-
3
-
-
4944221449
-
-
ZEPYAA
-
F. London, Z. Phys. 40, 193 (1927).ZEPYAA
-
(1927)
Z. Phys.
, vol.40
, pp. 193
-
-
London, F.1
-
4
-
-
85037240444
-
-
Quantum Phase and Phase Dependent Measurements, edited by W. P. Schleich and S. M. Barnett, special issue of Phys. Scr. T48 (1993)
-
Quantum Phase and Phase Dependent Measurements, edited by W. P. Schleich and S. M. Barnett, special issue of Phys. Scr. T48 (1993).
-
-
-
-
5
-
-
0003130033
-
-
PLRAAN
-
U. Leonhardt, J. A. Vaccaro, B. Böhmer, and H. Paul, Phys. Rev. A 51, 84 (1995).PLRAAN
-
(1995)
Phys. Rev. A
, vol.51
, pp. 84
-
-
Leonhardt, U.1
Vaccaro, J.A.2
Böhmer, B.3
Paul, H.4
-
14
-
-
21844517099
-
-
JPHAC5
-
T. Opatrný, J. Phys. A 27, 7201 (1994).JPHAC5
-
(1994)
J. Phys. A
, vol.27
, pp. 7201
-
-
Opatrný, T.1
-
15
-
-
0001241961
-
-
Springer, Berlin
-
A. S. Holevo, in Quantum Probability and Applications to the Quantum Theory of Irreversible Processes, edited by L. Accardi, A. Frigerio, and V. Gorini, Springer Lecture Notes in Mathematics Vol. 1055 (Springer, Berlin, 1984), p. 153.
-
(1984)
Quantum Probability and Applications to the Quantum Theory of Irreversible Processes
, pp. 153
-
-
Holevo, A.S.1
-
19
-
-
85037246388
-
-
S. J. Dolinar, Research Laboratory of Electronics, MIT, Quarterly Progress Report No. 111 (1973), p. 115; see also Quantum Detection and Estimation Theory (Ref
-
S. J. Dolinar, Research Laboratory of Electronics, MIT, Quarterly Progress Report No. 111 (1973), p. 115;see also Quantum Detection and Estimation Theory (Ref. 9), p. 163;
-
-
-
-
22
-
-
85037208981
-
-
This result shows that we would only expect the asymptotic lower bound (6.2) to be relevant for (Formula presented) greater than (Formula presented); that is, for (Formula presented). Thus the absolute lower bound due to the intrinsic phase variance of the squeezed states which comprise the POM is irrelevant unless we have a photon detection scheme that is perfect to 1 part in (Formula presented), which is practically impossible
-
This result shows that we would only expect the asymptotic lower bound (6.2) to be relevant for (Formula presented) greater than (Formula presented); that is, for (Formula presented). Thus the absolute lower bound due to the intrinsic phase variance of the squeezed states which comprise the POM is irrelevant unless we have a photon detection scheme that is perfect to 1 part in (Formula presented), which is practically impossible.
-
-
-
|