-
1
-
-
0005457412
-
-
W. V. Davis, M. Kauranen, E. M. Nagasako, R. J. Gehr, A. L. Gaeta, R. W. Boyd, and G. S. Agarwal, Phys. Rev. A 51, 4152 (1995).
-
(1995)
Phys. Rev. A
, vol.51
, pp. 4152
-
-
Davis, W.V.1
Kauranen, M.2
Nagasako, E.M.3
Gehr, R.J.4
Gaeta, A.L.5
Boyd, R.W.6
Agarwal, G.S.7
-
2
-
-
0028481721
-
-
M. Kauranen, A. L. Gaeta, R. W. Boyd, and G. S. Agarwal, Phys. Rev. A 50, R929 (1994).
-
(1994)
Phys. Rev. A
, vol.50
, pp. R929
-
-
Kauranen, M.1
Gaeta, A.L.2
Boyd, R.W.3
Agarwal, G.S.4
-
5
-
-
0031336813
-
-
IEEE, Piscataway, NJ
-
J. C. Camparo and W. F. Buell, in Proceedings of the 1997 IEEE International Frequency Control Symposium (IEEE, Piscataway, NJ, 1997), pp. 253–258.
-
(1997)
Proceedings of the 1997 IEEE International Frequency Control Symposium
, pp. 253-258
-
-
Camparo, J.C.1
Buell, W.F.2
-
6
-
-
0031999369
-
-
G. Mileti, J. Deng, F. L. Walls, D. A. Jennings, and R. E. Drullinger, IEEE J. Quantum Electron. 34, 233 (1998).
-
(1998)
IEEE J. Quantum Electron.
, vol.34
, pp. 233
-
-
Mileti, G.1
Deng, J.2
Walls, F.L.3
Jennings, D.A.4
Drullinger, R.E.5
-
7
-
-
0027678122
-
-
R. J. McLean, P. Hannaford, C. E. Fairchild, and P. L. Dyson, Opt. Lett. 18, 1675 (1993).
-
(1993)
Opt. Lett.
, vol.18
, pp. 1675
-
-
McLean, R.J.1
Hannaford, P.2
Fairchild, C.E.3
Dyson, P.L.4
-
8
-
-
0027699966
-
-
D. H. McIntyre, C. E. Fairchild, J. Cooper, and R. Walser, Opt. Lett. 18, 1816 (1993).
-
(1993)
Opt. Lett.
, vol.18
, pp. 1816
-
-
McIntyre, D.H.1
Fairchild, C.E.2
Cooper, J.3
Walser, R.4
-
9
-
-
3843050218
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-
The acronym TJS stands for transverse junction stripe, and refers to the physical construction of the diode laser. See D. Botez, J. Opt. Commun. 1, 42 (1980) for a more detailed discussion.
-
(1980)
J. Opt. Commun.
, vol.1
, pp. 42
-
-
Botez, D.1
-
10
-
-
85037186961
-
-
EOSI is a company trade name. For a brief description of this commercial system, see M. Lang, Laser Focus World 32, 187 (1996).
-
(1996)
Laser Focus World
, vol.32
, pp. 187
-
-
Lang, M.1
-
16
-
-
0018015183
-
-
See, for example, M. Nakamura, K. Aiki, N. Chinone, R. Ito, and J. Umeda, J. Appl. Phys. 49, 4644 (1978).
-
(1978)
J. Appl. Phys.
, vol.49
, pp. 4644
-
-
Nakamura, M.1
Aiki, K.2
Chinone, N.3
Ito, R.4
Umeda, J.5
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17
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0016986476
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This value is consistent with expectations for this type of laser, if it is remembered that ASE represents a sum over all but the main lasing mode. See, for example, W. Susaki, T. Tanaka, H. Kan, and M. Ishii, IEEE J. Quantum Electron. QE-13, 587 (1977).
-
(1977)
IEEE J. Quantum Electron.
, vol.QE-13
, pp. 587
-
-
Susaki, W.1
Tanaka, T.2
Kan, H.3
Ishii, M.4
-
20
-
-
0000972746
-
-
S. N. Dixit, P. Zoller, and P. Lambropoulos, Phys. Rev. A 21, 1289 (1980), and references therein.
-
(1980)
Phys. Rev. A
, vol.21
, pp. 1289
-
-
Dixit, S.N.1
Zoller, P.2
Lambropoulos, P.3
-
21
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-
85037240025
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-
A. Papoulis (McGraw-Hill, New York, 1984)
-
A. Papoulis (McGraw-Hill, New York, 1984).
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26
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85037185634
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J. Vanier and C. Audoin, The Quantum Physics of Atomic Frequency Standards (IOP, Bristol, 1989), Vol. 2, Chap. 7
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J. Vanier and C. Audoin, The Quantum Physics of Atomic Frequency Standards (IOP, Bristol, 1989), Vol. 2, Chap. 7.
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31
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0001050509
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We note that a comparison of the laser’s stochastic characteristics with the lamp’s is complicated by the fact that the laser may be described as a phase diffusion field, while the lamp corresponds to a chaotic field. For a discussion of the different stochastic characteristics of these fields, see A. T. Georges and P. Lambropoulos, Phys. Rev. A 20, 991 (1979).
-
(1979)
Phys. Rev. A
, vol.20
, pp. 991
-
-
Georges, A.T.1
Lambropoulos, P.2
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