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1

Rodwell, M. J. W., D. M. Bloom, and K. J. Weingarten. "Subpicosecond laser timing stabilization." IEEE Journal of Quantum Electronics 25, no. 4 (1989): 817–27. http://dx.doi.org/10.1109/3.17346.

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2

Zhenglan Bian, Zhenglan Bian, Chongde Huang Chongde Huang, Dijun Chen Dijun Chen, et al. "Seed laser frequency stabilization for Doppler wind lidar." Chinese Optics Letters 10, no. 9 (2012): 091405–91407. http://dx.doi.org/10.3788/col201210.091405.

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3

Shiguang Wang, Shiguang Wang, Jianwei Zhang Jianwei Zhang, Zhengbo Wang Zhengbo Wang, et al. "Frequency stabilization of a 214.5-nm ultraviolet laser." Chinese Optics Letters 11, no. 3 (2013): 031401–31403. http://dx.doi.org/10.3788/col201311.031401.

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4

Yuan Dandan, 苑丹丹, 胡姝玲 Hu Shuling, 刘宏海 Liu Honghai, and 马静 Ma Jing. "Research of Laser Frequency Stabilization." Laser & Optoelectronics Progress 48, no. 8 (2011): 081401. http://dx.doi.org/10.3788/lop48.081401.

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5

Robins, N. P., B. J. J. Slagmolen, D. A. Shaddock, J. D. Close, and M. B. Gray. "Interferometric, modulation-free laser stabilization." Optics Letters 27, no. 21 (2002): 1905. http://dx.doi.org/10.1364/ol.27.001905.

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6

Patel, A., M. Protopapas, D. G. Lappas, and P. L. Knight. "Stabilization with arbitrary laser polarizations." Physical Review A 58, no. 4 (1998): R2652—R2655. http://dx.doi.org/10.1103/physreva.58.r2652.

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7

Plewinski, Paweł. "Closed-loop Laser Stabilization System." ELEKTRONIKA - KONSTRUKCJE, TECHNOLOGIE, ZASTOSOWANIA 1, no. 12 (2016): 24–28. http://dx.doi.org/10.15199/13.2016.12.3.

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8

TAKO, Toshiharu, and Yoshiaki AKIMOTO. "Laser frequency stabilization and tuning." Review of Laser Engineering 15, no. 6 (1987): 365–69. http://dx.doi.org/10.2184/lsj.15.365.

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9

Osipenko, Georgii V., Mikhail S. Aleynikov, and Alina G. Sukhoverskaya. "Modulation transfer spectroscopy offset laser frequency stabilization laser." Izmeritel`naya Tekhnika, no. 1 (2023): 4–7. http://dx.doi.org/10.32446/0368-1025it.2023-1-4-7.

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10

Lyablin, M. V., and Yu V. Klemeshov. "Laser Power Stabilization in a Precision Laser Inclinometer." Physics of Particles and Nuclei Letters 20, no. 2 (2023): 140–55. http://dx.doi.org/10.1134/s1547477123020176.

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11

Gou, Qingzhe, Ning Wei, Haixu Tao, et al. "Miniature laser frequency stabilization module for cold atom sensing." Chinese Optics Letters 22, no. 10 (2024): 101302. http://dx.doi.org/10.3788/col202422.101302.

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12

Schuldt, Thilo, Klaus Döringshoff, Markus Oswald, Evgeny V. Kovalchuk, Achim Peters, and Claus Braxmaier. "Absolute laser frequency stabilization for LISA." International Journal of Modern Physics D 28, no. 12 (2019): 1845002. http://dx.doi.org/10.1142/s0218271818450025.

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The LISA space mission requires laser frequency pre-stabilization of the 1064[Formula: see text]nm laser sources. While cavity-based systems are the current baseline, laser frequencies stabilized to a hyperfine transition in molecular iodine near 532[Formula: see text]nm are a possible alternative. Several setups with respect to space applications were developed, putting special emphasis on compactness and mechanical and thermal stability of the optical setup. Vibration testing and thermal cycling were performed. These setups show frequency noise below 20[Formula: see text]Hz/[Formula: see tex
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13

Wang, Mengke, Jia Kong, Jiqing Fu, Hao Liu, and Xiao-Ming Lu. "Modulation-free portable laser frequency and power stabilization system." Review of Scientific Instruments 93, no. 5 (2022): 053001. http://dx.doi.org/10.1063/5.0083923.

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The performance of laser-based instruments heavily depends on the stability of their laser source. Some instruments, such as the Cs–4He magnetometer, even require the frequency stabilization and the power stabilization at the same time. In this work, we design a double-locking system with a fiber-coupled output on a small bread board and apply it to the pump laser of a Cs–4He magnetometer. By carefully choosing the stabilization methods, we significantly improve the long-term simultaneous stability of frequency and power of the pump laser. The laser frequency drifts in 2 h are reduced from 100
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14

Li, Wenjun, Lin Zhang, Yading Guo, et al. "Active Disturbance Rejection Control Based Feedback Control System for Quasi-Continuous-Wave Laser Beam Pointing Stabilization." Journal of Physics: Conference Series 2112, no. 1 (2021): 012016. http://dx.doi.org/10.1088/1742-6596/2112/1/012016.

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Abstract Because of the significant nonlinearity of fast steering mirror (FSM), which is actuated by lead zirconate titanate (PZT) stacks, designing a high-performance laser beam pointing stabilization system is always a difficult work. This paper reports an active disturbance rejection control (ADRC) based feedback control system for laser beam pointing stabilization of a high-power quasi-continuous-wave (QCW) Nd:YAG slab laser with a repetition frequency of 160 Hz and an average output power of 1.5 kW. The simulation and experiment show that the ADRC is faster and smoother than traditional p
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15

Liu, Xiao Dong, Hai Dong Lei, and Jian Jun Zhang. "Frequency Stabilization of the Diode Laser to the Extra Reference Cavity." Applied Mechanics and Materials 198-199 (September 2012): 1235–40. http://dx.doi.org/10.4028/www.scientific.net/amm.198-199.1235.

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The Semiconductor laser frequency stabilization is the important study topic because of its increasing popular. We introduce a simply experimental setup method of the frequency stabilization of a 780 nm diode laser by only a tiny current in the laser audio modulation, photodiode receiver, and locking the transmission peaks. Use this method, the laser can be locked to the resonance peak of the Fabry-Perot cavity. The linewidth of laser is below 400 kHz, and it runs continually above 3 hours.
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16

Hrabina, J., O. Acef, F. du Burck, et al. "Comparison of Molecular Iodine Spectral Properties at 514.7 and 532 nm Wavelengths." Measurement Science Review 14, no. 4 (2014): 213–18. http://dx.doi.org/10.2478/msr-2014-0029.

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Abstract We present results of investigation and comparison of spectral properties of molecular iodine transitions in the spectral region of 514.7 nm that are suitable for laser frequency stabilization and metrology of length. Eight Doppler-broadened transitions that were not studied in detail before were investigated with the help of frequency doubled Yb-doped fiber laser, and three of the most promising lines were studied in detail with prospect of using them in frequency stabilization of new laser standards. The spectral properties of hyperfine components (linewidths, signal-to-noise ratio)
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17

Lili Wang, Lili Wang, Zhaoshuo Tian Zhaoshuo Tian, Yanchao Zhang Yanchao Zhang, et al. "Frequency stabilization of pulsed CO2 laser using setup-time method." Chinese Optics Letters 10, no. 1 (2012): 011402–11404. http://dx.doi.org/10.3788/col201210.011402.

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18

Trad Nery, Marina, Jasper R. Venneberg, Nancy Aggarwal, et al. "Laser power stabilization via radiation pressure." Optics Letters 46, no. 8 (2021): 1946. http://dx.doi.org/10.1364/ol.422614.

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19

MORINAGA, Atsuo. "Dye laser spectrometer and frequency stabilization." Journal of the Spectroscopical Society of Japan 34, no. 2 (1985): 109–10. http://dx.doi.org/10.5111/bunkou.34.109.

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20

Chéron, B., H. Gilles, J. Hamel, O. Moreau, and H. Sorel. "Laser frequency stabilization using Zeeman effect." Journal de Physique III 4, no. 2 (1994): 401–6. http://dx.doi.org/10.1051/jp3:1994136.

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21

Karlson, Antonella, and Marvin H. Mittleman. "Stabilization of positronium by laser fields." Journal of Physics B: Atomic, Molecular and Optical Physics 29, no. 20 (1996): 4609–23. http://dx.doi.org/10.1088/0953-4075/29/20/016.

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22

Hammer, Daniel X., R. Daniel Ferguson, John C. Magill, Michael A. White, Ann E. Elsner, and Robert H. Webb. "Image stabilization for scanning laser ophthalmoscopy." Optics Express 10, no. 26 (2002): 1542. http://dx.doi.org/10.1364/oe.10.001542.

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23

Dasgupta, Soura, and David R. Andersen. "Feedback stabilization of semiconductor laser arrays." Journal of the Optical Society of America B 11, no. 2 (1994): 290. http://dx.doi.org/10.1364/josab.11.000290.

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24

Gavrila, Mihai. "Atomic stabilization in superintense laser fields." Journal of Physics B: Atomic, Molecular and Optical Physics 35, no. 18 (2002): R147—R193. http://dx.doi.org/10.1088/0953-4075/35/18/201.

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25

Ereifej, Heider N., and J. G. Story. "Laser-induced stabilization of autoionizing states." Physical Review A 60, no. 5 (1999): 3947–51. http://dx.doi.org/10.1103/physreva.60.3947.

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26

Salomon, Ch, D. Hils, and J. L. Hall. "Laser stabilization at the millihertz level." Journal of the Optical Society of America B 5, no. 8 (1988): 1576. http://dx.doi.org/10.1364/josab.5.001576.

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27

Wood, Roger M. "Frequency stabilization of semiconductor laser diodes." Optics & Laser Technology 27, no. 6 (1995): xiii. http://dx.doi.org/10.1016/0030-3992(95)90064-0.

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28

Piraux, Bernard, Etienne Huens, and Peter Knight. "Atomic stabilization in ultrastrong laser fields." Physical Review A 44, no. 1 (1991): 721–32. http://dx.doi.org/10.1103/physreva.44.721.

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29

Oksenhendler, T., F. Legrand, M. Perdrix, O. Gobert, and D. Kaplan. "Femtosecond laser pulse energy self-stabilization." Applied Physics B 79, no. 8 (2004): 933–35. http://dx.doi.org/10.1007/s00340-004-1681-5.

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30

Fellman, T., �. Lindberg, and B. St�hlberg. "Laser-frequency stabilization using forward scattering." Applied Physics B Laser and Optics 59, no. 6 (1994): 631–33. http://dx.doi.org/10.1007/bf01081184.

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31

Liu, Chang, Ziqian Yue, Zitong Xu, Ming Ding, and Yueyang Zhai. "Far Off-Resonance Laser Frequency Stabilization Technology." Applied Sciences 10, no. 9 (2020): 3255. http://dx.doi.org/10.3390/app10093255.

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In atomic physics experiments, a frequency-stabilized or ‘locked’ laser source is commonly required. Many established techniques are available for locking close to an atomic resonance. However, in many instances, such as atomic magnetometer and magic wavelength optical lattices in ultra-cold atoms, it is desirable to lock the frequency of the laser far away from the resonance. This review presents several far off-resonance laser frequency stabilization methods, by which the frequency of the probe beam can be locked on the detuning as far as several tens of gigahertz (GHz) away from atomic reso
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32

Cai, Yindi, Baokai Feng, Qi Sang, and Kuang-Chao Fan. "Real-Time Correction and Stabilization of Laser Diode Wavelength in Miniature Homodyne Interferometer for Long-Stroke Micro/Nano Positioning Stage Metrology." Sensors 19, no. 20 (2019): 4587. http://dx.doi.org/10.3390/s19204587.

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A low-cost miniature homodyne interferometer (MHI) with self-wavelength correction and self-wavelength stabilization is proposed for long-stroke micro/nano positioning stage metrology. In this interferometer, the displacement measurement is based on the analysis of homodyne interferometer fringe pattern. In order to miniaturize the interferometer size, a low-cost and small-sized laser diode is adopted as the laser source. The accuracy of the laser diode wavelength is real-time corrected by the proposed wavelength corrector using a modified wavelength calculation equation. The variation of the
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33

Dobosz, Marek. "Laser diode distance measuring interferometer - metrological properties." Metrology and Measurement Systems 19, no. 3 (2012): 553–64. http://dx.doi.org/10.2478/v10178-012-0048-1.

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Abstract A novel laser diode based length measuring interferometer for scientific and industrial metrology is presented. Wavelength the stabilization system applied in the interferometer is based on the optical wedge interferometer. Main components of the interferometer such as: laser diode stabilization assembly, photodetection system, measuring software, air parameters compensator and base optical assemblies are described. Metrological properties of the device such as resolution, measuring range, repeatability and accuracy are characterized.
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34

Mio, Norikatsu, Takafumi Ozeki, Kosuke Machida, and Shigenori Moriwaki. "Laser Intensity Stabilization System Using Laser-Diode-Pumped Nd:YAG Rod-Laser Amplifier." Japanese Journal of Applied Physics 46, no. 8A (2007): 5338–41. http://dx.doi.org/10.1143/jjap.46.5338.

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35

Paensin, N., R. Kaewuam, P. Phoonthong, N. Chattrapiban, and N. Thaicharoen. "Laser frequency stabilization using Pound-Drever-Hall technique for Yb+ atomic clock experiment." Journal of Physics: Conference Series 2934, no. 1 (2025): 012023. https://doi.org/10.1088/1742-6596/2934/1/012023.

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Abstract The precise stabilization of laser frequencies is crucial for various applications in atomic physics, particularly in atomic clock experiments and ion cooling. The Pound-Drever-Hall (PDH) technique is a technique for locking laser frequencies to high-finesse optical cavities, ensuring exceptional frequency stability. This study focuses on designing an optical cavity as well as implementing the PDH technique to stabilize a 369-nm laser, essential for ytterbium ion (Yb+) cooling in atomic clock experiments. The results show that the 369-nm laser can maintain stability within a range of
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36

Wang, Bowen, Xiang Peng, Haidong Wang, Yang Liu, and Hong Guo. "Laser-frequency stabilization with differential single-beam saturated absorption spectroscopy of 4He atoms." Review of Scientific Instruments 93, no. 4 (2022): 043001. http://dx.doi.org/10.1063/5.0084605.

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Differential single-beam saturated-absorption spectroscopy (DSSAS) is proposed to stabilize lasing frequency and suppress Doppler-broadened background and common-mode optical noise. The spectral first-derivative demodulated signal of metastable [Formula: see text] atoms is used as an error signal to stabilize a fiber laser around 1083 nm. Experimental results show that, compared with existing non-DSSAS frequency stabilization, DSSAS stabilization produces better stability and lower fluctuations, especially for frequency-noise-corrupted lasers. In DSSAS stabilization, for data acquired over 700
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37

Liu, Jianning, Jun Weng, Junbiao Jiang, et al. "Study of the Steady-State Operation of a Dual-Longitudinal-Mode and Self-Biasing Laser Gyroscope." Sensors 22, no. 16 (2022): 6300. http://dx.doi.org/10.3390/s22166300.

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In order to stabilize the self-biasing state of a laser gyroscope, a dual-longitudinal-mode asymmetric frequency stabilization technique was studied. The special frequency stabilization is based on the accurate control of the intensity tuning curve in the prism ring laser. In this study, the effects of the ratio of the Ne isotopes, the inflation pressure, and the frequencies coupling on the intensity tuning curve in a laser gyro were examined. The profiles of the intensity tuning curve were simulated under the mixing ratios of Ne20 and Ne22 of 1:1 and 7:3, and the inflation pressures were 350
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38

Qing, Chen, Lishuang Feng, and Dengke Zhang. "Laser frequency stabilization with a metasurface chip through atomic spectral manipulation." Chinese Optics Letters 23, no. 3 (2025): 033601. https://doi.org/10.3788/col202523.033601.

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39

Wang, Haidong, Teng Wu, He Wang, et al. "A Compact Laser Pumped 4He Magnetometer with Laser-Frequency Stabilization by Inhomogeneous Light Shifts." Applied Sciences 10, no. 10 (2020): 3608. http://dx.doi.org/10.3390/app10103608.

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We propose a compact 4He magnetometer realizing magnetic field measurement and laser-frequency stabilization simultaneously in a single 4He atomic cell. The frequency stabilization scheme is based on the asymmetric line shape of magnetic resonance which is induced by spatially inhomogeneous light shifts. We investigate the asymmetric line shape of the magnetic resonance signal theoretically and experimentally in laser pumped 4He magnetometer with the magneto-optical double-resonance configuration. Notice that, due to the asymmetric line shape, the in-phase component of the magnetic resonance s
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40

Afanador Delgado, Samuel Mardoqueo, Juan Hugo García López, Rider Jaimes Reátegui, Vicente Aboites, José Luis Echenausía Monroy, and Guillermo Huerta Cuellar. "High Efficiency and High Stability for SHG in an Nd:YVO4 Laser with a KTP Intracavity and Q-Switching through Harmonic Modulation." Photonics 10, no. 4 (2023): 454. http://dx.doi.org/10.3390/photonics10040454.

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In this paper, the stabilization and high efficiency of an unstable Second Harmonic Generation (SHG) of an Nd:YVO4 laser with a KTP intracavity is demonstrated. By using a passive Q-switching crystal (Cr4+:YAG) and a parametric modulation method (harmonic modulation), the stabilization of the laser is reached. An harmonic modulation was applied to the pumping of the Nd:YVO4-KTP laser to control the amplitude and frequency of the laser emission. The results were characterized by using power spectra analysis, optical spectrum, bifurcation diagrams, and temporal series of the laser intensity. The
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41

Kholmatov, S. K. "About application of micropulse laser cyclocoagulation in glaucoma." Russian ophthalmology of children 51, no. 1 (2025): 44–50. https://doi.org/10.25276/2307-6658-2025-1-44-50.

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This review represents data on the mechanism of action and effectiveness of a promising and relatively new technique of transcleral laser cyclocoagulation in micropulse mode. Based on a detailed analysis of the effect of this intervention on the stabilization of the glaucoma process, visual acuity, as well as the frequency of complications, the author concludes that micropulse laser cyclocoagulation can be used in patients with refractory and angle-closure glaucoma with high visual functions. Author emphasizes that stabilization of IOP after micropulse laser cycloagulation is achieved more eas
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42

Preuschoff, Tilman, Patrick Baus, Malte Schlosser, and Gerhard Birkl. "Wideband current modulation of diode lasers for frequency stabilization." Review of Scientific Instruments 93, no. 6 (2022): 063002. http://dx.doi.org/10.1063/5.0093520.

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We present a current modulation technique for diode laser systems, which is specifically designed for high-bandwidth laser frequency stabilization and wideband frequency modulation with a flat transfer function. It consists of a dedicated current source and an impedance matching circuit both placed close to the laser diode. The transfer behavior of the system is analyzed under realistic conditions employing an external cavity diode laser (ECDL) system. We achieve a phase lag smaller than 90° up to 25 MHz and a gain flatness of ±3 dB in the frequency range of DC to 100 MHz, while the passive st
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43

SU, Q., A. SANPERA, and L. ROSO-FRANCO. "ATOMIC STABILIZATION IN THE PRESENCE OF INTENSE LASER PULSES." International Journal of Modern Physics B 08, no. 13 (1994): 1655–98. http://dx.doi.org/10.1142/s0217979294000713.

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The nonperturbative response of atomic systems under strong laser radiation has been an important area of research both experimentally and theoretically. In a typical experiment, a very high power laser (operating at an intensity of the order of 1013 W/cm 2 or higher, delivering 1 µm wavelength light pulses with duration from a few pico-seconds down to a few hundred femto-seconds) is focused down to a tight spot in space filled with dilute gas where ionization occurs. These experiments have been successful in studying the single-atom strong-field physics where the predictions of ionization bas
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44

Fancher, C. T., K. L. Nicolich, K. M. Backes, et al. "A self-locking Rydberg atom electric field sensor." Applied Physics Letters 122, no. 9 (2023): 094001. http://dx.doi.org/10.1063/5.0137127.

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A crucial step toward enabling real-world applications for quantum sensing devices such as Rydberg atom electric field sensors is reducing their size, weight, power, and cost (SWaP-C) requirements without significantly reducing performance. Laser frequency stabilization is a key part of many quantum sensing devices and, when used for exciting non-ground state atomic transitions, is currently limited to techniques that require either large SWaP-C optical cavities and electronics or use significant optical power solely for frequency stabilization. Here, we describe a laser frequency stabilizatio
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45

Balakshy, V. I., Yu I. Kuznetsov, and S. N. Mantsevich. "Acousto-Optic Stabilization of Laser Beam Intensity." Bulletin of the Russian Academy of Sciences: Physics 77, no. 12 (2013): 1463–67. http://dx.doi.org/10.3103/s1062873813130029.

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46

Julsgaard, B., A. Walther, S. Kröll, and L. Rippe. "Understanding laser stabilization using spectral hole burning." Optics Express 15, no. 18 (2007): 11444. http://dx.doi.org/10.1364/oe.15.011444.

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47

Sonnenmoser, K. "Stabilization of atoms in superintense laser fields." Journal of Physics B: Atomic, Molecular and Optical Physics 26, no. 3 (1993): 457–75. http://dx.doi.org/10.1088/0953-4075/26/3/017.

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48

Hjelme, D. R., A. R. Mickelson, and R. G. Beausoleil. "Semiconductor laser stabilization by external optical feedback." IEEE Journal of Quantum Electronics 27, no. 3 (1991): 352–72. http://dx.doi.org/10.1109/3.81333.

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49

Fellman, Tomas, Peter Jungner, and Birger Stahlberg. "Stabilization of a green He–Ne laser." Applied Optics 26, no. 14 (1987): 2705. http://dx.doi.org/10.1364/ao.26.002705.

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50

Jeong, Taek, and Han Seb Moon. "Laser frequency stabilization using bichromatic crossover spectroscopy." Journal of Applied Physics 117, no. 9 (2015): 093102. http://dx.doi.org/10.1063/1.4913880.

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