Classical and quantum spreading of a charge pulse
arXiv:1406.7232 · doi:10.1109/IWCE.2014.6865808
Abstract
With the technical progress of radio-frequency setups, high frequency quantum transport experiments have moved from theory to the lab. So far the standard theoretical approach used to treat such problems numerically--known as Keldysh or NEGF (Non Equilibrium Green's Functions) formalism--has not been very successful mainly because of a prohibitive computational cost. We propose a reformulation of the non-equilibrium Green's function technique in terms of the electronic wave functions of the system in an energy-time representation. The numerical algorithm we obtain scales now linearly with the simulated time and the volume of the system, and makes simulation of systems with 10^5 - 10^6 atoms/sites feasible. We illustrate our method with the propagation and spreading of a charge pulse in the quantum Hall regime. We identify a classical and a quantum regime for the spreading, depending on the number of particles contained in the pulse. This numerical experiment is the condensed matter analogue to the spreading of a Gaussian wavepacket discussed in quantum mechanics textbooks.
arXiv comment4 pages, 5 figures; to be published in IEEE Xplore, in Proceedings to IEEE 17th International Workshop on Computational Electronics 2014, June 3 - 6, 2014, Paris, France. Correction of typographic mistakes and update of ref. 11
References in corpus (9)
- Kwant: a software package for quantum transport
- An On-Demand Coherent Single Electron Source
- Coherence and Indistinguishability of Single Electrons Emitted by Independent Sources
- Novel Edge Excitations of Two-dimensional Electron Liquid in a Magnetic Field
- A knitting algorithm for calculating Green functions in quantum systems
- Numerical simulations of time resolved quantum electronics
- Dynamical control of interference using voltage pulses in the quantum regime
- Carrier drift velocity and edge magnetoplasmons in graphene
- Numerical cookbook for electronic quantum transport at finite frequency