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K. Kambour, H. P. Hjalmarson, F. J. Zutavern and A. Mar

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Presentation on theme: "K. Kambour, H. P. Hjalmarson, F. J. Zutavern and A. Mar"— Presentation transcript:

1 Simulation of Current Filaments in Photoconductive Semiconductor Switches
K. Kambour, H. P. Hjalmarson, F. J. Zutavern and A. Mar Sandia National Laboratories* Charles W. Myles** Texas Tech University 15th International IEEE Pulsed Power Conference June 16, 2005 * Sandia is a multiprogram laboratory operated by Sandia Corporation, a Lockheed Martin company, for the United States Department of Energy under contract DE-AC04-94AL85000. ** Supported in part by an AFOSR MURI Contract

2 Outline Photoconductive Semiconductor Switches (PCSS's) Lock-on
Collective Impact Ionization Theory Monte Carlo Calculations Continuum Calculations Conclusions

3 A PCSS

4 Lock-on Characterized by a persistent or 'locked-on' electric field (~5 kV/cm) after laser turn off. High conductivity state Always accompanied by the formation of current filaments. The lock-on field is much lower than the bulk breakdown field for GaAs.

5 Current Filaments

6 Bistable Switch

7 Carrier Distribution Function

8 Collective Impact Ionization Theory
Explains highly conductive filaments sustained by a lock-on field lower than the breakdown field. Inside (high carrier density): the carrier-carrier scattering increases the efficiency of impact ionization for the hot carriers. Outside (low carrier density): the electric field is too low to create carriers by impact ionization.

9 Monte Carlo Calculations
Calculating the rate of change of particle number Determining the distribution function Ensemble Monte Carlo Maxwellian

10 Evolution to a Steady State Solution (no carrier-carrier scattering)

11 Steady State Solution (no carrier-carrier scattering)

12 Evolution to Steady State Solutions (carrier-carrier scattering included)

13 Steady State Solutions (carrier-carrier scattering)

14 GaAs

15 Continuum Calculations

16 Continuum Results

17 Continuum Results V0 (KV) t (sec) VLO 50 30 1x10-9 40 1x10-10
30 1x10-9 40 1x10-10 no lock-on 1x10-11 200 60

18 Conclusions Collective Impact ionization Theory (CIIT) predicts that lock-on will occur in GaAs at a field much less than the intrinsic breakdown field in GaAs, in qualitative agreement with experiment. CIIT also predicts that the lock-on field will be independent of rise time and that the lock-on current will flow in stable current filaments in agreement with experiment.


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