Physical basis for high-power semiconductor nanosecond opening switches

The physical basis for semiconductor nanosecond opening switches is a specially organized recovery process in the diode. There are two modes of this process: junction recovery (JR) mode and silicon opening switch (SOS) mode. In the JR mode, the current interruption occurs due to the recovery of pn-j...

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Published inIEEE transactions on plasma science Vol. 28; no. 5; pp. 1540 - 1544
Main Authors Grekhov, I.V., Mesyats, G.A.
Format Journal Article
LanguageEnglish
Published New York IEEE 01.10.2000
The Institute of Electrical and Electronics Engineers, Inc. (IEEE)
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Abstract The physical basis for semiconductor nanosecond opening switches is a specially organized recovery process in the diode. There are two modes of this process: junction recovery (JR) mode and silicon opening switch (SOS) mode. In the JR mode, the current interruption occurs due to the recovery of pn-junction blocking capability, and in the SOS mode, due to the drastic increase in resistance of low-doped part of p-layer, where reverse current density exceeds the saturated value j/sub r/>qN/sub d/V/sub s/. JR mode is preferable for generators with a pulse rise-time of 0.5-3 ns and a pulse of power of less than 50-80 MW, and SOS mode at pulse rise-time of more than 5 ns for any pulse power and at any pulse rise-time if power is higher than 100 MW.
AbstractList The physical basis for semiconductor nanosecond opening switches is a specially organized recovery process in the diode. There are two modes of this process: junction recovery (JR) mode and silicon opening switch (SOS) mode. In the JR mode, the current interruption occurs due to the recovery of pn-junction blocking capability, and in the SOS mode, due to the drastic increase in resistance of low-doped part of p-layer, where reverse current density exceeds the saturated value j/sub r/>qN/sub d/V/sub s/. JR mode is preferable for generators with a pulse rise-time of 0.5-3 ns and a pulse of power of less than 50-80 MW, and SOS mode at pulse rise-time of more than 5 ns for any pulse power and at any pulse rise-time if power is higher than 100 MW.
The physical basis for semiconductor nanosecond opening switches is a specially organized recovery process in the diode. There are two modes of this process: the junction recovery (JR) mode and the silicon opening switch (SOS) mode. In the JR mode, the current interruption occurs due to the recovery of pn-junction blocking capability, and in the SOS mode, due to the drastic increase in resistance of low-doped part of the p-layer, where reverse current density exceeds the saturated value j(r) > qN(d)V(S). The JR mode is preferable for generators with a pulse rise-time of 0.5-3 ns and a pulse of power of less than 50-80 MW, and the SOS mode at a pulse rise-time of more than 5 ns for any pulse power and at any pulse rise-time if the power is higher than 100 MW. (Author)
The physical basis for semiconductor nanosecond opening switches is a specially organized recovery process in the diode. There are two modes of this process: junction recovery (JR) mode and silicon opening switch (SOS) mode.
The physical basis for semiconductor nanosecond opening switches is a specially organized recovery process in the diode. There are two modes of this process: junction recovery (JR) mode and silicon opening switch (SOS) mode. In the JR mode, the current interruption occurs due to the recovery of pn-junction blocking capability, and in the SOS mode, due to the drastic increase in resistance of low-doped part of p-layer, where reverse current density exceeds the saturated value j sub(r)>qN sub(d)V sub(s). JR mode is preferable for generators with a pulse rise-time of 0.5-3 ns and a pulse of power of less than 50-80 MW, and SOS mode at pulse rise-time of more than 5 ns for any pulse power and at any pulse rise-time if power is higher than 100 MW
The physical basis for semiconductor nanosecond opening switches is a specially organized recovery process in the diode. There are two modes of this process: junction recovery (JR) mode and silicon opening switch (SOS) mode. In the JR mode, the current interruption occurs due to the recovery of pn-junction blocking capability, and in the SOS mode, due to the drastic increase in resistance of low-doped part of p-layer, where reverse current density exceeds the saturated value j(r) > qN(d)V(s). JR mode is preferable for generators with a pulse rise-time of 0.5-3 ns and a pulse of power of less than 50-80 MW, and SOS mode at pulse rise-time of more than 5 ns for any pulse power and at any pulse rise-time if power is higher than 100 MW
Author Mesyats, G.A.
Grekhov, I.V.
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Cites_doi 10.1109/PPC.1997.679367
10.1016/0038-1101(85)90130-3
10.1109/PPC.1997.674522
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References lyubutin (ref4) 1992
darznek (ref5) 1994; 334
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  doi: 10.1016/0038-1101(85)90130-3
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  year: 1992
  ident: ref4
  article-title: investigation of semiconductor opening switch using in high power pulse generators with inductive storage
  publication-title: Proc 9th Symp High-Current El
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    fullname: lyubutin
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  doi: 10.1109/PPC.1997.674522
– volume: 334
  start-page: 304
  year: 1994
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  article-title: sos-effect: nanosecond break of ultrahigh density current in semiconductors
  publication-title: Doklady RAN
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    fullname: darznek
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Snippet The physical basis for semiconductor nanosecond opening switches is a specially organized recovery process in the diode. There are two modes of this process:...
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StartPage 1540
SubjectTerms Current density
Diodes
Electricity
Immune system
Industrial power systems
Nanocomposites
Nanomaterials
Nanostructure
Physics
Plasma
Plasma applications
Power generation
Power semiconductor switches
Pulse generation
Pulse power systems
Recovery
Semiconductor diodes
Semiconductors
Silicon
Switches
Title Physical basis for high-power semiconductor nanosecond opening switches
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