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Journal articles on the topic 'Nonlinear light generation'

Author: Grafiati

Published: 4 June 2021

Last updated: 14 February 2022

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1

Kruk, Sergey, Alexander Poddubny, Daria Smirnova, et al. "Nonlinear light generation in topological nanostructures." Nature Nanotechnology 14, no. 2 (2018): 126–30. http://dx.doi.org/10.1038/s41565-018-0324-7.

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2

Yoshimura, Masashi, Tomosumi Kamimura, Yoke Khin Yap, Yusuke Mori, and Takatomo Sasaki. "Ultraviolet Light Generation with Nonlinear Optical Borate Crystal." IEEJ Transactions on Electronics, Information and Systems 120, no. 7 (2000): 902–5. http://dx.doi.org/10.1541/ieejeiss1987.120.7_902.

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3

Moody, Galan, Lin Chang, Trevor J. Steiner, and John E. Bowers. "Chip-scale nonlinear photonics for quantum light generation." AVS Quantum Science 2, no. 4 (2020): 041702. http://dx.doi.org/10.1116/5.0020684.

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4

Cai, W., A. P. Vasudev, and M. L. Brongersma. "Electrically Controlled Nonlinear Generation of Light with Plasmonics." Science 333, no. 6050 (2011): 1720–23. http://dx.doi.org/10.1126/science.1207858.

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5

ŚLIWA, I., P. SZLACHETKA, and K. GRYGIEL. "GENERATION OF STRONGLY CHAOTIC BEATS." International Journal of Bifurcation and Chaos 18, no. 03 (2008): 835–40. http://dx.doi.org/10.1142/s0218127408020689.

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This letter proposes a procedure for generating strongly chaotic beats that have been hardly obtainable hitherto. The beats are produced in a nonlinear optical system governing second-harmonic generation of light. The proposition is based on the concept of an optical coupler, but can be easily adopted to other nonlinear systems and Chua's circuits.

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6

DMITRIEV, V. G., and R. SINGH. "GENERATION OF POLARIZATION SQUEEZED LIGHT IN PPNC." International Journal of Quantum Information 01, no. 03 (2003): 403–16. http://dx.doi.org/10.1142/s0219749903000280.

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Theoretical analysis is presented on quantum state evolution of polarization light waves at frequencies ωo and ωe in a periodically poled nonlinear crystal (PPNC). It is shown that the variances of all the four Stokes parameters can be squeezed.

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7

Higuchi, Junichi, Norihiko Nishizawa, Masakazu Mori, Kazuo Yamane, and Toshio Goto. "Nonlinear Polarization Interferometer for Photon-Number Squeezed Light Generation." Japanese Journal of Applied Physics 40, Part 2, No. 11B (2001): L1220—L1222. http://dx.doi.org/10.1143/jjap.40.l1220.

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8

Schraml, Konrad, Armin Regler, Johannes Bartl, et al. "Metamorphic plasmonic nanoantennas for self-enhanced nonlinear light generation." Optica 3, no. 12 (2016): 1453. http://dx.doi.org/10.1364/optica.3.001453.

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9

Anderson, Matthew E., D. F. McAlister, M. G. Raymer та Mool C. Gupta. "Pulsed squeezed-light generation in χ^(2) nonlinear waveguides". Journal of the Optical Society of America B 14, № 11 (1997): 3180. http://dx.doi.org/10.1364/josab.14.003180.

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10

Alekseev, Kirill N. "Squeezed light generation in nonlinear system with chaotic dynamics." Optics Communications 116, no. 4-6 (1995): 468–77. http://dx.doi.org/10.1016/0030-4018(95)91254-y.

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11

Carusotto, Iacopo. "Superfluid light in bulk nonlinear media." Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 470, no. 2169 (2014): 20140320. http://dx.doi.org/10.1098/rspa.2014.0320.

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We review how the paraxial approximation naturally leads to a hydrodynamic description of light propagation in a bulk Kerr nonlinear medium in terms of a wave equation analogous to the Gross–Pitaevskii equation for the order parameter of a superfluid. The main features of the many-body collective dynamics of the fluid of light in this propagating geometry are discussed: generation and observation of Bogoliubov sound waves in the fluid of light is first described. Experimentally accessible manifestations of superfluidity are then highlighted. Perspectives in view of realizing analogue models of

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12

El-Orany, Faisal A. A., J. Perina, and M. Sebawe Abdalla. "Generation of squeezed light in a nonlinear asymmetric directional coupler." Journal of Optics B: Quantum and Semiclassical Optics 3, no. 2 (2001): 67–75. http://dx.doi.org/10.1088/1464-4266/3/2/308.

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13

Butler, Sween, Hongxing Jiang, Jingyu Lin, and Arup Neogi. "Hyperspectral Nonlinear Optical Light Generation from a Monolithic GaN Microcavity." Advanced Optical Materials 5, no. 6 (2017): 1600804. http://dx.doi.org/10.1002/adom.201600804.

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14

Xu, K., P. Loiseau, and G. Aka. "BaCaBO3F: A nonlinear optical crystal investigated for UV light generation." Journal of Crystal Growth 311, no. 8 (2009): 2508–12. http://dx.doi.org/10.1016/j.jcrysgro.2009.01.126.

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15

Mityurich, G. S., M. Aleksiejuk, P. V. Astakhov, P. A. Khilo, and A. N. Serdyukov. "Thermooptical Sound Generation by Bessel Light Beams in Nonlinear Crystals." International Journal of Thermophysics 32, no. 4 (2010): 844–51. http://dx.doi.org/10.1007/s10765-010-0749-1.

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16

Li, Yang, Zhijin Huang, Zhan Sui, et al. "Optical anapole mode in nanostructured lithium niobate for enhancing second harmonic generation." Nanophotonics 9, no. 11 (2020): 3575–85. http://dx.doi.org/10.1515/nanoph-2020-0222.

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AbstractSecond harmonic generation (SHG) with a material of large transparency is an attractive way of generating coherent light sources at exotic wavelength range such as VUV, UV and visible light. It is of critical importance to improve nonlinear conversion efficiency in order to find practical applications in quantum light source and high resolution nonlinear microscopy, etc. Here an enhanced SHG with conversion efficiency up to 10−2% at SH wavelength of 282.7 nm under 11 GW/cm2 pump intensity via the excitation of anapole in lithium niobite (LiNbO3, or LN) nanodisk through the dominating d

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17

Higuchi, Junichi, Norihiko Nishizawa, Masakazu Mori, Ryousuke Goto, Kazuo Yamane, and Toshio Goto. "Analysis of Photon-Number Squeezed Light Generation Using Nonlinear Polarization Interferometer." IEEJ Transactions on Electronics, Information and Systems 123, no. 3 (2003): 440–45. http://dx.doi.org/10.1541/ieejeiss.123.440.

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18

Mecozzi, Antonio. "Parametric amplification and squeezed-light generation in a nonlinear directional coupler." Optics Letters 13, no. 10 (1988): 925. http://dx.doi.org/10.1364/ol.13.000925.

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19

Chaiyasoonthorn, S., and P. P. Yupapin. "Generalized fast light generation with multi-stage nonlinear micro ring resonators." Optik 121, no. 3 (2010): 268–73. http://dx.doi.org/10.1016/j.ijleo.2008.07.006.

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20

MAGNON, ANNE. "NONLINEAR GRAVITON AND THE PROBLEM OF MASS GENERATION." Modern Physics Letters A 16, no. 14 (2001): 891–95. http://dx.doi.org/10.1142/s0217732301004194.

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We argue that the massless mediator of a long range interaction can acquire mass through collision with a nonlinear graviton. The process displays analogy with the Higgs mechanism, and compensates for a broken mirror symmetry (duality), at the past–future bifurcation. Mass is formulated as the electric charge of a suitable state emerging from the particle–antiparticle (self–antiself dual) confrontation. Such considerations suggest that the experimental quest of the Higgs boson could in fact shed light on the (so far theoretical) quantum gravity programme.

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21

SASAKI, TAKATOMO, YUSUKE MORI, and MASASHI YOSHIMURA. "DEVELOPMENT OF NEW NLO BORATE CRYSTALS." Journal of Nonlinear Optical Physics & Materials 10, no. 02 (2001): 249–63. http://dx.doi.org/10.1142/s0218863501000589.

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Interests in the use of borate crystals in ultraviolet nonlinear optics have increased because all-solid-state UV lasers obtained with NLO crystals are in highly demand for scientific and industrial applications. Recently, new borate crystals, CsLiB 6 O 10 and Gd x Y 1-x Ca 4 O ( BO 3)3 have been developed by the present authors. CsLiB 6 O 10 is for fourth- and fifth-harmonic generations of Nd:YAG laser, Gd x Y 1-x Ca 4 O ( BO 3)3 for third-harmonic generation. This paper reviews the growth and nonlinear optical properties of these new borate crystals and the progress in UV light generation.

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22

ASSANTO, GAETANO, and MARCO PECCIANTI. "ROUTING LIGHT AT WILL." Journal of Nonlinear Optical Physics & Materials 16, no. 01 (2007): 37–47. http://dx.doi.org/10.1142/s0218863507003536.

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We present a comprehensive review on the routing of self-confined light-beams in liquid crystals, i.e., generation, propagation and angular steering of self-induced waveguides or spatial solitons in a nonlinear non local dielectric with a large electro-optic response. We describe all-optical routing through soliton-soliton or soliton-beam interactions, as well as voltage-controlled steering in an anisotropic geometry via birefringence or refraction/reflection at a graded interface.

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23

Rigler, Martin, Tinkara Troha, Wei Guo, et al. "Second-Harmonic Generation of Blue Light in GaN Waveguides." Applied Sciences 8, no. 8 (2018): 1218. http://dx.doi.org/10.3390/app8081218.

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Second-harmonic generation was studied in III-metal-polar GaN films grown on sapphire substrates by metalorganic chemical vapor deposition and formed into ridge waveguides. Broadband near-IR femtosecond pulses of an optical parametric amplifier system were injected by end-fire coupling and the nonlinear response was measured while tuning the central wavelength. A prominent peak was found at 450 nm for 1140 nm thick and 10 μm wide GaN waveguides. The measured second-harmonic peak was in agreement with the modal-dispersion phase matching condition calculated using the dispersion of the extraordi

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24

Lin, Xianqing, Yingying Liu, Kang Wang, et al. "Hybrid Three-Dimensional Spiral WSe2 Plasmonic Structures for Highly Efficient Second-Order Nonlinear Parametric Processes." Research 2018 (December 9, 2018): 1–8. http://dx.doi.org/10.1155/2018/4164029.

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Two-dimensional (2D) layered materials, with large second-order nonlinear susceptibility, are currently growing as an ideal candidate for fulfilling tunable nanoscale coherent light through the second-order nonlinear optical parametric processes. However, the atomic thickness of 2D layered materials leads to poor field confinement and weak light-matter interaction at nanoscale, resulting in low nonlinear conversion efficiency. Here, hybrid three-dimensional (3D) spiral WSe2 plasmonic structures are fabricated for highly efficient second harmonic generation (SHG) and sum-frequency generation (S

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25

Jaque, Daniel. "Red, blue, and green laser-light generation from the NYAB nonlinear crystal." Optical Engineering 38, no. 11 (1999): 1794. http://dx.doi.org/10.1117/1.602298.

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26

Potasek, M. J., and B. Yurke. "Squeezed-light generation in a medium governed by the nonlinear Schrödinger equation." Physical Review A 35, no. 9 (1987): 3974–77. http://dx.doi.org/10.1103/physreva.35.3974.

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27

Skarka, V., V. I. Berezhiani, and R. Miklaszewski. "Generation of light spatiotemporal solitons from asymmetric pulses in saturating nonlinear media." Physical Review E 59, no. 1 (1999): 1270–73. http://dx.doi.org/10.1103/physreve.59.1270.

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28

Tricca, D., C. Sibilia, S. Severini, et al. "Photonic bandgap structures in planar nonlinear waveguides: application to squeezed-light generation." Journal of the Optical Society of America B 21, no. 3 (2004): 671. http://dx.doi.org/10.1364/josab.21.000671.

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29

Henstridge, M., C. Pfeiffer, D. Wang, et al. "Synchrotron radiation from an accelerating light pulse." Science 362, no. 6413 (2018): 439–42. http://dx.doi.org/10.1126/science.aat5915.

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Synchrotron radiation—namely, electromagnetic radiation produced by charges moving in a curved path—is regularly generated at large-scale facilities where giga–electron volt electrons move along kilometer-long circular paths. We use a metasurface to bend light and demonstrate synchrotron radiation produced by a subpicosecond pulse, which moves along a circular arc of radius 100 micrometers inside a nonlinear crystal. The emitted radiation, in the terahertz frequency range, results from the nonlinear polarization induced by the pulse. The generation of synchrotron radiation from a pulse revolvi

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30

Zhao, Wen Lei, and Lan Zhao. "Simulation Study on Characteristics of Nonlinear Photonic Crystal." Applied Mechanics and Materials 568-570 (June 2014): 577–80. http://dx.doi.org/10.4028/www.scientific.net/amm.568-570.577.

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Light propagation in the medium is light-matter interaction process. For such a dynamic process, the process can be viewed as consisting of two sub-components: radiative processes and media response process medium light. This paper describes a two-dimensional nonlinear optical microcavities coupling of changing circumstances, to study the two-dimensional photon - photon mixed gas condensation, quantum phase transition, the post also pointed out that the mixed gas of quantum phase transitions and non-traditional linear optics and frequency generation relationship.

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31

Borland, Michael, Glenn Decker, Louis Emery, Vadim Sajaev, Yipeng Sun, and Aimin Xiao. "Lattice design challenges for fourth-generation storage-ring light sources." Journal of Synchrotron Radiation 21, no. 5 (2014): 912–36. http://dx.doi.org/10.1107/s1600577514015203.

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Third-generation low-emittance storage-ring light sources based on double- and triple-bend cells and undulator magnets have been in operation around the world for more than two decades. On the horizon is a new generation based on the multi-bend achromat (MBA) lattice concept promising two to three orders of magnitude higher brightness than is available in today's sources. In this paper, the challenges inherent in designing MBA lattices, as well as potential solutions, are described. Topics covered include lattice concepts, scaling of storage-ring performance, brightness optimization, nonlinear

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32

Rodrigues, Sílvia M. G., Margarida Facão, and Mário F. S. Ferreira. "Supercontinuum generation in chalcogenide layered spiral microstructured optical fiber." Journal of Nonlinear Optical Physics & Materials 26, no. 04 (2017): 1750049. http://dx.doi.org/10.1142/s0218863517500497.

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The layered spiral microstructured optical fiber (LS-MOF) design allows higher nonlinearities than the most common microstructured optical fibers. Here, we have chosen a highly nonlinear glass for its composition, the arsenic trisulfide, and we have determined its dispersion and nonlinear characteristics. After adjusting the fiber’s parameters, we obtained a record value for the nonlinear parameter of 50.7[Formula: see text]W[Formula: see text]m[Formula: see text], at 1.550[Formula: see text][Formula: see text]m. We have simulated light propagation under these optimized circumstances, achievin

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33

Fox, A. M., M. Dabbicco, and J. F. Ryan. "Generation of Non-Classical Light by Four-Wave Mixing in Semiconductors." Journal of Nonlinear Optical Physics & Materials 07, no. 02 (1998): 167–80. http://dx.doi.org/10.1142/s0218863598000156.

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We describe experiments to generate non-classical quadrature squeezed states of light by four-wave mixing in semiconductors. Squeezing can be achieved with either the diagonal or off-diagonal components of the third-order nonlinear susceptibility tensor. We have demonstrated squeezing by self-phase modulation in ZnS at 780 nm, and by cross-phase modulation in ZnSe at 960 nm. Possibilities for generating squeezed light in other materials by these techniques are discussed.

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34

Tuniz, Alessandro. "Nanoscale nonlinear plasmonics in photonic waveguides and circuits." La Rivista del Nuovo Cimento 44, no. 4 (2021): 193–249. http://dx.doi.org/10.1007/s40766-021-00018-7.

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AbstractOptical waveguides are the key building block of optical fiber and photonic integrated circuit technology, which can benefit from active photonic manipulation to complement their passive guiding mechanisms. A number of emerging applications will require faster nanoscale waveguide circuits that produce stronger light-matter interactions and consume less power. Functionalities that rely on nonlinear optics are particularly attractive in terms of their femtosecond response times and terahertz bandwidth, but typically demand high powers or large footprints when using dielectrics alone. Pla

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35

SHABANOV, SERGEI V. "RESONANT LIGHT SCATTERING AND HIGHER HARMONIC GENERATION BY PERIODIC SUBWAVELENGTH ARRAYS." International Journal of Modern Physics B 23, no. 27 (2009): 5191–236. http://dx.doi.org/10.1142/s0217979209054478.

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Scattering of light on periodic subwavelength arrays is studied in the framework of the resonant scattering theory. With various examples of periodic structures it is demonstrated that: (i) an enhanced reflectance or transmittance is associated with the existence of trapped modes (quasi-stationary modes of light confined in the vicinity of the scattering structure); (ii) scattering structures may have trapped modes due to peculiarities their geometry (geometrical modes) and the dispersive properties of their material (material modes); a practical criterion based on the scaling symmetry of Maxw

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36

Korner, Kevin, Alexa S. Kuenstler, Ryan C. Hayward, Basile Audoly, and Kaushik Bhattacharya. "A nonlinear beam model of photomotile structures." Proceedings of the National Academy of Sciences 117, no. 18 (2020): 9762–70. http://dx.doi.org/10.1073/pnas.1915374117.

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Actuation remains a significant challenge in soft robotics. Actuation by light has important advantages: Objects can be actuated from a distance, distinct frequencies can be used to actuate and control distinct modes with minimal interference, and significant power can be transmitted over long distances through corrosion-free, lightweight fiber optic cables. Photochemical processes that directly convert photons to configurational changes are particularly attractive for actuation. Various works have reported light-induced actuation with liquid crystal elastomers combined with azobenzene photoch

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37

NGUYEN, BA AN, and THAI HOA TRAN. "GENERATION OF SQUEEZED EXCITONS IN SEMICONDUCTORS BY COHERENT LIGHT." Modern Physics Letters B 06, no. 07 (1992): 405–10. http://dx.doi.org/10.1142/s0217984992000491.

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In this letter, we show that semiconductor excitons generated by coherent light may become squeezed. This is due to their interactions both with the light and among themselves. Based on a polariton theory and using a secular approximation, analytical expressions for exciton quadrature variances have been derived, which enable us to study easily the dependence of exciton squeezing degree on the pumping light intensity, frequency detuning and strength of exciton-exciton, as well as exciton-photon, interactions.

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38

ŚLIWA, I., P. SZLACHETKA, and K. GRYGIEL. "CHAOTIC BEATS IN A NONAUTONOMOUS SYSTEM GOVERNING SECOND-HARMONIC GENERATION OF LIGHT." International Journal of Bifurcation and Chaos 17, no. 09 (2007): 3253–57. http://dx.doi.org/10.1142/s0218127407019019.

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This letter proposes a procedure for generation and control of chaotic beats in a dynamical system that is initially in the periodic state. The dynamical system describes a simple nonlinear optical process — second-harmonic generation of light. The periodic states of the system are found to be in analytical forms. We also investigate some aspects of synchronization of chaotic beats in two systems, detuned in the pump fields.

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39

Ducci, Sara, Perola Milman, and Eleni Diamanti. "Generation of quantum states of light in nonlinear AlGaAs chips: engineering and applications." Photoniques, no. 107 (March 2021): 28–34. http://dx.doi.org/10.1051/photon/202110728.

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Photonic quantum technologies represent a promising platform for applications ranging from long-distance secure communications to the simulation of complex phenomena. Among the different material platforms, direct bandgap semiconductors offer a wide range of functionalities opening promising perspectives for the implementation of future quantum technologies. In this paper, we review our progress on the generation and manipulation of quantum states of light in nonlinear AlGaAs chips and their use in quantum networks.

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40

Xu, Ke, Pascal Loiseau, Gerard Aka, and Julien Lejay. "A New Promising Nonlinear Optical Crystal for Ultraviolet Light Generation: Ca5(BO3)3F." Crystal Growth & Design 9, no. 5 (2009): 2235–39. http://dx.doi.org/10.1021/cg800958u.

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41

Kroychuk, Maria K., Alexander S. Shorokhov, Damir F. Yagudin, et al. "Enhanced Nonlinear Light Generation in Oligomers of Silicon Nanoparticles under Vector Beam Illumination." Nano Letters 20, no. 5 (2020): 3471–77. http://dx.doi.org/10.1021/acs.nanolett.0c00393.

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42

Chen, Yue-Yue, Karen Z. Hatsagortsyan та Christoph H. Keitel. "Generation of twisted γ-ray radiation by nonlinear Thomson scattering of twisted light". Matter and Radiation at Extremes 4, № 2 (2019): 024401. http://dx.doi.org/10.1063/1.5086347.

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43

Vidal, Xavier, Jose Raul Herance, Jordi Marquet, Jose Luis Bourdelande, and Jordi Martorell. "Modified triphenylmethane dye for the efficient nonlinear generation of light in nanostructured materials." Applied Physics Letters 91, no. 8 (2007): 081116. http://dx.doi.org/10.1063/1.2773934.

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44

Averbukh, B. B. "Generation of s-polarized surface-like electromagnetic waves during nonlinear resonant light scattering." Technical Physics Letters 38, no. 1 (2012): 4–5. http://dx.doi.org/10.1134/s1063785012010026.

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45

Hou, Z. Y., M. J. Xia, L. R. Wang, et al. "Ultrastable, high efficiency picosecond green light generation using K3B6O10Br series nonlinear optical crystals." Laser Physics 27, no. 9 (2017): 095401. http://dx.doi.org/10.1088/1555-6611/aa7f95.

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46

Ding, Wei, Liangcheng Zhou, and Stephen Y. Chou. "Enhancement and Electric Charge-Assisted Tuning of Nonlinear Light Generation in Bipolar Plasmonics." Nano Letters 14, no. 5 (2014): 2822–30. http://dx.doi.org/10.1021/nl5008294.

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47

Neogi, A., Y. Takahashi, and H. Kawaguchi. "Interband nonlinear optical generation in presence of intersubband light in asymmetric quantum wells." IEEE Journal of Quantum Electronics 32, no. 4 (1996): 701–11. http://dx.doi.org/10.1109/3.488845.

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48

Khalil, Sh M., F. Sharaf, and B. F. Mohamed. "Nonlinear second harmonic generation by light wave-plasma interaction in oscillating magnetic field." International Journal of Theoretical Physics 32, no. 11 (1993): 2053–58. http://dx.doi.org/10.1007/bf00675019.

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49

Khilo, P. A., and E. S. Petrova. "Second-harmonic generation by elliptic Bessel light beams in periodically polarized nonlinear crystals." Journal of Applied Spectroscopy 72, no. 6 (2005): 824–28. http://dx.doi.org/10.1007/s10812-006-0010-7.

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50

Frigenti, Gabriele, Daniele Farnesi, Gualtiero Nunzi Conti, and Silvia Soria. "Nonlinear Optics in Microspherical Resonators." Micromachines 11, no. 3 (2020): 303. http://dx.doi.org/10.3390/mi11030303.

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Nonlinear frequency generation requires high intensity density which is usually achieved with pulsed laser sources, anomalous dispersion, high nonlinear coefficients or long interaction lengths. Whispering gallery mode microresonators (WGMRs) are photonic devices that enhance nonlinear interactions and can be exploited for continuous wave (CW) nonlinear frequency conversion, due to their capability of confine light for long time periods in a very small volume, even though in the normal dispersion regime. All signals must be resonant with the cavity. Here, we present a review of nonlinear optic

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