Magnetophotorefractive Effect and Interference Filters in Lithium Niobate

Total Page:16

File Type:pdf, Size:1020Kb

Magnetophotorefractive Effect and Interference Filters in Lithium Niobate Risø-R-880(EN) Magnetophotorefractive Effect and Interference Filters in Lithium Niobate Carsten Dam-Hansen o- -3dB A;WIM = °-06 S -5- a (O ° " -D "i O cP • • o D a " D <u -in- • • * • • • -15" -0,20 -0,10 0,00 0,10 0,20 0,30 Wavelength detuning [Å] Risø National Laboratory, Roskilde, Denmark March 1996 ?• 7 ri 13 Magnetophotorefractive Effect and Interference Filters in Lithium Niobate Carsten Dam-Hansen Risø National Laboratory, Roskilde, Denmark March 1996 Abstract This thesis deals with the fundamental photorefractive and photo- voltaic properties of iron-doped lithium niobate crystals. Experimental observations of a strong magnetic field effect on the energy cou- pling and grating formation in a vectorial interaction scheme are presented. To the author's knowledge these are the first reported results in the field. It is shown that an enhancement of the diffraction efficiency of 60 % is possible by applying even a moderate magnetic field of 0.23 T. A new theoretical model of the magnetophotorefractive effect in the vectorial interaction scheme is presented. It describes the space-charge field formation, two- wave mixing and grating formation under the influence of an externally applied magnetic field. Good agreement with the experimental results and the first mea- surement of nondiagonal components of the magnetophotovoltaic tensor are re- ported. A theoretical model for the temperature properties of photorefractive interfer- ence filters with subangstrom bandwidths are presented and compared favourably with experimental investigations. A novel method for determining the spectral re- sponse of these filters from a combined thermal and angular response measurement is described. Front page figure: Spectral response of photorefractive interference filter with a centre wavelength at 514.5 nm written in a 10 mm long LiNbO3".Fe crystal. This thesis is submitted in partial fulfilment of the requirements for the degree of Doctor of Philosophy at the Technical University of Denmark. ISBN 87-550-2165-4 ISSN 0106-2840 Grafisk Service • Risø • 1996 Contents List of Figures Tables and Symbols 4 Preface 8 Dansk resumé 9 1 Introduction 11 2 Lithium Niobate 13 2.1 Structural and physical properties 13 2.2 Photorefractive effect 14 2.2.1 Band transport model 16 2.2.2 Linear electro-optic effect 18 2.3 Bulk photovoltaic effect 19 2.3.1 Physical origin 20 2.3.2 Phenomenological theory 22 2.4 Magnetophotovoltaic effect 24 2.4.1 Physical origin 24 2.4.2 Phenomenological theory 25 3 Magnetophotorefractive Effect 28 3.1 Vectorial interaction 31 3.1.1 Configuration and photovoltaic current 32 3.1.2 The space-charge field 34 3.1.3 Two-wave mixing 42 3.1.4 Diffraction efficiency 46 3.2 Experimental investigations 50 3.2.1 Experimental method 50 3.2.2 Experimental results 53 3.3 Discussion and perspectives 58 4 Photorefractive Interference Filters 51 4.1 Filter recording and response 63 4.2 Temperature properties 66 4.3 Experimental investigation 68 4.3.1 Experimental method 68 4.3.2 Experimental results 70 4.4 Discussion and perspectives 15 5 Conclusion 18 References 80 Appendices 85 A Physical tensors 85 B Material parameters 89 Risø-R-880(EN) List of Figures 1 Paraelectric and ferroelectric phase of LiNbC-3. 14 2 Measured absorption spectrum of LiNbC>3:Fe samples. 15 3 Light induced charge transport in LiNbO3. 16 4 Model of photovoltaic current generation. 20 5 Distribution of conduction band electrons. 21 6 Electron trajectory in a magnetic field. 24 7 Magnetophotorefractive geometries 28 8 Setup for vectorial interaction 32 9 Influence of diffusion mechanism vs. grating period. 38 10 Influence of diffusion mechanism vs. angle of incidence. 39 11 Vector diagram for spatially oscillating photovoltaic current. 40 12 Angular dependence of photovoltaic contributions. 41 13 Calculation of the perturbed space-charge field. 42 14 Exponential gain factor vs. angle of incidence. 45 15 Angular dependence of diffraction efficiency. 48 16 Magnetic field dependence of diffraction efficiency. 4$ 17 Experimental setup for vectorial interaction scheme. 50 18 Measured change in extraordinary intensity. 53 19 Measured diffraction efficiency vs. recording th\;e. 54 20 Measured diffraction efficiency vs. recording time. 56 21 Measured initial curvature of diffraction efficiency. 51 22 Geometries for filter recording. 64 23 Probing the photorefractive interference filter. 64 24 Calculated filter reflectance vs. phase mismatch. 65 25 Reflection geometry setup for filter recording. 68 26 Measured angular response of filter at different temperatures. 10 27 Measured optimal angle and center wavelength deviation. 11 28 Theoretical and measured and temperature sensitivity. 12 29 Measured temperature response of filter. 73 30 Spectral filter response. 14 List of Tables 1 Specification of LiNbC>3:Fe samples. 52 2 Sign of phase mismatch parameter. 68 3 Measured temperature sensitivities. 12 4 Characteristica of photorefractive interference filter. 14 5 Form of 4th-rank pseudo-tensor for 3m point group 81 6 Form of Sf^kl for 3m point group 88 7 Form of IS&.J for 3m point group. 88 8 Form of 5^fc for 3m point group. 89 9 Material parameters for LiNbC-3:Fe crystals. 89 List of Symbols 1 a, ao, ae intensity absorption coefficient [m" ] 0/ effective intensity absorption coefficient [m-1] Risø-R-880(EN) 1 aa, ac principal linear thermal expansion coefficients [K" ] B magnetic field [T] B modulus of magnetic field [T] P thermal excitation rate [s-1] Pijk bulk photovoltaic tensor [V"1] Ptjk>P?j linear and circular bulk photovoltaic tensor [V"1] c velocity of light [m/s] D diffusion constant's"1] 6ijk levi-cevita (symbol) tensor AT change in temperature [K] ATFWHM thermal bandwidth [K] AAFWHM spectral bandwidth [m] Afc phase or momentum mismatch [m-1] dn/dT thermo-optic coefficient [K-1] e numerical electronic charge [C] ED characteristic diffusion field [V/m] Eq characteristic saturation field [V/m] EM characteristic drift field [V/m] characteristic photovoltaic field [V/m] characteristic bulk photovoltaic field [V/m] characteristic magnetophotovoltaic field [V/m] ei • q effective photovoltaic magnetic coefficient [V"1] ec, e0 unit vector in the direction of polarization ei unit vector along grating wave vector and the space-charge field unit vector along perturbed bulk photovoltaic current unit vector along perturbed magnetophotovoltaic current E total electric field [V/m] E, Ee, Eo complex field amplitude [V/m] Eo, Ei unperturbed and perturbed space-charge field [V/m] e energy [J] es static permittivity tensor [F/m] £f!,£§3 transverse and longitudinal static permittivity [F/m] £0 vacuum permittivity [F/m] jrt recombination rate [m3s~1] -1 Fe collision frequency [s ] F exponential gain factor [m~J] 2 / , Ie, Io, Iu I2 intensity [W/m ] Io unperturbed (total) intensity [W/m2] I\ perturbed intensity [W/m2] j total current density [A/m2] jo, ji unperturbed and perturbed current density [A/m2] jpv photovoltaic current density [A/m2] JoVi Ji>V unperturbed and perturbed photovoltaic current density [A/m2] ks Boltzmann constant [JK"1] -1 k, ke, k0 wave vectors [m ] 1 k,kCtk0 modulus of wave vectors [m" ] K grating wave vector [m-1] K modulus of grating wave vector [m-1] K coupling coefficient [m-1] 2 Kpj, specific photoconductivity [mV~ ] L interaction length [m] A free space wavelength [m] Aw writing wavelength [m] Risø-R-880(EN) Ac center wavelength [m] Ag center wavelength at reference temperature [m] A grating period [m] m intensity ratio M intensity modulation coefficient m* effective mass of electron [g] fio vacuum permeability [Vs/(Am)j (i mobility of thermalised electrons [m2/(Vs)] /ZHp mobility of nonthermalised electrons [m2/(Vs)j n,no,ne average, ordinary and extraordinary refractive index nw refractive index at writing wavelength n, no, ni number density conduction band electrons [m~3] NA concentration of acceptors [m~3] ND concentration of donors [m~3] 3 N£, N£Q, N£t number density of ionized donors, [m~ ] 77 diffraction efficiency q photovoltaic magnetic coupling vector [V"1] r displacement vector [m] r& Larmor radius [m] r", r,-jfc electro-optic tensor [m/V] <Tp|, photoconductivity [fl^m"1] s photoexitation cross section^J"1] S temperature sensitivity of center wavelength [m/Kj Sijki magneto photovoltaic tensor [V~1T~1] Stjki'Suk linear and cirular magneto photovoltaic tensor [V~1T~1] t time [s] T absolute temperature [K] Tc Curie temperature [K] TQ absolute reference temperature [K] T,T' characteristic time for perturbed space-charge field [s] To characteristic time for unperturbed space-charge field [s] TJI relaxation time [s] Tjso momentum isotropisation time for nonthermalised electrons [s] r£ energy relaxation time [s] wo velocity of nonthermalised electrons [m/s] VT velocity of thermalised electrons [m/s] £ factor describing effect of diffusion and asymmetry parameter <p angle between the grating wave vector and the optical axis [rad] xp, 0, ©c, 0O internal angle of incidence [rad] •tp', Q', Q'el 0'o external angle of incidence [rad] <I> quantum efficiency -1 w0 generation rate [s ] wc cyclotron frequency [rad/s] u angular frequency [s"1] Abbreviations and indices BPV Bulk photovoltaic effect MPV Magnetophotovoltaic effect L Linear C Circular FWHM full width half maximum FOV field of view [rad] Risø-R-880(EN) o ordinary eigenwave e extraordinary eigenwave i,j,k,l,r,s,t,u tensor indices representing x,y and z or a,b and c 0 unperturbed p irameter or value at reference temperature 1 perturbed parameter a vector a unit vector <i tensor * denoting complex conjugation Risø-R-880(EN) Preface The present thesis describes the work carried out in the period from March 1993 to March 1996 at the Optics and Fluid Dynamics Department (OFD), at Risø National Laboratory in Denmark.
Recommended publications
  • Optical Data Storage in Photorefractive Materials
    OPTICAL DATASTORAGEDATA STORAGE IN PHOTOREFRACTIVE MATERIALS T. A. Rabson, F.F. K.K. TittelTittel and D. M. KimKirn Electrical EngineeringEngineering Department Rice University Houston, TexasTexas 77001 Abstract The basicbasic physicalphysical theorytheory ofof thethe photorefractivephotorefractive effecteffect willwill bebe presented.presented. Methods will be discussed forfor utilizing the effect for the storage of informationinformation as well as optical displaydisplay ofof information.information. The funda-funda- mental limitslimits on writing time,time, accessaccess timetime andand storagestorage densitydensity willwill bebe relatedrelated toto thethe physicalphysical propertiesproperties ofof the materials involved.involved. Particularly promising materials, such as LiNb03LiNbO^ will bebe discusseddiscussed inin detail.detail. Introduction The incidenceincidence of lightlight on certain ferroelectricferroelectric crystalscrystals cancan alteralter thethe indexindex ofof refractionrefraction ofof thethe crycry­ - stalstal(1). ^ ''. This physical phenomenonphenomenon isis knownknown asas thethe photorefractivephotorefractive effect.effect. Although thethe physicalphysical behaviorbehavior of this effect has been well studiedstudied thethe fundamentalfundamental photoexcitationphotoexcitat ion processprocess isis stillstill notnot wellwell understood.understood. This lacklack of understanding doesdoes notnot preventprevent thethe applicationapplication ofof thethe effecteffect toto thethe storagestorage ofof datadata inin crystalscrystals
    [Show full text]
  • Photorefractive Self-Focusing and Defocusing As an Optical Limiter
    Photorefractive self-focusing and defocusing as an optical limiter Galen C. Duree Jr. and Gregory J. Salamo University of Arkansas Physics Department Fayetteville, Arkansas 72701 Mordechai Segev and Amnon Yariv California Institute of Technology Department of Applied Phyiscs Pasadena, California 91125 Edward J. Sharp Army Research Laboratory Fort Belvoir, Virginia 22060 and Ratnakar R. Neurgankar Rockwell International Science Center Thousand Oaks, California 91360 ABSTRACT Focusing and defocusing of laser light has been observed for many years. Optical Kerr type materials exhibit this effect only for high intensities. We show experimental evidence that photorefractive materials can also produce dramatic focusing and defocusing. Whereas Kerr materials produce this effect for high intensities, photorefractive materials produce these effects independent of intensity indicating that this effect would be ideal for an optical limiter. We compare the characteristics of Kerr and photorefractive materials, discuss the physical models for both materials and present experimental evidence for photorefractive defocusing. Self-focusing and defocusing was observed for any incident polarization although the effect was more pronounced using extraordinary polarized light. In addition, self-focusing or defocusing could be observed depending on the direction of the applied electric field. When the applied field was in the same direction as the crystal spontaneous polarization, focusing was observed. When the applied field was opposite the material spontaneous polarization, the incident laser light was dramatically defocused. 192 I SPIE Vol. 2229 0-8194-1533-2194/$6.00 Downloaded From: http://proceedings.spiedigitallibrary.org/ on 10/18/2016 Terms of Use: http://spiedigitallibrary.org/ss/termsofuse.aspx INTRODUCTION One of the attractive features of laser light is that it can be focused to a very small spot.
    [Show full text]
  • Photorefractive Effect in Linbo 3
    Photorefractive effect in LiNbO 3 -based integrated-optical circuits for continuous variable experiments François Mondain, Floriane Brunel, Xin Hua, Elie Gouzien, Alessandro Zavatta, Tommaso Lunghi, Florent Doutre, Marc de Micheli, Sébastien Tanzilli, Virginia d’Auria To cite this version: François Mondain, Floriane Brunel, Xin Hua, Elie Gouzien, Alessandro Zavatta, et al.. Photorefrac- tive effect in LiNbO 3 -based integrated-optical circuits for continuous variable experiments. Optics Express, Optical Society of America - OSA Publishing, 2020. hal-02908852 HAL Id: hal-02908852 https://hal.archives-ouvertes.fr/hal-02908852 Submitted on 29 Jul 2020 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Photorefractive effect in LiNbO3-based integrated-optical circuits for continuous variable experiments Fran¸coisMondain,1 Floriane Brunel,1 Xin Hua,1 Elie´ Gouzien,1 Alessandro Zavatta,2, 3 Tommaso Lunghi,1 Florent Doutre,1 Marc P. De Micheli,1 S´ebastienTanzilli,1 and Virginia D'Auria1, ∗ 1Universit´eC^oted'Azur, CNRS, Institut de Physique de Nice (INPHYNI), UMR 7010, Parc Valrose, 06108 Nice Cedex 2, France. 2Istituto Nazionale di Ottica (INO-CNR) Largo Enrico Fermi 6, 50125 Firenze, Italy 3LENS and Department of Physics, Universit`adi Firenze, 50019 Sesto Fiorentino, Firenze, Italy (Dated: July 23, 2020) We investigate the impact of photorefractive effect on lithium niobate integrated quantum pho- tonic circuits dedicated to continuous variable on-chip experiments.
    [Show full text]
  • 4-2 Image Storage Techniques Using Photore- Fractive Effect
    4-2 Image Storage Techniques using Photore- fractive Effect TAKAYAMA Yoshihisa, ZHANG Jiasen, OKAZAKI Yumi, KODATE Kashiko, and ARUGA Tadashi Optical image storage techniques using the photorefractive effect are presented. In these techniques, the random reference multiplexing scheme is introduced to the holo- graphic recording process in order to increase the storage capacity. The common feature of our techniques is the use of a bundle of multimode fibers placed in the optical path of refer- ence wave. This approach can automatically impose quasi-random patterns on the wave- front when the reference wave penetrates the fiber bundle. As a proof-of-principle, experi- ments of recording holograms are performed with a LiNbO3 crystal. The results show that the use of fiber bundle enables us to build a simple and compact optical setup keeping the capacity of hologram multiplexing. Keywords Photorefractive, Hologram multiplexing, Optical memory, Fiber bundle 1 Introduction As well as the increase of storage capacity, to build a simple and compact setup is another Optical holographic data storage using the interest. For this purpose, a single multimode photorefractive effect has been extensively fiber has been replaced by a bundle of fibers studied. Several schemes for hologram multi- to steer the reference beam without any lenses plexing have been examined and successfully or mirrors[11][12]. In our first attempt, the improved the storage capacity [1]-[7]. Recently, recording medium is mounted on a linear an optical fiber has been employed in optical stage and moved along a direction perpendicu- setups as a device to impose a quasi-random lar to the axis of the fiber bundle.
    [Show full text]
  • Photorefractive Properties of Undoped, Cerium-Doped
    Photorefractive properties of undoped,undoped, ceriumcerium-doped,-doped, and iron-dopediron -doped single-crystalsingle-crystal Sr0.6Ba0.4Nb2O6 Sr0 George A. Rakuljic Abstract. We present the results of our theoretical andand experimental studies of Amnon Yariv the photorefractivephotorefractive effect effect in in single single-crystal -crystal SBN:60, SBN:60, SBN:Ce, SBN:Ce, and and SBN:Fe. SBN:Fe. TheThe California Institute ofof TechnologyTechnology twotwo-beam -beam couplingcoupling coefficients,coefficients, response times,times, and absorption coefficients of Department of Applied Physics these materials areare given. Pasadena, California California 9112591125 Subject terms: photorefractive materials;materials; non nonlinear linear optical optical materials; materials; optical optical phase phase con con­ - Ratnakar Neurgaonkar jugation; imageimage processingprocessing; opticaloptical signal signal processing. processing. Rockwell International Corporation Optical Engineering 25(11), 12121212-1216 -1216 (November 1986).1986). Science Center Thousand Oaks,Oaks, CaliforniaCalifornia 9136091360 CONTENTS The point groupgroup symmetrysymmetry of of SBN SBN isis 44 mm,mm, whichwhich impliesimplies 1. IntroductionIntroduction that itsits electroelectro-optic -optic tensortensor is nonzero.nonzero. The dominant electro-electro- 2. MaterialMaterial propertiesproperties optic coefficientcoefficient is r33,r33 , which ranges from 100100 pm/pm/V V inin 3. PhotorefractivePhotorefractive properties SBN:25 to 14001400 pm/ V in SBN:75. In order toto realizerealize thethe largelarge 4. SummarySummary ofof resultsresults values of electro-opticelectro -optic coefficients in SBN crystals, they must, 5. ConclusionConclusion in practice, be poled by first being heated toto above their Curie 6. AcknowledgmentsAcknowledgments points and then being cooled to roomroom temperaturetemperature with an 7. ReferencesReferences applied dc electric field of 5 to 88 kVkV/cm. /cm. 1. INTRODUCTIONINTRODUCTION 3.
    [Show full text]
  • Photorefractive Response and Real-Time Holographic Application of a Poly(4-(Diphenylamino)Benzyl Acrylate)-Based Composite
    Polymer Journal (2014) 46, 59–66 & 2014 The Society of Polymer Science, Japan (SPSJ) All rights reserved 0032-3896/14 www.nature.com/pj ORIGINAL ARTICLE Photorefractive response and real-time holographic application of a poly(4-(diphenylamino)benzyl acrylate)-based composite Ha Ngoc Giang, Kenji Kinashi, Wataru Sakai and Naoto Tsutsumi A photorefractive (PR) composite based on poly(4-(diphenylamino)benzyl acrylate) (PDAA) as a host photoconductive matrix is reported. The PR performance was investigated at three different wavelengths (532, 561, 594 nm), and an optimized operating wavelength of 532 nm was obtained. The PDAA composite had high sensitivity at 532 nm with a maximum diffraction efficiency of 480%, which was achieved at an applied electric field of 40 V lm À1. An application with a hologram display system using the PR composite was demonstrated. A clear and updatable hologram of an object was successfully reconstructed in real time, even at a low applied electric field of 25 V lm À1. Polymer Journal (2014) 46, 59–66; doi:10.1038/pj.2013.68; published online 14 August 2013 Keywords: composite; hologram; photoconductive polymer; photorefractive effect; wavelength INTRODUCTION temperature (Tg)of4200 1C. Low hole mobility will limit the speed Photorefractive (PR) polymers and composites have attracted much of space-charge field formation and consequently lead to a slow PR attention because of their interesting applications, such as data response time. storage, three-dimensional (3D) displays, image amplification and Another factor that will affect PR response time is the re- optical phase conjugation. The mechanism for a PR effect is a orientation of the chromophore, which has been shown to occur combination of several steps: (1) non-uniform material illumination inside a low Tg composite and has an essential role in high PR 8 through a laser interference pattern, (2) charge generation assisted by performance.
    [Show full text]
  • Photorefractive Effect in NLC Cells Caused by Anomalous Electrical
    crystals Review Photorefractive Effect in NLC Cells Caused by Anomalous Electrical Properties of ITO Electrodes Atefeh Habibpourmoghadam Department of Nonlinear Phenomena, Institute of Physics, Otto von Guericke University, 39106 Magdeburg, Germany; [email protected] Received: 8 September 2020; Accepted: 2 October 2020; Published: 4 October 2020 Abstract: In a pure nematic liquid crystal (NLC) cell, optically induced charge carriers followed by transports in double border interfaces of orientant/LC and indium-tin-oxide (ITO)/orientant (or LC) can cause removal of screening of the static electric field inside the LC film. This is called surface photorefractive effect (SPR), which induces director field reorientation at a low DC electric field beyond the threshold at a reduced Fréedericksz transition and, as a result, a modulation of the LC effective refractive index. The studies conducted on the photoinduced opto-electrical responses in pure nematic LC cells biased with uniform static DC electric fields support the SPR effect (attributed to the photoelectric activation of the double interfaces). The SPR effect was further studied in LC cells with photoresponsive substrates, which act as a source of a bell-shaped electric field distribution in the LC film if no ITO electrode was employed. In an equipped cell with ITO, the photovoltaic electric field induces charge carrier redistribution in the ITO film, hence the SPR effect. This paper is aimed at highlighting all the evidences supporting ITO film as one of the fundamental sources of the SPR effect in pure NLC cells under the condition of applying low optical power and low DC voltage. An optically induced fringe electric field stemming from inhomogeneous photo-charge profiles near the electrode surfaces is expected in the LC film due to the semiconducting behavior of the ITO layer.
    [Show full text]
  • Papers Theory and Applications of Four-Wwe Mixing in Photorefractive Media
    12 IEEE JOURNAL OF QUANTUMELECTRONICS, VOL.NO. QE-20, 1, JANUARY 1984 Papers Theory and Applications of Four-Wwe Mixing in Photorefractive Media MARK CRONIN-GOLOMB, BARUCH FISCHER, JEFFREY 0. WHITE, AND AMNON YARIV, FELLOW, IEEE (Invited Paper) Abstract-The development of a theory of four-wave mixing in photo- In the mid 1970’s the field of phase conjugate optics [35] refractive crystals is described. This theory is solved in the undepleted began to prosper because of potential applicationsin aberration pumpsapproximation with linear absorptionand without using the correction. The main problem to be faced was and still is the undepletedpumps approximation for negligibleabsorption. Both the transmission and reflectiongratings are treated individually. The results development of fastmedia with large nonlinearities. While are used to analyze several photorefractive phase conjugate mirrors, phase conjugationby four-wave mixing is oftenthought of yielding reflectivities and thresholds. The useof photorefractive crystals interms of nonlinearoptical susceptibilities, theformal as optical distortion correction elements and experimental demonstra- analogy with real-time holography [36] has made it clear that tions of several of the passive phase conjugate mirrors are described. PR materials could beused effectively in phase conjugation. 1. INTRODUCTION As a result, a whole new branch in phase conjugate optics has HROUGH therecent years’ boom innonlinear optical beendeveloped E371 -[40]. High reflectivityphase conjuga- T phase conjugation, photorefractive (PR) materials such as tion with low-power lasers has become an easy task. Feinberg LiNb03, Bi12Sizo O3 (BSO), BaTi03, and Sr, - xBa, Nb2 O6 hasdemonstrated a resonator using a PR phase conjugate (SBN) have been assuming ever increasing prominence due to mirror [41], andmany new nonlinearoptical deviceshave their unique capability for displaying strong nonlinear effects been demonstrated including ring oscillators by White et al.
    [Show full text]
  • Photorefractive Effect and Two-Beam Energy Exchange in Hybrid Liquid Crystal Cells
    Photorefractive effect and two-beam energy exchange in hybrid liquid crystal cells Igor Pinkevych Physics Faculty, Taras Shevchenko National University of Kyiv, Ukraine (joint work with Victor Reshetnyak, Tim Sluckin, Gary Cook, and Dean Evans) PHOTOREFRACTIVE EFFECT (1) The photorefractive effect is a phenomenon in which local index of refraction is changed in response to illumination by light with spatially varying intensity. Such effect was first observed in early 60s. Mechanism The photorefractive effect in crystals usually occurs in several stages: 1. A photorefractive material is illuminated by coherent light beams. Interference of the beams results in a pattern of dark and light fringes throughout the crystal. 2. In bright regions electrons can absorb the light and be photoexcited from an impurity level into the conduction band of the crystal, leaving an electron hole. ikar ikbr it E Eae Ebe e Ir I0 1 mcos Kr K kb ka PHOTOREFRACTIVE EFFECT (2) Mechanism 3. Once in the conduction band, the electrons diffuse towards the dark-fringe regions. Here they fall into the traps. The redistribution of electrons into the dark regions of the material and holes in the bright areas, causes a spatially periodic electric field, known as a space charge field. 4. The space charge field, via the electro-optic effect, changes the local refractive index of the crystal and creates a refractive index grating. 5. The refractive index grating can now diffract light and, as a result, energy exchange between beams at the grating is possible. What we will talk about We will study energy gain in system of two coherent beams propagating in medium with the refractive index grating (induced by these beams): there is an interaction between beams at the diffraction grating and, as a result, amplitude of one of the beams (signal beam) increases/decreases.
    [Show full text]
  • Photorefractive Mesogenic Composites
    Research News Photorefractive Mesogenic Composites By Hiroshi Ono,* Tomomi Kawamura, Nazarene Mocam Frias, Keiko Kitamura, Nobuhiro Kawatsuki, and Hideki Norisada Mesogenic composites, consisting of low-molar-mass liquid crystals, polymers, and photoconductive sensitizers, constitute novel organic materials possessing high-performance photorefractivity. Polymeric materials in the photorefractive mesogenic composites play a very important role in terms of improving the resolution, stabilizing the homeotropic alignment, and func- tionalizing the materials. 1. Introduction terial. Electric fields as large as 50±100 V/mm are used to pole these materials and several kilovolts of DC field are Photorefractive materials have been investigated exten- applied to the popular photorefractive polymer composites sively because of the possibility of applications in optical because the film thickness is about 50±150 mm. The high signal processing, dynamic holography, and phase conjuga- electric field causes serious problems, such as dielectric tion.[1] Photorefractive gratings appear in materials that ex- breakdown and phase separation, in these photorefractive hibit both an electric-field-dependent refractive index polymer composites. change and an optically induced charge distribution. The In 1994, Khoo et al. found that low-molar-mass nematic refractive-index modulation is out of phase with the optical liquid crystals (L-LCs) show high-performance photorefrac- interference pattern, and this phase shift can induce an tivity under low driving voltage (<1 V/mm) by giving photo- energy exchange between two coherent beams, which leads conductivity to the L-LCs.[5] This was accomplished by dop- to a variety of useful applications. Photorefractive materi- ing the L-LC 4¢-(n-pentyl)-4-cyanobiphenyl (5CB) with als are by far the most efficient nonlinear optical media for fullerene (C60).
    [Show full text]
  • Photorefractive Properties of Liquid Crystal-Filled Bacterial Cellulose Mats
    Photorefractive properties of liquid crystal-filled bacterial cellulose mats By Caroline Novak Department of Physics, Case Western Reserve University [email protected] Advisor Dr. Kenneth Singer Department of Physics, Case Western Reserve University [email protected] December 17, 2017 Table of Contents 1. Executive Summary............................................................................................................................ 3 2. Introduction....................................................................................................................................... 3 3. Background........................................................................................................................................ 3 3.1. Photorefractive Effect........................................................................................................ 3 3.2. Liquid Crystal...................................................................................................................... 4 3.3. Bacterial Cellulose.............................................................................................................. 5 4. Justification........................................................................................................................................ 5 5. Methods and Materials...................................................................................................................... 6 5.1. Two-Beam Coupling..........................................................................................................
    [Show full text]
  • Investigations of the Photorefractive Effect in Pot,Assium Tantalum
    Investigations of the Photorefractive Effect in Pot,assium Tantalum hTiobate Thesis by 1-ictor Leyva In Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy California Institute of Technology Pasadena, California 1991 (Submitted May 20, 1991) .. - 11- Acknowledgements I wili always recall with fondness the diverse and highly talented group of individuals I have encountered during my graduate studies. First and foremost I would like to thank Dr. Amnon I'ariv for the opportunity he opened to me and for his guidance. I have benefitted greatly from my work with Dr. Aharon Agranat. His assistance is appreciated. Of the many students of the Quantum Electronics group, I u~ouldespecially like to acknowledge those involved in the photorefractive field with whom I have had many productive discussions and collaborations. These include Korman Kwong. George Rakuljic, I'asuo Tomita, Koichi Sayano: =d Rudy HoRmeister. The group owes much to the excellent technical support of Jana htercado, Ali Ghaffari, Desrnond Armstrong: and Rex-in Cooper. I thank each of them for their assistance. In addition, the mechanical design and machine shop support of Larr>- Begaj-, Guy Duremberg, and Tony Stark is gratefully ackno~i,ledged. .. - 111- Abstract This thesis describes results of investigations of the photorefractive effect in potassium tantalum niobate (KTal-,Nb, 03)crystals. A band transport model is used to describe the photorefractive effect. The coupled mode equations are then introduced and used to solve self-consistently for the interaction of the light and space charge fields in a photorefractive material. The design and construction of a high te~peraturecrystal growth system is discussed.
    [Show full text]