2017
DOI: 10.1063/1.4997669
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The study of an extended hierarchy equation of motion in the spin-boson model: The cutoff function of the sub-Ohmic spectral density

Abstract: Following a recently proposed decomposition technique [C. R. Duan et al., Phys. Rev. B 95, 214308 (2017)], we inspect the zero-temperature spin-boson model for five different cutoff functions of the spectral density. With oscillatory and non-oscillatory exponentially decaying functions to decompose the bath correlation function, the hierarchy equation of motion is reliably extended to each spectral density under our investigation. The predicted spin dynamics is gradually converged with the increase of the hier… Show more

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Cited by 25 publications
(17 citation statements)
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“…136 To obtain a numerically converged solution as the thermal equilibrium state, it is important to express the noise correlation function in terms of the decaying functions as c j exp(−ζ j t) or c j exp(−ζ j ± iω j ), where c j , ζ j , and ω j characterize the noise correlation for the jth hierarchical elements, to maintain the positivity of the HEOM formalism. [137][138][139][140][141][142][143][144][145][146][147][148] Although the HEOM can be constructed for an arbitrary SDF in the form of a Fourier expansion 87 or in terms of special functions, [149][150][151][152][153][154][155][156] the HEOM that are derived from a finite set of non-timedecaying functions do not converge in time and thus may not describe phenomena toward the thermal equilibrium state.…”
Section: F the Bathentanglement States And The Positivity Of The Heommentioning
confidence: 99%
See 1 more Smart Citation
“…136 To obtain a numerically converged solution as the thermal equilibrium state, it is important to express the noise correlation function in terms of the decaying functions as c j exp(−ζ j t) or c j exp(−ζ j ± iω j ), where c j , ζ j , and ω j characterize the noise correlation for the jth hierarchical elements, to maintain the positivity of the HEOM formalism. [137][138][139][140][141][142][143][144][145][146][147][148] Although the HEOM can be constructed for an arbitrary SDF in the form of a Fourier expansion 87 or in terms of special functions, [149][150][151][152][153][154][155][156] the HEOM that are derived from a finite set of non-timedecaying functions do not converge in time and thus may not describe phenomena toward the thermal equilibrium state.…”
Section: F the Bathentanglement States And The Positivity Of The Heommentioning
confidence: 99%
“…Alternatively, we can extend the HEOM for arbitrary SDFs using Fourier, 89 Gauss-Legendre, or Chebyshevquadrature spectral decompositions (eHEOM). [149][150][151][152][153][154][155][156] This approach allowed the investigation of a spin-boson system coupled to a bath with sub-Ohmic SDF at zero temperature. [153][154][155] An extension of the HEOM for a combination of exponential/non-exponential bath correlation functions has also been presented.…”
Section: A Heom For Arbitrary Spectral Distribution Functionsmentioning
confidence: 99%
“…Much like our number of surrogate modes, the number of exponentials needed for an adequate fit is one of the main factors determining complexity of HEOM simulations, the other being the tier at which the hierarchy needs to be truncated. This number should be the same for the two methods if one requires the same accuracy and uses efficient expansion techniques for the correlation function [115,116] (these overcome the well-known problem of the more traditional Matsubara-frequency expansion [117,118], which at low temperatures needs a very large number of exponential terms in order to converge). HEOM scales with the complexity of the spectral density in a similar manner as our method and can likewise account implicitly for temperature through the approximate correlation function.…”
Section: Impactmentioning
confidence: 99%
“…While HEOM is, in principle, exact for systems interacting with arbitrary harmonic baths, practically, it has been mostly restricted to simulating the case of baths described by a Drude spectral densities. Attempts have been made to develop efficient HEOM-based algorithms that are applicable to general spectral densities [8,[10][11][12][13]. In case the solvent is atomistically defined and anharmonic effects are important, the IF does not have a closed-form expression.…”
Section: Introductionmentioning
confidence: 99%