-
1
-
-
0023364920
-
-
10.1080/09500348714550721
-
R. Loudon and P. L. Knight, J. Mod. Opt. 34, 709 (1987). 10.1080/09500348714550721
-
(1987)
J. Mod. Opt.
, vol.34
, pp. 709
-
-
Loudon, R.1
Knight, P.L.2
-
3
-
-
0343342536
-
-
edited by P. D. Drummond and Z. Ficek (Springer, New York
-
Quantum Squeezing, edited by, P. D. Drummond, and, Z. Ficek, (Springer, New York, 2004).
-
(2004)
Quantum Squeezing
-
-
-
4
-
-
0001669591
-
-
10.1103/PhysRevA.41.369
-
J. Gea-Banacloche, N. Lu, L. M. Pedrotti, S. Prasad, M. O. Scully, and K. Wodkiewicz, Phys. Rev. A 41, 369 (1990). 10.1103/PhysRevA.41.369
-
(1990)
Phys. Rev. A
, vol.41
, pp. 369
-
-
Gea-Banacloche, J.1
Lu, N.2
Pedrotti, L.M.3
Prasad, S.4
Scully, M.O.5
Wodkiewicz, K.6
-
5
-
-
38549149772
-
-
10.1103/PhysRevLett.100.033602;
-
H. Vahlbruch, M. Mehmet, S. Chelkowski, B. Hage, A. Franzen, N. Lastzka, S. Goszler, K. Danzmann, and R. Schnabel, Phys. Rev. Lett. 100, 033602 (2008) 10.1103/PhysRevLett.100.033602
-
(2008)
Phys. Rev. Lett.
, vol.100
, pp. 033602
-
-
Vahlbruch, H.1
Mehmet, M.2
Chelkowski, S.3
Hage, B.4
Franzen, A.5
Lastzka, N.6
Goszler, S.7
Danzmann, K.8
Schnabel, R.9
-
6
-
-
34147150584
-
-
see also 10.1364/OE.15.004321
-
see also Y. Takeno, M. Yukawa, H. Yonezawa and A. Furusawa, Opt. Express 15, 4321 (2007). 10.1364/OE.15.004321
-
(2007)
Opt. Express
, vol.15
, pp. 4321
-
-
Takeno, Y.1
Yukawa, M.2
Yonezawa, H.3
Furusawa, A.4
-
9
-
-
0000475439
-
-
10.1103/PhysRevLett.88.203601;
-
N. Treps, U. Andersen, B. Buchler, P. K. Lam, A. Mĝitre, H. A. Bachor, and C. Fabre, Phys. Rev. Lett. 88, 203601 (2002) 10.1103/PhysRevLett.88. 203601
-
(2002)
Phys. Rev. Lett.
, vol.88
, pp. 203601
-
-
Treps, N.1
Andersen, U.2
Buchler, B.3
Lam, P.K.4
Mĝitre, A.5
Bachor, H.A.6
Fabre, C.7
-
10
-
-
0042021864
-
-
10.1126/science.1086489
-
N. Treps, N. Grosse, W. P. Bowen, C. Fabre, H. -A. Bachor, and P. K. Lam, Science 301, 940 (2003). 10.1126/science.1086489
-
(2003)
Science
, vol.301
, pp. 940
-
-
Treps, N.1
Grosse, N.2
Bowen, W.P.3
Fabre, C.4
Bachor H, -A.5
Lam, P.K.6
-
12
-
-
0000181982
-
-
10.1103/PhysRevA.52.1675
-
A. Gatti and L. A. Lugiato, Phys. Rev. A 52, 1675 (1995). 10.1103/PhysRevA.52.1675
-
(1995)
Phys. Rev. A
, vol.52
, pp. 1675
-
-
Gatti, A.1
Lugiato, L.A.2
-
17
-
-
67650304317
-
-
arXiv:0901.2783.
-
Related experiments have been started for the simplest case (f=1) we treated in; see M. Lassen, G. Leuchs, and U. L. Anderson, e-print arXiv:0901.2783.
-
-
-
Lassen, M.1
Leuchs, G.2
Anderson, U.L.3
-
22
-
-
67650282675
-
-
Note that χ α0 in reads γs N in our notation.
-
Note that χ α0 in reads γs N in our notation.
-
-
-
-
23
-
-
67650295136
-
-
It is worth remarking one point on the diagonalization of operator Ll. Its eigensystem consists of two degenerate subspaces. How must the two eigenvectors expanding each degenerate subspace be chosen? As will become clearer later, the more appropriate choice is the one that makes the operators related to the projections cj be either Hermitian or anti-Hermitian, so that they coincide (up to a real or imaginary constant) with some observables of interest. For example, with our choice of eigenvectors we see that the operators related to c1l and c2l are c 1,2 l = a +l ± a +l † ± a -l + a -l † [see Eq. 29], which are Hermitian and anti-Hermitian, respectively.
-
It is worth remarking one point on the diagonalization of operator Ll. Its eigensystem consists of two degenerate subspaces. How must the two eigenvectors expanding each degenerate subspace be chosen? As will become clearer later, the more appropriate choice is the one that makes the operators related to the projections cj be either Hermitian or anti-Hermitian, so that they coincide (up to a real or imaginary constant) with some observables of interest. For example, with our choice of eigenvectors we see that the operators related to c1l and c2l are c 1,2 l = a +l ± a +l † ± a -l + a -l † [see Eq. 29], which are Hermitian and anti-Hermitian, respectively.
-
-
-
|