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3
-
-
0004196078
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-
Academic, San Diego
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See, for example, E. Kohen, R. Santus, and J. G. Hirschberg, Photobiology (Academic, San Diego, 1995).
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(1995)
Photobiology
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-
Kohen, E.1
Santus, R.2
Hirschberg, J.G.3
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4
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-
0003860656
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-
translated by S. I. Gaposchkin Van Nostrand, New York
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V. V. Sobolev, translated by S. I. Gaposchkin, A Treatise on Radiative Transfer (Van Nostrand, New York, 1963); B. V. Komberg, A. V. Kravtsov, and V. N. Lukash, Astron. Astrophys. 286, L19 (1994).
-
(1963)
A Treatise on Radiative Transfer
-
-
Sobolev, V.V.1
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5
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-
0011705515
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V. V. Sobolev, translated by S. I. Gaposchkin, A Treatise on Radiative Transfer (Van Nostrand, New York, 1963); B. V. Komberg, A. V. Kravtsov, and V. N. Lukash, Astron. Astrophys. 286, L19 (1994).
-
(1994)
Astron. Astrophys.
, vol.286
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-
Komberg, B.V.1
Kravtsov, A.V.2
Lukash, V.N.3
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8
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-
0000572780
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A. Walther, J. Opt. Soc. Am. 58, 1256 (1968); Yu. A. Kravtsov and L. A. Apresyan, in Progress in Optics XXXVI, edited by E. Wolf (North-Holland, Amsterdam, 1996), p. 179.
-
(1968)
J. Opt. Soc. Am.
, vol.58
, pp. 1256
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-
Walther, A.1
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9
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-
0343869457
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-
edited by E. Wolf North-Holland, Amsterdam
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A. Walther, J. Opt. Soc. Am. 58, 1256 (1968); Yu. A. Kravtsov and L. A. Apresyan, in Progress in Optics XXXVI, edited by E. Wolf (North-Holland, Amsterdam, 1996), p. 179.
-
(1996)
Progress in Optics XXXVI
, vol.36
, pp. 179
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-
Kravtsov, Yu.A.1
Apresyan, L.A.2
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13
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84975571252
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D. McAlister, M. Beck, L. Clarke, A. Mayer, and M. G. Raymer, Opt. Lett. 20, 1181 (1995).
-
(1995)
Opt. Lett.
, vol.20
, pp. 1181
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-
McAlister, D.1
Beck, M.2
Clarke, L.3
Mayer, A.4
Raymer, M.G.5
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16
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0343869456
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private communication
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J. E. Thomas (private communication).
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Thomas, J.E.1
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18
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0015404742
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mentioned that the (generalized) radiance obeys a transport equation under a small-angle-scattering approximation, although it is not clear from this context whether this transport equation is based on wave transport or energy (specific intensity) transport
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Early literature, e.g., D. Arnush, J. Opt. Soc. Am. 62, 1109 (1971), mentioned that the (generalized) radiance obeys a transport equation under a small-angle-scattering approximation, although it is not clear from this context whether this transport equation is based on wave transport or energy (specific intensity) transport.
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(1971)
J. Opt. Soc. Am.
, vol.62
, pp. 1109
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Arnush, D.1
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19
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0001543974
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L. Wang, P. P. Ho, C. Liu, G. Zhang, and R. R. Alfano, Science 253, 769 (1991).
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(1991)
Science
, vol.253
, pp. 769
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Wang, L.1
Ho, P.P.2
Liu, C.3
Zhang, G.4
Alfano, R.R.5
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21
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0342998129
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Ph.D. dissertation, University of Oregon
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Chung-Chieh Cheng, Ph.D. dissertation, University of Oregon, 1999.
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(1999)
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Cheng, C.-C.1
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22
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0342998130
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This approximation for the Mie scattering cross section may not be accurate for the behaviors of the SCF around s = 0. See Refs. [18] and [19]
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This approximation for the Mie scattering cross section may not be accurate for the behaviors of the SCF around s = 0. See Refs. [18] and [19].
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-
-
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24
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84893985658
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(private communication) (unpublished); Comité National Francais de la Radio-electricité Scientifique, Issy-les-Moulineaux, France
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H. T. Yura (private communication) (unpublished); in Union Radio Scientifique Internationale, Open Symposium, La Baule, Loire-Atlantique, France, 1977 (Comité National Francais de la Radio-electricité Scientifique, Issy-les-Moulineaux, France, 1977), pp. 65-69.
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(1977)
Union Radio Scientifique Internationale, Open Symposium, la Baule, Loire-Atlantique, France, 1977
, pp. 65-69
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-
Yura, H.T.1
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26
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0342998127
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C=0.14 rad
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C=0.14 rad.
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-
-
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27
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-
0342998131
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-
aL = 0.04
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aL = 0.04.
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-
-
-
28
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-
0342563816
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-
S] by zero
-
S] by zero.
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-
-
-
29
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-
0342998121
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-
N=0 except at s = 0, meaning there is no correlation between any two distinct spatial field points
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N=0 except at s = 0, meaning there is no correlation between any two distinct spatial field points.
-
-
-
-
30
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-
0342998124
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-
s⊥)
-
s⊥).
-
-
-
-
31
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-
0343433734
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-
NZ ≫ 1
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NZ ≫ 1.
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-
-
-
32
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-
0343869455
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-
Equation (44) is most easily obtained by evaluating the general solution [Eqs. (25)-(27)] in the special case under consideration
-
Equation (44) is most easily obtained by evaluating the general solution [Eqs. (25)-(27)] in the special case under consideration.
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-
-
-
34
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-
0342563814
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-
0∼25 μm. The input Gaussian beam radius (the half-width of the l/e maximum intensity) is a = 140 μm
-
0∼25 μm. The input Gaussian beam radius (the half-width of the l/e maximum intensity) is a = 140 μm.
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-
-
-
35
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0003918873
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-
Springer-Verlag, New York
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See, for example, B. Saleh, Photoelectron Statistics (Springer-Verlag, New York, 1978), pp. 123-128.
-
(1978)
Photoelectron Statistics
, pp. 123-128
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Saleh, B.1
|