-
1
-
-
0348107274
-
-
10.1103/PhysRevLett.91.207901
-
S. Bose, Phys. Rev. Lett. 91, 207901 (2003). 10.1103/PhysRevLett.91. 207901
-
(2003)
Phys. Rev. Lett.
, vol.91
, pp. 207901
-
-
Bose, S.1
-
2
-
-
34547416594
-
-
10.1080/00107510701342313;
-
S. Bose, Contemp. Phys. 48, 13 (2007) 10.1080/00107510701342313
-
(2007)
Contemp. Phys.
, vol.48
, pp. 13
-
-
Bose, S.1
-
3
-
-
68549101270
-
-
Ph.D. thesis, University College London
-
D. Burgarth, Ph.D. thesis, University College London, 2006.
-
(2006)
-
-
Burgarth, D.1
-
4
-
-
2942659839
-
-
10.1103/PhysRevLett.92.187902;
-
M. Christandl, N. Datta, A. Ekert, and A. J. Landahl, Phys. Rev. Lett. 92, 187902 (2004) 10.1103/PhysRevLett.92.187902
-
(2004)
Phys. Rev. Lett.
, vol.92
, pp. 187902
-
-
Christandl, M.1
Datta, N.2
Ekert, A.3
Landahl, A.J.4
-
7
-
-
68549132881
-
-
10.1016/j.physleta.2009.03.038
-
E. B. Fel'dman and A. I. Zenchuk, Phys. Lett. A 373, 1719 (2009). 10.1016/j.physleta.2009.03.038
-
(2009)
Phys. Lett. A
, vol.373
, pp. 1719
-
-
Fel'Dman, E.B.1
Zenchuk, A.I.2
-
9
-
-
34547200408
-
-
10.1103/PhysRevA.76.012317
-
J. Zhang, N. Rajendran, X. Peng, and D. Suter, Phys. Rev. A 76, 012317 (2007). 10.1103/PhysRevA.76.012317
-
(2007)
Phys. Rev. A
, vol.76
, pp. 012317
-
-
Zhang, J.1
Rajendran, N.2
Peng, X.3
Suter, D.4
-
11
-
-
33845672215
-
-
10.1103/PhysRevA.74.062312
-
T. S. Mahesh and D. Suter, Phys. Rev. A 74, 062312 (2006). 10.1103/PhysRevA.74.062312
-
(2006)
Phys. Rev. A
, vol.74
, pp. 062312
-
-
Mahesh, T.S.1
Suter, D.2
-
13
-
-
34547212324
-
-
10.1103/PhysRevLett.99.030501;
-
J. Fitzsimons, L. Xiao, S. C. Benjamin, and J. A. Jones, Phys. Rev. Lett. 99, 030501 (2007) 10.1103/PhysRevLett.99.030501
-
(2007)
Phys. Rev. Lett.
, vol.99
, pp. 030501
-
-
Fitzsimons, J.1
Xiao, L.2
Benjamin, S.C.3
Jones, J.A.4
-
15
-
-
40949127864
-
-
10.1140/epjst/e2007-00370-9
-
D. Burgarth, Eur. Phys. J. Spec. Top. 151, 147 (2007). 10.1140/epjst/e2007-00370-9
-
(2007)
Eur. Phys. J. Spec. Top.
, vol.151
, pp. 147
-
-
Burgarth, D.1
-
16
-
-
68549083145
-
-
In our experimental system, we directly implemented the backward time evolution U-τ of Q j,n -1 by forward evolution of -H. This is not necessary, but it simplified the presentation. Actually, one can design Qj,n in Eq. 6 for the reverse QST using -H. Hence, in the implementation of Q j,n -1 the evolution is still Uτ.
-
In our experimental system, we directly implemented the backward time evolution U-τ of Q j,n -1 by forward evolution of -H. This is not necessary, but it simplified the presentation. Actually, one can design Qj,n in Eq. 6 for the reverse QST using -H. Hence, in the implementation of Q j,n -1 the evolution is still Uτ.
-
-
-
-
17
-
-
0034555656
-
-
10.1246/cl.2000.1300
-
H. Takeuchi, Chem. Lett. 29, 1300 (2000). 10.1246/cl.2000.1300
-
(2000)
Chem. Lett.
, vol.29
, pp. 1300
-
-
Takeuchi, H.1
-
19
-
-
36549005463
-
-
10.1103/PhysRevLett.99.220501
-
M. K. Henry, C. Ramanathan, J. S. Hodges, C. A. Ryan, M. J. Ditty, R. Laflamme, and D. G. Cory, Phys. Rev. Lett. 99, 220501 (2007). 10.1103/PhysRevLett.99.220501
-
(2007)
Phys. Rev. Lett.
, vol.99
, pp. 220501
-
-
Henry, M.K.1
Ramanathan, C.2
Hodges, J.S.3
Ryan, C.A.4
Ditty, M.J.5
Laflamme, R.6
Cory, D.G.7
-
20
-
-
33845973729
-
-
Hamiltonian tomography for large-size liquid-crystal NMR systems is still a hard problem currently. New theoretical and experimental techniques are developing, e.g., 10.1016/S0066-4103(06)59001-5;
-
Hamiltonian tomography for large-size liquid-crystal NMR systems is still a hard problem currently. New theoretical and experimental techniques are developing, e.g., L. D. Field, Annu. Rep. NMR Spectrosc. 59, 1 (2006) 10.1016/S0066-4103(06)59001-5
-
(2006)
Annu. Rep. NMR Spectrosc.
, vol.59
, pp. 1
-
-
Field, L.D.1
-
23
-
-
0000536106
-
-
10.1063/1.449344;
-
J. Baum, J. Chem. Phys. 83, 2015 (1985) 10.1063/1.449344
-
(1985)
J. Chem. Phys.
, vol.83
, pp. 2015
-
-
Baum, J.1
-
24
-
-
19544367104
-
-
10.1103/PhysRevA.70.022330;
-
J.-S. Lee and A. K. Khitrin, Phys. Rev. A 70, 022330 (2004) 10.1103/PhysRevA.70.022330
-
(2004)
Phys. Rev. A
, vol.70
, pp. 022330
-
-
Lee, J.-S.1
Khitrin, A.K.2
-
26
-
-
33947194844
-
-
10.1088/0305-4470/39/49/008
-
G. B. Furman, J. Phys. A 39, 15197 (2006). 10.1088/0305-4470/39/49/008
-
(2006)
J. Phys. A
, vol.39
, pp. 15197
-
-
Furman, G.B.1
-
28
-
-
11344283019
-
-
10.1016/j.jmr.2004.11.004;
-
N. Khaneja, J. Magn. Reson. 172, 296 (2005) 10.1016/j.jmr.2004.11.004
-
(2005)
J. Magn. Reson.
, vol.172
, pp. 296
-
-
Khaneja, N.1
-
29
-
-
47749155271
-
-
10.1103/PhysRevA.78.012328
-
C. A. Ryan, C. Negrevergne, M. Laforest, E. Knill, and R. Laflamme, Phys. Rev. A 78, 012328 (2008). 10.1103/PhysRevA.78.012328
-
(2008)
Phys. Rev. A
, vol.78
, pp. 012328
-
-
Ryan, C.A.1
Negrevergne, C.2
Laforest, M.3
Knill, E.4
Laflamme, R.5
-
30
-
-
58949084080
-
-
10.1103/PhysRevA.79.012305
-
J. Zhang, F. M. Cucchietti, C. M. Chandrashekar, M. Laforest, C. A. Ryan, M. Ditty, A. Hubbard, J. K. Gamble, and R. Laflamme, Phys. Rev. A 79, 012305 (2009). 10.1103/PhysRevA.79.012305
-
(2009)
Phys. Rev. A
, vol.79
, pp. 012305
-
-
Zhang, J.1
Cucchietti, F.M.2
Chandrashekar, C.M.3
Laforest, M.4
Ryan, C.A.5
Ditty, M.6
Hubbard, A.7
Gamble, J.K.8
Laflamme, R.9
|