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Journal articles on the topic 'Lasers – Resonators'

Author: Grafiati

Published: 4 June 2021

Last updated: 6 February 2022

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1

Dzyubenko, M. I., V. A. Maslov, V. P. Radionov, and A. A. Fomin. "Methods for adjusting feedback in terahertz lasers." Radiotekhnika, no. 203 (December 23, 2020): 170–75. http://dx.doi.org/10.30837/rt.2020.4.203.17.

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The optimal feedback coefficient in an active open resonator is an important condition for high lasing efficiency. For precise selection of the optimum communication and maintaining the optimum in all modes of laser operation, the ability to adjust smoothly the communication is required. Terahertz (THz) lasers have a number of features that one should take into account when choosing feedback control schemes. The paper presents a review and comparative analysis of the schemes of laser resonators (THz) in the range with a smoothly controlled radiation output. The authors consider both long known

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2

Hao, Nguyen Van, Pham Van Duong, Pham Hong Minh, Do Quoc Khanh, and Antonio Agnesi. "Design and Development of the Folded 4-Mirror Resonators for Diode End-pumped Solid-State Cr:LiSAF Laser." Communications in Physics 24, no. 3S2 (2016): 109–20. http://dx.doi.org/10.15625/0868-3166/24/3s2/5056.

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We present the design and development of folded four-mirror resonators for diode end-pumped solid-state Cr:LiSAF lasers. The astigmatic effects due to the Brewster-cut laser crystal and two curved mirrors used at oblique incidence were taken into consideration. The obtained results showed the stability regions of resonator, the beam parameters in the resonator and within the laser crystal as well as other sensitive parameters and their variation ranges. Furthermore, the designed folded four-mirror resonators for diode end-pumped Cr:LiSAF laser were experimentally evaluated. The CW Cr:LiSAF las

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3

Ginzburg, Naum, Alexander Sergeev, Ekaterina Kocharovskaya, Andrey Malkin, Ekaterina Egorova, and Vladislav Zaslavsky. "Diffraction mode selection in planar lasers with Bragg resonators." ITM Web of Conferences 30 (2019): 06012. http://dx.doi.org/10.1051/itmconf/20193006012.

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Using the coupled-wave approach supplemented by the quasioptical approximation, we investigate the possibilities of diffraction mode selection with respect to the transverse index in planar distributed-feedback lasers. Quality factors and spatial structures of planar Bragg resonators with finite width and length of the corrugate area were found. Allowable values of the Fresnel parameter were determined at which the diffraction losses at the resonator edges lead to effective discrimination of modes with large numbers of transverse variations and thus provide conditions for the onset of a statio

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4

Savchenkov, Anatoliy, Skip Williams, and Andrey Matsko. "On Stiffness of Optical Self-Injection Locking." Photonics 5, no. 4 (2018): 43. http://dx.doi.org/10.3390/photonics5040043.

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Spectrally pure semiconductor lasers produced via self-injection locking to high quality factor monolithic optical resonators demonstrate sub-kHz instantaneous linewidth. The lasers are used in photonic sensor systems and microwave photonic oscillators benefitting from the improved spectral purity, the stability and the reduced environmental sensitivity of the lasers. The laser frequency stability is defined by both the optical resonator and the optical path of the entire system comprising the laser, the resonator, and the miscellaneous optical components. The impacts of the various destabiliz

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5

Yu, Jibo, Elfed Lewis, Gerald Farrell, and Pengfei Wang. "Compound Glass Microsphere Resonator Devices." Micromachines 9, no. 7 (2018): 356. http://dx.doi.org/10.3390/mi9070356.

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In recent years, compound glass microsphere resonator devices have attracted increasing interest and have been widely used in sensing, microsphere lasers, and nonlinear optics. Compared with traditional silica resonators, compound glass microsphere resonators have many significant and attractive properties, such as high-Q factor, an ability to achieve high rare earth ion, wide infrared transmittance, and low phonon energy. This review provides a summary and a critical assessment of the fabrication and the optical characterization of compound glasses and the related fabrication and applications

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6

Zhu, Song, Bowen Xiao, Bo Jiang, Lei Shi, and Xinliang Zhang. "Tunable Brillouin and Raman microlasers using hybrid microbottle resonators." Nanophotonics 8, no. 5 (2019): 931–40. http://dx.doi.org/10.1515/nanoph-2019-0070.

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AbstractWe realized a tunable Brillouin laser and a tunable Raman laser by using ultrahigh-quality-factor (Q) hybrid microbottle resonators. The whispering-gallery-mode microresonator-based Brillouin and Raman lasers possess unique advantages (e.g. low threshold, narrow line width, and flexible lasing wavelength region) and various potential applications. Efficient tuning of the Brillouin and Raman microresonator lasers is desirable in many cases. However, the corresponding lasing wavelength tunability is rarely reported. In this work, we realized the ultralow-threshold Brillouin and Raman las

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7

Lubatsch, Andreas, and Regine Frank. "Quantum Many-Body Theory for Exciton-Polaritons in Semiconductor Mie Resonators in the Non-Equilibrium." Applied Sciences 10, no. 5 (2020): 1836. http://dx.doi.org/10.3390/app10051836.

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We implement externally excited ZnO Mie resonators in a framework of a generalized Hubbard Hamiltonian to investigate the lifetimes of excitons and exciton-polaritons out of thermodynamical equilibrium. Our results are derived by a Floquet-Keldysh-Green’s formalism with Dynamical Mean Field Theory (DMFT) and a second order iterative perturbation theory solver (IPT). We find that the Fano resonance which originates from coupling of the continuum of electronic density of states to the semiconductor Mie resonator yields polaritons with lifetimes between 0.6 ps and 1.45 ps. These results are compa

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8

Koshelev, Kirill, Sergey Kruk, Elizaveta Melik-Gaykazyan, et al. "Subwavelength dielectric resonators for nonlinear nanophotonics." Science 367, no. 6475 (2020): 288–92. http://dx.doi.org/10.1126/science.aaz3985.

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Subwavelength optical resonators made of high-index dielectric materials provide efficient ways to manipulate light at the nanoscale through mode interferences and enhancement of both electric and magnetic fields. Such Mie-resonant dielectric structures have low absorption, and their functionalities are limited predominantly by radiative losses. We implement a new physical mechanism for suppressing radiative losses of individual nanoscale resonators to engineer special modes with high quality factors: optical bound states in the continuum (BICs). We demonstrate that an individual subwavelength

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9

Muñoz-Mármol, Rafael, Víctor Bonal, Giuseppe M. Paternò, et al. "Dual Amplified Spontaneous Emission and Lasing from Nanographene Films." Nanomaterials 10, no. 8 (2020): 1525. http://dx.doi.org/10.3390/nano10081525.

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Chemically synthesized zigzag-edged nanographenes (NG) have recently demonstrated great success as the active laser units in solution-processed organic distributed feedback (DFB) lasers. Here, we report the first observation of dual amplified spontaneous emission (ASE) from a large-size NG derivative (with 12 benzenoid rings) dispersed in a polystyrene film. ASE is observed simultaneously at the 685 and 739 nm wavelengths, which correspond to different transitions of the photoluminescence spectrum. Ultrafast pump-probe spectroscopy has been used to ascertain the underlying photophysical proces

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10

Balakireva, Irina V., and Yanne K. Chembo. "A taxonomy of optical dissipative structures in whispering-gallery mode resonators with Kerr nonlinearity." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 376, no. 2124 (2018): 20170381. http://dx.doi.org/10.1098/rsta.2017.0381.

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In this paper, the research related to the formation of optical dissipative structures in Kerr-nonlinear whispering-gallery mode resonators pumped with continuous-wave lasers is reviewed. Pattern formation in these systems can be analysed using the paradigmatic Lugiato–Lefever model, which is a partial differential equation ruling the dynamics of the intra-cavity laser field. Various dissipative structures such as Turing rolls, solitons, breathers and spatio-temporal chaos can emerge in the resonator depending on the laser power and frequency. The bifurcation analysis enables a classification

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11

Бабичев, А. В., Д. А. Пашнев, А. Г. Гладышев та ін. "Спектральные характеристики полукольцевых квантово-каскадных лазеров". Журнал технической физики 128, № 8 (2020): 1165. http://dx.doi.org/10.21883/os.2020.08.49715.2-20.

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A half-ring resonator design of a 7-8 μm range quantum-cascade laser with different radius values has been proposed and implemented. For a quantum-cascade laser with a radius of a half-ring resonator of 191 μm, lasing with a radiation spectrum width of 474 nm (82 cm^-1) was demonstrated at low temperatures. The FSR in such lasers was determined by the whispering gallery modes typical for ring resonators. At room temperature, the width of the lasing spectrum was 190 nm (31 cm^–1), which is caused by a decrease in gain and a possible increase in internal losses with increasing temperature. An in

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12

Zhang, Chuang, Chang-Ling Zou, Yan Zhao, et al. "Organic printed photonics: From microring lasers to integrated circuits." Science Advances 1, no. 8 (2015): e1500257. http://dx.doi.org/10.1126/sciadv.1500257.

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A photonic integrated circuit (PIC) is the optical analogy of an electronic loop in which photons are signal carriers with high transport speed and parallel processing capability. Besides the most frequently demonstrated silicon-based circuits, PICs require a variety of materials for light generation, processing, modulation, and detection. With their diversity and flexibility, organic molecular materials provide an alternative platform for photonics; however, the versatile fabrication of organic integrated circuits with the desired photonic performance remains a big challenge. The rapid develo

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13

Rosales-García, Andrea, Iván Cruz-Torres, and Juan Hernández-Cordero. "Fiber lasers with hybrid birefringence resonators." Optics and Lasers in Engineering 44, no. 10 (2006): 1027–38. http://dx.doi.org/10.1016/j.optlaseng.2005.08.002.

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14

Zaitsev, Oleg. "Gas lasers with wave-chaotic resonators." Journal of Physics B: Atomic, Molecular and Optical Physics 43, no. 24 (2010): 245402. http://dx.doi.org/10.1088/0953-4075/43/24/245402.

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15

Stone, A. Douglas. "Wave-chaotic optical resonators and lasers." Physica Scripta T90 (January 1, 2001): 248–62. http://dx.doi.org/10.1088/0031-8949/2001/t90/036.

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16

Solimeno, S., and A. Torre. "Optical resonators for free electron lasers." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 237, no. 1-2 (1985): 404–27. http://dx.doi.org/10.1016/0168-9002(85)90379-1.

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17

Eggleston, J. M. "Periodic resonators for average-power scaling of stable-resonator solid-state lasers." IEEE Journal of Quantum Electronics 24, no. 9 (1988): 1821–24. http://dx.doi.org/10.1109/3.7121.

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18

Cui, Libin, Anwer Hayat, Linzheng Lv, Zhiyang Xu, and Tianrui Zhai. "A Theoretical Model of Quasicrystal Resonators: A Guided Optimization Approach." Crystals 11, no. 7 (2021): 749. http://dx.doi.org/10.3390/cryst11070749.

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Fibonacci-spaced defect resonators were analytically investigated by cavity coupling, which exhibited a series of well-defined optical modes in fractals. The analytic model can be used to predict the output performance of microcavity lasers based on Fibonacci-spaced defect resonators, such as the mode number, resonant frequency, and Q factor. All results obtained by the analytical solution are in good consistency with that obtained by the finite-difference time-domain method. The simulation result shows that the Q factor of the resonant modes would increase dramatically with the appearance of

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19

Lavigne, Pierre, Nathalie McCarthy, André Parent, and Kevin J. Snell. "Laser mode control with variable reflectivity mirrors." Canadian Journal of Physics 66, no. 10 (1988): 888–95. http://dx.doi.org/10.1139/p88-147.

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Global efficiency, transverse mode discrimination, and the near- and far-field optical quality of unstable laser resonators are improved with variable reflectivity mirrors (VRMs). Analytical and numerical results are given for Gaussian and parabolic reflectivity mirrors. The VRM design is described, and experimental results obtained using different lasers with Cassegrain cavities are presented.

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20

Álvarez-Conde, Javier, Eva M. García-Frutos, and Juan Cabanillas-Gonzalez. "Organic Semiconductor Micro/Nanocrystals for Laser Applications." Molecules 26, no. 4 (2021): 958. http://dx.doi.org/10.3390/molecules26040958.

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Organic semiconductor micro/nanocrystals (OSMCs) have attracted great attention due to their numerous advantages such us free grain boundaries, minimal defects and traps, molecular diversity, low cost, flexibility and solution processability. Due to all these characteristics, they are strong candidates for the next generation of electronic and optoelectronic devices. In this review, we present a comprehensive overview of these OSMCs, discussing molecular packing, the methods to control crystallization and their applications to the area of organic solid-state lasers. Special emphasis is given t

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21

Nair, Prita. "Fiber Raman lasers using all‐fiber resonators." Optical Engineering 35, no. 1 (1996): 272. http://dx.doi.org/10.1117/1.600930.

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22

Bélanger, P. A., C. Paré, and M. Piché. "Propriétés spatiales et temporelles des résonateurs lasers munis de miroirs à conjugaison de phase." Canadian Journal of Physics 63, no. 2 (1985): 206–13. http://dx.doi.org/10.1139/p85-033.

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The properties of laser resonators with one phase-conjugate mirror are reviewed. All these resonators are geometrically stable; their resonant frequencies are determined by the frequencies of the pump waves, while the spacing between the satellite resonant frequencies is fixed by the cavity length. Their diffraction losses are higher on the phase-conjugate mirror than on the conventional mirror. Phase-conjugate resonators are less sensitive to intracavity aberrations than conventional resonators. They can be used for short-pulse compression when the phase-conjugate mirror is produced by degene

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23

Гинзбург, Н. С., А. С. Сергеев, Е. Р. Кочаровская, А. М. Малкин, Е. Д. Егорова та В. Ю. Заславский. "Дифракционная селекция мод в гетеролазерах с планарными брэгговскими структурами". Физика и техника полупроводников 54, № 9 (2020): 974. http://dx.doi.org/10.21883/ftp.2020.09.49842.38.

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Within the coupled waves method complemented by quasi-optical approach, we investigate a possibility of diffraction mode selection with respect to the transverse mode index in lasers with planar Bragg resonators. Allowable values of the Fresnel parameter are determined which provide for establishment of stationary single-mode oscillation regime with narrow angle spectrum due to diffraction losses from the edges of the Bragg structure. We show that at larger values of the Fresnel parameter, oscillation stability can be improved by shifting the operating transition frequency to the eigenfrequenc

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24

Lubatsch, Andreas, and Regine Frank. "A Self-Consistent Quantum Field Theory for Random Lasing." Applied Sciences 9, no. 12 (2019): 2477. http://dx.doi.org/10.3390/app9122477.

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The spatial formation of coherent random laser modes in strongly scattering disordered random media is a central feature in the understanding of the physics of random lasers. We derive a quantum field theoretical method for random lasing in disordered samples of complex amplifying Mie resonators which is able to provide self-consistently and free of any fit parameter the full set of transport characteristics at and above the laser phase transition. The coherence length and the correlation volume respectively is derived as an experimentally measurable scale of the phase transition at the laser

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25

Yasui, K. "Laser resonators with phase-unifying output couplers for high power lasers." Pure and Applied Optics: Journal of the European Optical Society Part A 3, no. 4 (1994): 593–99. http://dx.doi.org/10.1088/0963-9659/3/4/021.

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26

MAEDA, Mitsuo. "Fundamentals on Lasers. II. Theory of Optical Resonators." Review of Laser Engineering 25, no. 12 (1997): 894–904. http://dx.doi.org/10.2184/lsj.25.894.

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27

YAMAMOTO, Yohei. "Self-Assembled Conjugated Polymer Microsphere Resonators and Lasers." Review of Laser Engineering 46, no. 1 (2018): 25. http://dx.doi.org/10.2184/lsj.46.1_25.

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28

Mahler, Lukas, Alessandro Tredicucci, Richard P. Green, et al. "Terahertz quantum cascade lasers with quasi-periodic resonators." Physica E: Low-dimensional Systems and Nanostructures 40, no. 6 (2008): 2176–78. http://dx.doi.org/10.1016/j.physe.2007.10.114.

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29

Kovalenko, S. E., V. Losev, and M. R. Perrone. "Super-Gaussian resonators for long-pulse XeCl lasers." Applied Optics 33, no. 18 (1994): 4082. http://dx.doi.org/10.1364/ao.33.004082.

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30

Mudge, D., M. Ostermeyer, D. J. Ottaway, P. J. Veitch, J. Munch, and M. W. Hamilton. "High-power Nd:YAG lasers using stable–unstable resonators." Classical and Quantum Gravity 19, no. 7 (2002): 1783–92. http://dx.doi.org/10.1088/0264-9381/19/7/375.

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31

Gmachl, Claire, Federico Capasso, Deborah L. Sivco, et al. "Microlasers with Chaotic Resonators and Bow-tie Lasers." Optics and Photonics News 9, no. 12 (1998): 26. http://dx.doi.org/10.1364/opn.9.12.000026.

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32

Fang, H., and M. R. Perrone. "Numerical simulation of excimer lasers with unstable resonators." IEEE Journal of Quantum Electronics 30, no. 10 (1994): 2369–75. http://dx.doi.org/10.1109/3.328586.

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33

Gavrilov, V. F., I. E. Zuikov, N. V. Zuikova, and A. A. Kutsak. "Frequency characteristics of linear lasers with coupled resonators." Journal of Applied Spectroscopy 49, no. 4 (1988): 1005–8. http://dx.doi.org/10.1007/bf00657216.

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34

Hodgson, N., and H. Weber. "High-power solid-state lasers with unstable resonators." Optical and Quantum Electronics 22, S1 (1990): S39—S55. http://dx.doi.org/10.1007/bf02088999.

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35

Sytova, Svetlana N. "Nonlinear dynamics of radiation of high-current beams of charged particles in spatially periodic structures." Journal of the Belarusian State University. Physics, no. 1 (February 9, 2021): 62–72. http://dx.doi.org/10.33581/2520-2243-2021-1-62-72.

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Provided a review of physical processes underlying the functioning of vacuum electronic devices, namely, nonlinear processes of radiation of high-current beams of charged particles during their passage through spatially periodic structures (resonators) and their interaction with an electromagnetic field. Principles of functioning of travelling wave tubes, backward wave tubes, multi-wave Cherenkov generators, free electron lasers and free electron masers, volume free electron lasers are considered. These devices operate in a wide spectrum range from microwave to X-ray, have high efficiency, and

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36

Karnutsch, Christian, Marc Stroisch, Martin Punke, Uli Lemmer, Jing Wang, and Thomas Weimann. "Laser Diode-Pumped Organic Semiconductor Lasers Utilizing Two-Dimensional Photonic Crystal Resonators." IEEE Photonics Technology Letters 19, no. 10 (2007): 741–43. http://dx.doi.org/10.1109/lpt.2007.895894.

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37

Lu, Tsan-Wen, Yu-Kai Feng, Huan-Yeuh Chu, and Po-Tsung Lee. "Photonic Crystal Polymeric Thin-Film Dye-Lasers for Attachable Strain Sensors." Sensors 21, no. 16 (2021): 5331. http://dx.doi.org/10.3390/s21165331.

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In this report, using two-dimensional photonic crystals (PhC) and a one-dimensional PhC nano-beam cavity, we realized the development of all-polymeric dye-lasers on a dye-doped, suspended poly-methylmethacrylate film with a wavelength-scale thickness. In addition to the characterization of basic lasing properties, we also evaluated its capacity to serve as an attachable strain sensor. Through experimentation, we confirmed the stable lasing performances of the dye-laser attaching on a rough surface. Moreover, we also theoretically studied the wavelength responses of the utilized PhC resonators

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38

Dzyubenko, M. I., Yu Ye Kamenev, and V. P. Radionov. "TERAHERTZ RANGE GAS-DISCHARGE LASERS PART 2: RESONATORS OF THE LASERS AND APPLICATIONS." Telecommunications and Radio Engineering 76, no. 20 (2017): 1797–821. http://dx.doi.org/10.1615/telecomradeng.v76.i20.20.

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39

Balakireva, Irina V., Igor Yu Blinov, Vladislav I. Pavlov, and Nickolay P. Khatyrev. "State of the art and perspectives of the devices with the optical WGM resonators in time and frequency metrology." Izmeritel`naya Tekhnika, no. 3 (2020): 24–28. http://dx.doi.org/10.32446/0368-1025it.2020-3-24-28.

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One of the most important tasks in the metrological support of time and frequency measurements is a development of an extremely stable narrow-bandwidth laser sources and oscillators of the sets of the equidistant narrow optical spectral lines (the so-called “optical combs”). These devices are necessary for the transmission of the reference frequency signals and for use as part of mobile sources of time and frequency reference signals in optical and microwave spectral ranges. They are also required for precision ultra-high resolution spectroscopy. A promising direction for the creation of highl

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40

Taché, J. P., A. Le Floch, and R. Le Naour. "Lamb dip asymmetry in lasers with plane-parallel resonators." Applied Optics 25, no. 17 (1986): 2934. http://dx.doi.org/10.1364/ao.25.002934.

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41

Savin, A. V., S. Yu Strakhov, and S. L. Druzhinin. "Unstable resonators of high-power chemical oxygen—iodine lasers." Quantum Electronics 36, no. 9 (2006): 867–73. http://dx.doi.org/10.1070/qe2006v036n09abeh013407.

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42

Chen, Yu-Chuan, Xiang-Yang Zheng, Tian-Shu Lai, Xiang-Shao Xu, Dang Mo, and Wei-Zhu Lin. "Resonators for self-mode-locking Ti:sapphire lasers without apertures." Optics Letters 21, no. 18 (1996): 1469. http://dx.doi.org/10.1364/ol.21.001469.

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43

Unterrainer, Karl, Raffaele Colombelli, Claire Gmachl, et al. "Quantum cascade lasers with double metal-semiconductor waveguide resonators." Applied Physics Letters 80, no. 17 (2002): 3060–62. http://dx.doi.org/10.1063/1.1469657.

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44

Cerullo, G., S. De Silvestri, V. Magni, and L. Pallaro. "Resonators for Kerr-lens mode-locked femtosecond Ti:sapphire lasers." Optics Letters 19, no. 11 (1994): 807. http://dx.doi.org/10.1364/ol.19.000807.

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45

Hodgson, Norman, Georg Bostanjoglo, and Horst Weber. "Multirod unstable resonators for high-power solid-state lasers." Applied Optics 32, no. 30 (1993): 5902. http://dx.doi.org/10.1364/ao.32.005902.

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46

Cojocaru, E. "Simple relations for different resonators of solid-state lasers." Applied Optics 33, no. 16 (1994): 3454. http://dx.doi.org/10.1364/ao.33.003454.

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47

Braasch, J. C., and W. Holzapfel. "Frequency stabilisation of monomode semiconductor lasers to birefringent resonators." Electronics Letters 28, no. 9 (1992): 849. http://dx.doi.org/10.1049/el:19920537.

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48

Berggren, M., A. Dodabalapur, R. E. Slusher, Z. Bao, A. Timko, and O. Nalamasu. "Organic lasers based on lithographically defined photonic-bandgap resonators." Electronics Letters 34, no. 1 (1998): 90. http://dx.doi.org/10.1049/el:19980119.

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49

Jin, Leisheng, Hao Zhao, Zhi Li, Zongqing Jiang, Lijie Li, and Xiaohong Yan. "Nonlinear dynamic control of GaAs nanomechanical resonators using lasers." Nanotechnology 32, no. 29 (2021): 295502. http://dx.doi.org/10.1088/1361-6528/abf3f1.

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50

Mudge, D., P. J. Veitch, J. Munch, D. Ottaway, and M. W. Hamilton. "High-power diode-laser-pumped CW solid-state lasers using stable-unstable resonators." IEEE Journal of Selected Topics in Quantum Electronics 3, no. 1 (1997): 19–25. http://dx.doi.org/10.1109/2944.585808.

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