Relevant bibliographies by topics / Optical resonance

Academic literature on the topic 'Optical resonance'

Author: Grafiati
Published: 4 June 2021
Last updated: 28 July 2024

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Journal articles on the topic "Optical resonance"

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Jinhua Hu, Jinhua Hu, Xiuhong Liu Xiuhong Liu, Jijun Zhao Jijun Zhao, and and Jun Zou and Jun Zou. "Investigation of Fano resonance in compound resonant waveguide gratings for optical sensing." Chinese Optics Letters 15, no. 3 (2017): 030502–30505. http://dx.doi.org/10.3788/col201715.030502.

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Dongyang Wang, Dongyang Wang, Jiaguang Han Jiaguang Han, and Shuang Zhang Shuang Zhang. "Optical cavity resonance with magnetized plasma." Chinese Optics Letters 16, no. 5 (2018): 050005. http://dx.doi.org/10.3788/col201816.050005.

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Halas, Naomi. "Playing with Plasmons: Tuning the Optical Resonant Properties of Metallic Nanoshells." MRS Bulletin 30, no. 5 (May 2005): 362–67. http://dx.doi.org/10.1557/mrs2005.99.

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AbstractNanoshells, concentric nanoparticles consisting of a dielectric core and a metallic shell, are simple spherical nanostructures with unique, geometrically tunable optical resonances. As with all metallic nanostructures, their optical properties are controlled by the collective electronic resonance, or plasmon resonance, of the constituent metal, typically silver or gold. In striking contrast to the resonant properties of solid metallic nanostructures, which exhibit only a weak tunability with size or aspect ratio, the optical resonance of a nanoshell is extraordinarily sensitive to the inner and outer dimensions of the metallic shell layer. The underlying reason for this lies beyond classical electromagnetic theory, where plasmon-resonant nanoparticles follow a mesoscale analogue of molecular orbital theory, hybridizing in precisely the same manner as the individual atomic wave functions in simple molecules. This plasmon hybridization picture provides an essential “design rule” for metallic nanostructures that can allow us to effectively predict their optical resonant properties. Such a systematic control of the far-field optical resonances of metallic nanostructures is accomplished simultaneously with control of the field at the surface of the nanostructure. The nanoshell geometry is ideal for tuning and optimizing the near-field response as a stand-alone surface-enhanced Raman spectroscopy (SERS) nanosensor substrate and as a surface-plasmon-resonant nanosensor.Tuning the plasmon resonance of nanoshells into the near-infrared region of the spectrum has enabled a variety of biomedical applications that exploit the strong optical contrast available with nanoshells in a spectral region where blood and tissue are optimally transparent.
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Aşırım, Özüm Emre, and Mustafa Kuzuoğlu. "Numerical Study of Resonant Optical Parametric Amplification via Gain Factor Optimization in Dispersive Microresonators." Photonics 7, no. 1 (December 25, 2019): 5. http://dx.doi.org/10.3390/photonics7010005.

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The achievement of wideband high-gain optical parametric amplification has not been shown in micrometer-scale cavities. In this paper we have computationally investigated the optical parametric amplification process in a few micrometer-long dispersive microresonator. By performing a gain medium resonance frequency dependent analysis of optical parametric amplification, we have found that it is possible to achieve a wideband high-gain optical amplification in a dispersive microresonator. In order to account for the effects of dispersion (modeled by the polarization damping coefficient) and the resonance frequency of the gain medium on optical parametric amplification, we have solved the wave equation in parallel with the nonlinear equation of electron cloud motion, using the finite difference time domain method. Then we have determined the resonance frequency values that yield an enhanced or a resonant case of optical parametric amplification, via gain factor optimization. It was observed that if the microresonator is more dispersive (has a lower polarization damping coefficient), then there are more resonance frequencies that yield an optical gain resonance. At these gain resonances, a very wideband, high-gain optical amplification seems possible in the micron scale, which, to our knowledge, has not been previously reported in the context of nonlinear wave mixing theory.
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Jáuregui-López, Irati, Pablo Rodriguez-Ulibarri, Sergei Kuznetsov, Nazar Nikolaev, and Miguel Beruete. "THz Sensing With Anomalous Extraordinary Optical Transmission Hole Arrays." Sensors 18, no. 11 (November 9, 2018): 3848. http://dx.doi.org/10.3390/s18113848.

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Subwavelength hole array (HA) metasurfaces support the so-called extraordinary optical transmission (EOT) resonance that has already been exploited for sensing. In this work, we demonstrate the superior performance of a different resonant regime of HA metasurfaces called anomalous EOT, by doing a thorough numerical and experimental study of its ability in thin-film label-free sensing applications in the terahertz (THz) band. A comprehensive analysis using both the regular and anomalous EOT resonances is done by depositing thin layers of dielectric analyte slabs of different thicknesses on the structures in different scenarios. We carry out a detailed comparison and demonstrate that the best sensing performance is achieved when the structure operates in the anomalous EOT resonance and the analyte is deposited on the non-patterned side of the metasurface, improving by a factor between 2 and 3 the results of the EOT resonance in any of the considered scenarios. This can be explained by the comparatively narrower linewidth of the anomalous EOT resonance. The results presented expand the reach of subwavelength HAs for sensing applications by considering the anomalous EOT regime that is usually overlooked in the literature.
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Sun, Linshan, Bo Zhao, Jiaqi Yuan, Yanrong Zhang, Ming Kang, and Jing Chen. "Optical resonance in inhomogeneous parity-time symmetric systems." Chinese Optics Letters 19, no. 7 (2021): 073601. http://dx.doi.org/10.3788/col202119.073601.

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HORING, NORMAN J. MORGENSTERN, and H. L. CUI. "SURFACE-PLASMON-RESONANCE BASED OPTICAL SENSING." International Journal of High Speed Electronics and Systems 18, no. 01 (March 2008): 71–78. http://dx.doi.org/10.1142/s012915640800514x.

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Over the past twenty years, surface plasmon resonance has been developed as an effective technique for use in real-time biotechnological measurements of the kinetics of label-free biomolecular interactions with high sensitivity.1-16 On a fundamental level, it is the dielectric-imaging involvement of the adsorbed biomolecular layer (DNA for example) in shifting the surface plasmon resonance (SPR) frequency by means of electrostatic coupling at the interface with the metal film substrate that facilitates SPR-based optical sensing. Of course, there are various factors that can influence surface plasmon resonance, including plasma nonlocality, phonons, multiplicity of layers, all of which should be carefully examined. Moreover, tunable SPR phenomenology based on the role of a magnetic field (both classically and quantum mechanically) merits consideration in regard to the field's effects on both the substrate17 and the adsorbed layer(s).18 This paper is focused on the establishment of the basic equations governing surface plasmon resonance, incorporating all the features cited above. In it, we present the formulation and closed-form analytical solution for the dynamic, nonlocal screening function of a thick substrate material with a thin external adsorbed layer, which can be extended to multiple layers. The result involves solution of the random phase approximation (RPA) integral equation for the spatially inhomogeneous system of the substrate and adsorbed layer,19-25 given the individual polarizabilities of the thick substrate and the layer. (This is tantamount to the space-time matrix inversion of the inhomogeneous joint dielectric function of the system.) The frequency poles of the resulting screening function determine the shifted surface (and bulk) plasmon resonances and the associated residues at the resonance frequencies provide their relative excitation amplitudes. The latter represent the response strengths of the surface plasmon resonances (oscillator strengths), and will be of interest in optimizing the materials to be employed.
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Babunts, R. A., Yu A. Uspenskaya, A. S. Gurin, A. P. Bundakova, G. V. Mamin, A. N. Anisimov, E. N. Mokhov, and P. G. Baranov. "Manifestations of Electron–Nuclear Interactions in the High-Frequency ENDOR/ODMR Spectra for Triplet Si–C Divacancies in 13C-Enriched SiC." JETP Letters 116, no. 7 (October 2022): 485–92. http://dx.doi.org/10.1134/s0021364022601865.

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The frequencies of electron–nuclear interactions with 13C and 29Si nuclei on remote coordination spheres are determined in triplet spin centers in the form of neutral VSi–VC divacancies in a silicon carbide crystal of the hexagonal polytype 6H–SiC enriched tenfold in the 13C isotope. High-frequency electron–nuclear double resonance and optically detected magnetic resonance under conditions of optical alignment of spins are used. Oscillations of the electron spin density on 29Si and 13C nuclei are found. Nuclear magnetic resonance transitions at Larmor and close-to-Larmor frequencies of 13C and 29Si cause giant changes in the populations of spin sublevels with the transformation of these resonances into electron paramagnetic resonance and optical signals.
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Husnik, Martin, Felix von Cube, Stephan Irsen, Stefan Linden, Jens Niegemann, Kurt Busch, and Martin Wegener. "Comparison of electron energy-loss and quantitative optical spectroscopy on individual optical gold antennas." Nanophotonics 2, no. 4 (October 1, 2013): 241–45. http://dx.doi.org/10.1515/nanoph-2013-0031.

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AbstractUsing a rather large set of different individual metallic optical antennas, we compare directly measured electron energy-loss spectra with measured quantitative optical extinction and scattering cross-section spectra on the identical antennas. All antenna resonances lie near 1.4 µm wavelength. In contrast to other reports, we find identical resonance positions for electrons and photons to within the experimental errors. We discuss possible artifacts which can lead to seemingly different resonance positions in experiments. Our experimental results agree well with complete numerical calculations of both sorts of spectra.
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Zheng, Ningxuan, Wenliang Liu, Jizhou Wu, Yuqing Li, Vladimir Sovkov, and Jie Ma. "Parametric Excitation of Ultracold Sodium Atoms in an Optical Dipole Trap." Photonics 9, no. 7 (June 22, 2022): 442. http://dx.doi.org/10.3390/photonics9070442.

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Parametric modulation is an effective tool to measure the trap frequency and investigate the atom dynamics in an optical dipole trap or lattices. Herein, we report on experimental research of parametric resonances in an optical dipole trap. By modulating the trapping potential, we have measured the atomic loss dependence on the frequency of the parametric modulations. The resonance loss spectra and the evolution of atom populations at the resonant frequency have been demonstrated and compared under three modulation waveforms (sine, triangle and square waves). A phenomenological theoretical simulation has been performed and shown good accordance with the observed resonance loss spectra and the evolution of atom populations. The theoretical analysis can be easily extended to a complex waveform modulation and reproduce enough of the experiments.
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Dissertations / Theses on the topic "Optical resonance"

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Barrett, C. P. "Optical-microwave double resonance." Thesis, University of East Anglia, 1985. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.355527.

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Zongo, Sidiki. "Nonlinear optical properties of natural dyes based on optical resonance." Thesis, University of the Western Cape, 2012. http://hdl.handle.net/11394/4635.

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>Magister Scientiae - MSc
Recent research shows that the study of optical properties of organic material natural dyes has gained much consideration. The specific functional groups in several natural dyes remain essential for the large nonlinear absorption expressed in terms of nonlinear optical susceptibilities or other mechanism of absorption such as two photon absorption (TPA), reverse saturable absorption (RSA) or intensitydependent refractive index characteristic. In this thesis we highlight the optical limiting responses of selected natural dyes as nonlinear response in the femtosecond regime. This technique refers to the decrease of the transmittance of the material with the increased incident light intensity.Three dyes derived from beetroot, flame flower and mimosa flower dyes were investigated. The results showed a limiting behaviour around 795 mW for the beetroot and the flame dye while there is total transmission in the flame dye sample. The performance of the nonlinearity i.e. the optical limiting is related to the existence of alternating single and double bonds (i.e. C-C and C=C bonds) in the molecules that provides the material with the electron delocalization, but also it is related to the light intensity.Beside nonlinearity study, crystallographic investigation was carried out for more possible applicability of the selected dyes and this concerned only the mimosa and flame flower dye thin film samples since the beetroot thin film was very sensitive to strong irradiation (i.e. immediately destroyed when exposed to light with high intensity). For more stability,dye solutions were encapsulated in gels for further measurements.
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Tsia, Kin Man. "Optical resonances in photonic-crystal-embedded microcavities /." View abstract or full-text, 2005. http://library.ust.hk/cgi/db/thesis.pl?ELEC%202005%20TSIA.

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Chinowsky, Timothy Mark. "Optical multisensors based on surface plasmon resonance /." Thesis, Connect to this title online; UW restricted, 2000. http://hdl.handle.net/1773/5857.

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Rajaram, Bhavani. "Optical-optical double resonance study of the 3¹ A¹ state of HCP." Thesis, Massachusetts Institute of Technology, 1995. http://hdl.handle.net/1721.1/32155.

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HOLM, DAVID ALLEN. "QUANTUM THEORY OF MULTIWAVE MIXING (RESONANCE FLUORESCENCE, SATURATION SPECTROSCOPY, MODULATION, PHASE CONJUGATION, QUANTUM NOISE)." Diss., The University of Arizona, 1985. http://hdl.handle.net/10150/187980.

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This dissertation formulates and applies a theory describing how one or two strong classical waves and one or two weak quantum mechanical waves interact in a two-level medium. The theory unifies many topics in quantum optics, such as resonance fluorescence, saturation spectroscopy, modulation spectroscopy, the build up of laser and optical bistability instabilities, and phase conjugation. The theory is based on a quantum population pulsation approach that resembles the semiclassical theories, but is substantially more detailed. Calculations are performed to include the effects of inhomogeneous broadening, spatial hole burning, and Gaussian transverse variations. The resonance fluorescence spectrum in a high finesse optical cavity is analyzed in detail, demonstrating how stimulated emission and multiwave processes alter the spectrum from the usual three peaks. The effects of quantum noise during the propagation of weak signal and conjugate fields in phase conjugation and modulation spectroscopy are studied. Our analysis demonstrates that quantum noise affects not only the intensities of the signal and conjugate, but also their relative phase, and in particular we determine a quantum limit to the semiclassical theory of FM modulation spectroscopy. Finally, we derive the corresponding theory for the two-photon, two-level medium. This yields the first calculation of the two-photon resonance fluorescence spectrum. Because of the greater number of possible interactions in the two-photon two-level model, the theoretical formalism is considerably more complex, and many effects arise that are absent in the one-photon problem. We discuss the role of the Stark shifts on the emission spectrum and show how the Rayleigh scattering is markedly different.
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Booker, Annette Casandra. "Optical Characterization and Evaluation of Dye-Nanoparticle Interactions." Thesis, Virginia Tech, 2006. http://hdl.handle.net/10919/36370.

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Surface plasmon resonance has become a widely investigated phenomenon in the past few years. Initially descriptive of light interactions with metallic films, research has branched out to encompass the nanoparticles as well. Generation of the maximum surface plasmon resonance for nanostructures is based on the resonance condition that the oscillatory behavior of the 'free' electrons on the surface of the particle become equivalent to the frequency of the excitation light; for films this required a specific geometry. Metallic nanoparticles have also interested researchers because of their unique optical properties. Depending on the metal, observations of quenching as well as fluorescence enhancement have been reported. Based on the phenomenon of surface plasmon resonance as well as the properties of metallic nanoparticles, this research reports the interaction of gold and silver nanoparticles in an aqueous dye solution. Our research is the basis for developing an optical sensor used for water treatment centers as an alarm mechanism. Due to the inefficiency of the fluorophore used in similar optodes, sufficient fluorescence was not obtained. With the addition of the nanoparticles, we hoped to observe the transfer of energy from the nanoparticle to the fluorophore to increase the overall intensity, thereby creating a sufficient signal. Using the excitation theories discovered by Raman, Mie, and Forster and Dexter as our foundation, we mixed a strongly fluorescent dye with gold nanoparticles and aagain with silver nanoparticles. After taken measurements via fluorescence spectroscopy, absorption spectroscopy, and photoluminescence excitation, we observed that the silver nanoparticles seemed to enhance the fluorescence of the dye while the gold nanoparticles quenched the fluorescence.
Master of Science
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Vukusic, Peter. "Sensing thin layers using surface plasmon resonance." Thesis, University of Exeter, 1993. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.358142.

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Ma, Ning. "Laterally coupled hexagonal micro-pillar resonator add-drop filters for optical communications /." View abstract or full-text, 2004. http://library.ust.hk/cgi/db/thesis.pl?ELEC%202004%20MA.

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Thesis (M. Phil.)--Hong Kong University of Science and Technology, 2004.
Includes bibliographical references (leaves 131-141). Also available in electronic version. Access restricted to campus users.
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Booth, Ian. "Optical detection of paramagnetic and cyclotron resonance in semiconductors." Thesis, University of British Columbia, 1985. http://hdl.handle.net/2429/25566.

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Optical Detection of Magnetic Resonance (ODMR) has been used to observe both paramagnetic and diamagnetic resonance of photo-excited electrons and holes in GaP, ZnTe and AgBr. Paramagnetic resonance of conduction electrons in GaP has been studied and the microwave frequency and power dependence of the effect analysed. The maximum signal strength was observed to produce approximately 1% change in luminescence at 1.6 K. The g value deduced from the resonance was 2.000 ± 0.005. The resonance was homogeneously broadened giving the electron lifetime as approximately 4 nanoseconds. Paramagnetic resonance of electrons and holes has also been detected in AgBr. The background signals present in ODMR experiments have been investigated and are shown to be caused by diamagnetic or cyclotron resonance heating of photoexcited carriers. Measurements at microwave frequencies of 9.2 and 36.3 GHz have been made on GaP,ZnTe and AgBr, and cyclotron resonance of electrons and holes observed. The effective masses of light and heavy holes in GaP were found to be 0.154 ± 0.01 and 0.626 ± 0.06 respectively while the electron effective mass was 0.36 ± 0.10. The electron scattering time was shorter than that for holes by a factor of approximately three, most likely due to scattering by isoelectronic nitrogen impurities. Resonances were observed in ZnTe at effective mass values of 0.30 ± 0.20 and 0.76 ± 0.20 corresponding to electrons and heavy holes. In both GaP and ZnTe resonances due to electrons and holes appeared in different luminescence bands indicating the sensitivity of different recombination centres to heating of either carrier type. Cyclotron resonance of electrons and holes was also observed in AgBr and showed the effects of conduction and valence band non-parabolicity. A feature in the electron resonance indicated enhanced trapping of electrons with certain energies by emission of one or more LO phonons.
Science, Faculty of
Physics and Astronomy, Department of
Graduate
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Books on the topic "Optical resonance"

1

Barrett, Christopher Paul. Optical-microwave double resonance. Norwich: University of East Anglia, 1985.

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1935-, Eberly J. H., ed. Optical resonance and two-level atoms. New York: Dover, 1987.

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S, Warren Warren, ed. Advances in magnetic and optical resonance. San Diego: Academic Press, 1996.

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Oraevskiĭ, A. N. Gaussian beams and optical resonators. Commack, N.Y: Nova Science Publishers, 1995.

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Ram, Kossowsky, Jelínek Miroslav, Novák Josef Ing, North Atlantic Treaty Organization. Scientific Affairs Division., and NATO Advanced Research Workshop on Optical Resonators: Theory and Design (1997 : Smolenice, Slovakia), eds. Optical resonators: Science and engineering. Dordrecht: Kluwer Academic Publishers, 1998.

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K, Lindner D., and United States. National Aeronautics and Space Administration., eds. Optical distributed sensors for feedback control. Blacksburg, VA: Virginia Polytechnic Institute and State University, 1992.

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K, Lindner D., and United States. National Aeronautics and Space Administration., eds. Optical distributed sensors for feedback control. Blacksburg, VA: Virginia Polytechnic Institute and State University, 1992.

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Geru, Ion. Resonance Effects of Excitons and Electrons: Basics and Applications. Berlin, Heidelberg: Springer Berlin Heidelberg, 2013.

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Hodgson, Norman. Optical resonators: Fundamentals, advanced concepts, and applications. London: Springer, 1997.

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A, Copeland Richard, and United States. National Aeronautics and Space Administration., eds. Collisional removal of O₂ (c¹ Sigma⁻[subscript u], nu=9) by O₂, N₂, and He. [Washington, DC: National Aeronautics and Space Administration, 1996.

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Book chapters on the topic "Optical resonance"

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Gawad, Shady, Ana Valero, Thomas Braschler, David Holmes, Philippe Renaud, Vanni Lughi, Tomasz Stapinski, et al. "Optical Resonance Biosensor." In Encyclopedia of Nanotechnology, 1969. Dordrecht: Springer Netherlands, 2012. http://dx.doi.org/10.1007/978-90-481-9751-4_100607.

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Mathur, S., and U. N. Upadhyaya. "Quantum Optical Resonance." In Trends in Atomic and Molecular Physics, 189–218. Boston, MA: Springer US, 2000. http://dx.doi.org/10.1007/978-1-4615-4259-9_12.

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Parson, William W. "Resonance Energy Transfer." In Modern Optical Spectroscopy, 325–52. Berlin, Heidelberg: Springer Berlin Heidelberg, 2015. http://dx.doi.org/10.1007/978-3-662-46777-0_7.

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Semaan, Georges, Andrey Komarov, Mohamed Salhi, and François Sanchez. "Dissipative Soliton Resonance." In Dissipative Optical Solitons, 61–77. Cham: Springer International Publishing, 2022. http://dx.doi.org/10.1007/978-3-030-97493-0_4.

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Parson, William W., and Clemens Burda. "Resonance Energy Transfer." In Modern Optical Spectroscopy, 377–408. Cham: Springer International Publishing, 2023. http://dx.doi.org/10.1007/978-3-031-17222-9_7.

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Homola, Jiří. "Surface Plasmon Resonance Biosensors for Food Safety." In Optical Sensors, 145–72. Berlin, Heidelberg: Springer Berlin Heidelberg, 2004. http://dx.doi.org/10.1007/978-3-662-09111-1_7.

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Vollmer, Frank, and Deshui Yu. "Surface Plasmon Resonance." In Optical Whispering Gallery Modes for Biosensing, 63–118. Cham: Springer International Publishing, 2022. http://dx.doi.org/10.1007/978-3-031-06858-4_2.

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Denz, Cornelia. "Optical Realizations of Adaptive Resonance Theory Networks." In Optical Neural Networks, 421–33. Wiesbaden: Vieweg+Teubner Verlag, 1998. http://dx.doi.org/10.1007/978-3-663-12272-2_12.

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Esherick, P., and A. Owyoung. "Ionization-Raman Double-Resonance Spectroscopy." In Springer Series in Optical Sciences, 192–95. Berlin, Heidelberg: Springer Berlin Heidelberg, 1985. http://dx.doi.org/10.1007/978-3-540-39664-2_56.

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Gupta, Banshi Dhar, Anand Mohan Shrivastav, and Sruthi Prasood Usha. "Basics of Resonance." In Optical Sensors for Biomedical Diagnostics and Environmental Monitoring, 33–74. Boca Raton, FL : CRC Press, Taylor & Francis Group, [2017]: CRC Press, 2017. http://dx.doi.org/10.1201/9781315156033-2.

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Conference papers on the topic "Optical resonance"

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Kelley, P. L., O. Blum, and T. K. Gustafson. "Radiative Renormalization Analysis of Optical Double Resonance." In Nonlinear Optics. Washington, D.C.: Optica Publishing Group, 1992. http://dx.doi.org/10.1364/nlo.1992.tud4.

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The problem of optical double resonance as shown in the Figure is a familiar one in optics.[1-3] In this case, a near-resonant field at frequency ν l connects level 1 with level 2 while a near resonant field at frequency v u connects level 2 with level 3. When level 2 is below level 3, the excitation of level 3 involves two photon absorption; if level 2 is above level 3, the excitation of level 3 is a Raman process.
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Hester, Brooke, Kristian Helmerson, Carly Levin, and Naomi J. Halas. "Optical Trapping Near Resonance." In Frontiers in Optics. Washington, D.C.: OSA, 2008. http://dx.doi.org/10.1364/fio.2008.pdpb4.

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Eckardt, Robert C., C. D. Nabors, W. J. Kozlovsky, and R. L. Byer. "Simultaneous electrooptical and temperature tuning of a double resonant optical parametric oscillator." In OSA Annual Meeting. Washington, D.C.: Optica Publishing Group, 1988. http://dx.doi.org/10.1364/oam.1988.tun4.

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Doubly resonant optical parametric oscillators (DR OPOs) have simultaneous resonance of both signal and idler waves. This simultaneous resonance allows lower pump threshold and better frequency selection compared to singly resonant optical parametric oscillators. The stable operation of DR OPOs requires pump lasers with narrow bandwidth, good frequency stability, and good spatial mode quality. We used a semiconductor-diode-laser-pumped nonplanar-ring-oscillator miniature solid-state laser with its output converted to second harmonic at 532 nm for OPO pumping. The combined requirements of double resonance and conservation of energy can result in discontinuous wavelength tuning of DR OPOs. When the crystal temperature is changed, the output jumps from one spectral region to another. Stepwise tuning with continuous spectral coverage is possible when the OPO resonances are finely controlled with electrooptical or pump frequency tuning. An analysis of this tuning that considers temperature- dependent dispersion, thermal expansion, and the electrooptical and piezoelectric effects is presented. Results are compared with the observed performance of a monolithic doubly resonant MgO:LiNbO3 optical parametric oscillator. Pulsed parametric oscillation with single-mode signal and idler waves was observed tunable from 1.01 to 1.12 μm by temperature change and an applied electric field.
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Kelly-Richard, Alexandre, and Jacques Albert. "Improving the Limit of Detection of Tilted Fiber Bragg Gratings by Multiresonant Data Extraction." In Optical Sensors. Washington, D.C.: Optica Publishing Group, 2022. http://dx.doi.org/10.1364/sensors.2022.sm2c.4.

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A multiresonant approach using shifts of 27 cladding mode resonances of a tilted fiber Bragg grating refractometer yields a four-fold improvement in the limit of detection relative to using only the single-most sensitive resonance.
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Reece, Peter J. "Magnetic resonance sensing with optically trapped nanodiamonds." In Optical Trapping and Optical Micromanipulation XX, edited by Kishan Dholakia and Gabriel C. Spalding. SPIE, 2023. http://dx.doi.org/10.1117/12.2677182.

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Enoch, Stefan, Hassan Akhouayri, and C. Amra. "Resonant second-harmonic scattering from rough thin films." In Optical Interference Coatings. Washington, D.C.: Optica Publishing Group, 1997. http://dx.doi.org/10.1364/oic.1998.tha.5.

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Recent theoretical and experimental studies of the scattering from non-linear rough metal surface have been published [1-4], Effects arising from the resonant excitation of a plasmon resonance have been investigated and peaks or dips in the angular distribution of the scattered harmonic light have been demonstrated. These peaks arise from the excitation of both a fundamental or an harmonic resonance.
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Norton, Scott M., Daniel H. Raguin, and G. Michael Morris. "Effective Medium Theory Approach to Guided-Mode Resonances." In Optical Design for Photonics. Washington, D.C.: Optica Publishing Group, 1993. http://dx.doi.org/10.1364/odp.1993.wa.8.

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Brooks, Juliana H. J. "Hidden variables: the resonance factor." In SPIE Optical Engineering + Applications, edited by Chandrasekhar Roychoudhuri, Al F. Kracklauer, and Andrei Yu Khrennikov. SPIE, 2009. http://dx.doi.org/10.1117/12.834292.

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Lu, Hsiao-Yen, Cheng-Lun Lu, Yang-Min Chang, Ming-Wei Lai, and Shih-Hsiang Hsu. "Fano-resonance Biosensing through Windowed Fourier Transform." In Optical Sensors. Washington, D.C.: OSA, 2021. http://dx.doi.org/10.1364/sensors.2021.sm2c.4.

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Gadomski, W., and B. Ratajska-Gadomska. "Dynamic Bistability in Parametric Resonance in Crystals." In Optical Bistability. Washington, D.C.: Optica Publishing Group, 1985. http://dx.doi.org/10.1364/obi.1985.md1.

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Abstract:
The bistable parametric resonance occurs in a crystal interacting with a biharmonic optical field if the difference between optical frequencies equals twice the vibrational frequency of a lattice mode [1,2].The square of the amplitude of the lattice vibrations, a, is resonantly enhanced and exhibits bistable behaviour with respect to both the difference frequency and the field amplitudes E and E'. The stationary dependence of a on E has the form of the unfoldings of pitchfork bifurcation [3], corresponding to different values of E' (Eig.1a). Although the pitchfork branches are separated we demonstrate the complex hysteresis loops linking those branches together (Fig.1b).
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Reports on the topic "Optical resonance"

1

Kispert, Lowell. Magnetic Resonance and Optical Spectroscopic Studies of Carotenoids. Office of Scientific and Technical Information (OSTI), May 2014. http://dx.doi.org/10.2172/1132066.

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Gallagher, Thomas F. Optical/Millimeter-Wave Double-Resonance Spectroscopy of Rydberg Atoms. Fort Belvoir, VA: Defense Technical Information Center, January 2003. http://dx.doi.org/10.21236/ada427191.

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Yariv, Amnon. Semiconductor Based Transverse Bragg Resonance (TBR) Optical Amplifiers and Laser. Fort Belvoir, VA: Defense Technical Information Center, November 2005. http://dx.doi.org/10.21236/ada448611.

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Yariv, Amnon. Semiconductor Based Transverse Bragg Resonance (TBR) Optical Amplifiers and Lasers. Fort Belvoir, VA: Defense Technical Information Center, February 2007. http://dx.doi.org/10.21236/ada472485.

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Kispert, L. D. Magnetic resonance and optical spectroscopic studies of carotenoids. Progress report, December 1, 1991--November 30, 1994. Office of Scientific and Technical Information (OSTI), May 1994. http://dx.doi.org/10.2172/10196714.

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Kispert, L. D. Magnetic resonance and optical spectroscopic studies of carotenoids. Progress report, December 1, 1994--November 30, 1995. Office of Scientific and Technical Information (OSTI), June 1995. http://dx.doi.org/10.2172/179206.

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Maxwell, R., T. Baumann, and B. Taylor. Development of Direct and Optical Polarized Nuclear Magnetic Resonance (NMR) Methods for Characterization and Engineering of Mesophased Molecular Structures. Office of Scientific and Technical Information (OSTI), January 2002. http://dx.doi.org/10.2172/15005321.

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Valentine, Jason G. Low-Loss Optical Metamaterials Based on Mie Resonances in Semiconductor Nanoparticle Composites. Fort Belvoir, VA: Defense Technical Information Center, December 2012. http://dx.doi.org/10.21236/ada569867.

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Chen, Ying. Optically Detected Magnetic Resonance Studies on π-conjugated semiconductor systems. Office of Scientific and Technical Information (OSTI), January 2011. http://dx.doi.org/10.2172/1048514.

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Ross, D. M., C. Brune, and C. D. Marrs. Phase-Shift Parameters and Small Vibrations in Resonant Optical Cavities. Fort Belvoir, VA: Defense Technical Information Center, September 1987. http://dx.doi.org/10.21236/ada197450.

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