Nonlinear Guided Waves and Their Applications最新文献_第6页

Beam control and switching in nonlinear meso-optical structures 非线性介光结构中的光束控制与开关

Nonlinear Guided Waves and Their Applications Pub Date : 1900-01-01 DOI: 10.1364/nlgw.1998.nwa.4

D. Citrin, S. Tomsovic, W. Torruellas

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Parametric Amplification and Squeezing in Quasi-Phase-Matched Waveguides 准相位匹配波导中的参量放大和压缩

Nonlinear Guided Waves and Their Applications Pub Date : 1900-01-01 DOI: 10.1364/nlgw.1995.nthc3

Matthew E. Anderson, M. Beck, M. Raymer, J. Bierlein

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Generation and propagation of stable periodic arrays of soliton stripes in a bulk Kerr liquid 大块克尔液体中稳定周期孤子条纹阵列的产生和传播

Nonlinear Guided Waves and Their Applications Pub Date : 1900-01-01 DOI: 10.1364/nlgw.1998.nthc.2

H. Maillotte, R. Grasser

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Self-writing channel waveguides in As2S3 thin films by two-photon absorption 基于双光子吸收的As2S3薄膜自写通道波导

Nonlinear Guided Waves and Their Applications Pub Date : 1900-01-01 DOI: 10.1364/nlgw.1998.nwb.5

C. Meneghini, A. Villeneuve

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Cascading of second-order processes in a type II phase-matched SHG crystal applied to mode-locking of a CW Nd:YAG laser II型相位匹配SHG晶体的二阶级联过程应用于连续Nd:YAG激光器的锁模

Nonlinear Guided Waves and Their Applications Pub Date : 1900-01-01 DOI: 10.1364/nlgw.1998.nfa.4

V. Couderc, O. Guy, L. Lefort, A. Barthélémy

{"title":"Cascading of second-order processes in a type II phase-matched SHG crystal applied to mode-locking of a CW Nd:YAG laser","authors":"V. Couderc, O. Guy, L. Lefort, A. Barthélémy","doi":"10.1364/nlgw.1998.nfa.4","DOIUrl":"https://doi.org/10.1364/nlgw.1998.nfa.4","url":null,"abstract":"It has been shown recently that a quadratic non-linear crystal may be used for all-optical signal processing. It was demonstrated that amplitude modulation, phase modulation, transistor action, phase conjugaison was feasible thanks to parametric interactions occurring in crystals cut for second harmonic generation (SHG). The main part of these applications was considered under phase mismatched condition1,2,3,4 and relied on the cascading of sum and difference frequency generation (SFG+DFG). With the use of type II crystal a cascading effect still happens in the case of perfect phase-matching provided the two orthogonally polarized inputs at the fundamental frequency carry different intensity5,6,7. This is even one of the most efficient configuration to achieve all-optical processing with the lowest control powers. The interaction between the two waves at the fundamental frequency and the second harmonic wave may be used in specific arrangement to achieve ultrafast switching, pulse compression8, and saturable absorption or transparency9,10. In particular, we have already demonstrated that a type II SHG crystal excited by unbalanced fundamental intensities on its neutral axis gives rise at the output to an electromagnetic field whose state of polarization is intensity dependent (figure 1). In the case of high imbalance between the two fundamental inputs, the weakest fundamental input may completely vanish during propagation because of the SHG process and be further regenerated by difference frequency generation with an opposite phase. The nonlinear evolution of the polarization was previously exploited in a polarization gate geometry to realize a device with self induced transparency9. It was suggested that the same set-up could be used intracavity to achieve mode-locking of a laser. This forms the subject of the present communication since we report the mode locking operation of a diode pumped CW Nd:YAG laser by means of intensity dependent polarization evolution in a KTP crystal.","PeriodicalId":262564,"journal":{"name":"Nonlinear Guided Waves and Their Applications","volume":"30 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"130490285","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}

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Vector CW and solitary wave interactions with mixed Type 1-Type II second-harmonic generation 矢量连续波和孤波与混合型1-型2次谐波的相互作用

Nonlinear Guided Waves and Their Applications Pub Date : 1900-01-01 DOI: 10.1364/nlgw.1998.nthe.6

A. Boardman, P. Bontemps, D. Parker, K. Xie

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Sub-Femtosecond Pulses in 2π-Solitons of the Cascade Stimulated Raman Scattering 级联受激拉曼散射2π孤子中的亚飞秒脉冲

Nonlinear Guided Waves and Their Applications Pub Date : 1900-01-01 DOI: 10.1364/nlgw.1995.nfb5

A. E. Kaplan

{"title":"Sub-Femtosecond Pulses in 2π-Solitons of the Cascade Stimulated Raman Scattering","authors":"A. E. Kaplan","doi":"10.1364/nlgw.1995.nfb5","DOIUrl":"https://doi.org/10.1364/nlgw.1995.nfb5","url":null,"abstract":"The shortest to date optical pulse length of 6 fs [1] was achieved by using pulse compression technique. Further shortening could be attained by using a Fourier synthesizer [2] of separate lasers synchronized by nonlinear phase-locking [3]. Here, we propose a new approach [4] based on multi-frequency cascade Raman stimulated scattering (CSRS) whose components are mode-locked within 2π soliton reminiscent to the self-induced transparency solitons [5], We show that Raman active materials can support solitons consisting of pump laser wave with the frequency ω\u0000 L\u0000 and many cascade-excited Stocks and anti-Stocks component with their frequencies ω\u0000 j\u0000 = ω\u0000 L\u0000 + jω0, j =±1, +2, +3…, mode-locked to each other through a fast \"fullswing\" 2π-nutation of population at the Raman transition with the frequency ω0 ≪ ω\u0000 L\u0000 . Similarly to \"bright-bright\" 2π-solitons in CSRS with two [6] and three [7] components, these solitons have a new, very simple, Lorentzian intensity profile. Due to the engagement of many mode-locked components, however, their total EM field in the time domain consists of the train of ultra-short pulses (separated by the interval 2π/ω0) with their length being of the same order of magnitude or even shorter than the pump cycle, 2π/ω\u0000 L\u0000 . The major feature of the proposed effect is that all the frequency components of the new soliton are so called bright solitons (in contrast to the well known bright+dark soliton combination in SRS [8]) locked to each other and propagating with the same group velocity. The high-order CSRS required to observe the proposed effect, was first observed experimentally in [9] and later in many other experiments, with the total number of components up to ~10-15. The lock-in of all these components into \"all-bright-SRS\" 2π soliton, however, has never been observed in experiment; its feasibility and resulting effects are discussed here.","PeriodicalId":262564,"journal":{"name":"Nonlinear Guided Waves and Their Applications","volume":"1 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"124974240","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}

引用次数: 0

Exact soliton solutions of the cubic-quintic complex Ginzburg-Landau equation 三次五次复金兹堡-朗道方程的精确孤子解

Nonlinear Guided Waves and Their Applications Pub Date : 1900-01-01 DOI: 10.1364/nlgw.1995.pd7

N. Akhmediev, V. V. Afanasjev, J. Soto-Crespo

引用次数: 0

Modulation instability in a nonlinear dispersive fiber cavity including stimulated Raman scattering 包含受激拉曼散射的非线性色散光纤腔中的调制不稳定性

Nonlinear Guided Waves and Their Applications Pub Date : 1900-01-01 DOI: 10.1364/nlgw.1996.sad.17

J. Garcia-Mateos, F. Canal, M. Haelterman

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Chemical Patterning Technique for Periodic Poling of KTP Waveguides KTP波导周期性极化的化学图像化技术

Nonlinear Guided Waves and Their Applications Pub Date : 1900-01-01 DOI: 10.1364/nlgw.1996.fc.6

W. Risk, S. Lau

引用次数: 0