Dissertations / Theses on the topic 'Sagnac interferometer'
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McConnell, Sean R. "Gas detection by use of Sagnac interferometer." Thesis, Queensland University of Technology, 2008. https://eprints.qut.edu.au/16701/1/Sean_McConnell_Thesis.pdf.
Full textMcConnell, Sean R. "Gas detection by use of Sagnac interferometer." Queensland University of Technology, 2008. http://eprints.qut.edu.au/16701/.
Full textSchubert, Christian [Verfasser]. "Grossflächiges Sagnac Interferometer mit kalten Atomen / Christian Schubert." Hannover : Technische Informationsbibliothek und Universitätsbibliothek Hannover (TIB), 2012. http://d-nb.info/1024389138/34.
Full textKaufer, Henning [Verfasser]. "Opto-mechanics in a Michelson-Sagnac interferometer / Henning Kaufer." Hannover : Technische Informationsbibliothek und Universitätsbibliothek Hannover (TIB), 2014. http://d-nb.info/1051038162/34.
Full textDutta, Indranil. "Stability improvement of a sagnac cold atom interferometer : towards continuous operation." Thesis, Paris 6, 2015. http://www.theses.fr/2015PA066572/document.
Full textThis thesis aims at pushing the performances of a cold atom interferometer principally sensitive to rates of rotation in a particular axis. In our experiment, Cesium atoms are laser cooled, trapped and launched in a fountain configuration. According to the Sagnac effect, the sensitivity of the interferometer to rotation is proportional to the area enclosed by the interferometer arms. We use stimulated Raman transitions to split the atoms in two paths and to form a folded Mach-Zehnder-like interferometer architecture using four Raman pulses. With an interrogation time of the atoms of 800 ms, we achieve a Sagnac area as high as 11 cm^2. The thesis describes the improvements to the experimental setup to operate the gyroscope with such a high Sagnac area. A procedure for the relative alignment of the Raman beams at the microrad level is presented, which is critical to meet the interference condition of the cold atoms at the interferometer output. The characterization and mitigation of the vibration noise, affecting the gyroscope, is also demonstrated. We finally demonstrate a short term rotation stability of 160 nrad/s at 1 s and a long term stability of 1.8 nrad/s after 10 000 s of integration time. This stability level represents a factor 5 improvement compared to the previous SYRTE gyroscope experiment of 2009 and a factor 15 compared to other published results. The thesis work also presents a new method of interrogation to operate the gyroscope without dead times, which is important for various applications of cold atom sensors in inertial navigation, geophysics and in fundamental physics
Schreiber, Michael Stuart. "ADVANCES IN THE OPTO-MECHANICAL DESIGN AND ALIGNMENT OF THE HEHSI IMAGING SPECTROMETER BASED ON A SAGNAC INTERFEROMETER." Master's thesis, University of Central Florida, 2005. http://digital.library.ucf.edu/cdm/ref/collection/ETD/id/2463.
Full textM.S.M.E.
Department of Mechanical, Materials and Aerospace Engineering;
Engineering and Computer Science
Mechanical Engineering
Altorio, Matteo. "Novel atom interferometry techniques for a cold-atom gyroscope of large Sagnac area Atom interferometry with top-hat laser beams Improving the phase response of an atom interferometer by means of temporal pulse shaping." Thesis, Sorbonne université, 2019. http://www.theses.fr/2019SORUS449.
Full textThis thesis describes the implementation of new atom interferometry techniques to improve the stability and accuracy of a cold-atom gyroscope located at the SYRTE laboratory. Stimulated Raman transitions are used to split and recombine the atomic waves. A sequence of four light pulses generates an interferometer with a Sagnac area of 11 cm2. I present the implementation of an interleaved interrogation scheme, where three atomic clouds are interrogated simultaneously in an atom interferometer featuring a sampling rate of 3.75 Hz and an interrogation time of 801 ms. With this scheme we demonstrate a short-term sensitivity of 30 nrad·s-1·Hz-1/2. We then present measurements of dynamic rotation rates in a so far unexplored range for a cold atom sensor. An important bias of the sensor originates from a coupling between a relative misalignment of the mirrors which retro-reflect the Raman beams and the trajectory of the atom. A technique is introduced to reduce this bias at the level of 3 nrad·s-1 and to achieve a long-term stability of 0.3 nrad·s-1 which represents the state of the art for atomic gyroscopes. The manuscript then describes the first characterization of the scale factor of the gyroscope using different techniques. In particular, the implementation of a rotation stage below the sensor enables us to vary the projection of the Erath rotation rate vector onto the interferometer area and therefore to modulate the rotation phase shift. The implementation of the techniques presented in this thesis pave paving the way to a test of the Sagnac effect for matter waves with a relative accuracy level below 100 parts per million
Secmen, Basak. "Simulation On Interferometric Fiber Optic Gyroscope With Amplified Optical Feedback." Master's thesis, METU, 2003. http://etd.lib.metu.edu.tr/upload/1253657/index.pdf.
Full texts position. Main problem in navigation is how to determine position and rotation in three dimensions. If position and rotation is determined, navigation will also be determined with respect to their initial point. There is a technology that vehicle velocity can be discovered, but a technology that rotation can be discovered is needed. Sensor which sense rotation is called gyroscope. If this instrument consists of optical and solid state material, it&rsquo
s defined by Fiber Optic Gyroscope (FOG). There are various studies in order to increase the sensitivity of fiber optic gyroscopes, which is an excellent vehicle for sensing rotation. One of them is interferometric fiber optic gyroscope with amplified optical feedback (FE_FOG). In this system, a feedback loop, which sent the output pulse through the input again, is used. The total output is the summation of each interference and it is in pulse state. The peak position of the output pulse is shifted when rotation occurs. Analyzing this shift, the rotation angle can be determined. In this study, fiber optic gyroscopes, their components and performance characteristics were reviewed. The simulation code was developed by VPIsystems and I used VPItransmissionMakerTM software in this work. The results getting from both rotation and nonrotation cases were analyzed to determine the rotation angle and sensitivity of the gyroscope.
PLAZAS, ORTEGA Lucero. "Compressão de ruído quântico em um interferômetro Sagnac em fibra com laser pulsado em 1,55 microns." Universidade Federal de Pernambuco, 2015. https://repositorio.ufpe.br/handle/123456789/18323.
Full textMade available in DSpace on 2017-02-15T13:05:07Z (GMT). No. of bitstreams: 2 license_rdf: 1232 bytes, checksum: 66e71c371cc565284e70f40736c94386 (MD5) Compressão de Ruído Quantico em um Interferometro Sagnac em Fibra com um Laser Pulsado em 1,55 Microns - Dissertação de Mestrado em Física - Lucero Plazas Ortega.pdf: 7191693 bytes, checksum: 4eba611a9cee045f7f06747bb63a80cb (MD5) Previous issue date: 2015-02-24
CAPES
Componentesemquadraturadocampoeletromagn´eticoobedecemaoprincipio de incerteza de Heisenberg. Como resultado a Mecˆanica Quˆantica prevˆe que estas componentes n˜ao podem ser especificadas simultaneamente com precis˜ao ilimitada. Estados de incerteza m´ınima (estados coerentes) permitem atingir o menor produto das incertezas em cada quadratura, ambas de mesma magnitude. Al´em disto ´e poss´ıvel construir estados quˆanticos comprimidos, para os quais uma das suas quadraturas atinge um valor menor para o desvio padr˜ao queaqueledefinidoparaumestadodem´ınimaincerteza,incrementandoconsequentemente a incerteza na outra quadratura. Nesta disserta¸c˜ao fazemos uma revis˜ao destes conceitos e apresentamos um esquema experimental com o qual geramosestadoscomprimidos(squeezedstates)daradia¸c˜ao. Este´ebaseadoem umlaserdefibrapulsado(comprimentodeondaλ = 1.56µm, taxaderepeti¸c˜ao fR = 146MHz, largura de pulso τp = 200fs) associado a um interferˆometro de Sagnac n˜ao linear em fibra. Al´em de uma descri¸c˜ao dos principais componentes ´opticos ser˜ao discutidos os mecanismos de gera¸c˜ao e caracteriza¸c˜ao dos estados comprimidos.
QuadraturecomponentsofthefieldobeyaHeisenberguncertaintyrelation. As a result, quantum mechanics predicts that these components cannot be specified simultaneously with unlimited accuracy. Minimum uncertainty states or coherent states, allow reaching the lowest value of the uncertainty in each quadrature component, both having the same magnitude. It is still possible to construct squeezed quantum states, for which, one of its quadrature components achieves a less value for standard deviation than one that have a state of minimum uncertainty, with the consequence of an increase in the uncertainty of the other quadrature. In this dissertation, these concepts are reviewed and we provide an experimental scheme in order to generate squeezed states of light. This design is based on a pulsed fiber laser (λ = 1.56µm, repetition rate fR = 146MHz, pulse width τp = 200fs) coupled with a nonlinear interferometer, which is composed by a fiber loop in a Sagnac configuration. In order to discuss the experimental results obtained with this scheme, will be carried out adescriptionofthemainopticalcomponents,takingintoaccounttheprincipal mechanisms of generating and measuring of squeezed states.
Shaddock, Daniel Anthony, and Daniel Shaddock@jpl nasa gov. "Advanced Interferometry for Gravitational Wave Detection." The Australian National University. Faculty of Science, 2001. http://thesis.anu.edu.au./public/adt-ANU20020227.171850.
Full textKurth, Martin Lyndon. "Scattering of guided waves in thick gratings at extreme angles." Thesis, Queensland University of Technology, 2006. https://eprints.qut.edu.au/16347/1/Martin_Kurth_Thesis.pdf.
Full textKurth, Martin Lyndon. "Scattering of guided waves in thick gratings at extreme angles." Queensland University of Technology, 2006. http://eprints.qut.edu.au/16347/.
Full textYan, Wenhua. "Design of a magnetic guide for rotation sensing by on chip atom interferometry." Thesis, Paris 6, 2014. http://www.theses.fr/2014PA066548.
Full textThis manuscript present the design and realization of an experimental setup for the development of a cold atom interferometer using 87Rb atoms guided on an atom chip, the final goal being the realization of an inertial sensor for rotation measurements. We have therefore study theoretically the magnetic confinement of these atoms in a circular guide. Such a study allowed us to identify the main challenges linked to the atomic wave packet propagation along a stable circular orbit in a magnetic guide, namely: the roughness of the guiding potential, the magnetic potential defects associated to the pattern of the micro wires used to produce this potential, and the Majorana losses. In this thesis we propose original solutions to these questions based on preliminary studies and on the results of our calculations. From the experimental point of view, we have assembled a new cold atom experiment with the main feature of being compact and therefore transportable for in situ measurement of rotations. We have along this work put together an efficient ultra high vacuum system, developed a compact optical bench containing the laser sources for cooling and trapping, a Bragg laser for the atom interferometer, as well as all the needed electronics to control the experiment
Ferreira, Vinícius Castro. "Espectroscopia ótica não linear em anel antirressonante." reponame:Biblioteca Digital de Teses e Dissertações da UFRGS, 2016. http://hdl.handle.net/10183/150054.
Full textAn introduction to nonlinear optics will be addressed in this work, presenting results of optical characterization to many different materials as well as results from a new characterization technique. Basic aspects to nonlinear index refraction measurement will be presented through Z-scan, which is a well-established method. This technique is not efficient for thin films or samples presenting low nonlinearity. Using a interferometric setup is possible to produce an increase in sensibility, attenuanting local oscillator without degrading the generated nonlinear signal, what establishes a better signal-noise relation.
Queiroz, Alex Sander Barros. "Estudo do desempenho de componentes baseados em fibras Ãpticas especiais: fibras de cristal fotÃnico e de metamateriais e suas aplicaÃÃes em comunicaÃÃes." Universidade Federal do CearÃ, 2015. http://www.teses.ufc.br/tde_busca/arquivo.php?codArquivo=15842.
Full textNeste trabalho foi realizado um estudo numÃrico do interferÃmetro de Sagnac baseado em cristais fotÃnicos e de acoplador Ãptico de metamaterial. Na simulaÃÃo do interferÃmetro foram analisados os efeitos da propagaÃÃo da luz, considerando-se a dispersÃo de velocidade de grupo (GVD) e de terceira ordem (TOD), espalhamento Raman intrapulso, auto-inclinaÃÃo (Self-steepening) e auto-modulaÃÃo de fase na equaÃÃo nÃo linear de SchrÃdinger generalizada. No primeiro momento foi realizado o estudo para quatro fatores de razÃo de divisÃo da potÃncia incidente em uma das portas do dispositivo e trÃs dimensÃes para o comprimento do anel do dispositivo. Para caracterizar o desempenho do sistema, foram analisadas as curvas de transmissÃo, taxa de extinÃÃo, crosstalk e fator de compressÃo do pulso transmitido. No segundo momento, foi verificada a performance do chaveamento nÃo-linear para obtenÃÃo de porta lÃgica sob ModulaÃÃo por Amplitude de Pulsos (PAM). Excitando-se as duas portas de entrada do dispositivo com nÃveis lÃgicos "0" e "1", observando o seu comportamento em uma das saÃdas do dispositivo. Inicialmente, variou-se o parÃmetro de ajuste da modulaÃÃo (|ε|), obtendo-se apenas a porta lÃgica OR. E, em uma segunda aplicaÃÃo, manteve-se o parÃmetro da modulaÃÃo fixa e variou-se a fase de uma das portas de entrada, de 0 a 2π rad, encontrando-se portas lÃgicas do tipo OR, AND e XOR. TambÃm foram estudadas as caracterÃsticas de um guia metamaterial que possui a parte real da permissividade elÃtrica e da permeabilidade magnÃtica negativas. Esse guia metamaterial à acoplado com um guia convencional, observando-se as caracterÃsticas de transmissÃo e potÃncia crÃtica desse tipo de acoplador e, comparando-se com um acoplador convencional. Para essa anÃlise foi utilizado um perfil de automodulaÃÃo decrescente linearmente com cinco valores mÃnimo, observando-se um comportamento de histerese.
In this paper we present a numerical study of the Sagnac interferometer based on photonic crystals and optical coupler metamaterial. In the simulation of the interferometer effects of light propagation were analyzed, considering the dispersion of the group velocity (GVD) and third order (TOD), intrapulse Raman scattering, self-slope (self-steepening) and self-modulation phase in the generalized non-linear SchrÃdinger equation. The first time the study was conducted for four power division ratio of factors incident in one of the device ports and three dimensions for the device ring length. To characterize the system performance, were analyzed the transmission curves, extinction ratio, crosstalk and compression factor of the transmitted pulse. In the second moment, the performance of the non-linear switching was observed for obtaining gate under Pulse Amplitude Modulation (PAM). Exciting the two device input ports with logical levels "0" and "1", observing their behavior in one of the device outputs. Initially, the modulation is varied adjustment parameter (| ε |), obtaining only the logical OR gate. And in a second application, the fixed modulation parameter remained and was varied the phase of the input ports 0 to 2π rad, lying type logic gate OR, AND and XOR. The characteristics of a metamaterial guide that has the real part of electrical permittivity and magnetic permeability negatives were also studied. This metamaterial guide is coupled to a conventional guide, observing the transmission characteristics and critical power of this type of coupler and compared with a conventional coupler. For this analysis we used a decreasing automodulation profile linearly with five minimum, observing a hysteresis behavior.
Noble, Adam. "Sagnac interferometry and fundamental physics." Thesis, Lancaster University, 2006. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.441781.
Full textKajari, Endre [Verfasser]. "Perspectives on Relativistic Sagnac Interferometry / Endre Kajari." München : Verlag Dr. Hut, 2011. http://d-nb.info/1018981160/34.
Full textBogdanski, Jan. "Experimental multiuser secure quantum communications." Doctoral thesis, Stockholms universitet, Fysikum, 2009. http://urn.kb.se/resolve?urn=urn:nbn:se:su:diva-26498.
Full textYu, Aihua. "Application of optical fibre Sagnac interferometers in optical modulators and sensors." Thesis, University of Essex, 1993. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.332807.
Full textHarvey, David. "Automatically phase-locked fibre optic electronic speckle pattern interferometry using laser vibrometry." Thesis, Heriot-Watt University, 1996. http://hdl.handle.net/10399/715.
Full textXia, Jing. "Optical studies of broken time-reversal symmetry in solids using Sagnac interferometry /." May be available electronically:, 2008. http://proquest.umi.com/login?COPT=REJTPTU1MTUmSU5UPTAmVkVSPTI=&clientId=12498.
Full textSkalský, Michal. "Snímač úhlové rychlosti se Sagnacovým interferometrem." Master's thesis, Vysoké učení technické v Brně. Fakulta elektrotechniky a komunikačních technologií, 2016. http://www.nusl.cz/ntk/nusl-240886.
Full textPiani, Goffredo. "Sull'interferenza quantistica indotta dal potenziale gravitazionale." Bachelor's thesis, Alma Mater Studiorum - Università di Bologna, 2019. http://amslaurea.unibo.it/19167/.
Full textSavoie, Denis. "Fonctionnements continu et entrelacé d'un gyromètre à atomes froids et amélioration de sa stabilité." Thesis, Paris 6, 2017. http://www.theses.fr/2017PA066585/document.
Full textSagnac atomic gyroscopes have great potential due to their high sensitivity to rotation. The SYRTE atomic gyroscope uses laser cooled cesium atoms. Thank to stimulated Raman transitions, we form a folded Mach-Zehnder type interferometer. The instrument allows interrogation times up to 800~ms, which corresponds to a 11~cm$^2$ Sagnac area, the largest demonstrated for atom interferometers. This is a major step toward the use of such instruments in inertial navigation. I describe the methods implemented to push the short-term sensitivity and performed the first detailed study of systematics, such as those linked to light-shifts due to the preparation and the detection of the atoms and those linked to misalignment of parallelism of the mirrors and of the trajectories of the atoms. I demonstrated a short-term stability of 30~nrad.s$^{-1}$.Hz$^{-1/2}$ in triple interleaved joint interrogation which improves the state of the art by a factor 3. The state of the art has also been improved by a factor 5 in long-term with a 0,2~nrad.s$^{-1}$ stability in 30~000~s
Cheng, Bi-Chang, and 鄭必章. "The Novel Sagnac Interferometer for Designing Hydrophones." Thesis, 2004. http://ndltd.ncl.edu.tw/handle/75144243275733520673.
Full text國立中山大學
電機工程學系研究所
92
The main purpose of the optical fiber sensing technology is to detect perturbation of physical fields. By means of some demodulating scheme, we can extract the real signal from those light beams which modified by physical fields. In the thesis, we proposed a configuration of modified Sagnac Interferometer as a sensing system. The optical sensing and demodulation system are exploited separately. Next, we study the advantages and disadvantages of the configuration. Besides, we are also measured the sensitivity and dynamic range. The sensing system used a low coherence light source to reduce cost. This system also improves the shortage of a Sagnac Interferometer which has a blind point in the middle position. In addition, the structure is easily implemented and can detect weak signal in a high noisy water environment. For matching the main structure, we make many kinds of sensing heads for detecting signals under water. We also use the mathematical model as the base of the theory. The dynamic range is 40 dB and the sensitivity is -231.47 dB re V/uPa.
Ramana, Sree M. "New applications of geometric phase in optics using Sagnac interferometer." Thesis, 2003. http://hdl.handle.net/2009/1038.
Full textChan, Hsin-Han, and 詹昕翰. "Study of Fiber Pulse Laser Using Sagnac Interferometer With PZT." Thesis, 2018. http://ndltd.ncl.edu.tw/handle/7uv682.
Full text國立清華大學
光電工程研究所
106
In this paper, we incorporate a Sagnac interferometer and a PZT in a fiber-optic linear-type laser cavity. We use the Sagnac interferometer and the PZT to generate periodic cavity loss and active mode-locking, and then generate pulses. We modify the length of the Sagnac interferometer to adjust the period of the optical pulse train, in generating optical pulses of several hundred nanoseconds in width. We then compare the influence of the square wave signal and the sine wave signal given by the signal generator on the light pulse. Finally, a discussion on the influence of the environment, which includes the sound, temperature and vibration, on pulse generation is given.
LU, TING-CHIA, and 呂庭嘉. "WDM Optical Fiber Acoustic Sensor Array Based on Sagnac Interferometer." Thesis, 2019. http://ndltd.ncl.edu.tw/handle/3bf54h.
Full text國立高雄科技大學
電子工程系
107
In this thesis, the optical fiber Sagnac interferometer was used to design an optical fiber acoustic sensor and a sensor array system. The signal-channel and multi-channel acoustic sensors were investigated. In the signal-channel fiber Sagnac interferometer system, the influences of different light sources and length of delay fiber on the acoustic sensor were investigated. The wideband light source, which was filtered through an optical multiplexer, can be used in the fiber Sagnac acoustic sensor. The optimal length of delay fiber was about 4km to 6km. Using the 2×2 optical coupler, the fiber Sagnac acoustic sensor had a frequency response range from 1.2 kHz to 8.1 kHz, a sensitivity of -69.37 dBV/μbar, and a signal-to-noise ratio (SNR) of 50 dB. Using the 3×3 optical coupler, the fiber Sagnac acoustic sensor had a frequency response range from 1.1 kHz to 20.5 kHz, a sensitivity of -10.38 dBV/μbar, and an SNR of 60 dB. In the multi-channel fiber Sagnac interferometer, the optical multiplexers were inserted in the fiber loop and at the signal output ends to realize an eight-channel fiber acoustic sensor array system. There were four channels to implement the acoustic wave detection. For the four channels, the frequency response range all is from 1.2 kHz to 20 kHz; the sensitivity is from -137.46 to -154.28 dBV/μbar; and the SNR is from 25 to 33 dB. Using the same acoustic source, the interval between the sensor heads can be estimated.
Chen, Han-Yang, and 陳漢揚. "The Promotion of the Performance Based on Dual Sagnac Interferometer Hydrophones." Thesis, 2006. http://ndltd.ncl.edu.tw/handle/67131211720183324454.
Full text國立中山大學
電機工程學系研究所
94
An interferometer is used for phase detection. Thus, the hydrophone which is based on interferometric optic fiber sensor has extremely high sensitivity. Sagnac interferometric hydrophone has low noise of marine environment, which is more suitably used to detect underwater acoustic signal than that of a Mach-Zehnder interferometer. In this paper, a configuration of dual Sagnac interferometer was proposed. The mathematical model was derived and analyzed. The fiber optic sensor head contains mandrel type and planar one. The acoustic window are made of silicon rubbers. It was should that we can increase their sensitivities by increase number of wrapping fiber coils. In our experiment, the result shows that among all the mandrel sensor heads, the most highest dynamic range is up to 37.6±1.4 dB, and its sensitivity is -223.3±1.7 dB re V/1µPa ; while the dynamic range of the planar sensor head is 42.1±1.5 dB, and its sensitivity is -213.8±1.3 dB re V/1µPa。 As for the configuration of the optical interferometers, the intensity of the dual Sagnac interferometer is 20 dB larger than its Sagnac counterpart. Its dynamic range is above 66 dB, which is 24 dB larger than that of the Sagnac interferometer with the sensitivity of -192.0 dB re V/1µPa. In addition, by using software simulation to design optimal lengths of delay fibers , we can increase interferometer’s the dynamic range of underwater acoustic detection. This paper verify that, by means of adjusting the length of these two delay fibers, we can actually increase the dynamic range of acoustic signal detection.
Smith, Devin Hugh. "An Ultrafast Source of Polarization Entangled Photon Pairs based on a Sagnac Interferometer." Thesis, 2009. http://hdl.handle.net/10012/4259.
Full textJhuang, Tian-yi, and 莊田易. "The study of Fresnel lens in twisted-nematic liquid crystal fabricated by Sagnac interferometer." Thesis, 2017. http://ndltd.ncl.edu.tw/handle/32qyse.
Full text國立中山大學
物理學系研究所
105
This study presents a focusing efficiency and focal length tunable Fresnel lens with liquid crystals fabricated by a Sagnac interferometer. When the Fresnel-pattern green beam, formed by the Sagnac interferometer, is irradiated on the azo-dye doped liquid-crystal mixture, the azo-dye molecules will undergo the trans-cis photoisomerization and then generate photo-alignment effect in the bright (odd) zone, which results that the direction of liquid-crystal molecules will perpendicular to the linearly polarized pump beam. The various structures of liquid crystals in the odd and even zones will produce the phase difference, resulting in a Fresnel lens generated. The focusing efficiency of proposed Fresnel lens can be controlled by the external AC voltages. The experimental results show that the focusing efficiency can reach its maximum of 31.5 % under applied voltage of 3.1 V. In addition, the photo-alignment effect of azo dyes can be erased through the thermally method and rewritten by the pump beam with different Fresnel-like pattern, which leads to the Fresnel lens with various focal lengths.
Mathew, Reuble. "Creating and Imaging Surface Acoustic Waves on GaAs." Thesis, 2009. http://hdl.handle.net/1974/5351.
Full textThesis (Master, Physics, Engineering Physics and Astronomy) -- Queen's University, 2009-12-08 12:28:35.962
Lin, Chia-Ju, and 林佳儒. "Study on Photo-annealing Effect of Super-fluorescent Fiber Source and Its Application in Sagnac Interferometer." Thesis, 2015. http://ndltd.ncl.edu.tw/handle/d3y9v4.
Full text國立臺灣科技大學
電子工程系
103
In this thesis, the characteristics of super-fluorescent fiber source (SFS), the recovery of photo-annealing effect and the application of fiber optic gyroscope (FOG) were discussed. The main scheme used here was a double-pass backward SFS (DPB-SFS) based on a broadband fiber Bragg grating (BFBG), which is temperature-compensated by carbon fiber reinforced plastic (CFRP). First, two types of Erbium-doped fiber (EDF), HG980 B1 and AG980H, in different lengths were used in the DPB-SFS. The properties of DPB-SFS using both types of EDFs were studied in their output power, mean-wavelength and 3 dB bandwidth. The best output power, mean-wavelength and 3 dB bandwidth were 10.65 dBm, 1549.3 nm and 16.92 nm, respectively, using 5 m EDF (HG980 B1). Then, we discussed the photo-annealing effect. The EDFs were exposed in 60Co gamma-radiation with a total dose of 200 krad. Because the molecular bonding of EDF would be damaged by the radiation, a 637 nm red light laser was used to recovery the radiation-induced loss. The properties of radiation-induced loss and recovery were characterized by measuring the absorption spectra of EDFs which were pumped by a 980 nm broadband light source. Results showed that both types of EDF could be photo-annealed by the 637 nm red light laser. The AG980H EDF suffered greater loss than the other, but the loss could be healed up to 12.71 dB after photo-annealed. After that, the thermal and real-time radiation stabilities of DPB-SFS were discussed. In this part, we discussed the thermal stability by using 5 m EDF (HG980B1) and the temperature ranging from 0 to 70 oC. The measured variation of output power, mean-wavelength and 3 dB bandwidth were 0.12 dB, 2 ppm/oC and 2.2 %, respectively. To verify real-time radiation stability, a 5 m HG980B1 EDF was set in the radiation chamber for 4.55-hour 60Co gamma-radiation exposure with a total dose of 200 krad. Again, a 637 nm red light laser was used to the DPB-SFS for in-time recovery of radiation-induced loss. The measured variation of output power, mean-wavelength and 3 dB bandwidth were 1.31 dB, 178.67 ppm and 0.7 %, respectively. Finally, for the investigation of Sagnac interferometer, the horizontal sensing based on Sagnac effect was introduced, and the DPB-SFS with 5 m HG980B1 EDF was used as sensing light source. Three interferometer schemes based on 2x2 fiber couplers in different lengths of EDF (3 m, 4 m and 5m) were investigated. The results showed that the variation of output power was periodic up and down in cosine function when the rotation angles varys from 0o to 90o both on clockwise and counter-clockwise direction. Taking 5 m interferometer for example; the slope on linear region is 0.05 mW power per rotation angle.
黃渝瑄. "The study of multiwavelength fiber laser incorporating dual-pass in-line Sagnac interferometer and nonlinear polarization rotation effect." Thesis, 2010. http://ndltd.ncl.edu.tw/handle/63468848428143981042.
Full text高雄師範大學
光電與通訊工程學系
98
We present a multiwavelength fiber laser using nonlinear polarization rotation effect to suppress mode competition from the erbium doped fiber. The proposed new type of comb filter used in the multiwavelength fiber laser can produce more available and continuous operation wavelengths with better performances of FSR, SNR and linewidth. The fiber laser substitute dual pass in-line Sagnac interferometer for single pass in-line Sagnac interferometer . We use this new type of dual pass comb filters in our proposed fiber laser to successfully increase the SNR of lasing spectrum more than 30dB. The combination of the nonlinear polarization rotation effect devices and the dual pass comb filter can share an in-line fiber polarizer so as to simply the laser structure and reduce the cost. We properly adjust the phase of nonlinear polarization rotation effect, cavity length and pumping power respectively. The phase adjusting of the nonlinear polarization rotation effect can obtain three kinds of wavelength fiber laser spectra which bandwidth are 47 nm, 41 nm and 29 nm respectively. The optima cavity length is set at 2km to achieve the better laser performances. Various pumping powers injected into the multi-wavelength fiber laser can obtain different lasing spectra. The pumping power operating at 700mW can get the 6dB bandwidth of 47nm and SNR more than 20dB. When the pumping power operates at 200mW with fixed phase of nonlinear polarization rotation, an ultra broadband of lasing spectrum with 110 wavelength-lasing peaks periodically distributed from 1564nm to 1608nm accompanied with average lasing linewidth of 0.08nm, average FSR of 0.4nm and average SNR of 37dB. To the best of our knowledge, these results are the best performances than the previous references that ever announced in the field of multiwavelength fiber laser spectra more than 110 peaks.
Shaddock, Daniel. "Advanced Interferometry for Gravitational Wave Detection." Phd thesis, 2000. http://hdl.handle.net/1885/48188.
Full textHuang, Guo-ting, and 黃國挺. "The Design and Demodulation of Fiber-optic Hydrophones Based on Dual Sagnac Interferometers." Thesis, 2004. http://ndltd.ncl.edu.tw/handle/93231720852406794834.
Full text國立中山大學
電機工程學系研究所
92
Because the acoustic wave is capable of propagating at a long-distance in water, the hydrophone plays a key role in the underwater acoustic sensing all the time. The hydrophone based on fiber optic interferometry has an extremely high sensitivity and large dynamic range. In addition, the electrically passive, immunity to electromagnetic interference, and multiplexing properties of fiber optic sensor offer great advantages over traditional piezoelectric hydrophone. Due to the complete path-balance between the two counterpropagating waves, a Sagnac interferometric configuration can employ a low-coherent light source to reduce the cost. This configuration can easily route optical paths and replace sensor heads to compare with each other. But, the sensitivity varying with frequency and the polarization-induced signal fading problem make it unsuitable for applications in need of detecting correct amplitude of signals. The Michelson interferometric configuration with Farady rotator mirror (FRM) has a constant sensitivity and solves the polarization-induced signal fading problem. But, this configuration uses a high-coherent light source and expensive FRMs, and be difficult to route. In this paper, we use the polarization-insensitive Michelson fiber optic sensor to adjust the demodulation circuits we design. In this paper, we establish the interferometric hydrophones. The fiber optic coil of the sensor head is embedded with the special materials in order to acoustic impedance matching and waterproofing. We employ phase generated carrier demodulation technology to get the acoustic signal of interest from the output of the interferometer. In our experiment, the dual Sagnac configuration has a dynamic range of 23 dB and a sensitivity of -226 dB re V/1uPa, the Michelson configuration with FRMs has a dynamic range of 25 dB and a sensitivity of -204 dB re V/1uPa.
Azodi, Aval Golnaz. "Phononic Crystal Waveguiding in GaAs." Thesis, 2013. http://hdl.handle.net/1974/8492.
Full textThesis (Master, Physics, Engineering Physics and Astronomy) -- Queen's University, 2013-11-29 15:53:46.369