Wigner equation for general electromagnetic fields: The Weyl-Stratonovich transform

M. Nedjalkov, J. Weinbub, M. Ballicchia, S. Selberherr, I. Dimov, and D. K. Ferry
Phys. Rev. B 99, 014423 – Published 22 January 2019

Abstract

Gauge-invariant Wigner theories are formulated in terms of the kinetic momentum, which—being a physical quantity—is conserved after a change of the gauge. These theories rely on a transform of the density matrix, originally introduced by Stratonovich, which generalizes the Weyl transform by involving the vector potential. We thus present an alternative derivation of the Weyl-Stratonovich transform, which bridges the concepts and notions used by the different, available gauge-invariant approaches and thus links physically intuitive with formal mathematical viewpoints. Furthermore, an explicit form of the Wigner equation, suitable for numerical analysis and corresponding to general, inhomogeneous, and time-dependent electromagnetic conditions, is obtained. For a constant magnetic field, the equation reduces to two models: in the case of a constant electric field, this is the ballistic Boltzmann equation, where classical particles are driven by local forces. The second model, derived for general electrostatic conditions, involves novel physics, where the magnetic field acts locally via the Liouville operator, while the electrostatics is determined by the manifestly nonlocal Wigner potential. A significant consequence of our work is the fact that now the constant magnetic field case can be treated with existing numerical approaches developed for the standard, scalar potential Wigner theory. Therefore, in order to demonstrate the feasibility of the approach, a stochastic method is applied to simulate a physically intuitive evolution problem.

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  • Received 11 June 2018
  • Revised 17 December 2018

DOI:https://doi.org/10.1103/PhysRevB.99.014423

©2019 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied PhysicsNonlinear Dynamics

Authors & Affiliations

M. Nedjalkov1, J. Weinbub2,*, M. Ballicchia1, S. Selberherr1, I. Dimov3, and D. K. Ferry4

  • 1Institute for Microelectronics, TU Wien, Gußhausstraße 27-29/E360, 1040 Vienna, Austria
  • 2Christian Doppler Laboratory for High Performance TCAD, Institute for Microelectronics, TU Wien, Gußhausstraße 27-29/E360, 1040 Vienna, Austria
  • 3Institute of Information and Communication Technologies, Bulgarian Academy of Sciences, Acad. G. Bonchev St., Block 25A, 1113 Sofia, Bulgaria
  • 4School of Electrical, Computer, and Energy Engineering, Arizona State University, 85287-5706 Tempe, Arizona, USA

  • *Corresponding author: josef.weinbub@tuwien.ac.at

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Vol. 99, Iss. 1 — 1 January 2019

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