-
4
-
-
0040179749
-
-
H. Haken, Z. Phys. 190, 327 (1966).
-
(1966)
Z. Phys.
, vol.190
, pp. 327
-
-
Haken, H.1
-
7
-
-
85037178847
-
-
Ya. I Khanin, Principles of Laser Dynamics (North-Holland, Amsterdam, 1996)
-
Ya. I Khanin, Principles of Laser Dynamics (North-Holland, Amsterdam, 1996).
-
-
-
-
9
-
-
0039963033
-
-
E. Roldán, G. J. de Valcárcel, R. Vilaseca, R. Corbalán, V. J. Martínez, and R. Gilmore, Quantum Semiclassic. Opt. 9, 1 (1997).
-
(1997)
Quantum Semiclassic. Opt.
, vol.9
, pp. 1
-
-
Roldán, E.1
de Valcárcel, G.J.2
Vilaseca, R.3
Corbalán, R.4
Martínez, V.J.5
Gilmore, R.6
-
10
-
-
85037211728
-
-
Strictu senso, the Lorenz-Haken instability has been observed only in ammonia lasers
-
Strictu senso, the Lorenz-Haken instability has been observed only in ammonia lasers 89, but it has been recognized that the mechanism that leads to dynamical emission in other laser systems although with specific features is, in fact, the same 67.
-
-
-
-
11
-
-
0001033774
-
-
E. M. Pessina, G. Bonfrate, F. Fontana, and L. A. Lugiato, Phys. Rev. A 56, 4086 (1997).
-
(1997)
Phys. Rev. A
, vol.56
, pp. 4086
-
-
Pessina, E.M.1
Bonfrate, G.2
Fontana, F.3
Lugiato, L.A.4
-
12
-
-
51249186736
-
-
The analog of the RNGH instability in passive systems was predicted [R. Bonifacio and L. Lugiato, Lett. Nuovo Cimento 21, 510 (1978)] and observed in a large microwave resonator [
-
(1978)
Lett. Nuovo Cimento
, vol.21
, pp. 510
-
-
Bonifacio, R.1
Lugiato, L.2
-
14
-
-
13044298574
-
-
B. Segard, B. Macke, L. A. Lugiato, F. Prati, and M. Brambilla, Phys. Rev. A 39, 706 (1989)] for optical bistability.
-
(1989)
Phys. Rev. A
, vol.39
, pp. 706
-
-
Segard, B.1
Macke, B.2
Lugiato, L.A.3
Prati, F.4
Brambilla, M.5
-
15
-
-
85037197600
-
-
Actually there is not a constraint on the cavity length for the RNGH instability to be observed. What occurs is that below a critical value of the cavity length
-
Actually there is not a constraint on the cavity length for the RNGH instability to be observed. What occurs is that below a critical value of the cavity length 6 the instability pump threshold grows very quickly in the standard two-level laser model, and thus it is usually considered as unobservable below that cavity length value (see Sec. III for details).
-
-
-
-
18
-
-
0000345759
-
-
F. Sanchez, P. Le Boudec, P.-L. Francoise, and G. Stephan, Phys. Rev. A 48, 2220 (1993).
-
(1993)
Phys. Rev. A
, vol.48
, pp. 2220
-
-
Sanchez, F.1
Le Boudec, P.2
Francoise, P.-L.3
Stephan, G.4
-
24
-
-
0029223762
-
-
F. Fontana, M. Begotti, E. M. Pessina, and L. A. Lugiato, Opt. Commun. 114, 89 (1995).
-
(1995)
Opt. Commun.
, vol.114
, pp. 89
-
-
Fontana, F.1
Begotti, M.2
Pessina, E.M.3
Lugiato, L.A.4
-
28
-
-
0000116077
-
-
L. A. Lugiato, L. M. Narducci, E. V. Eschenazi, D. K. Bandy, and N. B. Abraham, Phys. Rev. A 32, 1563 (1985).
-
(1985)
Phys. Rev. A
, vol.32
, pp. 1563
-
-
Lugiato, L.A.1
Narducci, L.M.2
Eschenazi, E.V.3
Bandy, D.K.4
Abraham, N.B.5
-
29
-
-
85037239898
-
-
Note that T is not in general a true transmissivity; only in the case of two mirrors with equal amplitude reflectivities (Formula presented) does the transmissivity (Formula presented) coincide with that of a single mirror
-
Note that T is not in general a true transmissivity; only in the case of two mirrors with equal amplitude reflectivities (Formula presented) does the transmissivity (Formula presented) coincide with that of a single mirror.
-
-
-
-
31
-
-
0004242249
-
-
Cambridge University Press, Cambridge
-
W. T. Silfvast, Laser Fundamentals (Cambridge University Press, Cambridge, 1996).
-
(1996)
Laser Fundamentals
-
-
Silfvast, W.T.1
|