- •1 Introduction
- •1.1 Historical Survey
- •1.2 Patterns in Nonlinear Optical Resonators
- •1.2.1 Localized Structures: Vortices and Solitons
- •1.2.2 Extended Patterns
- •1.3.3 Optical Feedback Loops
- •1.4 The Contents of this Book
- •References
- •2 Order Parameter Equations for Lasers
- •2.1 Model of a Laser
- •2.2 Linear Stability Analysis
- •2.3 Derivation of the Laser Order Parameter Equation
- •2.3.1 Adiabatic Elimination
- •2.3.2 Multiple-Scale Expansion
- •References
- •3 Order Parameter Equations for Other Nonlinear Resonators
- •3.1 Optical Parametric Oscillators
- •3.2.1 Linear Stability Analysis
- •3.2.2 Scales
- •3.2.3 Derivation of the OPE
- •3.3.1 Linear Stability Analysis
- •3.3.2 Scales
- •3.3.3 Derivation of the OPE
- •3.4 The Order Parameter Equation for Photorefractive Oscillators
- •3.4.1 Description and Model
- •3.4.2 Adiabatic Elimination and Operator Inversion
- •3.5 Phenomenological Derivation of Order Parameter Equations
- •References
- •4.1 Hydrodynamic Form
- •4.2 Optical Vortices
- •4.2.3 Intermediate Cases
- •4.3 Vortex Interactions
- •References
- •5.2 Domains of Tilted Waves
- •5.3 Square Vortex Lattices
- •References
- •6 Resonators with Curved Mirrors
- •6.1 Weakly Curved Mirrors
- •6.2 Mode Expansion
- •6.2.1 Circling Vortices
- •6.2.2 Locking of Transverse Modes
- •6.3 Degenerate Resonators
- •References
- •7 The Restless Vortex
- •7.1 The Model
- •7.2 Single Vortex
- •7.3 Vortex Lattices
- •7.3.2 Parallel translation of a vortex lattice
- •7.4.1 Mode Expansion
- •7.4.2 Phase-Insensitive Modes
- •7.4.3 Phase-Sensitive Modes
- •References
- •8 Domains and Spatial Solitons
- •8.1 Subcritical Versus Supercritical Systems
- •8.2 Mechanisms Allowing Soliton Formation
- •8.2.1 Supercritical Hopf Bifurcation
- •8.2.2 Subcritical Hopf Bifurcation
- •8.3 Amplitude and Phase Domains
- •8.4 Amplitude and Phase Spatial Solitons
- •References
- •9 Subcritical Solitons I: Saturable Absorber
- •9.1 Model and Order Parameter Equation
- •9.2 Amplitude Domains and Spatial Solitons
- •9.3 Numerical Simulations
- •9.3.1 Soliton Formation
- •9.4 Experiments
- •References
- •10.2 Spatial Solitons
- •10.2.1 One-Dimensional Case
- •10.2.2 Two-Dimensional Case
- •References
- •11 Phase Domains and Phase Solitons
- •11.2 Phase Domains
- •11.3 Dynamics of Domain Boundaries
- •11.3.1 Variational Approach
- •11.4 Phase Solitons
- •11.5 Nonmonotonically Decaying Fronts
- •11.7 Domain Boundaries and Image Processing
- •References
- •12 Turing Patterns in Nonlinear Optics
- •12.1 The Turing Mechanism in Nonlinear Optics
- •12.2.1 General Case
- •12.2.2 Laser with Saturable Absorber
- •12.3.1 Turing Instability in a DOPO
- •12.3.2 Stochastic Patterns
- •References
- •13 Three-Dimensional Patterns
- •13.1 The Synchronously Pumped DOPO
- •13.1.1 Order Parameter Equation
- •13.3 The Nondegenerate OPO
- •13.4 Conclusions
- •13.4.1 Tunability of a System with a Broad Gain Band
- •13.4.2 Analogy Between 2D and 3D Cases
- •References
- •14 Patterns and Noise
- •14.1 Noise in Condensates
- •14.1.1 Spatio-Temporal Noise Spectra
- •14.1.2 Numerical Results
- •14.1.3 Consequences
- •14.2 Noisy Stripes
- •14.2.1 Spatio-Temporal Noise Spectra
- •14.2.2 Stochastic Drifts
- •14.2.3 Consequences
- •References
48 2 Order Parameter Equations for Lasers
Both of these relations will be useful later, at the next order. From (2.35c), we obtain
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At the order O(ε3), the equations read |
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(2.39a) |
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κ ∂T2 |
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= e3 − p3 + µe1 + d2e1 . |
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This system reduces, by applying a solvability condition that actually consists in eliminating the dependence on third-order contributions, to
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κ2 |
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= µe1 −e1 |e1|2 +iΘe2 − |
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Θ2e1 , (2.40) |
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where, in obtaining the last term, we have used |
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κ2 |
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iΘ |
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Θ2e1 . (2.41) |
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κ + γ |
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(κ + γ ) |
Equation (2.40) depends now only on the field amplitude at di erent orders. Let us now define an order parameter A = εe1 + ε2e2. The evolution of the order parameter with respect to the original time t is given by
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∂T1 + ε |
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κ + γ iΘe1 |
+ ε |
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∂T1 |
+ ∂T2 . |
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∂e2 |
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2 κγ |
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(2.42) |
Finally, (2.42), expressed in terms of the original variables, gives the evolution equation of the order parameter,
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+i a 2 − ω A − |
κ2 |
a 2 − ω |
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A , (2.43) |
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which coincides with (2.26), obtained by using the adiabatic-elimination procedure.
References
1.M.C. Cross and P.C. Hohenberg, Pattern formation outside of equilibrium, Rev. Mod. Phys. 65, 851 (1993). 33
References 49
2.R. Graham and H. Haken, Laserlight – first example of a second order phase transition far from thermal equilibrium, Z. Phys. 237, 31 (1970). 34, 41
3.K. Staliunas, Laser Ginzburg–Landau equation and laser hydrodynamics, Phys. Rev. A 48, 1573 (1993). 41
4.J. Lega, J.V. Moloney and A.C. Newell, Swift–Hohenberg equation for lasers, Phys. Rev. Lett. 73, 2978 (1994). 41, 46
5.J.B. Swift and P.C. Hohenberg, Hydrodynamic fluctuations at the convective instability, Phys. Rev. A 15, 319 (1977). 45
6.L.A. Lugiato and R. Lefever, Spatial dissipative structures in passive optical systems, Phys. Rev. Lett. 58, 2209 (1987). 46