1973
DOI: 10.1088/0022-3719/6/9/005
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On the Green function for a particle in a uniform electric field

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Cited by 38 publications
(24 citation statements)
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“…Multiplying both sides of (9) by 1 / (Z a 2 −Z 2 ) we integrate over (a, ∞) with respect to Z. Interchanging the order of integration and using (30) we obtain (28). Taking the Hilbert transform of (28) yields (29).…”
Section: Proofmentioning
confidence: 99%
“…Multiplying both sides of (9) by 1 / (Z a 2 −Z 2 ) we integrate over (a, ∞) with respect to Z. Interchanging the order of integration and using (30) we obtain (28). Taking the Hilbert transform of (28) yields (29).…”
Section: Proofmentioning
confidence: 99%
“…To deal with the transient current in open systems, a major approach is the embedding scheme (calculate a finite region in an extended environment with the help of self‐energy). For example, the open boundary condition derived from partitioned propagators is employed for the equation of motions (EOM) of the density matrix ; and the transparent boundary condition is employed for the wavefunction propagations . Another approach is to use finite leads with large lengths to mimic the open terminals and calculate the currents in a limited duration, as in Ref.…”
Section: Introductionmentioning
confidence: 99%
“…When |z| is large, we employ Hankel's asymptotic series 27 for the Hankel functions in Eq. (23), in this way obtaining for any α > −1/2 and |arg(z)| < π:…”
Section: Application Class: the Spherical Wave Continuummentioning
confidence: 94%
“…Poles in the complex E-plane of the continued resolvent operator for H 0 + V (i.e., resonances) also have been studied for this model potential. [23][24][25][26] Again, one of these is characterized by a real part that approaches E b as F → 0 (plus an imaginary part that vanishes exponentially with F in this limit). In fact, the equation for the resonance energies is just Eq.…”
Section: B Example: Particle Bound To a Delta Well In A Uniform Fieldmentioning
confidence: 99%