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Journal articles on the topic 'Optical cavity'

To see the other types of publications on this topic, follow the link: Optical cavity.

Author: Grafiati

Published: 4 June 2021

Last updated: 25 May 2024

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1

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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2

Chang, Pengfa, Chen Wang, Tao Jiang, Longsheng Wang, Tong Zhao, Hua Gao, Zhiwei Jia, Yuanyuan Guo, Yuncai Wang, and Anbang Wang. "Optical scrambler using WGM micro-bottle cavity." Chinese Optics Letters 21, no. 6 (2023): 060601. http://dx.doi.org/10.3788/col202321.060601.

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3

Maayani, Shai, Leopoldo L. Martin, Samuel Kaminski, and Tal Carmon. "Cavity optocapillaries." Optica 3, no. 5 (May 20, 2016): 552. http://dx.doi.org/10.1364/optica.3.000552.

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4

Moddel, Garret, Ayendra Weerakkody, David Doroski, and Dylan Bartusiak. "Optical-Cavity-Induced Current." Symmetry 13, no. 3 (March 22, 2021): 517. http://dx.doi.org/10.3390/sym13030517.

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The formation of a submicron optical cavity on one side of a metal–insulator–metal (MIM) tunneling device induces a measurable electrical current between the two metal layers with no applied voltage. Reducing the cavity thickness increases the measured current. Eight types of tests were carried out to determine whether the output could be due to experimental artifacts. All gave negative results, supporting the conclusion that the observed electrical output is genuinely produced by the device. We interpret the results as being due to the suppression of vacuum optical modes by the optical cavity on one side of the MIM device, which upsets a balance in the injection of electrons excited by zero-point fluctuations. This interpretation is in accord with observed changes in the electrical output as other device parameters are varied. A feature of the MIM devices is their femtosecond-fast transport and scattering times for hot charge carriers. The fast capture in these devices is consistent with a model in which an energy ∆E may be accessed from zero-point fluctuations for a time ∆t, following a ∆E∆t uncertainty-principle-like relation governing the process.

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5

Webster, Stephen, and Patrick Gill. "Force-insensitive optical cavity." Optics Letters 36, no. 18 (September 9, 2011): 3572. http://dx.doi.org/10.1364/ol.36.003572.

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6

Son, Jun Ho, SoonGweon Hong, Amanda J. Haack, Lars Gustafson, Minsun Song, Ori Hoxha, and Luke P. Lee. "Rapid Optical Cavity PCR." Advanced Healthcare Materials 5, no. 1 (November 23, 2015): 167–74. http://dx.doi.org/10.1002/adhm.201500708.

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7

Yeh, Chia Hung, Liang Gie Huang, and Man Yee Chan. "Optimal Lighting of Optical Devices for Oral Cavity." International Journal of Optics 2020 (January 30, 2020): 1–13. http://dx.doi.org/10.1155/2020/1370917.

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Oral surgery mainly provides surgical scope illumination by doctors wearing headlamps, but there are still clinical restrictions on use. The limitations are (1) due to the angle of the head swing and the shadow of the visual field during the operation and (2) due to projection of the light source being worn on the doctor’s head and the length of the wire, and the fiber-optic wire will affect the relative position of the surgical instrument and limit the scope of the doctor’s activity. This study will focus on the development of oral lighting optical microstructure devices to solve and improve the abovementioned clinical use limitations. The production method is to make an oral lighting mold by 3D printing technology and use the polydimethylsiloxane (PDMS) of liquid silicone material to make an oral lighting device with mold casting technology. The results show that the optical simulation achieves the target light distribution by optimizing the three geometric reflection surfaces combined with the lens design by the optimization method, and the maximum illumination value can reach 5102 lux. According to the measurement results of mold casting technology, the average errors of the profile of the 3D printing finished product and the PDMS finished product of the oral device structure are about 1.4% and 16.9%, respectively. Because the contour of the PDMS finished product’s error caused the light to shift by 0.5∼3 mm distance, the light is still concentrated in the range of the tonsils, so this study can be defined as within the acceptable range of within 16.9% of the intra lighting error. The development of oral lighting devices in this study will reduce the burden on physicians in nonprofessional fields, reduce the time of surgery for patients to maintain the health of doctors, and rise the level of medical equipment to increase surgical safety.

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8

Chen, Fei, Ming Li, Reda Hassanien Emam Hassanien, Xi Luo, Yongrui Hong, Zhikang Feng, Mengen Ji, and Peng Zhang. "Study on the Optical Properties of Triangular Cavity Absorber for Parabolic Trough Solar Concentrator." International Journal of Photoenergy 2015 (2015): 1–9. http://dx.doi.org/10.1155/2015/895946.

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A theoretical analytical method for optical properties of cavity absorber was proposed in this paper and the optical design software TracePro was used to analyze the optical properties of triangular cavity absorber. It was found that the optimal optical properties could be achieved with appropriate aperture width, depth-to-width ratio, and offset distance from focus of triangular cavity absorber. Based on the results of orthogonal experiment, the optimized triangular cavity absorber was designed. Results showed that the standard deviation of irradiance and optical efficiency of optimized designed cavity absorber were 30528 W/m2and 89.23%, respectively. Therefore, this study could offer some valuable references for designing the parabolic trough solar concentrator in the future.

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9

Deffner, Sebastian. "Optimal control of a qubit in an optical cavity." Journal of Physics B: Atomic, Molecular and Optical Physics 47, no. 14 (July 4, 2014): 145502. http://dx.doi.org/10.1088/0953-4075/47/14/145502.

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10

Petnikova, V. M., and Vladimir V. Shuvalov. "Optimal feedback in efficient single-cavity optical parametric oscillators." Quantum Electronics 40, no. 7 (September 10, 2010): 619–23. http://dx.doi.org/10.1070/qe2010v040n07abeh014276.

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11

Gan Xuetao, 甘雪涛, and 赵建林 Zhao Jianlin. "Resonance Lineshapes in Optical Cavity." Acta Optica Sinica 41, no. 8 (2021): 0823007. http://dx.doi.org/10.3788/aos202141.0823007.

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12

Dolan, Philip R., Gareth M. Hughes, Fabio Grazioso, Brian R. Patton, and Jason M. Smith. "Femtoliter tunable optical cavity arrays." Optics Letters 35, no. 21 (October 19, 2010): 3556. http://dx.doi.org/10.1364/ol.35.003556.

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13

Jin, Miao, Jiang Yan-Yi, Fang Su, Bi Zhi-Yi, and Ma Long-Sheng. "Vibration insensitive optical ring cavity." Chinese Physics B 18, no. 6 (June 2009): 2334–39. http://dx.doi.org/10.1088/1674-1056/18/6/037.

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14

Lee, C. F., and N. F. Johnson. "Spin-glasses in optical cavity." EPL (Europhysics Letters) 81, no. 3 (December 31, 2007): 37004. http://dx.doi.org/10.1209/0295-5075/81/37004.

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15

Wen, Pengyue, Michael Sanchez, Matthias Gross, and Sadik Esener. "Vertical-cavity optical AND gate." Optics Communications 219, no. 1-6 (April 2003): 383–87. http://dx.doi.org/10.1016/s0030-4018(03)01271-9.

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16

Wen, Pengyue, Michael Sanchez, Matthias Gross, and Sadik C. Esener. "Optical bistability in vertical-cavity semiconductor optical amplifiers." Applied Optics 45, no. 25 (September 1, 2006): 6349. http://dx.doi.org/10.1364/ao.45.006349.

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17

Brown, M. D., E. Z. Zhang, B. E. Treeby, P. C. Beard, and B. T. Cox. "Reverberant cavity photoacoustic imaging." Optica 6, no. 6 (June 19, 2019): 821. http://dx.doi.org/10.1364/optica.6.000821.

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18

Ke Di, Ke Di, Xudong Yu Xudong Yu, Fengyu Cheng Fengyu Cheng, and Jing Zhang Jing Zhang. "Phase-sensitive reflection of squeezed vacuum field in optical cavity." Chinese Optics Letters 10, no. 9 (2012): 091901–91904. http://dx.doi.org/10.3788/col201210.091901.

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19

Li, Kanglin, Jiangbing Du, Weihong Shen, Jiacheng Liu, and Zuyuan He. "Improved optical coupling based on a concave cavity lens fabricated by optical fiber facet etching." Chinese Optics Letters 19, no. 5 (2021): 050602. http://dx.doi.org/10.3788/col202119.050602.

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20

Wang, Yadi, Masanobu Haraguchi, Xingbo Zhang, Pingping Wang, and Shufeng Sun. "Improvement of Optical Confinement for Terahertz Vertical-Cavity Surface-Emitting Laser with Square-Lattice Photonic Crystal Structure." Coatings 13, no. 6 (May 23, 2023): 972. http://dx.doi.org/10.3390/coatings13060972.

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A new method proposed to enhance the optical confinement of the terahertz band in a vertical cavity surface emitting laser involves introducing a square-lattice photonic crystal structure. This structure’s filling factor was optimized by computing the energy band structure and optical band values of the photonic crystal. The optimal optical band value is 0.436–0.528 a/λ. At a specific carrier concentration, the real part of dielectric constant of GaAs/AlGaAs materials will gradually increase with the increase of Al elements. By adjusting the length of the resonant cavity, a vertical cavity surface emitting laser with two wavelengths can be created without utilizing current injection. Additionally, the photonic crystal structure’s control effect on the transverse mode of the vertical cavity surface emitting laser and the release effect of the PN junction light confinement were analyzed. Numerical calculations indicated that incorporating a cubic photonic crystal structure in the vertical cavity surface emitting laser resulted in a 2× increase in the difference frequency intensity and a 6.33× increase in the optical field intensity.

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21

Li, Guoyao, and Zhang-Qi Yin. "Squeezing Light via Levitated Cavity Optomechanics." Photonics 9, no. 2 (January 22, 2022): 57. http://dx.doi.org/10.3390/photonics9020057.

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Squeezing light is a critical resource in both fundamental physics and precision measurement. Squeezing light has been generated through optical-parametric amplification inside an optical resonator. However, preparing the squeezing light in an optomechanical system is still a challenge for the thermal noise inevitably coupled to the system. We consider an optically levitated nano-particle in a bichromatic cavity, in which two cavity modes could be excited by the scattering photons of the dual tweezers, respectively. Based on the coherent scattering mechanism, the ultra-strong coupling between the cavity field and the torsional motion of nano-particle could be achieved for the current experimental conditions. With the back-action of the optically levitated nano-particle, the broad single-mode squeezing light can be realized in the bad cavity regime. Even at room temperature, the single-mode light can be squeezed for more than 17 dB, which is far beyond the 3 dB limit. The two-mode squeezing light can also be generated, if the optical tweezers contain two frequencies, one is on the red sideband of the cavity mode, the other is on the blue sideband. The two-mode squeezing can be maximized near the boundary of the system stable regime and is sensitive to both the cavity decay rate and the power of the optical tweezers.

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22

BEAULIEU, Y., S. JANZ, H. DAI, E. FRLAN, C. FERNANDO, A. DELÂGE, P. VAN DER MEER, M. DION, and R. NORMANDIN. "SURFACE EMITTED HARMONIC GENERATION FOR SENSOR AND DISPLAY APPLICATIONS." Journal of Nonlinear Optical Physics & Materials 04, no. 04 (October 1995): 893–927. http://dx.doi.org/10.1142/s0218863595000410.

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We review briefly some of the basic principles involved in quasi-phase matched multilayer semiconductor films for second-harmonic generation in waveguided, reflection and intra-cavity geometries. New applications in optical ranging for length, temperature, deformation sensors, real time optical reflectometry and vertical cavity second-harmonic generation for displays are presented. The enhancement of quasi-phase matched second-harmonic generation in vertical cavity Fabry-Perot structures is also investigated. When the optimal quasi-phase matching conditions are satisfied in the Fabry-Perot core, the second-harmonic conversion efficiency of a 4 μm thick cavity is enhanced by 1.75 × 106 relative to a homogeneous GaAs slab. This geometry is most suitable for intracavity harmonic generation in vertical cavity surface emitting lasers.

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23

Milosevic, Milos, Nenad Mitrovic, Vesna Miletić, Uroš Tatic, and Andrea Ezdenci. "Analysis of Composite Shrinkage Stresses on 3D Premolar Models with Different Cavity Design Using Finite Element Method." Key Engineering Materials 586 (September 2013): 202–5. http://dx.doi.org/10.4028/www.scientific.net/kem.586.202.

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Local polymerization stress occurs due to polymerization shrinkage of resin based composites adhesively bonded to tooth tissues. Shrinkage causes local displacements of cavity walls, with possible occurrence of micro-cracks in the enamel, dentin and/or material itself. In order to design a cavity for experimental testing of polymerization shrinkage of dental composites using 3D optical analysis, in this paper finite element method (FEM) was used to analyze numerical models with different cavity radiuses. 3D optical strain and displacement analysis of composite materials and cavity walls is limited by equipment sensitivity i.e. 0.01% for strain and 1 micron for displacement. This paper presents the development of 3D computer premolar models with varying cavity radiuses, and local stress, strain and displacement analysis using FEM. Model verification was performed by comparing obtained results with data from the scientific literature. Using the FEM analysis of local strains, displacements and stresses exerted on cavity walls, it was concluded that the model with 1 mm radius was optimal for experimental optical 3D displacement analysis.

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24

Petnikova, V. M., and Vladimir V. Shuvalov. "Optimal feedback in efficient ring double-cavity optical parametric oscillators." Quantum Electronics 40, no. 7 (September 10, 2010): 624–28. http://dx.doi.org/10.1070/qe2010v040n07abeh014311.

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25

Ehrlichman, Yossef, Anatol Khilo, and Miloš A. Popović. "Optimal design of a microring cavity optical modulator for efficient RF-to-optical conversion." Optics Express 26, no. 3 (January 23, 2018): 2462. http://dx.doi.org/10.1364/oe.26.002462.

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26

Loock, Hans-Peter, Jack A. Barnes, Gianluca Gagliardi, Runkai Li, Richard D. Oleschuk, and Helen Wächter. "Absorption detection using optical waveguide cavities." Canadian Journal of Chemistry 88, no. 5 (May 2010): 401–10. http://dx.doi.org/10.1139/v10-006.

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Cavity ring-down spectroscopy is a spectroscopic method that uses a high quality optical cavity to amplify the optical loss due to the light absorption by a sample. In this presentation we highlight two applications of phase-shift cavity ring-down spectroscopy that are suited for absorption measurements in the condensed phase and make use of waveguide cavities. In the first application, a fiber loop is used as an optical cavity and the sample is introduced in a gap in the loop to allow absorption measurements of nanoliters of solution at the micromolar level. A second application involves silica microspheres as high finesse cavities. Information on the refractive index and absorption of a thin film of ethylene diamine on the surface of the microresonator is obtained simultaneously by the measurements of the wavelength shift of the cavity mode spectrum and the change in optical decay time, respectively.

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27

Smowton, P. M., J. D. Thomson, M. Yin, S. V. Dewar, P. Blood, A. C. Bryce, J. H. Marsh, C. J. Hamilton, and C. C. Button. "Optical loss in large optical cavity 650 nm lasers." Semiconductor Science and Technology 16, no. 10 (September 6, 2001): L72—L75. http://dx.doi.org/10.1088/0268-1242/16/10/104.

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28

Martinez-Lorente, R., G. J. de Valcarcel, A. Esteban-Martin, J. Garcia-Monreal, E. Roldán, and F. Silva. "Making of a nonlinear optical cavity." Optica Pura y Aplicada 49, no. 3 (September 30, 2016): 125–42. http://dx.doi.org/10.7149/opa.49.3.49004.

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29

Gupta, Manish, Hong Jiao, and Anthony O’Keefe. "Cavity-enhanced spectroscopy in optical fibers." Optics Letters 27, no. 21 (November 1, 2002): 1878. http://dx.doi.org/10.1364/ol.27.001878.

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30

Kranz, Michael, Tracy Hudson, Brian Grantham, and Michael Whitley. "Optical Cavity Interrogation for MEMS Accelerometers." Additional Conferences (Device Packaging, HiTEC, HiTEN, and CICMT) 2015, DPC (January 1, 2015): 001649–70. http://dx.doi.org/10.4071/2015dpc-wp34.

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MEMS accelerometers utilizing electrostatic, piezoelectric, and magnetic proof mass displacement readout approaches have achieved success in both commercial- and defense-related applications. However, there is a desire for improved acceleration resolution suitable for navigation-grade applications. Optical readout of mechanical displacements has demonstrated high levels of resolution in macro-scale applications including precision movement and placement systems. In addition, optical techniques are common in high performance inertial sensors such as fiber optic gyros and ring laser gyros. Incorporating optical readout approaches into MEMS acceleration devices may yield sufficient resolution to achieve navigation-grade performance. Therefore, the U.S. Army AMRDEC is developing MEMS accelerometers based on optical cavity resonance readout. In the device, an optical cavity is formed between a MEMS proof mass and a reference reflector. A tunable laser excites the cavity on the edge of its resonance peak. Small displacements of the cavity from its rest position are detected by frequency shifts of the resonance, leading to high-resolution proof mass displacement detection and therefore high acceleration resolutions. This paper will present modeling associated with the design concept, as well predictions of device geometries and performance with the goal of achieving less than 1 micro-g bias instability and a velocity random walk of better than 0.2 micro-g/rt.Hz.

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31

Nayak, K. P., Pengfei Zhang, and K. Hakuta. "Optical nanofiber-based photonic crystal cavity." Optics Letters 39, no. 2 (January 6, 2014): 232. http://dx.doi.org/10.1364/ol.39.000232.

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32

Sun, Yi-zhi, Yang Yu, Hui-lan Liu, Zhi-yuan Li, and Wei Ding. "Optical microfiber-based photonic crystal cavity." Journal of Physics: Conference Series 680 (January 2016): 012029. http://dx.doi.org/10.1088/1742-6596/680/1/012029.

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33

Lu, Weiping, Dejin Yu, and Robert G. Harrison. "Excitability in a nonlinear optical cavity." Physical Review A 58, no. 2 (August 1, 1998): R809—R811. http://dx.doi.org/10.1103/physreva.58.r809.

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34

MORIN, STEVEN E., QILIN WU, and THOMAS W. MOSSBERG. "CAVITY QUANTUM ELECTRODYNAMICS AT OPTICAL FREQUENCIES." Optics and Photonics News 3, no. 8 (August 1, 1992): 8. http://dx.doi.org/10.1364/opn.3.8.000008.

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35

Lee, Sang Hyun, Takenari Goto, Hiroshi Miyazaki, Jiho Chang, and Takafumi Yao. "Optical Resonant Cavity in a Nanotaper." Nano Letters 10, no. 6 (June 9, 2010): 2038–42. http://dx.doi.org/10.1021/nl100100z.

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36

Della Valle, F., E. Milotti, A. Ejlli, U. Gastaldi, G. Messineo, L. Piemontese, G. Zavattini, R. Pengo, and G. Ruoso. "Extremely long decay time optical cavity." Optics Express 22, no. 10 (May 6, 2014): 11570. http://dx.doi.org/10.1364/oe.22.011570.

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37

Hochrein, Thomas, Rafal Wilk, Michael Mei, Ronald Holzwarth, Norman Krumbholz, and Martin Koch. "Optical sampling by laser cavity tuning." Optics Express 18, no. 2 (January 13, 2010): 1613. http://dx.doi.org/10.1364/oe.18.001613.

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38

Li, Ziyuan, R. G. T. Bennett, and G. E. Stedman. "Swept-frequency induced optical cavity ringing." Optics Communications 86, no. 1 (October 1991): 51–57. http://dx.doi.org/10.1016/0030-4018(91)90242-6.

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39

Doostkam, Rasool, and Mohammad Mahmoudi. "Optical multistability generation via cavity series." Optics Communications 424 (October 2018): 123–26. http://dx.doi.org/10.1016/j.optcom.2018.04.048.

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40

Scalora, Michael, Joseph W. Haus, and Charles M. Bowden. "Intrinsic optical bistability in a cavity." Physical Review A 41, no. 11 (June 1, 1990): 6320–30. http://dx.doi.org/10.1103/physreva.41.6320.

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41

Gorbach, Andrey V., Sergey Denisov, and Sergej Flach. "Optical ratchets with discrete cavity solitons." Optics Letters 31, no. 11 (June 1, 2006): 1702. http://dx.doi.org/10.1364/ol.31.001702.

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42

Haelterman, M. "Coupled-cavity configuration for optical bistability." Optics Communications 68, no. 4 (October 1988): 305–9. http://dx.doi.org/10.1016/0030-4018(88)90405-1.

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43

Borshch, A. A., and V. I. Volkov. "Cavity-Less Optical Bistability in Semiconductors." physica status solidi (b) 150, no. 2 (December 1, 1988): 471–75. http://dx.doi.org/10.1002/pssb.2221500219.

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44

C. Mignosi, M. Bordovsky, C. N. Mor. "Novel Optical Vibration Sensor Using External Cavity Feedback: Novel Optical Vibration Sensor Using External Cavity Feedback." Fiber and Integrated Optics 20, no. 1 (January 2001): 71–81. http://dx.doi.org/10.1080/01468030121192.

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45

Mignosi, C., M. Bordovsky, C. N. Morgan, I. H. White, R. P. Griffiths, and N. A. J. Lieven. "Novel Optical Vibration Sensor Using External Cavity Feedback: Novel Optical Vibration Sensor Using External Cavity Feedback." Fiber and Integrated Optics 20, no. 1 (January 1, 2001): 71–81. http://dx.doi.org/10.1080/01468030151073056.

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46

Yalla, Ramachandrarao, K. Muhammed Shafi, Kali P. Nayak, and Kohzo Hakuta. "One-sided composite cavity on an optical nanofiber for cavity QED." Applied Physics Letters 120, no. 7 (February 14, 2022): 071108. http://dx.doi.org/10.1063/5.0079624.

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47

Desbois, Thibault, Irène Ventrillard, and Daniele Romanini. "Simultaneous cavity-enhanced and cavity ringdown absorption spectroscopy using optical feedback." Applied Physics B 116, no. 1 (November 9, 2013): 195–201. http://dx.doi.org/10.1007/s00340-013-5675-z.

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48

Telfah, Hamzeh, Anam C. Paul, and Jinjun Liu. "Aligning an optical cavity: with reference to cavity ring-down spectroscopy." Applied Optics 59, no. 30 (October 16, 2020): 9464. http://dx.doi.org/10.1364/ao.405189.

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49

Mejia-Beltran, Efrain, and Oscar J. Ballesteros-Llanos. "Investigation of Optical Cavity Dynamics with Raman and Ytterbium-Doped Gain Media Integration." Photonics 10, no. 10 (October 12, 2023): 1148. http://dx.doi.org/10.3390/photonics10101148.

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This study delves into a comprehensive examination of an optical cavity system that integrates Raman and Yb-doped gain media, with a focus on understanding their interactions. The research implies a characterization of each gain medium within the cavity while subjecting them to diverse co-pumping conditions with the other. When the Raman-lasing cavity is co-pumped by exciting the Yb-doped section, the resulting composite laser exhibits significant threshold reductions and there is an optimal co-pumping regime that enhances energy transfer from pump to Stokes. As for the complementary cavity, where the Yb-doped gain is influenced by the co-pumped Raman gain, at moderate pump powers a light-controlling-light behavior phenomenon arises. Within this regime, the 1064 nm signal suppresses the Yb-generated 1115 nm signal, suggesting potential applications in intracavity optical modulation. For higher pump levels, a cooperative effect emerges whereby both lasers mutually enhance each other. Minor variations in the primary 974 nm pump power, even by just a few milliwatts, result in significant capabilities for switching or modulating the Stokes signal. Under these conditions of mutual enhancement, the hybrid optical system validates notable improvements regarding energy transfer efficiency and threshold reduction. This research provides valuable insights into the intricate dynamics of optical cavity systems and reveals promising avenues for applications in advanced optical modulation technologies.

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50

Baoquan Yao, Baoquan Yao, Xiaolei Li Xiaolei Li, Hongwei Shi Hongwei Shi, Tongyu Dai Tongyu Dai, Zheng Cui Zheng Cui, Chuanpeng Qian Chuanpeng Qian, Youlun Ju Youlun Ju, and Yuezhu Wang Yuezhu Wang. "Diode-pumped electro-optical cavity-dumped Tm:YAP laser at 1996.9 nm." Chinese Optics Letters 13, no. 10 (2015): 101402–5. http://dx.doi.org/10.3788/col201513.101402.

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