-
1
-
-
40749108504
-
-
10.1103/PhysRevLett.100.010401
-
M. Taglieber, A.-C. Voigt, T. Aoki, T. W. Hänsch, and K. Dieckmann, Phys. Rev. Lett. 100, 010401 (2008). 10.1103/PhysRevLett.100.010401
-
(2008)
Phys. Rev. Lett.
, vol.100
, pp. 010401
-
-
Taglieber, M.1
Voigt, A.-C.2
Aoki, T.3
Hänsch, T.W.4
Dieckmann, K.5
-
2
-
-
38949194304
-
-
10.1103/PhysRevLett.100.053201
-
E. Wille, Phys. Rev. Lett. 100, 053201 (2008). 10.1103/PhysRevLett.100. 053201
-
(2008)
Phys. Rev. Lett.
, vol.100
, pp. 053201
-
-
Wille, E.1
-
3
-
-
59249093791
-
-
10.1103/PhysRevLett.102.020405
-
A.-C. Voigt, Phys. Rev. Lett. 102, 020405 (2009). 10.1103/PhysRevLett. 102.020405
-
(2009)
Phys. Rev. Lett.
, vol.102
, pp. 020405
-
-
Voigt, A.-C.1
-
4
-
-
55049106049
-
-
10.1103/PhysRevLett.101.170401
-
Y. Nishida and S. Tan, Phys. Rev. Lett. 101, 170401 (2008). 10.1103/PhysRevLett.101.170401
-
(2008)
Phys. Rev. Lett.
, vol.101
, pp. 170401
-
-
Nishida, Y.1
Tan, S.2
-
5
-
-
60849093460
-
-
10.1016/j.aop.2008.10.011
-
Y. Nishida, Ann. Phys. 324, 897 (2009). 10.1016/j.aop.2008.10.011
-
(2009)
Ann. Phys.
, vol.324
, pp. 897
-
-
Nishida, Y.1
-
6
-
-
34848878903
-
-
10.1103/PhysRevLett.99.130407
-
D. S. Petrov, G. E. Astrakharchik, D. J. Papoular, C. Salomon, and G. V. Shlyapnikov, Phys. Rev. Lett. 99, 130407 (2007). 10.1103/PhysRevLett.99.130407
-
(2007)
Phys. Rev. Lett.
, vol.99
, pp. 130407
-
-
Petrov, D.S.1
Astrakharchik, G.E.2
Papoular, D.J.3
Salomon, C.4
Shlyapnikov, G.V.5
-
7
-
-
33645017002
-
-
10.1038/nature04626
-
T. Kraemer, Nature (London) 440, 315 (2006). 10.1038/nature04626
-
(2006)
Nature (London)
, vol.440
, pp. 315
-
-
Kraemer, T.1
-
8
-
-
62049083062
-
-
10.1038/nphys1203
-
S. Knoop, Nat. Phys. 5, 227 (2009). 10.1038/nphys1203
-
(2009)
Nat. Phys.
, vol.5
, pp. 227
-
-
Knoop, S.1
-
9
-
-
66249121551
-
-
arXiv:0901.4584.
-
G. Barontini, e-print arXiv:0901.4584.
-
-
-
Barontini, G.1
-
10
-
-
56849114857
-
-
10.1103/PhysRevLett.101.203202
-
T. B. Ottenstein, T. Lompe, M. Kohnen, A. N. Wenz, and S. Jochim, Phys. Rev. Lett. 101, 203202 (2008). 10.1103/PhysRevLett.101.203202
-
(2008)
Phys. Rev. Lett.
, vol.101
, pp. 203202
-
-
Ottenstein, T.B.1
Lompe, T.2
Kohnen, M.3
Wenz, A.N.4
Jochim, S.5
-
11
-
-
67650323857
-
-
10.1103/PhysRevLett.102.165302
-
J. H. Huckans, J. R. Williams, E. L. Hazlett, R. W. Stites, and K. M. O'Hara, Phys. Rev. Lett. 102, 165302 (2009). 10.1103/PhysRevLett.102.165302
-
(2009)
Phys. Rev. Lett.
, vol.102
, pp. 165302
-
-
Huckans, J.H.1
Williams, J.R.2
Hazlett, E.L.3
Stites, R.W.4
O'Hara, K.M.5
-
12
-
-
0037243507
-
-
10.1103/PhysRevA.67.010703
-
D. S. Petrov, Phys. Rev. A 67, 010703 (R) (2003). 10.1103/PhysRevA.67. 010703
-
(2003)
Phys. Rev. A
, vol.67
, pp. 010703
-
-
Petrov, D.S.1
-
13
-
-
66249145900
-
-
The Born-Oppenheimer approximation gives 0.907 for s0, while the exact value is 1.02. Therefore the error of the Efimov parameter computed here is expected to be of the order of 10%.
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The Born-Oppenheimer approximation gives 0.907 for s0, while the exact value is 1.02. Therefore the error of the Efimov parameter computed here is expected to be of the order of 10%.
-
-
-
-
16
-
-
66249147370
-
-
However, in the low-energy limit, the odd-parity channel is subleading in the atom-dimer scattering and the even-parity channel exhibiting no Efimov effect is dominant.
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However, in the low-energy limit, the odd-parity channel is subleading in the atom-dimer scattering and the even-parity channel exhibiting no Efimov effect is dominant.
-
-
-
-
18
-
-
39249084528
-
-
10.1103/PhysRevLett.87.160407
-
E. Braaten and H. W. Hammer, Phys. Rev. Lett. 87, 160407 (2001). 10.1103/PhysRevLett.87.160407
-
(2001)
Phys. Rev. Lett.
, vol.87
, pp. 160407
-
-
Braaten, E.1
Hammer, H.W.2
-
21
-
-
33645996026
-
-
10.1016/j.physrep.2006.03.001;
-
E. Braaten and H. W. Hammer, Phys. Rep. 428, 259 (2006) 10.1016/j.physrep.2006.03.001
-
(2006)
Phys. Rep.
, vol.428
, pp. 259
-
-
Braaten, E.1
Hammer, H.W.2
-
22
-
-
33845678600
-
-
10.1016/j.aop.2006.10.011
-
E. Braaten and H. W. Hammer, Ann. Phys. 322, 120 (2007). 10.1016/j.aop.2006.10.011
-
(2007)
Ann. Phys.
, vol.322
, pp. 120
-
-
Braaten, E.1
Hammer, H.W.2
-
23
-
-
66249118847
-
-
This exponent is given by 6+2γ, where γ=-0.804 is the scaling exponent of three-body wave function in the p -wave channel found, for example, in Ref.
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This exponent is given by 6+2γ, where γ=-0.804 is the scaling exponent of three-body wave function in the p -wave channel found, for example, in Ref.
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