-
3
-
-
33846840504
-
Relaxation in a completely integrable many-body Quantum system: An Ab initio study of the dynamics of the highly excited states of 1D lattice hard-core bosons
-
DOI 10.1103/PhysRevLett.98.050405
-
M. Rigol, V. Dunjko, V. Yurovsky, and M. Olshanii, Phys. Rev. Lett. 98, 050405 (2007). PRLTAO 0031-9007 10.1103/PhysRevLett.98.050405 (Pubitemid 46203541)
-
(2007)
Physical Review Letters
, vol.98
, Issue.5
, pp. 050405
-
-
Rigol, M.1
Dunjko, V.2
Yurovsky, V.3
Olshanii, M.4
-
4
-
-
42249112261
-
Thermalization and its mechanism for generic isolated quantum systems
-
DOI 10.1038/nature06838, PII NATURE06838
-
M. Rigol, V. Dunjko, and M. Olshanii, Nature (London) 452, 854 (2008). NATUAS 0028-0836 10.1038/nature06838 (Pubitemid 351550863)
-
(2008)
Nature
, vol.452
, Issue.7189
, pp. 854-858
-
-
Rigol, M.1
Dunjko, V.2
Olshanii, M.3
-
5
-
-
33749990876
-
Effect of suddenly turning on interactions in the Luttinger model
-
DOI 10.1103/PhysRevLett.97.156403
-
M.A. Cazalilla, Phys. Rev. Lett. 97, 156403 (2006). PRLTAO 0031-9007 10.1103/PhysRevLett.97.156403 (Pubitemid 44570421)
-
(2006)
Physical Review Letters
, vol.97
, Issue.15
, pp. 156403
-
-
Cazalilla, M.A.1
-
6
-
-
34547354363
-
Strongly correlated fermions after a quantum quench
-
DOI 10.1103/PhysRevLett.98.210405
-
S.R. Manmana, S. Wessel, R.M. Noack, and A. Muramatsu, Phys. Rev. Lett. 98, 210405 (2007). PRLTAO 0031-9007 10.1103/PhysRevLett.98.210405 (Pubitemid 47139673)
-
(2007)
Physical Review Letters
, vol.98
, Issue.21
, pp. 210405
-
-
Manmana, S.R.1
Wessel, S.2
Noack, R.M.3
Muramatsu, A.4
-
7
-
-
40849083709
-
Dephasing and the steady state in quantum many-particle systems
-
DOI 10.1103/PhysRevLett.100.100601
-
T. Barthel and U. Schollwöck, Phys. Rev. Lett. 100, 100601 (2008). PRLTAO 0031-9007 10.1103/PhysRevLett.100.100601 (Pubitemid 351399128)
-
(2008)
Physical Review Letters
, vol.100
, Issue.10
, pp. 100601
-
-
Barthel, T.1
Schollwock, U.2
-
8
-
-
77953033198
-
-
NJOPFM 1367-2630 10.1088/1367-2630/12/5/055015
-
D. Fioretto and G. Mussardo, New J. Phys. 12, 055015 (2010). NJOPFM 1367-2630 10.1088/1367-2630/12/5/055015
-
(2010)
New J. Phys.
, vol.12
, pp. 055015
-
-
Fioretto, D.1
Mussardo, G.2
-
9
-
-
34247866257
-
Quench dynamics and nonequilibrium phase diagram of the Bose-Hubbard model
-
DOI 10.1103/PhysRevLett.98.180601
-
C. Kollath, A.M. Läuchli, and E. Altman, Phys. Rev. Lett. 98, 180601 (2007). PRLTAO 0031-9007 10.1103/PhysRevLett.98.180601 (Pubitemid 46693406)
-
(2007)
Physical Review Letters
, vol.98
, Issue.18
, pp. 180601
-
-
Kollath, C.1
Lauchli, A.M.2
Altman, E.3
-
10
-
-
78650101606
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.105.250401
-
G. Biroli, C. Kollath, and A.M. Läuchli, Phys. Rev. Lett. 105, 250401 (2010). PRLTAO 0031-9007 10.1103/PhysRevLett.105.250401
-
(2010)
Phys. Rev. Lett.
, vol.105
, pp. 250401
-
-
Biroli, G.1
Kollath, C.2
Läuchli, A.M.3
-
13
-
-
78049480881
-
-
PRBMDO 1098-0121 10.1103/PhysRevB.82.144302
-
D. Rossini, S. Suzuki, G. Mussardo, G.E. Santoro, and A. Silva, Phys. Rev. B 82, 144302 (2010). PRBMDO 1098-0121 10.1103/PhysRevB.82.144302
-
(2010)
Phys. Rev. B
, vol.82
, pp. 144302
-
-
Rossini, D.1
Suzuki, S.2
Mussardo, G.3
Santoro, G.E.4
Silva, A.5
-
14
-
-
41349114178
-
Real-time dynamics in spin-1/2 chains with adaptive time-dependent density matrix renormalization group
-
DOI 10.1103/PhysRevE.71.036102, 036102
-
D. Gobert, C. Kollath, U. Schollwöck, and G. Schütz, Phys. Rev. E 71, 036102 (2005). PLEEE8 1539-3755 10.1103/PhysRevE.71.036102 (Pubitemid 40619782)
-
(2005)
Physical Review e - Statistical, Nonlinear, and Soft Matter Physics
, vol.71
, Issue.3
-
-
Gobert, D.1
Kollath, C.2
Schollwock, U.3
Schutz, G.4
-
15
-
-
84888594068
-
-
JSMTC6 1742-5468 10.1088/1742-5468/2013/10/P10028
-
B. Pozsgay, J. Stat. Mech.: Theory Exp. (2013) P10028. JSMTC6 1742-5468 10.1088/1742-5468/2013/10/P10028
-
J. Stat. Mech.: Theory Exp.
, vol.2013
-
-
Pozsgay, B.1
-
17
-
-
77953046353
-
-
NJOPFM 1367-2630 10.1088/1367-2630/12/5/055017
-
P. Barmettler, M. Punk, V. Gritsev, E. Demler, and E. Altman, New J. Phys. 12, 055017 (2010). NJOPFM 1367-2630 10.1088/1367-2630/12/5/055017
-
(2010)
New J. Phys.
, vol.12
, pp. 055017
-
-
Barmettler, P.1
Punk, M.2
Gritsev, V.3
Demler, E.4
Altman, E.5
-
18
-
-
84903550382
-
-
arXiv:1308.0277.
-
M. Fagotti, arXiv:1308.0277.
-
-
-
Fagotti, M.1
-
19
-
-
33846900525
-
-
ZEPYAA 1434-6001 10.1007/BF01341708
-
H.A. Bethe, Z. Phys. 71, 205 (1931). ZEPYAA 1434-6001 10.1007/BF01341708
-
(1931)
Z. Phys.
, vol.71
, pp. 205
-
-
Bethe, H.A.1
-
20
-
-
84857338164
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.108.077206
-
M. Ganahl, E. Rabel, F.H.L. Essler, and H.G. Evertz, Phys. Rev. Lett. 108, 077206 (2012). PRLTAO 0031-9007 10.1103/PhysRevLett.108.077206
-
(2012)
Phys. Rev. Lett.
, vol.108
, pp. 077206
-
-
Ganahl, M.1
Rabel, E.2
Essler, F.H.L.3
Evertz, H.G.4
-
21
-
-
84885612793
-
-
NATUAS 0028-0836 10.1038/nature12541
-
T. Fukuhara, P. Schauß, M. Endres, S. Hild, M. Cheneau, I. Bloch, and C. Gross, Nature (London) 502, 76 (2013). NATUAS 0028-0836 10.1038/nature12541
-
(2013)
Nature (London)
, vol.502
, pp. 76
-
-
Fukuhara, T.1
Schauß, P.2
Endres, M.3
Hild, S.4
Cheneau, M.5
Bloch, I.6
Gross, C.7
-
22
-
-
45549120261
-
-
PYLAAG 0375-9601 10.1016/0375-9601(88)90465-3
-
V. Yudson, Phys. Lett. A 129, 17 (1988). PYLAAG 0375-9601 10.1016/0375-9601(88)90465-3
-
(1988)
Phys. Lett. A
, vol.129
, pp. 17
-
-
Yudson, V.1
-
23
-
-
33747353944
-
-
SPHJAR 0038-5646
-
V. Yudson, Sov. Phys. JETP 88, 1757 (1985). SPHJAR 0038-5646
-
(1985)
Sov. Phys. JETP
, vol.88
, pp. 1757
-
-
Yudson, V.1
-
24
-
-
84866414161
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.109.115304
-
D. Iyer and N. Andrei, Phys. Rev. Lett. 109, 115304 (2012). PRLTAO 0031-9007 10.1103/PhysRevLett.109.115304
-
(2012)
Phys. Rev. Lett.
, vol.109
, pp. 115304
-
-
Iyer, D.1
Andrei, N.2
-
25
-
-
84878517730
-
-
PLRAAN 1050-2947 10.1103/PhysRevA.87.053628
-
D. Iyer, H. Guan, and N. Andrei, Phys. Rev. A 87, 053628 (2013). PLRAAN 1050-2947 10.1103/PhysRevA.87.053628
-
(2013)
Phys. Rev. A
, vol.87
, pp. 053628
-
-
Iyer, D.1
Guan, H.2
Andrei, N.3
-
26
-
-
84903522537
-
-
The argument in Refs. [22-25], which proceeds via contours that avoid pole contributions, cannot be applied here. Instead, the proof proceeds via a delicate cancellation of residues [27].
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The argument in Refs. [22-25], which proceeds via contours that avoid pole contributions, cannot be applied here. Instead, the proof proceeds via a delicate cancellation of residues [27].
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28
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84903534797
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For example, in Ref. [21], the coupling (Equation presented). Thus, the dimensionless time unit (Equation presented) in our convention corresponds to (Equation presented) ms in their experiment. See Fig. 2 for details of this comparison.
-
For example, in Ref. [21], the coupling (Equation presented). Thus, the dimensionless time unit (Equation presented) in our convention corresponds to (Equation presented) ms in their experiment. See Fig. 2 for details of this comparison.
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-
-
-
29
-
-
36149006652
-
-
PHRVAO 0031-899X 10.1103/PhysRev.112.309
-
R. Orbach, Phys. Rev. 112, 309 (1958). PHRVAO 0031-899X 10.1103/PhysRev.112.309
-
(1958)
Phys. Rev.
, vol.112
, pp. 309
-
-
Orbach, R.1
-
32
-
-
84903549780
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The Heaviside step function (Equation presented) is defined as (Equation presented) when (Equation presented), (Equation presented) when (Equation presented). The definition of (Equation presented) is not necessary here, since (Equation presented).
-
The Heaviside step function (Equation presented) is defined as (Equation presented) when (Equation presented), (Equation presented) when (Equation presented). The definition of (Equation presented) is not necessary here, since (Equation presented).
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33
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84903525865
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In the region (Equation presented), one moves the back-running contours to (Equation presented) instead of (Equation presented), so the order of strings generated is restricted by the value of the anisotropy (Equation presented). This feature agrees with the traditional thermodynamic Bethe ansatz.
-
In the region (Equation presented), one moves the back-running contours to (Equation presented) instead of (Equation presented), so the order of strings generated is restricted by the value of the anisotropy (Equation presented). This feature agrees with the traditional thermodynamic Bethe ansatz.
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-
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34
-
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84903541251
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-
For the region (Equation presented), there is actually another term (Equation presented). But it is trivial, since the integral without an (Equation presented)-matrix can be decoupled for each (Equation presented).
-
For the region (Equation presented), there is actually another term (Equation presented). But it is trivial, since the integral without an (Equation presented)-matrix can be decoupled for each (Equation presented).
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-
-
-
35
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84903519085
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-
According to the dispersion relation of an (Equation presented)-string [31], the maximum velocities are given by (Equation presented), (Equation presented).
-
According to the dispersion relation of an (Equation presented)-string [31], the maximum velocities are given by (Equation presented), (Equation presented).
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-
-
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36
-
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84903536108
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-
According to the dispersion relation of an (Equation presented)-string [31], the maximum velocities are given by (Equation presented), (Equation presented).
-
According to the dispersion relation of an (Equation presented)-string [31], the maximum velocities are given by (Equation presented), (Equation presented).
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