-
1
-
-
0029410457
-
-
PLRAAN 1050-2947 10.1103/PhysRevA.52.R3429
-
T. B. Pittman, Y. H. Shih, D. V. Strekalov, and A. V. Sergienko, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.52.R3429 52, 3429 (1995).
-
(1995)
Phys. Rev. A
, vol.52
, pp. 3429
-
-
Pittman, T.B.1
Shih, Y.H.2
Strekalov, D.V.3
Sergienko, A.V.4
-
3
-
-
18244363356
-
Two-photon imaging with thermal light
-
DOI 10.1103/PhysRevLett.94.063601, 063601
-
A. Valencia, G. Scarcelli, M. D'Angelo, and Y. Shih, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.94.063601 94, 063601 (2005). (Pubitemid 40629953)
-
(2005)
Physical Review Letters
, vol.94
, Issue.6
, pp. 1-4
-
-
Valencia, A.1
Scarcelli, G.2
D'Angelo, M.3
Shih, Y.4
-
4
-
-
27144541819
-
High-resolution ghost image and ghost diffraction experiments with thermal light
-
DOI 10.1103/PhysRevLett.94.183602, 183602
-
F. Ferri, D. Magatti, A. Gatti, M. Bache, E. Brambilla, and L. A. Lugiato, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.94.183602 94, 183602 (2005). (Pubitemid 41493046)
-
(2005)
Physical Review Letters
, vol.94
, Issue.18
, pp. 1-4
-
-
Ferri, F.1
Magatti, D.2
Gatti, A.3
Bache, M.4
Brambilla, E.5
Lugiato, L.A.6
-
5
-
-
62549140607
-
-
PLRAAN 1050-2947 10.1103/PhysRevA.79.023833
-
B. I. Erkmen and J. H. Shapiro, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.79.023833 79, 023833 (2009).
-
(2009)
Phys. Rev. A
, vol.79
, pp. 023833
-
-
Erkmen, B.I.1
Shapiro, J.H.2
-
6
-
-
79961147286
-
-
PLRAAN 1943-8206 10.1364/AOP.2.000405
-
B. I. Erkmen and J. H. Shapiro, Adv. Opt. Photon. PLRAAN 1943-8206 10.1364/AOP.2.000405 2, 405 (2010).
-
(2010)
Adv. Opt. Photon.
, vol.2
, pp. 405
-
-
Erkmen, B.I.1
Shapiro, J.H.2
-
7
-
-
58149136815
-
-
PLRAAN 1050-2947 10.1103/PhysRevA.78.061802
-
J. H. Shapiro, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.78.061802 78, 061802 (2008).
-
(2008)
Phys. Rev. A
, vol.78
, pp. 061802
-
-
Shapiro, J.H.1
-
8
-
-
66149131411
-
-
PLRAAN 1050-2947 10.1103/PhysRevA.79.053840
-
Y. Bromberg, O. Katz, and Y. Silberberg, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.79.053840 79, 053840 (2009).
-
(2009)
Phys. Rev. A
, vol.79
, pp. 053840
-
-
Bromberg, Y.1
Katz, O.2
Silberberg, Y.3
-
10
-
-
41949117673
-
Ghost-imaging experiment by measuring reflected photons
-
DOI 10.1103/PhysRevA.77.041801
-
R. E. Meyers, K. S. Deacon, and Y. Shih, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.77.041801 77, 041801 (2008). (Pubitemid 351514251)
-
(2008)
Physical Review A - Atomic, Molecular, and Optical Physics
, vol.77
, Issue.4
, pp. 041801
-
-
Meyers, R.1
Deacon, K.S.2
Shih, Y.3
-
11
-
-
66549083551
-
-
OPEXFF 1094-4087 10.1364/OE.17.007916
-
J. Cheng, Opt. Express OPEXFF 1094-4087 10.1364/OE.17.007916 17, 7916 (2009).
-
(2009)
Opt. Express
, vol.17
, pp. 7916
-
-
Cheng, J.1
-
12
-
-
77957882522
-
-
PSISDG 0277-786X 10.1117/12.863544
-
N. D. Hardy and J. H. Shapiro, Proc. SPIE PSISDG 0277-786X 10.1117/12.863544 7815, 78150L (2010).
-
(2010)
Proc. SPIE
, vol.7815
-
-
Hardy, N.D.1
Shapiro, J.H.2
-
13
-
-
83655179679
-
-
For the sake of generality, we have allowed there to be turbulence in the reference path, although a lens could be used to cast a minified reference-beam pattern onto a CCD camera within a protected environment near the source, hence avoiding turbulence on that path.
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For the sake of generality, we have allowed there to be turbulence in the reference path, although a lens could be used to cast a minified reference-beam pattern onto a CCD camera within a protected environment near the source, hence avoiding turbulence on that path.
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-
-
15
-
-
0016125661
-
-
[J. H. Shapiro, Appl. Opt. APOPAI 0003-6935 10.1364/AO.13.002614 13, 2614 (1974)].
-
(1974)
Appl. Opt.
, vol.13
, pp. 2614
-
-
Shapiro, J.H.1
-
16
-
-
0003429990
-
-
Academic, New York
-
A. Ishimaru, Wave Propagation and Scattering in Random Media. Vol. 2: Multiple Scattering, Turbulence, Rough Surfaces, and Remote-Sensing (Academic, New York, 1978).
-
(1978)
Wave Propagation and Scattering in Random Media. Vol. 2: Multiple Scattering, Turbulence, Rough Surfaces, and Remote-Sensing
-
-
Ishimaru, A.1
-
18
-
-
83655163522
-
-
A similar square-law approximation is available for cases in which the turbulence strength is not uniformly distributed along each propagation path, but we have opted to limit our attention to uniform distributions.
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A similar square-law approximation is available for cases in which the turbulence strength is not uniformly distributed along each propagation path, but we have opted to limit our attention to uniform distributions.
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-
-
-
21
-
-
72149133935
-
-
IJSQEN 1077-260X 10.1109/JSTQE.2009.2024959
-
J. H. Shapiro, IEEE J. Sel. Top. Quantum Electron. IJSQEN 1077-260X 10.1109/JSTQE.2009.2024959 15, 1547 (2009).
-
(2009)
IEEE J. Sel. Top. Quantum Electron.
, vol.15
, pp. 1547
-
-
Shapiro, J.H.1
-
22
-
-
0028459545
-
-
JOBPDE 0740-3224 10.1364/JOSAB.11.001130
-
J. H. Shapiro and K.-X. Sun, J. Opt. Soc. Am. B JOBPDE 0740-3224 10.1364/JOSAB.11.001130 11, 1130 (1994).
-
(1994)
J. Opt. Soc. Am. B
, vol.11
, pp. 1130
-
-
Shapiro, J.H.1
Sun, K.-X.2
-
23
-
-
33144472904
-
Can two-photon correlation of chaotic light be considered as correlation of intensity fluctuations?
-
DOI 10.1103/PhysRevLett.96.063602
-
G. Scarcelli, V. Berardi, and Y. Shih, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.96.063602 96, 063602 (2006). (Pubitemid 43271066)
-
(2006)
Physical Review Letters
, vol.96
, Issue.6
, pp. 063602
-
-
Scarcelli, G.1
Berardi, V.2
Shih, Y.3
-
24
-
-
0005683924
-
-
JOSAAH 0030-3941 10.1364/JOSA.70.000745
-
S. M. Wandzura, J. Opt. Soc. Am. JOSAAH 0030-3941 10.1364/JOSA.70.000745 70, 745 (1980).
-
(1980)
J. Opt. Soc. Am.
, vol.70
, pp. 745
-
-
Wandzura, S.M.1
-
25
-
-
84855268287
-
-
We say "appear classical" because the phase-sensitive cross-correlation function from Eq. always exceeds the classical limit set by the autocorrelation functions from Eq. . However, for I1, that cross-correlation function is so close in value to the classical limit, given in Eq. , to render this measure of nonclassicality exceedingly small.
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We say "appear classical" because the phase-sensitive cross-correlation function from Eq. always exceeds the classical limit set by the autocorrelation functions from Eq.. However, for I 1, that cross-correlation function is so close in value to the classical limit, given in Eq., to render this measure of nonclassicality exceedingly small.
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26
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70349690737
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OPEXFF 1094-4087 10.1364/OE.17.001240
-
J. Le Gouët, D. Venkatraman, F. N. C. Wong, and J. H. Shapiro, Opt. Express OPEXFF 1094-4087 10.1364/OE.17.001240 17, 17874 (2009).
-
(2009)
Opt. Express
, vol.17
, pp. 17874
-
-
Le Gouët, J.1
Venkatraman, D.2
Wong, F.N.C.3
Shapiro, J.H.4
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