Stimulated Raman adiabatic passage in a -system in the presence of quantum noise
arXiv:1008.1549 · doi:10.1103/PhysRevA.83.012101
Abstract
We exploit a microscopically derived master equation for the study of STIRAP in the presence of decay from the auxiliary level toward the initial and final state, and compare our results with the predictions obtained from a phenomenological model previously used [P. A. Ivanov, N. V. Vitanov, and K. Bergmann, Phys. Rev. A 72, 053412 (2005)]. It is shown that our approach predicts a much higher efficiency. The effects of temperature are also taken into account, proving that in b-STIRAP thermal pumping can increase the efficiency of the population transfer.
10 pages, 7 figures
References in corpus (6)
- Microscopic derivation of the Jaynes-Cummings model with cavity losses
- The quantitative condition is necessary in guaranteeing the validity of the adiabatic approximation
- Dissipation and entanglement dynamics for two interacting qubits coupled to independent reservoirs
- Stimulated Raman adiabatic passage in an open quantum system: Master equation approach
- Population trapping due to cavity losses
- Theory versus experiment for vacuum Rabi oscillations in lossy cavities (II): Direct test of uniqueness of vacuum
Cited by in corpus (10)
- Microscopic description of dissipative dynamics of a level crossing transition
- Avoiding leakage and errors caused by unwanted transitions in Lambda systems
- Stimulated Raman Adiabatic control of a nuclear spin in diamond
- Interaction-free evolution in the presence of time-dependent Hamiltonians
- Steepest Entropy Ascent for Two-State Systems with Slowly Varying Hamiltonians
- Stimulated Raman Adiabatic Passage via bright state in Lambda medium of unequal oscillator strengths
- Explicit construction of nonadiabatic passages for stimulated Raman transitions
- Fast and robust production of quantum superposition states by the fractional shortcut to adiabaticity
- Adiabatic manipulation of a system interacting with a spin-bath
- Robust switching of superposition-states via a coherent double stimulated Raman adiabatic passage