-
1
-
-
36048980898
-
Cavity QED with a Bose-Einstein condensate
-
DOI 10.1038/nature06120, PII NATURE06120
-
F. Brennecke, Nature (London) NATUAS 0028-0836 10.1038/nature06120 450, 268 (2007); (Pubitemid 350100530)
-
(2007)
Nature
, vol.450
, Issue.7167
, pp. 268-271
-
-
Brennecke, F.1
Donner, T.2
Ritter, S.3
Bourdel, T.4
Kohl, M.5
Esslinger, T.6
-
2
-
-
36048975989
-
Strong atom-field coupling for Bose-Einstein condensates in an optical cavity on a chip
-
DOI 10.1038/nature06331, PII NATURE06331
-
Y. Colombe, Nature (London) 0028-0836 NATUAS 10.1038/nature06331 450, 272 (2007). (Pubitemid 350100551)
-
(2007)
Nature
, vol.450
, Issue.7167
, pp. 272-276
-
-
Colombe, Y.1
Steinmetz, T.2
Dubois, G.3
Linke, F.4
Hunger, D.5
Reichel, J.6
-
3
-
-
4544254582
-
Strong coupling of a single photon to a superconducting qubit using circuit quantum electrodynamics
-
DOI 10.1038/nature02851
-
A. Wallraff, Nature (London) NATUAS 0028-0836 10.1038/nature02851 431, 162 (2004); (Pubitemid 39243464)
-
(2004)
Nature
, vol.431
, Issue.7005
, pp. 162-167
-
-
Wallraff, A.1
Schuster, D.I.2
Blais, A.3
Frunzio, L.4
Huang, R.-S.5
Majer, J.6
Kumar, S.7
Girvin, S.M.8
Schoelkopf, R.J.9
-
4
-
-
68949102092
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.103.083601
-
J. M. Fink, R. Bianchetti, M. Baur, M. Goppl, L. Steffan, S. Filipp, P. J. Leek, A. Blais, and A. Wallraff, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.103.083601 103, 083601 (2009);
-
(2009)
Phys. Rev. Lett.
, vol.103
, pp. 083601
-
-
Fink, J.M.1
Bianchetti, R.2
Baur, M.3
Goppl, M.4
Steffan, L.5
Filipp, S.6
Leek, P.J.7
Blais, A.8
Wallraff, A.9
-
5
-
-
59349106135
-
-
PRLTAO 1745-2473 10.1038/nphys1154
-
L. S. Bishop, Nat. Phys. PRLTAO 1745-2473 10.1038/nphys1154 5, 105 (2009);
-
(2009)
Nat. Phys.
, vol.5
, pp. 105
-
-
Bishop, L.S.1
-
6
-
-
9144260766
-
Strong coupling in a single quantum dot-semiconductor microcavity system
-
DOI 10.1038/nature02969
-
J. P. Reithmaier, Nature (London) NATUAS 0028-0836 10.1038/nature02969 432, 197 (2004); (Pubitemid 39545845)
-
(2004)
Nature
, vol.432
, Issue.7014
, pp. 197-200
-
-
Reithmaier, J.P.1
Sek, G.2
Loffler, A.3
Hofmann, C.4
Kuhn, S.5
Reitzenstein, S.6
Keldysh, L.V.7
Kulakovskii, V.D.8
Reinecke, T.L.9
Forchel, A.10
-
7
-
-
9244245742
-
Vacuum Rabi splitting with a single quantum dot in a photonic crystal nanocavity
-
DOI 10.1038/nature03119
-
T. Yoshie, Nature (London) 0028-0836 10.1038/nature03119 432, 200 (2004); (Pubitemid 39549307)
-
(2004)
Nature
, vol.432
, Issue.7014
, pp. 200-203
-
-
Yoshle, T.1
Scherer, A.2
Hendrickson, J.3
Khitrova, G.4
Gibbs, H.M.5
Rupper, G.6
Ell, C.7
Shchekin, O.B.8
Deppe, D.G.9
-
8
-
-
62249087854
-
-
0028-0836 10.1038/nature07838
-
G. Gunter, Nature (London) 0028-0836 10.1038/nature07838 458, 178 (2009).
-
(2009)
Nature (London)
, vol.458
, pp. 178
-
-
Gunter, G.1
-
9
-
-
3843049908
-
-
In fact, the √N behavior was observed in thermal atoms before., PRLTAO 0031-9007 10.1103/PhysRevLett.63.240
-
In fact, the √ N behavior was observed in thermal atoms before. See M. G. Raizen, R. J. Thompson, R. J. Brecha, H. J. Kimble, and H. J. Carmichael, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.63.240 63, 240 (1989);
-
(1989)
Phys. Rev. Lett.
, vol.63
, pp. 240
-
-
Raizen, G.S.M.1
Thompson, R.J.2
Brecha, R.J.3
Kimble, H.J.4
Carmichael, H.J.5
-
10
-
-
2942562182
-
-
PLRAAN 1050-2947 10.1103/PhysRevA.69.043805
-
S. Leslie, N. Shenvi, K. R. Brown, D. M. Stamper-Kurn, and K. B. Whaley, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.69.043805 69, 043805 (2004);
-
(2004)
Phys. Rev. A
, vol.69
, pp. 043805
-
-
Leslie, S.1
Shenvi, N.2
Brown, K.R.3
Stamper-Kurn, D.M.4
Whaley, K.B.5
-
11
-
-
67549146536
-
-
1050-2947 10.1103/PhysRevA.79.061803
-
X. Yu, D. Xiong, H. Chen, P. Wang, M. Xiao, and J. Zhang, Phys. Rev. A 1050-2947 10.1103/PhysRevA.79.061803 79, 061803 (R) (2009). However, the superradiant phase can be more easily realized in the cold-atom BEC systems as demonstrated in the very recent experiment in.
-
(2009)
Phys. Rev. A
, vol.79
, pp. 061803
-
-
Yu, X.1
Xiong, D.2
Chen, H.3
Wang, P.4
Xiao, M.5
Zhang, J.6
-
12
-
-
34547196138
-
-
PHRVAO 0031-899X 10.1103/PhysRev.93.99
-
R. H. Dicke, Phys. Rev. PHRVAO 0031-899X 10.1103/PhysRev.93.99 93, 99 (1954).
-
(1954)
Phys. Rev.
, vol.93
, pp. 99
-
-
Dicke, R.H.1
-
13
-
-
0001673603
-
-
APNYA6 0003-4916 10.1016/0003-4916(73)90039-0
-
K. Hepp and E. H. Lieb, Ann. Phys. (NY) APNYA6 0003-4916 10.1016/0003-4916(73)90039-0 76, 360 (1973);
-
(1973)
Ann. Phys. (NY)
, vol.76
, pp. 360
-
-
Hepp, K.1
Lieb, E.H.2
-
14
-
-
0001204362
-
-
PLRAAN 1050-2947 10.1103/PhysRevA.7.831
-
Y. K. Wang and F. T. Hioe, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.7.831 7, 831 (1973).
-
(1973)
Phys. Rev. A
, vol.7
, pp. 831
-
-
Wang, Y.K.1
Hioe, F.T.2
-
17
-
-
18144372771
-
Instability and entanglement of the ground state of the Dicke model
-
DOI 10.1103/PhysRevLett.94.163601, 163601
-
V. Buzek, M. Orszag, and M. Rosko, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.94.163601 94, 163601 (2005). (Pubitemid 40620305)
-
(2005)
Physical Review Letters
, vol.94
, Issue.16
, pp. 1-4
-
-
Buzek, V.1
Orszag, M.2
Rosko, M.3
-
18
-
-
0035894239
-
-
PRLTAO 1098-0121 10.1103/PhysRevB.64.235101
-
P. R. Eastham and P. B. Littlewood, Phys. Rev. B PRLTAO 1098-0121 10.1103/PhysRevB.64.235101 64, 235101 (2001).
-
(2001)
Phys. Rev. B
, vol.64
, pp. 235101
-
-
Eastham, P.R.1
Littlewood, P.B.2
-
19
-
-
0037473845
-
-
2 symmetry, see, PRLTAO 0031-9007 10.1103/PhysRevLett.90.044101
-
2 symmetry, see C. Emary and T. Brandes, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett. 90.044101 90, 044101 (2003);
-
(2003)
Phys. Rev. Lett.
, vol.90
, pp. 044101
-
-
Emary, C.1
Brandes, T.2
-
20
-
-
37649026898
-
-
PRLTAO 1539-3755 10.1103/PhysRevE.67.066203
-
C. Emary and T. Brandes, Phys. Rev. E PRLTAO 1539-3755 10.1103/PhysRevE.67.066203 67, 066203 (2003);
-
(2003)
Phys. Rev. e
, vol.67
, pp. 066203
-
-
Emary, C.1
Brandes, T.2
-
21
-
-
1642632678
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.92.073602
-
2 Dicke model at a finite N has completely different properties than the U(1) model at a finite N and will be presented in a separate publication.
-
(2004)
Phys. Rev. Lett.
, vol.92
, pp. 073602
-
-
Lambert, N.1
Emary, C.2
Brandes, T.3
-
22
-
-
0004275291
-
-
In this paper, we study the steady state superradiant phase, which involves the quantum phase transition. It is quite different from the conventional nonequilibrium spontaneous superradiant radiation, which can be understood from a simple Golden rule calculation; see Chap. 6.7 in, John Wiley & Sons, Inc.
-
In this paper, we study the steady state superradiant phase, which involves the quantum phase transition. It is quite different from the conventional nonequilibrium spontaneous superradiant radiation, which can be understood from a simple Golden rule calculation; see Chap. 6.7 in Y. Yamamoto and A. Imamoglu, Mesoscopic Quantum Optics (John Wiley & Sons, Inc., 1999). For the recent advances on the superradiance prepared by single-photon absorption
-
(1999)
Mesoscopic Quantum Optics
-
-
Yamamoto, Y.1
Imamoglu, A.2
-
23
-
-
42449143018
-
Dynamical evolution of correlated spontaneous emission of a single photon from a uniformly excited cloud of N atoms
-
DOI 10.1103/PhysRevLett.100.160504
-
see A. A. Svidzinsky, J. T. Chang, and M. O. Scully, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.100.160504 100, 160504 (2008); (Pubitemid 351574597)
-
(2008)
Physical Review Letters
, vol.100
, Issue.16
, pp. 160504
-
-
Svidzinsky, A.A.1
Chang, J.-T.2
Scully, M.O.3
-
24
-
-
64549155678
-
-
0031-9007 10.1103/PhysRevLett.102.143601
-
M. O. Scully, Phys. Rev. Lett. 0031-9007 10.1103/PhysRevLett.102.143601 102, 143601 (2009);
-
(2009)
Phys. Rev. Lett.
, vol.102
, pp. 143601
-
-
Scully, M.O.1
-
25
-
-
70349345901
-
-
SCIEAS 0036-8075 10.1126/science.1176695
-
M. O. Scully and A. A. Svidzinsky, Science SCIEAS 0036-8075 10.1126/science.1176695 325, 1510 (2009).
-
(2009)
Science
, vol.325
, pp. 1510
-
-
Scully, M.O.1
Svidzinsky, A.A.2
-
26
-
-
0030494207
-
-
The U(1) Dicke (Tavis-Cummings) model is integrable at any finite N, so, in the "face" value, the system's eigenenergy spectra could be "exactly" solvable by Bethe-ansatz-like methods. For example, see, 0305-4470 10.1088/0305-4470/29/19/015
-
The U(1) Dicke (Tavis-Cummings) model is integrable at any finite N, so, in the "face" value, the system's eigenenergy spectra could be "exactly" solvable by Bethe-ansatz-like methods. For example, see N. M. Bogoliubov, R. K. Bullough, and J. Timonen, J. Phys. A 0305-4470 10.1088/0305-4470/29/19/015 29, 6305 (1996). However, so far, the Bethe-ansatz-like solutions have been at a very "formal" level from which even the system's eigenenergy cannot be obtained analytically, let alone extracting any underlying physics. Furthermore, it is well known that the Bethe ansatz method is not able to get any dynamic correlation functions.
-
(1996)
J. Phys. A
, vol.29
, pp. 6305
-
-
Bogoliubov, N.M.1
Bullough, R.K.2
Timonen, J.3
-
27
-
-
80052298301
-
-
J. Ye (unpublished)
-
J. Ye (unpublished).
-
-
-
-
28
-
-
0030529690
-
-
RMPHAT 0034-6861 10.1103/RevModPhys.68.127
-
L. Davidovich, Rev. Mod. Phys. RMPHAT 0034-6861 10.1103/RevModPhys.68.127 68, 127 (1996).
-
(1996)
Rev. Mod. Phys.
, vol.68
, pp. 127
-
-
Davidovich, L.1
-
29
-
-
70350219245
-
-
PLRAAN 1050-2947 10.1103/PhysRevA.80.043822
-
C. F. Wildfeuer, A. J. Pearlman, J. Chen, J. Fan, A. Migdall, and J. P. Dowling, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.80.043822 80, 043822 (2009).
-
(2009)
Phys. Rev. A
, vol.80
, pp. 043822
-
-
Wildfeuer, C.F.1
Pearlman, A.J.2
Chen, J.3
Fan, J.4
Migdall, A.5
Dowling, J.P.6
-
30
-
-
0001466605
-
-
PLRAAN 1098-0121 10.1103/PhysRevB.44.10173
-
J. Ye and S. Sachdev, Phys. Rev. B PLRAAN 1098-0121 10.1103/PhysRevB.44. 10173 44, 10173 (1991);
-
(1991)
Phys. Rev. B
, vol.44
, pp. 10173
-
-
Ye, J.1
Sachdev, S.2
-
31
-
-
30244458887
-
-
1098-0121 10.1103/PhysRevB.49.11919
-
A. Chubukov, S. Sachdev, and J. Ye, Phys. Rev. B 1098-0121 10.1103/PhysRevB.49.11919 49, 11919 (1994).
-
(1994)
Phys. Rev. B
, vol.49
, pp. 11919
-
-
Chubukov, A.1
Sachdev, S.2
Ye, J.3
-
32
-
-
80052276806
-
-
We are indebted to B. Halperin and S. Sachdev for stressing the importance of this Berry phase term
-
We are indebted to B. Halperin and S. Sachdev for stressing the importance of this Berry phase term.
-
-
-
-
33
-
-
0000348028
-
-
The well-studied "phase-diffusion" process of cold-atom BEC always involves a sudden quenching of the Hamiltonians of the system, which leads to collapse and revival in real time. However, the width of the phase distribution increases linearly in the real time t, instead of √t, so the phrase "phase diffusion" may not be a suitable one in this context. See Eq. 7 and Ref. 18 for comparisons. See, PRLTAO 0031-9007 10.1103/PhysRevLett.77.2158
-
The well-studied "phase-diffusion" process of cold-atom BEC always involves a sudden quenching of the Hamiltonians of the system, which leads to collapse and revival in real time. However, the width of the phase distribution increases linearly in the real time t, instead of √ t, so the phrase "phase diffusion" may not be a suitable one in this context. See Eq. 7 and Ref. 18 and for comparisons. See E. M. Wright, D. F. Walls, and J. C. Garrison, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.77.2158 77, 2158 (1996);
-
(1996)
Phys. Rev. Lett.
, vol.77
, pp. 2158
-
-
Wright, E.M.1
Walls, D.F.2
Garrison, J.C.3
-
34
-
-
0000550722
-
-
0031-9007 10.1103/PhysRevLett.77.3489
-
M. Lewenstein and L. You, Phys. Rev. Lett. 0031-9007 10.1103/PhysRevLett. 77.3489 77, 3489 (1996);
-
(1996)
Phys. Rev. Lett.
, vol.77
, pp. 3489
-
-
Lewenstein, M.1
You, L.2
-
36
-
-
0000070912
-
-
0031-9007 10.1103/PhysRevLett.78.4675
-
J. Javanainen and M. Wilkens, Phys. Rev. Lett. 0031-9007 10.1103/PhysRevLett.78.4675 78, 4675 (1997);
-
(1997)
Phys. Rev. Lett.
, vol.78
, pp. 4675
-
-
Javanainen, J.1
Wilkens, M.2
-
37
-
-
0037026477
-
Collapse and revival of the matter wave field of a Bose-Einstein condensate
-
DOI 10.1038/nature00968
-
M. Greiner, O. Mandel, T. W. Hansch, and I. Bloch, Nature (London) NATUAS 0028-0836 10.1038/nature00968 419, 51 (2002). (Pubitemid 34987866)
-
(2002)
Nature
, vol.419
, Issue.6902
, pp. 51-54
-
-
Greiner, M.1
Mandel, O.2
Hansch, T.W.3
Bloch, I.4
-
38
-
-
80052280123
-
-
Note that the classical phase diffusion due to random spontaneous-emission events in a laser is in real time and leads to the natural linewidth of a laser
-
Note that the classical phase diffusion due to random spontaneous-emission events in a laser is in real time and leads to the natural linewidth of a laser;
-
-
-
-
39
-
-
84994613817
-
-
see Eq. 11.4.8 in, Cambridge University Press, Cambridge
-
see Eq. 11.4.8 in M. O. Scully and M. S. Zubairy, Quantum Optics (Cambridge University Press, Cambridge, 1997). Because the Berry phase is a completely quantum effect, there is no Berry phase analog in this classical phase-diffusion process.
-
(1997)
Quantum Optics
-
-
Scully, M.O.1
Zubairy, M.S.2
-
40
-
-
70350405076
-
-
For a two-mode quadrature squeezing of photons emitted from an exciton superfluid, see, PRLTAO 0031-9007 10.1103/PhysRevLett.103.177401
-
For a two-mode quadrature squeezing of photons emitted from an exciton superfluid, see J. Ye, T. Shi, and L. Jiang, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.103.177401 103, 177401 (2009);
-
(2009)
Phys. Rev. Lett.
, vol.103
, pp. 177401
-
-
Ye, J.1
Shi, T.2
Jiang, L.3
-
41
-
-
77956317334
-
-
PRLTAO 1098-0121 10.1103/PhysRevB.81.235402
-
T. Shi, L. Jiang, and J. Ye, Phys. Rev. B PRLTAO 1098-0121 10.1103/PhysRevB.81.235402 81, 235402 (2010);
-
(2010)
Phys. Rev. B
, vol.81
, pp. 235402
-
-
Shi, T.1
Jiang, L.2
Ye, J.3
-
42
-
-
80052277254
-
-
T. Shi, L. Liang, and J. Ye, e-print arXiv: 0802.1065v6
-
T. Shi, L. Liang, and J. Ye, e-print arXiv: 0802.1065v6.
-
-
-
-
43
-
-
33846381211
-
Proposed realization of the Dicke-model quantum phase transition in an optical cavity QED system
-
DOI 10.1103/PhysRevA.75.013804
-
F. Dimer, B. Estienne, A. S. Parkins, and H. J. Carmichael, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.75.013804 75, 013804 (2007). (Pubitemid 46130338)
-
(2007)
Physical Review A - Atomic, Molecular, and Optical Physics
, vol.75
, Issue.1
, pp. 013804
-
-
Dimer, F.1
Estienne, B.2
Parkins, A.S.3
Carmichael, H.J.4
-
44
-
-
0346885951
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.91.203001
-
A. T. Black, H. W. Chan, and V. Vuletic, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.91.203001 91, 203001 (2003).
-
(2003)
Phys. Rev. Lett.
, vol.91
, pp. 203001
-
-
Black, A.T.1
Chan, H.W.2
Vuletic, V.3
-
45
-
-
77951849893
-
-
NATUAS 0028-0836 10.1038/nature09009
-
K. Baumann, Nature (London) NATUAS 0028-0836 10.1038/nature09009 464, 1301 (2010).
-
(2010)
Nature (London)
, vol.464
, pp. 1301
-
-
Baumann, K.1
|