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Analytic propagators for spin–orbit interactions

Bailey C Hsu and Jean-François S Van Huele

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We derive analytic expressions for propagators in spin–orbit coupled systems. In addition to their kinetic energy, these systems exhibit a potential energy that mixes position, momentum and spin operators. We consider Hamiltonians with limited noncommutativities: the confined spin–orbit coupled Hamiltonian H_{\rm SO}^{c}=\frac{{\bf p}^2}{2m}+\gamma {\bm \sigma} {\,\bm \cdot\,} {\bf L}+\frac{1}{2}m\eta ^2 (x^2+y^2) , the confined Equal–Strength–Rashba–Dresselhaus Hamiltonian H_{\rm ESRD}^{c}=\frac{{\bf p}^2}{2m}+\frac{\alpha}{\hbar}(p_x+ p_y)(\sigma _x-\sigma _y)+\frac{1}{2}m\eta ^2(x^2+y^2) and the confined Opposite–Strength–Rashba–Dresselhaus Hamiltonian H_{\rm OSRD}^{c}=\frac{{\bf p}^2}{2m}+\frac{\alpha}{\hbar}(p_x- p_y)(\sigma _x+\sigma _y)+\frac{1}{2}m\eta ^2(x^2+y^2) . We use both a classical action method and an algebraic method in our derivations. We mention specific applications for these propagators and illustrate their significance with examples of wavepacket evolution.


PACS

31.15.-p Calculations and mathematical techniques in atomic and molecular physics

31.10.+z Theory of electronic structure, electronic transitions, and chemical binding

02.10.Ud Linear algebra

MSC

17Bxx Lie algebras and Lie superalgebras (For Lie groups, see 22Exx)

70Hxx Hamiltonian and Lagrangian mechanics (See also 37Jxx)

81V45 Atomic physics

Subjects

Atomic and molecular physics

Mathematical physics

Computational physics

Dates

Issue 47 (27 November 2009)

Received 22 June 2009, in final form 28 September 2009

Published 6 November 2009



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