-
8
-
-
0029223762
-
-
F. Fontana, M. Begotti, E.M. Pessina, 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
-
9
-
-
0001033774
-
-
E.M. Pessina, G. Bonfrate, F. Fontana, 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
-
-
0032614076
-
-
E.M. Pessina, F. Prati, J. Redondo, E. Roldán, G.J. de Valcárcel: Phys. Rev. A 60, 2517 (1999)
-
(1999)
Phys. Rev. A
, vol.60
, pp. 2517
-
-
Pessina, E.M.1
Prati, F.2
Redondo, J.3
Roldán, E.4
De Valcárcel, G.J.5
-
14
-
-
0000116077
-
-
L.A. Lugiato, L.M. Narducci, E.V. Eschenazi, D.K. Bandy, 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
-
17
-
-
0028459827
-
-
P. Franco, M. Midrio, A. Tozzato, M. Romagnoli, F. Fontana: J. Opt. Soc. Am. B 11, 1090 (1994)
-
(1994)
J. Opt. Soc. Am. B
, vol.11
, pp. 1090
-
-
Franco, P.1
Midrio, M.2
Tozzato, A.3
Romagnoli, M.4
Fontana, F.5
-
21
-
-
0141454888
-
-
E. Roldan, G.J. de Valcárcel, F. Silva, F. Prati: J. Opt. Soc. Am. B 18, 1601 (2001)
-
(2001)
J. Opt. Soc. Am. B
, vol.18
, pp. 1601
-
-
Roldan, E.1
De Valcárcel, G.J.2
Silva, F.3
Prati, F.4
-
24
-
-
85039499085
-
-
note
-
inh/ γ⊥ is the inhomogeneous to homogeneous broadening ratio. The lasing threshold occurs at r = 1. Notice that the symbol r entering the above equation does not have the same meaning as the one used in the present article: in [23], and in the above equation, r represents the normalized pump in a two-level laser
-
-
-
-
25
-
-
0342521551
-
-
J.F. Urchueguia, G.J. de Valcárcel, E. Roldán, F. Prati: Phys. Rev. A 62, 041 801(R) (2000)
-
(2000)
Phys. Rev. A
, vol.62
, pp. 041801
-
-
Urchueguia, J.F.1
De Valcárcel, G.J.2
Roldán, E.3
Prati, F.4
-
27
-
-
0029732570
-
-
J.L. Zhang, C.Y. Yue, G.W. Schinn, W.R.L. Clements, J.W.Y. Lit: IEEE J. Lightwave Technol. 14, 104 (1996)
-
(1996)
IEEE J. Lightwave Technol.
, vol.14
, pp. 104
-
-
Zhang, J.L.1
Yue, C.Y.2
Schinn, G.W.3
Clements, W.R.L.4
Lit, J.W.Y.5
-
28
-
-
0030246071
-
-
D.I. Chang, M.J. Guy, S.V. Chernikov, J.R. Taylor, H.J. Kong: Electron. Lett. 32, 1786 (1996)
-
(1996)
Electron. Lett.
, vol.32
, pp. 1786
-
-
Chang, D.I.1
Guy, M.J.2
Chernikov, S.V.3
Taylor, J.R.4
Kong, H.J.5
-
31
-
-
0028548116
-
-
T.W. Carr, Th. Erneux: Phys. Rev. A 50, 724 (1994); Phys. Rev. A 50, 4219 (1994)
-
(1994)
Phys. Rev. A
, vol.50
, pp. 4219
-
-
-
32
-
-
85039501319
-
-
note
-
The reader may wonder why we have not tried to test this hypothesis by numerical integration of the model in [23]. As discussed elsewhere [22, 33], the numerical integration for class B lasers is extremely difficult because of the enormous stiffness of the problem. In fact, the first numerical integrations of the Maxwell-Bloch equations with inhomogeneous broadening in the uniform-field limit have been carried out only very recently [22], and much work needs to be done in this direction. In any case, there is numerical evidence that, with inhomogeneous broadening, the RNGHI can also be subcritical (F. Prati, Universitá dell'Insubria, private communication)
-
-
-
-
33
-
-
18844477892
-
-
A. Amon, M. Nizette, M. Lefranc, T. Emeux: Phys. Rev. A 68, 023 801 (2003)
-
(2003)
Phys. Rev. A
, vol.68
, pp. 023801
-
-
Amon, A.1
Nizette, M.2
Lefranc, M.3
Emeux, T.4
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