Non-Reciprocity of the Wave Packet Scattering Delay in Ballistic Two-Terminal Devices
arXiv:2009.07584 · doi:10.1103/PhysRevB.103.035404
Abstract
In the linear regime, transport properties of ballistic two-terminal devices are generally considered to be independent of the direction of the current. This two-terminal reciprocity applies to both the electron transmission and reflection probabilities. However, it does not apply to the scattering delays of wave packets. Indeed, \emph{four} different time delays describe the transmission and reflection processes of wave packets arriving from the two terminals, respectively. Unlike the probabilities, these delays are direction dependent if the channel exchange symmetry of the scattering matrix is broken.
References in corpus (11)
- Partial Densities of States, Scattering Matrices, and Green's Functions
- Magnetic-field asymmetry of nonlinear mesoscopic transport
- Electrical control of a solid-state flying qubit
- Wigner time delay and related concepts -- Application to transport in coherent conductors
- Mesoscopic fluctuations of nonlinear conductance of chaotic quantum dots
- Picosecond coherent electron motion in a silicon single-electron source
- Direct measurement of the Wigner time-delay for the scattering of light by a single atom
- Control of the transmission phase in an asymmetric four-terminal Aharonov-Bohm interferometer
- Magnetic-field asymmetry of electron wave packet transmission in bent channels capacitively coupled to a metal gate
- Violation of Onsager symmetry for a ballistic channel Coulomb coupled to a quantum ring
- Topologically protected wave packets and quantum rings in silicene
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- Asymmetric Transmission Through a Classical Analogue of the Aharonov-Bohm Ring
- Non-unitary Quantum Electronics: Novel Functions from the Edge of the Quantum World