed, and in the reverse current decline stage, the electric current in energy storage original part is transferred on load resistance, thus negative It carries and forms voltage pulse on resistance, is i.e. the extraction speed of minority carrier determines the voltage pulse forward position of pulse system output Leading-edge pulse time, voltage build-up rate and voltage peak.Wherein, since 3 width of N-type base area is larger, so what is wherein stored lacks The extraction time of number carrier hole becomes one of the principal element for influencing leading-edge pulse time.N-type staged of the invention Varying doping base area 3, it is built in field from bottom to top that direction is introduced in N-type base area, in silicon carbide DSRD device in pulse The backward pumping stage of electric discharge, being accelerated to so that the minority carrier hole in N-type base area is extracted faster, and earlier Saturated velocity, so that the time in backward pumping stage reduces, so that the voltage formed in the load in pulse discharge loop The voltage change ratio of pulse front edge is bigger, the time is shorter, while also reducing the energy loss on silicon carbide DSRD device, from And it is transformed into more energy in load, increase peak impulse voltage, improves the efficiency of pulse system.
It is the conventional p of 12kV with same pressure resistance+-p-n0-n+Silicon carbide DSRD device (base doping concentration and with a thickness of 7e14cm-3/ 80 μm) (the N-type staged varying doping base area number of plies takes n=3, base area concentration with silicon carbide DSRD device of the invention And thickness is respectively 1.5e15cm from top to bottom-3/ 30 μm, 1e15cm-3/ 30 μm, 2e14cm-3/ 20 μm) carry out emulation comparison, two For a device other than base doping mode is different, the other parameters including device size and pressure voltage are all the same, electric discharge Circuit and simulated conditions are also identical, and discharge circuit is as shown in figure 3, output voltage peak value is all 11kV.Such as Fig. 4 and Fig. 5 institute It is shown as the device inside cavity speed and hole concentration distribution at initial stage in backward pumping stage (225.7ns moment shown in fig. 6), it can To find out, the minority carrier inside synchronization, silicon carbide DSRD device N-type base area of the invention close to PN junction side is empty Cave speed is greater than conventional device, although the cavity speed far from PN junction side decreases, but the area far from PN junction side The concentration in domain minority carrier hole well below close to PN junction side region, so to overall hole extract influence compared with It is small, so that allowing for overall minority carrier hole can be extracted faster, reduce the time in voltage pulse forward position.Such as Fig. 6 show the voltage waveform of pulse system output, it can be seen that and the leading-edge pulse time of silicon carbide DSRD of the invention is shorter, It is substantially better than conventional p+-p-n0-n+Silicon carbide DSRD device.Therefore, silicon carbide DSRD device of the present invention is suitable for ultra wide band system System.

Claims (1)

1. a kind of silicon carbide drift step recovery diode, structure cell includes the N-type Europe being cascading from bottom to top Nurse contacts electrode (1), N-type silicon carbide substrates (2), N-type staged varying doping base area (3), p-type plasma accumulation layer (4), p-type Heavy doping anode (5), p-type Ohm contact electrode (6);
The N-type silicon carbide substrates (2) include N+ substrate layer (21) and the N+buffer layer for being located at N+ substrate layer (21) upper surface (22);
The N-type staged varying doping base area (3) includes the N-type silicon carbide epitaxial layers of n-layer different levels of doping, and n >=2, often The doping concentration changing rule of layer N-type epitaxy layer is to successively decrease from bottom to top, shows as stepped concentration distribution.
CN201810961593.6A 2018-08-22 2018-08-22 A kind of silicon carbide drift step recovery diode Pending CN109087954A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201810961593.6A CN109087954A (en) 2018-08-22 2018-08-22 A kind of silicon carbide drift step recovery diode

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201810961593.6A CN109087954A (en) 2018-08-22 2018-08-22 A kind of silicon carbide drift step recovery diode

Publications (1)

Publication Number Publication Date
CN109087954A true CN109087954A (en) 2018-12-25

Family

ID=64794329

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201810961593.6A Pending CN109087954A (en) 2018-08-22 2018-08-22 A kind of silicon carbide drift step recovery diode

Country Status (1)

Country Link
CN (1) CN109087954A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112563320A (en) * 2020-11-29 2021-03-26 中国电子科技集团公司第五十五研究所 Method for improving performance of high-voltage drift step recovery device
CN113009425A (en) * 2021-02-23 2021-06-22 电子科技大学 Pulse compression structure based on SiC DSRD device

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102956822A (en) * 2011-08-19 2013-03-06 三星电子株式会社 Nonvolatile memory elements and memory devices including same
CN104201211A (en) * 2014-08-27 2014-12-10 温州大学 Base region gradient P<+>-N-N<+> type SiC ultrafast recovery diode manufactured on 4H type single crystal silicon carbide epitaxial layer and process
CN106960788A (en) * 2017-03-31 2017-07-18 华中科技大学 A kind of preparation method of drift step recovery diode and products thereof

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102956822A (en) * 2011-08-19 2013-03-06 三星电子株式会社 Nonvolatile memory elements and memory devices including same
CN104201211A (en) * 2014-08-27 2014-12-10 温州大学 Base region gradient P<+>-N-N<+> type SiC ultrafast recovery diode manufactured on 4H type single crystal silicon carbide epitaxial layer and process
CN106960788A (en) * 2017-03-31 2017-07-18 华中科技大学 A kind of preparation method of drift step recovery diode and products thereof

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112563320A (en) * 2020-11-29 2021-03-26 中国电子科技集团公司第五十五研究所 Method for improving performance of high-voltage drift step recovery device
CN113009425A (en) * 2021-02-23 2021-06-22 电子科技大学 Pulse compression structure based on SiC DSRD device
CN113009425B (en) * 2021-02-23 2022-08-05 电子科技大学 Pulse compression structure based on SiC DSRD device

Similar Documents

Publication Publication Date Title
CN103383957B (en) A kind of inverse conductivity type IGBT device
CN109075214A (en) Groove MOS type Schottky diode
CN106206701B (en) The reversed conductive IGBT of control
CN102544114B (en) Accumulation type grooved-gate diode
CN110352498A (en) Groove MOS type Schottky diode
CN103346084A (en) Gallium nitride Schottky diode of novel structure and manufacturing method thereof
CN105826399A (en) Soft fast recovery diode of multi-mixture structure and preparation method thereof
CN109087954A (en) A kind of silicon carbide drift step recovery diode
US9543462B2 (en) Insulated-gate photoconductive semiconductor switch
CN102593154B (en) Trench gate diode with P-type buried layer structure
CN103956381B (en) MOS grid-control thyristor
CN102709317B (en) Low-threshold voltage diode
CN107393970B (en) Silicon carbide junction barrier diode
Grekhov et al. Sub-nanosecond semiconductor opening switches based on 4H–SiC p+ pon+-diodes
CN108574016A (en) A kind of the silicon carbide DSRD devices and Pulsed power generator of super-junction structure
CN108155225A (en) Constant current device and its manufacturing method
Wessels et al. Vertical channel field-controlled thyristors with high gain and fast switching speeds
CN203179900U (en) A fast recovery diode FRD chip
CN105826406B (en) A kind of insulated-gate type photoconductivity switching
CN108735832B (en) Transverse insulated gate type photoconductive switch and manufacturing method thereof
CN109065636A (en) A kind of drift step recovery diode
RU156013U1 (en) SILICON CARBIDE SILICON DRIFT DIODE
CN110061048B (en) MOS field-controlled thyristor based on Schottky diode and manufacturing method thereof
CN109065614A (en) A kind of silicon carbide gate level turn-off thyristor
CN210325811U (en) Silicon carbide heterojunction diode power device

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
RJ01 Rejection of invention patent application after publication
RJ01 Rejection of invention patent application after publication

Application publication date: 20181225