Quantum Noise: A Handbook of Markovian and Non-Markovian Quantum Stochastic Methods with Applications to Quantum Optics

By A. Galindo, P. Pascual. 2004

1,172 citations recorded by the source corpus.

View Paper: https://www.semanticscholar.org/paper/41da4d7f08b638ca4443e15f2d597d3cd8098f63

Citations in the corpus

• Attosecond chronoscopy of photoemission (2015, unknown): “For large systems with many degrees of freedom (“open quantum systems”) classical time information is expected to emerge from time-dependent quantum dynamics via decoherence and dephasing (Zurek, 2003; Gardiner and Zoller, 2004; Weiss, 2012).”
• Control of quantum phenomena: past, present and future (2009, unknown): “Various types of quantum master equations can be derived from the Kraus OSR under additional assumptions [168, 169].”
• Dispersive regime of circuit QED : Photon-dependent qubit dephasing and relaxation rates (2008, unknown): “In a homodyne measurement, with a local oscillator set to ∼ ωr, the bath is projected in an eigenstate of the operator dBκ,r + dB † κ,r (where dBκ,r is defined in appendix B), with measurement result J [33].”
• System-reservoir dynamics of quantum and classical correlations (2009, unknown): “Although the master equation approach is widely used, especially in quantum optics [30], there is another way to treat open quantum systems, which is more appropriate for our”
• Quantum physics of simple optical instruments (2003, unknown): “To understand how to model such irreversible processes requires some theory [33, 42, 56, 57, 120].”
• Ultracold atomic gases in optical lattices: mimicking condensed matter physics and beyond (2006, unknown): “Perhaps the most sophisticated theoretical contributions concerned understanding of quantum fluctuations and quantum noise [6, 7].”
• Unconventional photon blockade (2017, unknown): “For zero thermal occupations n̄th = 0 all the normally ordered field/noise correlations vanish [46] and the subsequent output occupation and second order correlation read [29]”
• Superconducting qubit in a waveguide cavity with a coherence time approaching 0.1 ms (2012, unknown): “We represent thermal driving of the resonator by the master equation [13]”
• Cold atoms in cavity-generated dynamical optical potentials (2012, unknown): “by a Heisenberg-Langevin equation (Gardiner and Zoller, 2004) for the cavity field operator a,”
• Quantum Measurement and Control: Frontmatter (2009, unknown): “with a Planck distribution of photon numbers [GZ04]).”
• Interacting two-level defects as sources of fluctuating high-frequency noise in superconducting circuits (2015, unknown): “We note that in a master equation description of dissipative quantum dynamics the relaxation rate of a qubit is proportional to the unsymmetrized spectrum of its environment at the frequency of the qubit’s level-splitting, Γ1 ∝ C(ω10) [34].”
• Quantum trajectory approach to circuit QED: Quantum jumps and the Zeno effect (2007, unknown): “The evolution equation of this conditional state is referred to as a stochastic master equation (SME) [1, 2, 3, 4, 5, 13, 15, 19].”
• Giant acoustic atom: A single quantum system with a deterministic time delay (2016, unknown): “(C1) can be computed through the so-called quantum regression formula [18,59] 〈c1(t1)c2(t2) .”
• Rare‐region effects and dynamics near the many‐body localization transition (2016, unknown): “plus bath can be described by a quantum master equation in Lindblad form [92, 93].”
• Random Quantum Circuits (2022, unknown): “the Bloch sphere, with measurements causing “quantum jumps” (99, 100, 101, 102, 103, 104) to the North or South pole (Sec.”