Theory of electron-avalanche breakdown in solids

M. Sparks, D. L. Mills, R. Warren, T. Holstein, A. A. Maradudin, L. J. Sham, E. Loh, Jr., and D. F. King
Phys. Rev. B 24, 3519 – Published 15 September 1981
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Abstract

Electron-avalanche breakdown in solids is explained by a theory that agrees with experimental results for the magnitude of the breakdown field and its temperature dependence, pulse-duration dependence, material-to-material variation, and wavelength dependence for λ1 μ m. The good agreement between experiment and theory with no parameters adjusted is obtained by using improved magnitudes and energy dependences of the electron-phonon relaxation frequencies. The contributions of both optical and acoustical phonons to electron loss and energy-space diffusion must be included. The breakdown field EB is calculated by solving an eigenvalue equation obtained from the diffusion-transport equation. Simple models and interpretations of the diffusion equation afford physical insight into breakdown and render the breakdown conditions predictable. Preliminary results indicate that the diffusion approximation fails for wavelengths considerably shorter than 1 μ m, where multiphoton absorption must also be considered.

  • Received 21 May 1981

DOI:https://doi.org/10.1103/PhysRevB.24.3519

©1981 American Physical Society

Authors & Affiliations

M. Sparks, D. L. Mills*, R. Warren, T. Holstein, A. A. Maradudin*, L. J. Sham, E. Loh, Jr.§, and D. F. King

  • Pacific-Sierra Research Corporation, Santa Monica, California 90404

  • *Permanent address: University of California at Irvine, Irvine, California.
  • Permanent address: University of California at Los Angeles, Los Angeles, California.
  • Permanent address: University of California at San Diego, La Jolla, California.
  • §Permanent address: Malibu, California.

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Vol. 24, Iss. 6 — 15 September 1981

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