2021
DOI: 10.1021/acs.jpcb.1c08552
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Autobiography of Yoshitaka Tanimura

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Cited by 5 publications
(5 citation statements)
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“…For this approach an underdamped HEOM is derived from the multi-component spectral density resulting in a multi-component HEOM. [63] Note that when the vibration is subsumed into the bath, γ 1 introduces additional damping which is not present when the vibration is contained in the Hamiltonian. Approaching the limit γ 1 → 0, the two approaches become equivalent as discussed within ref.…”
Section: B Open System Modelmentioning
confidence: 99%
“…For this approach an underdamped HEOM is derived from the multi-component spectral density resulting in a multi-component HEOM. [63] Note that when the vibration is subsumed into the bath, γ 1 introduces additional damping which is not present when the vibration is contained in the Hamiltonian. Approaching the limit γ 1 → 0, the two approaches become equivalent as discussed within ref.…”
Section: B Open System Modelmentioning
confidence: 99%
“…This is handled in a consistent manner by the theory of open quantum systems. [ 1,2 ] Open system ideas find use in a wide range of fields ranging from quantum optics, [ 3,4 ] to condensed matter, [ 5,6 ] quantum statistical physics, [ 7–9 ] quantum chemistry, [ 10–12 ] and quantum biology. [ 13 ] In the last decade, its applications to the field of quantum information have seen phenomenal growth.…”
Section: Introductionmentioning
confidence: 99%
“…The typically computed ZPL and PSB (often called phonon wing) assume Lorentzian shape (which is a consequence of employing nearly Debye spectral density‐like, vide supra ) in the frequency domain. This is also a consequence of exponential dephasing in the time domain, which may be ascribed to a host of factors (e. g., neglecting nonMarkovianity, [38–51] nonCondonicity, [52–60] anharmonicity, [60–78] etc.) when modeling the total Hamiltonian to be used in the time evolution operator.…”
Section: Introductionmentioning
confidence: 99%