Academic literature on the topic 'Laser stabilization'

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Journal articles on the topic "Laser stabilization"

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Zhenglan Bian, Zhenglan Bian, Chongde Huang Chongde Huang, Dijun Chen Dijun Chen, Jiaobo Peng Jiaobo Peng, Min Gao Min Gao, Zuoren Dong Zuoren Dong, Jiqiao Liu Jiqiao Liu, Haiwen Cai Haiwen Cai, Ronghui Qu Ronghui Qu, and Shangqing Gong Shangqing Gong. "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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Shiguang Wang, Shiguang Wang, Jianwei Zhang Jianwei Zhang, Zhengbo Wang Zhengbo Wang, Bo Wang Bo Wang, Weixin Liu Weixin Liu, Yanying Zhao Yanying Zhao, and Lijun Wang Lijun Wang. "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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Rodwell, M. J. W., D. M. Bloom, and K. J. Weingarten. "Subpicosecond laser timing stabilization." IEEE Journal of Quantum Electronics 25, no. 4 (April 1989): 817–27. http://dx.doi.org/10.1109/3.17346.

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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 (April 1, 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 7000 s, the root mean square frequency fluctuation of the fiber laser is 16.4 kHz, and the frequency stability described by the modified Allan deviation is 4.1 × 10−12 at 100 s. Even for a defective laser with poor frequency stability, the proposed scheme demonstrates experimentally high capability of noise suppression and reduces the frequency fluctuations by two orders of magnitude. Given its simplicity and compact design, frequency stabilization by DSSAS is promising for quantum-sensor applications, such as atomic magnetometers, atomic gyroscopes, and atomic clocks.
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Zhou, Yueting, Jianxin Liu, Songjie Guo, Gang Zhao, Weiguang Ma, Zhensong Cao, Lei Dong, et al. "Laser frequency stabilization based on a universal sub-Doppler NICE-OHMS instrumentation for the potential application in atmospheric lidar." Atmospheric Measurement Techniques 12, no. 3 (March 19, 2019): 1807–14. http://dx.doi.org/10.5194/amt-12-1807-2019.

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Abstract. Lidar is an effective tool for high-altitude atmospheric measurement in which a weak absorption line for the target gas is selected to ensure a large optical depth. The laser frequency stabilization to the line center is required, and a sub-Doppler (sD) spectroscopy of the target line is preferred as a frequency reference. In this paper, a novel universal sD noise-immune cavity-enhanced optical heterodyne molecular spectroscopy (NICE-OHMS) instrumentation based on a fiber-coupled optical single-sideband electro-optic modulator (f-SSM) for the potential application in atmospheric lidar for different target gases with different types of lasers is reported. The f-SSM can replace all frequency actuators in the system, so as to eliminate the individual design of feedback servos that often are tailored for each laser. The universality of the instrumentation was demonstrated by the alternative use of either an Er-doped fiber laser or a whispering-gallery-mode laser. Then the instruments based on both lasers were used to produce the sD signals of acetylene, which worked as a frequency reference to stabilize the laser. By performing the lockings, relative frequency stabilizations of 8.3×10-13 and 7.5×10-13 at an integration time of 240 s were demonstrated.
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Kim, Junwoo, Keumhyun Kim, Dowon Lee, Yongha Shin, Sungsam Kang, Jung-Ryul Kim, Youngwoon Choi, Kyungwon An, and Moonjoo Lee. "Locking Multi-Laser Frequencies to a Precision Wavelength Meter: Application to Cold Atoms." Sensors 21, no. 18 (September 18, 2021): 6255. http://dx.doi.org/10.3390/s21186255.

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We herein report a simultaneous frequency stabilization of two 780-nm external cavity diode lasers using a precision wavelength meter (WLM). The laser lock performance is characterized by the Allan deviation measurement in which we find σy=10−12 at an averaging time of 1000 s. We also obtain spectral profiles through a heterodyne spectroscopy, identifying the contribution of white and flicker noises to the laser linewidth. The frequency drift of the WLM is measured to be about 2.0(4) MHz over 36 h. Utilizing the two lasers as a cooling and repumping field, we demonstrate a magneto-optical trap of 87Rb atoms near a high-finesse optical cavity. Our laser stabilization technique operates at broad wavelength range without a radio frequency element.
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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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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 (November 1, 2002): 1905. http://dx.doi.org/10.1364/ol.27.001905.

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Patel, A., M. Protopapas, D. G. Lappas, and P. L. Knight. "Stabilization with arbitrary laser polarizations." Physical Review A 58, no. 4 (October 1, 1998): R2652—R2655. http://dx.doi.org/10.1103/physreva.58.r2652.

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Plewinski, Paweł. "Closed-loop Laser Stabilization System." ELEKTRONIKA - KONSTRUKCJE, TECHNOLOGIE, ZASTOSOWANIA 1, no. 12 (December 5, 2016): 24–28. http://dx.doi.org/10.15199/13.2016.12.3.

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Dissertations / Theses on the topic "Laser stabilization"

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Kwee, Patrick. "Laser characterization and stabilization for precision interferometry." Hannover Technische Informationsbibliothek und Universitätsbibliothek Hannover, 2010. http://d-nb.info/1000893626/34.

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Pugla, Sarika. "Ultrastable high finesse cavities for laser frequency stabilization." Thesis, Imperial College London, 2008. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.490789.

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Lasers with stability of the order of 10.15 or more form the basis of frequency metrology and several other experiments including gravitational wave detection, high-precision spectroscopy and tests of relativity. This thesis describes the frequency stabilization of 1064nm, Nd:YAG lasers to ultra-stable, high finesse Fabry-Perot cavities using the PoundDrever- Halliocking scheme. These lasers will be used as flywheel oscillators for optical atomic clocks. The first part of this thesis describes the design and development of a stable laser using a cryogenic, all-sapphire, high finesse Fabry-Perot cavity. Two similar systems have been developed and the beat frequency between the two systems has been measured. This beat frequency measurement provides a measure of relative stability of the laser. In addition experiments have also been performed with ULE (ultra-low expansivity) glass cavities. The thermal expansivity of ULE has a zero near room temperature and a turning point was found. A beat frequency measurement was made for a pair of lasers locked to ULE cavities.The frequency stabilization techniques applied to the lasers described in this thesis will be used for future frequency standards based on optical transitions.
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Sievers, Charles A. (Charles Anders) 1979. "Frequency stabilization for a 486nm dye-ring laser." Thesis, Massachusetts Institute of Technology, 2004. http://hdl.handle.net/1721.1/32754.

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Thesis (S.B.)--Massachusetts Institute of Technology, Dept. of Physics, 2004.
Includes bibliographical references (p. 43).
For my thesis, I worked towards using two reference cavities to provide frequency stabilization to a 486nm dye-ring laser. After a doubling cavity doubles the frequency to 243nm, the laser beam is used to excite ground state hydrogen to the 2S state: the first step of an experiment to accurately measure the 2S-NS transitions of hydrogen and measure the Lamb shift and Rydberg's constant. Two stabilization cavities were used to prevent the frequency from drifting and to narrow the laser's line-width. I aligned the majority of the optics and coupling light into fiber-optic cables and Fabrey-Perot cavities. Coupling light into a high finesse Fabrey-Perot cavity requires matching the radius of curvature of constant phase of the laser with the geometry of the cavity. To do this, I first measured the physical properties of the laser beam and then numerical arrived at a solution using two lenses to match the conditions imposed by the cavity's geometry. I aligned the cavity and then observed a Pound-Drever-Hall error signal. This error signal will be fed back into the laser to stabilize the frequency. It is anticipated that when the electronics to utilize the error signals are completed, the laser frequency will be stabilized to a hundred hertz, an four order of magnitude improvement over the stability provided by the commericial laser.
by Charles A. Sievers.
S.B.
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Abu-Taha, M. I. A. "Optoacoustic frequency stabilization of a carbon dioxide laser." Thesis, Keele University, 1987. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.377921.

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Kwee, Patrick [Verfasser]. "Laser characterization and stabilization for precision interferometry / Patrick Kwee." Hannover : Technische Informationsbibliothek und Universitätsbibliothek Hannover, 2010. http://d-nb.info/1000893626/34.

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Ahmed, H. H. I. S. "Frequency selection and stabilization of semiconductor laser diode systems." Thesis, Swansea University, 2004. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.635861.

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Different types of semiconductor diode laser sources were tested in a range of spectroscopic and metrological applications to demonstrate the versatility of our laser set-up implementations. Two main topics were pursued in this study: (a) experiments on absorption spectroscopy were carried out using external cavity laser diode modules in the wavelength range (410 – 1550 nm) while vertical cavity surface emitting lasers (VCSELs) were used in the experiments involving opto-galvanic spectroscopy and laser frequency stabilization at 800.6 nm. Absorption experiments were performed for the quantitative detection of (atmospheric) trace gases such as H2O, CO,  and CO2. The Tuneable Diode Laser Absorption Spectroscopy (TDLAS) was realised without the need for sophisticated detection electronics (e.g. lock-in amplifiers, etc.). A notebook-data acquisition system in conjunction with dedicated software developed during this study was fully adequate and allowed us to generate “any” desired shape of the modulation signal; and – after the data had been acquired – post-collection processing could be carried out (like averaging, noise removal, signal normalization, trend plots, etc.). In order to implement the opto-galvanic (OG) spectroscopy experiment, the opto-galvanic driver, control and detection unit was designed and built in-house. This electronic device was one of the centrepieces of the set-up for locking the laser diode frequency to an atomic transition in a hollow cathode discharge lamp. An integrated device such as the one required in this study is not available commercially. The observed OG signal revealed a series of sub-structures in the form of doublets (0.0074 nm or 4 GHz apart). The doublet frequency splitting results from the fact that VCSEL light is composed of two clearly-resolved spectral components, both linearly polarized, associated with transverse mode oscillation. Locking the laser frequency in the OG signal of the Argon transition at 800.6 nm was achieved using modulation of the injection current of the laser diode. This was done by feeding the OG signal into the data acquisition and control card to generate the suitable error signal (in magnitude and sign) to the laser current driver. This process was entirely controlled by a software program written during the course of this work. Incomplete attempts were made to couple the Fabry-Perout (FP) laser radiation to a fibre Bragg grating (FBG) due to some technical problems. Specifically, the fabricated FB didn’t match fully to any diodes available to us during the time of the experiments. Thus, only very weak feedback on FBG side-bands was observed which was insufficient to push the laser into single-wavelength oscillation.
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Cunado, Jose. "CONTROL AND STABILIZATION OF LASER PLASMASOURCES FOR EUV LITHOGRAPHY." Master's thesis, University of Central Florida, 2007. http://digital.library.ucf.edu/cdm/ref/collection/ETD/id/2746.

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Extreme Ultraviolet (EUV) sources rely on droplet laser plasmas for EUV generation. These sources consist of a small (30 μm diameter) droplet which is excited into plasma emitting EUV around 13.5 nm, the industry's chosen wavelength for EUV lithography (EUVL). These sources are the best candidates for the commercialization of EUVL allowing mass production of computer chips with 32 nm or even smaller feature size. However, the biggest challenges which EUV source developers encounter today are the issues of conversion efficiency (CE) and debris.In order to satisfy the technology requirements, the source will need to meet high levels of stability, performance, and lifetime. Our tin-doped droplet plasma has demonstrated high CE and low debris resulting in long lifetime. Long term stability is obtained through the use of novel tracking techniques and active feedback. The laser plasma targeting system combines optical illumination and imaging, droplet technology innovation, advanced electronics, and custom software which act in harmony to provide complete stabilization of the droplets. Thus, a stable, debris-free light source combined with suitable collection optics can provide useful EUV radiation power. Detailed description of the targeting system and the evaluation of the system will be presented.
M.S.E.E.
School of Electrical Engineering and Computer Science
Engineering and Computer Science
Electrical Engineering MSEE
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Trad, Nery Marina [Verfasser]. "Laser power stabilization via radiation pressure / Marina Trad Nery." Hannover : Gottfried Wilhelm Leibniz Universität, 2021. http://d-nb.info/1234147564/34.

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Byrne, Nicole (Nicole Malenie). "Phase stabilization of laser beams in a cold atom accelerometer." Thesis, Massachusetts Institute of Technology, 2014. http://hdl.handle.net/1721.1/96460.

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Thesis: S.M., Massachusetts Institute of Technology, Department of Mechanical Engineering, 2014.
Cataloged from PDF version of thesis.
Includes bibliographical references (pages 95-97).
A cold atom accelerometer measures the displacement of a proof mass of laser cooled atoms with respect to an instrument reference frame. The cold atom interferometer's reference frame is defined by a pair of specially prepared, counter-propagating laser beams, that measure inertially induced atom displacements with nm scale resolution. This corresponds to acceleration sensitivities comparable to state of the art electro-mechanical accelerometers. In dynamic environments, sensitivity is limited by the stability of the relative laser phase of the two interrogation laser beams, which is adversely affected by vibrations and temperature fluctuations of the interrogation beam optics. Without an independent measurement, the cold atom interferometer cannot distinguish platform acceleration from laser phase fluctuations, which thus are a potentially serious source of error. In this thesis, a Michelson optical interferometer and an optical feedback loop were used to stabilize the relative phase of the interrogation laser beams in a cold atom accelerometer. A digital controller stabilized the relative phase via an electro-optic phase modulator. This control loop's bandwidth encompasses 98.8% of the noise power as determined from the power spectral density of the open loop 795nm Michelson signal. Increasing the controller bandwidth would gain the system marginal improvement in noise reduction. At an atom interferometer dwell time of 1 msec, active laser phase stabilization improved the atom interferometer sensitivity; at an atom interferometer dwell time of 8msec, an improvement was no longer evident. Improvements to the laser phase stabilization system are proposed to increase atom interferometer stability at longer dwell times.
by Nicole Byrne.
S.M.
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Chong, Michael. "Optical power stabilization of a laser diode for qnd measurement." Master's thesis, Alma Mater Studiorum - Università di Bologna, 2013. http://amslaurea.unibo.it/5892/.

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La realizzazione di stati non classici del campo elettromagnetico e in sistemi di spin è uno stimolo alla ricerca, teorica e sperimentale, da almeno trent'anni. Lo studio di atomi freddi in trappole di dipolo permette di avvicinare questo obbiettivo oltre a offrire la possibilità di effettuare esperimenti su condesati di Bose Einstein di interesse nel campo dell'interferometria atomica. La protezione della coerenza di un sistema macroscopico di spin tramite sistemi di feedback è a sua volta un obbiettivo che potrebbe portare a grandi sviluppi nel campo della metrologia e dell'informazione quantistica. Viene fornita un'introduzione a due tipologie di misura non considerate nei programmi standard di livello universitario: la misura non distruttiva (Quantum Non Demolition-QND) e la misura debole. Entrambe sono sfruttate nell'ambito dell'interazione radiazione materia a pochi fotoni o a pochi atomi (cavity QED e Atom boxes). Una trattazione delle trappole di dipolo per atomi neutri e ai comuni metodi di raffreddamento è necessaria all'introduzione all'esperimento BIARO (acronimo francese Bose Einstein condensate for Atomic Interferometry in a high finesse Optical Resonator), che si occupa di metrologia tramite l'utilizzo di condensati di Bose Einstein e di sistemi di feedback. Viene descritta la progettazione, realizzazione e caratterizzazione di un servo controller per la stabilizzazione della potenza ottica di un laser. Il dispositivo è necessario per la compensazione del ligh shift differenziale indotto da un fascio laser a 1550nm utilizzato per creare una trappola di dipolo su atomi di rubidio. La compensazione gioca un ruolo essenziale nel miglioramento di misure QND necessarie, in uno schema di feedback, per mantenere la coerenza in sistemi collettivi di spin, recentemente realizzato.
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Books on the topic "Laser stabilization"

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Trad Nery, Marina. Laser Power Stabilization via Radiation Pressure. Cham: Springer International Publishing, 2022. http://dx.doi.org/10.1007/978-3-030-95868-8.

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Trad Nery, Marina. Laser Power Stabilization via Radiation Pressure. Cham: Springer International Publishing, 2022. http://dx.doi.org/10.1007/978-3-030-95868-8.

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S, Sudo, and Sakai Yoshihisa, eds. Frequency stabilization of semiconductor laser diodes. Boston: Artech House, 1995.

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Yaakov, Shevy, and Society of Photo-optical Instrumentation Engineers., eds. Laser frequency stabilization and noise reduction: 9-10 February 1995, San Jose, California. Bellingham, Wash: SPIE, 1995.

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1934-, Hall J. L., Ye Jun 1967-, and Society of Photo-optical Instrumentation Engineers., eds. Laser frequency stabilization, standards, measurement, and applications: 24-26 January, 2001, San Jose, USA. Bellingham, Wash: SPIE, 2001.

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United States. National Aeronautics and Space Administration., ed. Sub-Hertz relative frequency stabilization of two diode laser pumped Nd:YAG lasers locked to a Fabry-Perot interferometer: A final report to NASA for the SUNLITE program. [Washington, D.C: National Aeronautics and Space Administration, 1990.

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United States. National Aeronautics and Space Administration., ed. Sub-Hertz relative frequency stabilization of two diode laser pumped Nd:YAG lasers locked to a Fabry-Perot interferometer: A final report to NASA for the SUNLITE program. [Washington, D.C: National Aeronautics and Space Administration, 1990.

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Udupa, D. V. The design, fabrication, and testing of an air spaced Fabry-Perot etalon for dye laser wavelength stabilization system. Mumbai, India: Bhabha Atomic Research Centre, 1997.

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United States. National Aeronautics and Space Administration, ed. Equipment grant to support NASA research on frequency stabilization of diode-laser-pumped solid state lasers: Final technical report, NASA grant NAG-1-828. Stanford, Calif: W.W. Hansen Laboratories of Physics, Ginzton Laboratory, Stanford University, 1988.

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Vàzquez, Rafael. Control of turbulent and magnetohydrodynamic channel flows: Boundary stabilization and state estimation. Boston: Birkhäuser, 2008.

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Book chapters on the topic "Laser stabilization"

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Hall, John L. "External Laser Stabilization." In Laser Physics at the Limits, 51–59. Berlin, Heidelberg: Springer Berlin Heidelberg, 2002. http://dx.doi.org/10.1007/978-3-662-04897-9_6.

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Fedorov, M. V. "Interference Stabilization." In Super-Intense Laser-Atom Physics IV, 11–21. Dordrecht: Springer Netherlands, 1996. http://dx.doi.org/10.1007/978-94-009-0261-9_2.

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Dumitras, D. C., D. C. A. Dutu, V. Draganescu, and N. Comaniciu. "Optogalvanic Laser Frequency Stabilization." In Trends in Quantum Electronics, 161–64. Berlin, Heidelberg: Springer Berlin Heidelberg, 1986. http://dx.doi.org/10.1007/978-3-662-10624-2_13.

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Muller, H. G. "Weakly Relativistic Stabilization." In Super-Intense Laser-Atom Physics, 339–44. Dordrecht: Springer Netherlands, 2001. http://dx.doi.org/10.1007/978-94-010-0754-2_32.

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DeVoe, R. G., C. Fabre, and R. G. Brewer. "Laser Frequency Division and Stabilization." In Methods of Laser Spectroscopy, 187–90. Boston, MA: Springer US, 1986. http://dx.doi.org/10.1007/978-1-4615-9459-8_24.

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DeVoe, R. G., C. Fabre, and R. G. Brewer. "Laser Frequency Division and Stabilization." In Springer Series in Optical Sciences, 358–61. Berlin, Heidelberg: Springer Berlin Heidelberg, 1985. http://dx.doi.org/10.1007/978-3-540-39664-2_110.

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Caves, Carlton M. "Laser Stabilization Using Squeezed Light." In Squeezed and Nonclassical Light, 29–38. Boston, MA: Springer US, 1989. http://dx.doi.org/10.1007/978-1-4757-6574-8_2.

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Barwood, G. P., and P. Gill. "Laser Stabilization for Precision Measurements." In Handbook of Laser Technology and Applications, 111–26. 2nd ed. 2nd edition. | Boca Raton : CRC Press, 2021– |: CRC Press, 2021. http://dx.doi.org/10.1201/9781003130123-7.

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Reiss, H. R., and N. Hatzilambrou. "Atomic State Effects in Stabilization." In Super-Intense Laser-Atom Physics, 213–24. Boston, MA: Springer US, 1993. http://dx.doi.org/10.1007/978-1-4615-7963-2_18.

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Véniard, V., A. Maquet, and T. Ménis. "Stabilization Within a Classical Context." In Super-Intense Laser-Atom Physics, 225–32. Boston, MA: Springer US, 1993. http://dx.doi.org/10.1007/978-1-4615-7963-2_19.

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Conference papers on the topic "Laser stabilization"

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Balakshy, Vladimir I., and Alexandre V. Kazaryan. "Laser beam parameter stabilization." In 6th International Conference on Industrial Lasers and Laser Applications '98, edited by Vladislav Y. Panchenko and Vladimir S. Golubev. SPIE, 1999. http://dx.doi.org/10.1117/12.337489.

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Wishon, Michael Joe, Daeyoung Choi, Tobias Niebur, Nathan Webster, Yanne K. Chembo, Evgeny A. Viktorov, David Citrin, and Alexandre Locquet. "External-cavity based optoelectronic oscillator stabilization (Conference Presentation)." In Semiconductor Lasers and Laser Dynamics, edited by Krassimir Panajotov, Marc Sciamanna, and Rainer Michalzik. SPIE, 2018. http://dx.doi.org/10.1117/12.2306088.

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Medina Pardell, Judith, Ramon Herrero Simon, Muriel Botey Cumella, and Kestutis Staliunas. "Spatiotemporal stabilization of PT-symmetric BAS lasers." In Semiconductor Lasers and Laser Dynamics IX, edited by Krassimir Panajotov, Marc Sciamanna, Rainer Michalzik, and Sven Höfling. SPIE, 2020. http://dx.doi.org/10.1117/12.2556807.

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Sun, Ke-Xun, Patrick Lu, and Robert Byer. "Laser Stabilization Using Diffractive Grating Angular Sensors." In Laser Science. Washington, D.C.: OSA, 2007. http://dx.doi.org/10.1364/ls.2007.lmb2.

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Harter, D. J., Y. B. Band, H. Samelson, and E. P. Ippen. "Stabilization and Passive Mode Locking of CW Alexandrite Lasers." In Instabilities and Dynamics of Lasers and Nonlinear Optical Systems. Washington, D.C.: Optica Publishing Group, 1985. http://dx.doi.org/10.1364/idlnos.1985.fc3.

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Alexandrite is a solid state laser material which lases in the range of 700-800 nm. Alexandrite has been lased continuously by pumping with a krypton ion laser1 and by pumping with xenon and mercury arc lamps2. When alexandrite is pumped with the krypton ion laser, the output is very stable and, when the pump source is removed, the output damps through population oscillations which can be well described by rate equations3. However, when alexandrite is pumped by the xenon or mercury arc lamps, the output is very noisy at certain pumping levels. Experimental data showing this noisy operation will be presented and sources of this noise will be discussed.
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Lee, Sungman, and Lloyd W. Hillman. "Frequency stabilization and control of laser diodes." In OSA Annual Meeting. Washington, D.C.: Optica Publishing Group, 1993. http://dx.doi.org/10.1364/oam.1993.tua.3.

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We have demonstrated wavelength tuning of diode lasers using precise temperature control. We have then stabilized the FM noise fluctuations of these lasers by using feedback control of the injection current. With these lasers and by using the saturation spectroscopy, we have resolved the Rb-D2 hyperfine absorption lines. We are using the hyperfine lines as frequency standard for stabilizing the laser. This work includes a comprehensive study of the Zeeman effect in Rb.
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Klee, Anthony, Kristina Bagnell, and Peter J. Delfyett. "Coupled Opto-Electronic Oscillator with Three-Point Stabilization." In Laser Science. Washington, D.C.: OSA, 2015. http://dx.doi.org/10.1364/ls.2015.lth4d.2.

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Pan, Ci-Ling. "Zeeman laser-based active laser interferometer." In OSA Annual Meeting. Washington, D.C.: Optica Publishing Group, 1988. http://dx.doi.org/10.1364/oam.1988.mgg3.

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Wavelength tunable laser diodes have recently been used for interferometric fringe stabilization and displacement measurement in the so-called active laser interferometers.1 The basic idea is to compensate for any changes in the interference signal by tuning the frequency of the laser. A frequency- and amplitude-stabilized Zeeman He–Ne laser2 is used instead in this work. Utilizing the extreme narrow linewidth (<1 MHz) of the laser, we have demonstrated that subnanometer resolution in the measurement of the displacement of a piezoelectric transducer is possible. While the single-mode tuning range of the laser is only ~300 MHz, displacement measurements over many wavelengths can be realized by adjusting the optical path length difference of the two arms of the Michelson interferometer. Interferometric fringe stabilization has also been realized with a stabilization factor of more than 2 orders of magnitude.
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Acef, Ouali, Olivier Jeannin, Pierre Prat, Eric Plagnol, Jacques Berthon, Oscar Turazza, Hubert Halloin, et al. "Molecular laser stabilization for LISA." In International Conference on Space Optics 2008, edited by Josiane Costeraste, Errico Armandillo, and Nikos Karafolas. SPIE, 2017. http://dx.doi.org/10.1117/12.2308256.

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Plewinski, Pawel, Dariusz Makowski, Aleksander Mielczarek, and Andrzej Napieralski. "Closed-loop laser stabilization system." In 2016 MIXDES - 23rd International Conference "Mixed Design of Integrated Circuits and Systems". IEEE, 2016. http://dx.doi.org/10.1109/mixdes.2016.7529705.

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Reports on the topic "Laser stabilization"

1

Koch, Tad H. Chemical Stabilization of Laser Dyes. Fort Belvoir, VA: Defense Technical Information Center, April 1990. http://dx.doi.org/10.21236/ada224219.

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2

Kielpinski, Dave, and Erik Streed. Laser Stabilization for Doppler Lidar of the Ionosphere. Fort Belvoir, VA: Defense Technical Information Center, February 2011. http://dx.doi.org/10.21236/ada536872.

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3

Venus, George, Vadim Smirnov, Leonid Glebov, and Manoj Kanskar. Spectral Stabilization of Laser Diodes by External Bragg Resonator. Fort Belvoir, VA: Defense Technical Information Center, January 2004. http://dx.doi.org/10.21236/ada452556.

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4

Barry, Matthew. Evaluation of Laser Stabilization and Imaging Systems for LCLS-II. Office of Scientific and Technical Information (OSTI), August 2015. http://dx.doi.org/10.2172/1212281.

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5

Barry, Matthew. Evaluation of Laser Stabilization and Imaging Systems for LCLS-II - Final Paper. Office of Scientific and Technical Information (OSTI), August 2015. http://dx.doi.org/10.2172/1212279.

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6

Barry, Matthew. Evaluation of Laser Stabilization and Imaging Systems for LCLS-II - Oral Presentation. Office of Scientific and Technical Information (OSTI), August 2015. http://dx.doi.org/10.2172/1212282.

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7

Vivek Khanna. LASER STABILIZATION FOR NEAR ZERO NO{sub x} GAS TURBINE COMBUSTION SYSTEMS. Office of Scientific and Technical Information (OSTI), September 2002. http://dx.doi.org/10.2172/825743.

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8

Delfyett, Peter J., and Jr. Stabilization of the Absolute Frequency and Phase of a Compact, Low Jitter Modelocked Semiconductor Diode Laser. Fort Belvoir, VA: Defense Technical Information Center, March 2005. http://dx.doi.org/10.21236/ada432366.

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9

Behnood, Ali, and Jan Olek. Development of Subgrade Stabilization and Slab Undersealing Solutions for PCC Pavements Restoration and Repairs. Purdue University, 2020. http://dx.doi.org/10.5703/1288284317128.

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The loss of functionality and the development of distress in concrete pavements is often attributable to the poor subbase and subgrade conditions and/or loss of support due to the development of the voids underneath the slab. Subgrade soil stabilization can be used as an effective approach to restore the functionality of the subgrades in patching projects. This research had two main objectives: (1) identifying the best practices for soil stabilization of the existing subgrade during pavement patching operations and (2) identifying and developing new, modified grouting materials for slab stabilization and undersealing. Various stabilization scenarios were tested and showed improved performance of the subgrade layer. The use of geotextile along with aggregate course was found to significantly reduce the settlement. Non-removable flowable fill was also found to significantly reduce the subgrade settlement. Cement-treated aggregate and lean concrete provided the best performance, as they prevented formation of any noticeable settlement in the underlying subgrade.
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Gorte, Raymond. Cost-effective Stabilization of Nanostructured Cathodes by Atomic Layer Deposition (ALD). Office of Scientific and Technical Information (OSTI), February 2020. http://dx.doi.org/10.2172/1600013.

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