1988
DOI: 10.1103/physreva.37.3896
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Stationary spatial patterns in passive optical systems: Two-level atoms

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Cited by 115 publications
(53 citation statements)
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“…One of the most extensively studied systems has been photorefractive oscillators, where the theoretical background was set out [26], complicated structures experimentally observed [27,28] and order parameter equations derived [29]. Intensive studies of pattern formation in passive, driven, nonlinear Kerr resonators were also performed [30][31][32][33]. Also, the patterns in optical parametric oscillators received a lot of attention.…”
Section: Historical Surveymentioning
confidence: 99%
“…One of the most extensively studied systems has been photorefractive oscillators, where the theoretical background was set out [26], complicated structures experimentally observed [27,28] and order parameter equations derived [29]. Intensive studies of pattern formation in passive, driven, nonlinear Kerr resonators were also performed [30][31][32][33]. Also, the patterns in optical parametric oscillators received a lot of attention.…”
Section: Historical Surveymentioning
confidence: 99%
“…H(z) = e hxxz e hxyz − e −hxyz e hyxz − e −hyxz e hyy z (18) This matrix extends the scalar transformation used by Lugiato and Oldano in their original paper [41], devoted to the study of stationary spatial patterns in optical systems with two-level atoms, to a vectorial case. It is easy to verify that H(0) is the identity matrix while H(L) = RM R −1 and thus all the elements of the matrix h ij can be explicitly calculated:…”
Section: Appendixmentioning
confidence: 99%
“…[41], if p and δ are small parameters (of the order of the transmittivity T=1-r of the mirror) one can calculate a set of first order (in T) equations by expanding all coefficients up to this order. After long but straightforward calculations, the final result is a set of coupled equations for the vector A ′ = [A x , A y ] T , that still contains both ∂ z and ∂ t operators, but includes the boundary conditions.…”
Section: Appendixmentioning
confidence: 99%
“…Many contexts for optical-switching [6,7] and optical-memory [8] applications are based upon bistable dynamics, where the system's input-output curve has a characteristic "S" shape. The origin of these hysteretic response curves tends to lie in external boundary conditions, typically cavity feedback.…”
Section: Introductionmentioning
confidence: 99%
“…This intrinsic phenomenon [12] is potentially useful for switching applications exploiting spatial solitons in planar waveguides [13], as opposed to cavity solitons [6][7][8]14]. For a wide class of nonlinearity, there is often a parameter regime where one finds the coexistence of degenerate bright solitons -that is, beam solutions with different propagation constants but the same power [15,16].…”
mentioning
confidence: 99%