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Volumn 59, Issue 19, 1999, Pages 12398-12418

Thermodynamics of the dissipative two-state system: a bethe-ansatz study

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[No Author keywords available]

Indexed keywords


EID: 0000269885     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.59.12398     Document Type: Article
Times cited : (52)

References (72)
  • 8
    • 0004258958 scopus 로고
    • Yu Lu World Scientific, Singapore, S. O. Lundquist I. E. Dzyaloshinskii, Vol. 2.
    • U. Weiss, in Series in Modern Condensed Matter Physics, edited by I. E. Dzyaloshinskii, S. O. Lundquist, and Yu Lu (World Scientific, Singapore, 1993), Vol. 2.
    • (1993) Series in Modern Condensed Matter Physics
    • Weiss, U.1
  • 11
    • 85037902105 scopus 로고    scopus 로고
    • For a review, see Refs. 4 and 5. For some recent work see Refs. 22, 23, 24, 25
    • For a review, see Refs. 4 and 5. For some recent work see Refs. 22232425;
  • 15
    • 85037901943 scopus 로고    scopus 로고
    • We define “coherence” to mean the presence of oscillatory contributions to real time dynamical quantities, such as (Formula presented) and (Formula presented) This implies that the system exhibits phase coherence in time.
    • We define “coherence” to mean the presence of oscillatory contributions to real time dynamical quantities, such as (Formula presented) and (Formula presented) This implies that the system exhibits phase coherence in time.
  • 16
    • 85037902008 scopus 로고    scopus 로고
    • Certain correlations, such as (Formula presented) have long time (Formula presented) tails at (Formula presented) as their leading contribution. The exponential decay then refers to the oscillatory contribution which is a subleading contribution.
    • Certain correlations, such as (Formula presented) have long time (Formula presented) tails at (Formula presented) as their leading contribution. The exponential decay then refers to the oscillatory contribution which is a subleading contribution.
  • 32
    • 85037884280 scopus 로고    scopus 로고
    • This difficulty is due to the fact that the local (Formula presented) in the AKM is not conserved as opposed to total (Formula presented) component of the spin. A discussion where this problem arises for similar quantities can be found in
    • This difficulty is due to the fact that the local (Formula presented) in the AKM is not conserved as opposed to total (Formula presented) component of the spin. A discussion where this problem arises for similar quantities can be found in
  • 38
    • 85037920319 scopus 로고    scopus 로고
    • By tunneling regime we mean the regime where there is a finite renormalized tunneling amplitude (Formula presented) In the limit (Formula presented) this region is (Formula presented) For finite (Formula presented) it depends also on (Formula presented) as discussed in Sec. II C. The tunneling regime consists of two qualitatively different regions, distinguished by the presence (for (Formula presented) or absence (for (Formula presented) of tunneling oscillations in time-dependent quantities.
    • By tunneling regime we mean the regime where there is a finite renormalized tunneling amplitude (Formula presented) In the limit (Formula presented) this region is (Formula presented) For finite (Formula presented) it depends also on (Formula presented) as discussed in Sec. II C. The tunneling regime consists of two qualitatively different regions, distinguished by the presence (for (Formula presented) or absence (for (Formula presented) of tunneling oscillations in time-dependent quantities.
  • 43
    • 85037884095 scopus 로고    scopus 로고
    • Note, however, that in region (Formula presented) (Formula presented) can be irrelevant to start with for (Formula presented) but will eventually become relevant once α decreases to (Formula presented) This does not happen in regions (Formula presented) and (Formula presented)
    • Note, however, that in region (Formula presented) (Formula presented) can be irrelevant to start with for (Formula presented) but will eventually become relevant once α decreases to (Formula presented) This does not happen in regions (Formula presented) and (Formula presented)
  • 44
    • 85037875046 scopus 로고    scopus 로고
    • The appearance of the factor of α relating the two scales (Formula presented) and (Formula presented) stems from the introduction of electron-electron interactions into the AKM to ensure integrability within the Bethe ansatz (without such interactions we could simply write (Formula presented). This results in susceptibilities being renormalized by a factor (Formula presented) within the Bethe-ansatz calculations (see Sec. III B 3 for details), so in order to relate the scales of the AKM and the Ohmic two-state system from the (Formula presented) susceptibility of the Bethe-ansatz calculation one needs to include this factor.
    • The appearance of the factor of α relating the two scales (Formula presented) and (Formula presented) stems from the introduction of electron-electron interactions into the AKM to ensure integrability within the Bethe ansatz (without such interactions we could simply write (Formula presented). This results in susceptibilities being renormalized by a factor (Formula presented) within the Bethe-ansatz calculations (see Sec. III B 3 for details), so in order to relate the scales of the AKM and the Ohmic two-state system from the (Formula presented) susceptibility of the Bethe-ansatz calculation one needs to include this factor.
  • 48
    • 85037900722 scopus 로고    scopus 로고
    • We emphasize the distinction we are making between the susceptibility of the AKM and the susceptibility of the AKM calculated from the BA which involves modifications to the model in order to make it integrable. The distinction, as shown below, is important.
    • We emphasize the distinction we are making between the susceptibility of the AKM and the susceptibility of the AKM calculated from the BA which involves modifications to the model in order to make it integrable. The distinction, as shown below, is important.
  • 51
    • 4444357821 scopus 로고    scopus 로고
    • G. Zaránd and Jan von Delft Phys Rev. B (to be published).
    • Jan von Delft, G. Zaránd, and M. Fabrizio, Phys. Rev. Lett. 81, 196 (1998);G. Zaránd and Jan von Delft Phys Rev. B (to be published).
    • (1998) Phys. Rev. Lett. , vol.81 , pp. 196
    • Zaránd, G.1    Fabrizio, M.2
  • 55
    • 85037923269 scopus 로고    scopus 로고
    • The appearance of a well-defined oscillatory mode, in the sense we have described, should be distinguished with the appearance of tunneling oscillations or “coherence” which happens at (Formula presented) (Ref. 8
    • The appearance of a well-defined oscillatory mode, in the sense we have described, should be distinguished with the appearance of tunneling oscillations or “coherence” which happens at (Formula presented) (Ref. 8).
  • 71
    • 85037903000 scopus 로고    scopus 로고
    • We used those in the Numerical Algorithms Group (NAG) library.
    • We used those in the Numerical Algorithms Group (NAG) library.
  • 72
    • 85037900989 scopus 로고    scopus 로고
    • The reason for the exponential decay of (Formula presented) (Formula presented) for (Formula presented) (Formula presented) is clear from the form of (Formula presented) (Formula presented) and the values which the functions (Formula presented) take at the boundaries (Formula presented) For definiteness consider (Formula presented) then (Formula presented) It can be shown that the (Formula presented) are monotonically decreasing and for (Formula presented) take on values at (Formula presented) of order (Formula presented) Due to the negative driving term in (Formula presented) the sign of the term in the exponential will change at some (Formula presented) and the magnitude of this term will therefore also change close to (Formula presented) from a very large positive to a very large negative value thereby giving rise to the exponential decay in (Formula presented) A similar reason holds for the function (Formula presented) in the case (Formula presented) for (Formula presented) (the large terms in the exponential now being (Formula presented) and (Formula presented).
    • The reason for the exponential decay of (Formula presented) (Formula presented) for (Formula presented) (Formula presented) is clear from the form of (Formula presented) (Formula presented) and the values which the functions (Formula presented) take at the boundaries (Formula presented) For definiteness consider (Formula presented) then (Formula presented) It can be shown that the (Formula presented) are monotonically decreasing and for (Formula presented) take on values at (Formula presented) of order (Formula presented) Due to the negative driving term in (Formula presented) the sign of the term in the exponential will change at some (Formula presented) and the magnitude of this term will therefore also change close to (Formula presented) from a very large positive to a very large negative value thereby giving rise to the exponential decay in (Formula presented) A similar reason holds for the function (Formula presented) in the case (Formula presented) for (Formula presented) (the large terms in the exponential now being (Formula presented) and (Formula presented).


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