-
1
-
-
0004015336
-
-
S. A. Wolf Plenum, New York M. Goldman
-
A. J. Leggett, in Percolation, Localization and Superconductivity, Vol. 109 of NATO Advanced Study Institute, Series B: Physics, edited by M. Goldman and S. A. Wolf (Plenum, New York, 1984).
-
(1984)
Percolation, Localization and Superconductivity, Vol. 109 of NATO Advanced Study Institute, Series B: Physics
-
-
Leggett, A.J.1
-
3
-
-
0001637935
-
-
A. Leclair, F. Lesage, S. Lukyanov, and H. Saleur, Phys. Lett. A 235, 203 (1997).
-
(1997)
Phys. Lett. A
, vol.235
, pp. 203
-
-
Leclair, A.1
Lesage, F.2
Lukyanov, S.3
Saleur, H.4
-
6
-
-
33750926031
-
-
For a review, see A. J. Leggett, S. Chakravarty, A. T. Dorsey, M. P. A. Fisher, A. Garg, and W. Zwerger, Rev. Mod. Phys. 59, 1 (1987);
-
(1987)
Rev. Mod. Phys.
, vol.59
, pp. 1
-
-
Leggett, A.J.1
Chakravarty, S.2
Dorsey, A.T.3
Fisher, M.P.A.4
Garg, A.5
Zwerger, W.6
-
8
-
-
0004258958
-
-
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
-
-
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
-
-
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
-
-
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
-
-
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
-
-
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
-
-
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
-
-
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
-
-
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
-
-
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
-
-
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).
-
-
-
-
60
-
-
3943069526
-
-
T. Brugger T. Schreiner, G. Roth, P. Adelmann, and G. Czjzek, Phys. Rev. Lett. 71, 2481 (1993).
-
(1993)
Phys. Rev. Lett.
, vol.71
, pp. 2481
-
-
Brugger, T.1
Schreiner, T.2
Roth, G.3
Adelmann, P.4
Czjzek, G.5
-
65
-
-
0003463679
-
-
Elsevier, Amsterdam H. van Beijeren M. H. Ernst
-
For a review, see V. J. Emery and S. A. Kivelson, in Fundamental Problems in Statistical Mechanics VIII, edited by H. van Beijeren and M. H. Ernst (Elsevier, Amsterdam, 1994), pp. 1–24.
-
(1994)
Fundamental Problems in Statistical Mechanics VIII
, pp. 1-24
-
-
Emery, V.J.1
Kivelson, S.A.2
-
66
-
-
0001259627
-
-
G. Morandi S. Lundquist World Scientific, Singapore
-
N. Andrei, in Series on Modern Condensed Matter Physics, Lecture Notes of ICTP Summer Course, September 1992, edited by S. Lundquist, G. Morandi, and Yu Lu (World Scientific, Singapore, 1995), Vol. 6, pp. 458–551.
-
(1995)
Series on Modern Condensed Matter Physics, Lecture Notes of ICTP Summer Course, September 1992
, vol.6
, pp. 458-551
-
-
Andrei, N.1
Lu, Y.2
-
71
-
-
85037903000
-
-
We used those in the Numerical Algorithms Group (NAG) library.
-
We used those in the Numerical Algorithms Group (NAG) library.
-
-
-
-
72
-
-
85037900989
-
-
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).
-
-
-
|