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Nonlinear optics : phenomena, materials, and devices /

"This book is based on tried and tested courses taught by the author, George Stegeman, who is one of the experimental pioneers in nonlinear optics. The book starts with second order phenomena, goes on to explain the derivation of nonlinear susceptibilities, and finishes with a thorough discussi...

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Detalles Bibliográficos
Clasificación:Libro Electrónico
Autor principal: Stegeman, G. I.
Otros Autores: Stegeman, Robert A.
Formato: Electrónico eBook
Idioma:Inglés
Publicado: Hoboken, N.J. : Wiley, 2012.
Colección:Wiley series in pure and applied optics.
Temas:
Acceso en línea:Texto completo

MARC

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245 1 0 |a Nonlinear optics :  |b phenomena, materials, and devices /  |c George I. Stegeman, Robert A. Stegeman. 
260 |a Hoboken, N.J. :  |b Wiley,  |c 2012. 
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588 0 |a Print version record. 
505 0 |6 880-01  |a pt. A. Second-order phenomena -- pt. B. Nonlinear susceptibilities -- pt. C. Third-order phenomena. 
546 |a English. 
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650 0 |a Nonlinear optics. 
650 0 |a Light  |x Scattering. 
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650 4 |a Nonlinear optics. 
650 4 |a SCIENCE  |x Optics. 
650 6 |a Optique non linéaire. 
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880 0 |6 505-00/(S  |a Nonlinear Optics: Phenomena, Materials, and Devices; CONTENTS; PREFACE; 1. Introduction; 1.1 What is Nonlinear Optics and What is it Good for; 1.2 Notation; 1.3 Classical Nonlinear Optics Expansion; 1.4 Simple Model: Electron on a Spring and its Application to Linear Optics; 1.5 Local Field Correction; Problems; Suggested Further Reading; PART A: SECOND-ORDER PHENOMENA; 2. Second-Order Susceptibility and Nonlinear Coupled Wave Equations; 2.1 Anharmonic Oscillator Derivation of Second-Order Susceptibilities; 2.2 Input Eigenmodes, Permutation Symmetry, and Properties of χ(2). 
880 8 |6 505-00/(S  |a 3.1.4.1 Birefringent Wave-Vector-Matched Uniaxial Crystals3.1.4.2 Quasi-Phase-Matched Crystals; 3.1.5 Noncollinear Wave-Vector Match; 3.1.6 Biaxial Crystals; 3.2 Optimizing deff(22); 3.3 Numerical Examples; Problems; References; Suggested Further Reading; 4. Solutions for Plane-Wave Parametric Conversion Processes; 4.1 Solutions of the Type 1 SHG Coupled Wave Equations; 4.1.1 SHG with Wave-Vector Match (Δs = 0); 4.1.2 SHG with Wave-Vector Mismatch (Δs 6 ≠ 0); 4.1.3 Arbitrary Inputs with Δs = 0; 4.2 Solutions of the Three-Wave Coupled Equations; 4.2.1 Sum Frequency Generation. 
880 8 |6 505-00/(S  |a 4.2.2 Difference Frequency Generation4.3 Characteristic Lengths; 4.4 Nonlinear Modes; 4.4.1 Type 1 SHG; 4.4.2 Type 2 SHG; Problems; References; Suggested Further Reading; 5. Second Harmonic Generation with Finite Beams and Applications; 5.1 SHG with Gaussian Beams; 5.1.1 Case I: L ± z0; 5.1.2 Case II: L ≈ 2z0(ω) (Optimum Conversion); 5.1.3 Pulsed Fundamental Finite Beam; 5.1.4 Beam Walk-Off in Space; 5.1.5 Examples of Finite Beam SHG; 5.2 Unique and Performance-Enhanced Applications of Periodically Poled LiNbO3 (PPLN); 5.2.1 Tunable Frequency Conversion. 
880 8 |6 505-01/(S  |a 5.2.2 Enhanced Frequency Bandwidth at Doubled Frequencies5.2.3 Doubling of Ultrashort Pulses; Problems; References; Suggested Further Reading; 6. Three-Wave Mixing, Optical Amplifiers, and Generators; 6.1 Three-Wave Mixing Processes; 6.2 Manley-Rowe Relations; 6.3 Sum Frequency Generation; 6.3.1 Low Depletion Limit with Wave-Vector Mismatch; 6.3.2 Strong Interaction Limit with Depletion; 6.4 Optical Parametric Amplifiers; 6.4.1 Undepleted Pump Approximation (ε (z, ωc) = constant); 6.4.2 Strong Interaction Limit; 6.5 Optical Parametric Oscillator; 6.5.1 Doubly Resonant Cavity. 
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