Relevant bibliographies by topics / Magneto-optic effect

Contents

  1. Journal articles
  2. Dissertations / Theses
  3. Book chapters
  4. Conference papers
  5. Reports

Academic literature on the topic 'Magneto-optic effect'

Author: Grafiati
Published: 4 June 2021
Last updated: 27 April 2022

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Journal articles on the topic "Magneto-optic effect"

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ILISCA, Ernest. "MAGNETO-OPTIC AND MAGNETO-CATALYTIC EFFECT." Journal of the Magnetics Society of Japan 11, S_1_ISMO (1987): S1_13–18. http://dx.doi.org/10.3379/jmsjmag.11.s1_13.

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Dattagupta, S., R. Ghosh, and J. Singh. "Magneto-Optic Piston Effect." Physical Review Letters 83, no. 4 (July 26, 1999): 710–13. http://dx.doi.org/10.1103/physrevlett.83.710.

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Qiu, Z. Q., and S. D. Bader. "Surface magneto-optic Kerr effect." Review of Scientific Instruments 71, no. 3 (March 2000): 1243–55. http://dx.doi.org/10.1063/1.1150496.

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Hasan, Zaid A. "Effect Magneto – Optic on Ferromagnetic Nanoparticle Polymer Composite Films." NeuroQuantology 19, no. 6 (July 14, 2021): 25–29. http://dx.doi.org/10.14704/nq.2021.19.6.nq21063.

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Optical properties of a composite material made of ferromagnetic matel nanoparticles embedded in dielectric host are studied. A nonlinear dependence of the optical rotation on magnetic field resulting from the reorientation of nanoparticles is demonstrated. The data of optical properties finding were applied to the magneto – optic experimental data of nickel ferrite (NiFe2 O4) ferromagnetic nanoparticles embedded in polymer (PMMA) host. The magneto – optic is applied at wavelength (540 nm) and magnetic field intensity (450 m T), from result we found the affect magneto – optical on samples.
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Qiu, Z. Q., and S. D. Bader. "Surface magneto-optic Kerr effect (SMOKE)." Journal of Magnetism and Magnetic Materials 200, no. 1-3 (October 1999): 664–78. http://dx.doi.org/10.1016/s0304-8853(99)00311-x.

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Semchuk, A. Y. "Magneto-optic effect in ferromagnetic semiconductors." IEEE Transactions on Magnetics 29, no. 6 (November 1993): 3420–21. http://dx.doi.org/10.1109/20.281182.

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Hwang, Chan-Yong. "Understanding the Surface Magneto-optic Kerr Effect." Journal of the Korean Magnetics Society 21, no. 4 (August 31, 2011): 141–46. http://dx.doi.org/10.4283/jkms.2011.21.4.141.

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Qiu, Z. Q., and S. D. Bader. "Surface Magnetism and Kerr Spectroscopy." MRS Bulletin 20, no. 10 (October 1995): 34–37. http://dx.doi.org/10.1557/s0883769400045322.

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Magneto-optic effects were first discovered in 1845 by Michael Faraday, but these effects continue to make a major impact on the materials community to this day. The need for new magnetic information-storage media has stimulated new approaches and opened new scientific opportunities in the exploration of thin-film and surface magnetism. This article provides background to some of these developments and highlights examples of contemporary issues that provide a focus for the field. In the Faraday effect, the polarization plane of linearly polarized light rotates when a magnetic field is applied in the propagation direction. The analogous phenomenon was subsequently discovered by the Rev. John Kerr in 1877 for light reflected from opaque materials. The works of Faraday and Kerr serve as cornerstones for our present understanding of magneto-optic effects in magnetic materials. Magnetooptics is presently described in the context of either microscopic quantum theory or macroscopic dielectric theory. Microscopically, the coupling between the electric field of the propagating light and the electron spin in a magnetic medium occurs through the spin-orbit interaction. Macroscopically, magneto-optic effects arise from the antisymmetric, off-diagonal elements in the dielectric tensor, as discussed in the next section.Magneto-optic characterizations of surface magnetism began only a decade ago. The first surface magneto-optic Kerr-effect study, better known by its acronym SMOKE, concerned the magnetichysteresis loops for ultrathin Fe films grown epitaxially on Au(100). Since then, SMOKE has emerged as a premier surface-magnetism technique. SMOKE has been applied to various topics in low-dimensional magnetism, ranging from the detection of magnetic order to the characterization of critical behavior, magnetic surface anisotropies, and the oscillatory antiferromagnetic coupling exhibited by giant-magnetoresistanceheterostructures. Additional interest in SMOKE has been generated by the recent commercialization of high-density, magneto-optic information-storage media, and especially by the next-generation candidate material based on Co/Pt superlattices.
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MAEDA, T., K. TAKEDA, S. SAITO, and T. SOUMURA. "MAGNETO-OPTIC KERR EFFECT IN Fe-Ni ALLOYS." Journal of the Magnetics Society of Japan 15, S_1_MORIS_91 (1991): S1_109–112. http://dx.doi.org/10.3379/jmsjmag.15.s1_109.

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Wang Li-Cen, Qiu Xiao-Dong, Zhang Zhi-You, and Shi Rui-Ying. "Photon spin splitting in magneto-optic Kerr effect." Acta Physica Sinica 64, no. 17 (2015): 174202. http://dx.doi.org/10.7498/aps.64.174202.

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Dissertations / Theses on the topic "Magneto-optic effect"

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Meng, Xiadong. "Surface magneto-optic Kerr effect of NiCoCu multilayers." Thesis, McGill University, 1994. http://digitool.Library.McGill.CA:80/R/?func=dbin-jump-full&object_id=22775.

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A phenomenological theory of magneto-optic Kerr effect (MOKE) is presented to illustrate the connection between the magnetization and the polarization of light reflection in an isotropic medium. An apparatus measuring the MOKE of magnetic medium was designed and constructed. The surface magneto-optic Kerr effect (SMOKE) of a magnetic multilayer is a measurement of the average magnetization of several layers within the penetration depth of the light.
SMOKE measurements on a series of sputtered $ rm Ni sb{80}Co sb{20}15 A$/CU$(t sb{Cu}),$ where $t sb{Cu}$ is the thickness of Cu spacer layer, multilayers confirms that the coupling strength in these multilayers oscillates from antiferromagnetic (AF) coupling to ferromagnetic coupling as a function of Cu spacer layer thickness. Low-angle x-ray diffraction and SMOKE measurements on a series of AF-coupled $ rm (Ni sb{80}Co sb{20}15 A$/Cu20A) $ times$ N multilayers with bilayer numbers N ranging from 8 to 100 shows that cumulative interface roughness increases with increasing N, as do the saturation field and coercivity. This is possibly due to the out-of-plane anisotropy associated with cumulative interface roughness in multilayers.
An AF-coupled $ rm (Ni sb{70}Co sb{30}15 A$/Cu20A) $ times$ 10 was continually annealed up to 400$ sp circ$C in several steps, and the magnetic behaviour of the sample was evaluated as a function of annealing temperatures. $ rm (Ni sb{70}Co sb{30}15 A$/CU20A/Ni$ rm sb{70}Co sb{30} A$/CU20A) $ times$ 5 multilayer was used for investigating the AF coupling between magnetic layers of unequal thicknesses. Finally, an AF-coupled $ rm (Ni sb{70}Co sb{30}15 A$/Cu20A/Ni$ rm sb{70}Co sb{30}15 A$/Cu35A) $ times$ 5 multilayer was sputtered and used to study the magnetization of an AF-coupled multilayer with two different coupling strengthes.
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Alexandrou, Marios. "Magneto-optic Kerr and Hall effect measurements for the characterisation of bit patterned media." Thesis, University of Manchester, 2011. https://www.research.manchester.ac.uk/portal/en/theses/magnetooptic-kerr-and-hall-effect-measurements-for-the-characterisation-of-bit-patterned-media(fba9cd67-86c0-4382-ad65-52c521f70e5d).html.

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For the past 50 years, the magnetic storage industry has been the ultimate provider, covering the ever-expanding needs of digital mass storage. Up to now, scaling to smaller dimensions has been the core approach for achieving higher areal densities in conventional media. However, recent studies have shown that further miniaturisation is physically bound by superparamagnetic effects. Bit patterned media (BPM) is one of the most promising solutions for extending the areal densities beyond 1Tbit/in². The ability to magnetically characterise novel BPM is a key requirement for its future commercialisation. The work presented in this thesis describes the investigation of the Magneto-Optic Kerr Effect (MOKE) and the Anomalous Hall Effect (AHE) techniques, used in the characterisation of BPM samples. These samples were produced as part of this work using a customised subtractive fabrication process. Continuous thin magnetic films with Ptseed(10nm)/[Co(0.4nm)/Pt(1nm)]x15 composition and perpendicular anisotropy, were deposited using electron-beam (e-beam) evaporation, and subsequently patterned into magnetic nano-islands through means of e-beam lithography and Ar⁺ ion milling. In terms of the MOKE technique, a fully customised polar MOKE system has been developed and successfully used to observe the hysteretic behaviour of magnetic nano-island arrays with varying dimensions. An expected reduction in the MOKE signal due to pattering has been observed, as well as an additional signal reduction due to the scattering effect arising from the non-vertical sidewalls of the dome-shaped islands. In the case of islands with improved shape profile, the magnetic reversal of BPM arrays with islands sizes down to 35nm has been successfully detected, demonstrating a sensitivity of approximately 6x10⁻¹³emu for the MOKE system. In terms of the AHE technique, Au Hall crosses were deposited on top of the BPM arrays that had been previously characterised by MOKE, allowing the direct comparison and cross-verification of the results obtained by the two techniques. A revised Hall cross design, where the Hall crosses were generated by direct patterning of the Pt seed layer, has provided a significant improvement in AHE signal. This has allowed the detection of the magnetic reversal of individual sub-50nm magnetic islands, demonstrating a sensitivity of approximately 6.6x10⁻¹⁵emu for the AHE technique. The spatial sensitivity of these Hall cross structures has been experimentally determined, indicating a decrease in sensitivity with increasing distance from the cross centre and with decreasing island diameter. In conclusion, the sensitivity profile of Hall cross structures must be taken into account for the accurate interpretation of BPM characterisation results obtained by the AHE technique. Finally, some suggestions are outlined with regard to the future improvement of the developed characterisation techniques and the further continuation of the work presented in this thesis.
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Persson, Måns, and Filip Lindh. "Optimisation of measuring magneticproperties of micro-structuresusing the magneto-optic Kerr effect." Thesis, Uppsala universitet, Materialfysik, 2016. http://urn.kb.se/resolve?urn=urn:nbn:se:uu:diva-306118.

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Magnetic storage means storage of data using magnetised medium and is widespreadover the world today, especially in hard disk drives. Using this kind of storagerequires knowledge about these materials. A way to study thin magnetic materials isto use MOKE(magneto optical Kerr effect). A Moke-system is a setup to measure thinmagnetic films by shooting a laser and analyze the reflected beam.The purpose of this report is to document and if possible improve a MOKE-system,named HOMER. This includes temperature regulation, filters, amplifiers, opticalchopper, Helmholtz coils and a laser. HOMER was documented and some changeswere made. The PID-parameters were set successfully. A low pass filter wasremoved, which decreased the noise. Using an optical chopper and lock in amplifierhowever did not decrease the noise. A labview program was written to demagnetizethe samples in a certain time which seemed to work properly. The hall probe in thesystem was successfully calibrated.
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Vähäkangas, J. (Jarkko). "Extended and finite graphenes:computational studies of magnetic resonance and magneto-optic properties." Doctoral thesis, University of Oulu, 2016. http://urn.fi/urn:isbn:9789526208619.

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Abstract In this thesis, the magnetic resonance and magneto-optical rotation parameters are studied in single-layer carbon systems of two different dimensionalities. Based on electronic structure calculations, the spectral parameters are predicted for both extended (2D) and finite, molecular (0D) systems consisting of pure sp²-hybridised pristine graphene (G), as well as hydrogenated and fluorinated, sp³-hybridised graphene derivatives, graphane (HG) and fluorographene (FG), respectively. Nuclear magnetic resonance (NMR) parameters are calculated for G, HG and FG systems at their large-system limit. For their 0D counterparts, graphene flakes, qualitative spectral trends are predicted as functions of their size and perimeter type. The last group of studied carbon systems consists of 2D graphenes containing spin-1/2 paramagnetic defects. Electron spin resonance (ESR) parameters and paramagnetic NMR shieldings are predicted for four different paramagnetic systems, including the vacancy-defected graphane and fluorographene, as well as graphene with hydrogen and fluorine adatoms. The magneto-optic properties of G and HG flakes are studied in terms of Faraday optical rotation and nuclear spin optical rotation parameters, to investigate the effects of their finite size and also the different level of hydrogenation. All the different investigated parameters displayed characteristic sensitivity to the electronic and atomic structure of the studied graphenes. The parameters obtained provide an insight into the physics of these 0D and 2D carbon materials, and encourage experimental verification.
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Hernandez, Sarah Christine. "Investigation of magnetostatics of exchange-coupled nano-dots using the magneto-optic Kerr effect technique." Oxford, Ohio : Miami University, 2009. http://rave.ohiolink.edu/etdc/view?acc%5Fnum=miami1249430747.

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Hernandez, Sarah Christine. "IInvestigation of Magnetostatics of Exchange-Coupled Nano-dots using the Magneto-optic Kerr Effect Technique." Miami University / OhioLINK, 2009. http://rave.ohiolink.edu/etdc/view?acc_num=miami1249430747.

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Tveten, Erlend Grytli. "Optical coatings for enhancement of the longitudinal Magneto-optic Kerr Effect from magnetic ultra-thin films." Thesis, Norges teknisk-naturvitenskapelige universitet, Institutt for fysikk, 2011. http://urn.kb.se/resolve?urn=urn:nbn:no:ntnu:diva-13266.

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The effect of optical coatings on the longitudinal magneto-optic Kerr effect response from 10 nm thin films of permalloy (Ni84Fe16) has been studied. Enhancement of the magneto-optic Kerr effect signal contrast of a factor 1.76 has been observed for P- polarized incident light on a trilayer configuration of aluminium, magnesium fluoride, and permalloy. A quadrilayer structure where the trilayer is overcoated with zinc sulphide enhances the signal contrast by a factor 4.05 for P-polarized light. The enhancement is also observed for S-polarized light, and is shown to be reproducible using nickel as the magnetic material and gold instead of aluminium.The experimental data are compared to a simplified theoretical model where the electric field components are calculated using a 4 x 4 matrix algorithm. The model is found to be inadequate in predicting the longitudinal magneto-optic Kerr effect response from complex multilayer structures. This is believed to be due to a simplification in the model disregarding the phase factors of the different components reflected off the multilayered samples.
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Addis, Matthew James. "Transitional metal trilayers and films investigated using Brillouin light scattering and the magneto-optic Kerr effect." Thesis, University of Southampton, 1996. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.243210.

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Shinn, Mannix Anderson. "DEVELOPMENT OF MAGNETO-OPTIC SENSORS WITH GALLIUM IN BISMUTH DOPED RARE-EARTH IRON-GARNET THICK FILMS." Diss., Temple University Libraries, 2017. http://cdm16002.contentdm.oclc.org/cdm/ref/collection/p245801coll10/id/472839.

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Physics
Ph.D.
We have investigated the Faraday effect of bismuth-doped rare-earth iron-garnets with varying doping levels of gallium from z = 1.0 to 1.35. We used lutetium to control the film's in-plane magnetic properties and found that gallium doping levels above the compensation point caused a loss of anisotropy control, a canted out-of-plane magnetization in the film, and an extremely weak but linear coercivity above 10 micro-Tesla fields. Using these results we focused on in-plane films to create 8 layer stacks of 500 um thick films to achieve a minimum detectable field of 50 pT at 1 kHz. Unlike previous Magneto-Optic (MO) studies that typically used thin films of approximately 1um thickness, we used approximately 400um thick films to allow experimentation with the final, robust, ideal form the MO sensor would take. We measured what most other MO studies with garnets neglected: the magnetic anisotropy axis or structure within the film. Knowledge of this structure is essential in improving the sensitivity of a stacked MO probe. Studying thick films proved to be key to understanding the magnetic anisotropy and domain properties that can degrade or enhance the sensitivity of the Faraday rotation in bismuth doped rare-earth iron-garnets to an applied magnetic field and to pointing the direction of future research to develop the conditions for rugged magnetometer sensors.
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Lawrence, Andrew James. "Development of a Hybrid Atomic Force and Scanning Magneto-Optic Kerr Effect Microscope for Investigation of Magnetic Domains." PDXScholar, 2011. https://pdxscholar.library.pdx.edu/open_access_etds/147.

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We present the development of a far-field magneto-optical Kerr effect microscope. An inverted optical microscope was constructed to accommodate Kerr imaging and atomic force microscopy. In Kerr microscopy, magnetic structure is investigated by measuring the polarization rotation of light reflected from a sample in the presence of a magnetic field. Atomic force microscopy makes use of a probe which is scanned over a sample surface to map the topography. The design was created virtually in SolidWorks, a three-dimensional computer-aided drafting environment, to ensure compatibility and function of the various components, both commercial and custom-machined, required for the operation of this instrument. The various aspects of the microscope are controlled by custom circuitry and a field programmable gate array data acquisition card at the direction of the control code written in National Instrument LabVIEW. The microscope has proven effective for both Kerr and atomic force microscopy. Kerr images are presented which reveal the bit structure of magneto-optical disks, as are atomic force micrographs of an AFM calibration grid. Also discussed is the future direction of this project, which entails improving the resolution of the instrument beyond the diffraction limit through near-field optical techniques. Preliminary work on fiber probe designs is presented along with probe fabrication work and the system modifications necessary to utilize such probes.
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Book chapters on the topic "Magneto-optic effect"

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Nakagawa, Takeshi. "Surface Magneto-Optic Kerr Effect." In Compendium of Surface and Interface Analysis, 667–71. Singapore: Springer Singapore, 2018. http://dx.doi.org/10.1007/978-981-10-6156-1_108.

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Bland, J. A. C. "Magneto-Optic Kerr Effect Studies of Ultrathin Magnetic Structures." In Polarized Electron/Polarized Photon Physics, 269–94. Boston, MA: Springer US, 1995. http://dx.doi.org/10.1007/978-1-4899-1418-7_21.

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Araya-Pochet, J., C. A. Ballentine, T. Y. Hsieh, and J. L. Erskine. "Magneto-Optic Kerr Effect Studies of Two-Dimensional Magnetism." In Solvay Conference on Surface Science, 461–66. Berlin, Heidelberg: Springer Berlin Heidelberg, 1988. http://dx.doi.org/10.1007/978-3-642-74218-7_41.

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Bader, S. D., E. R. Moog, and P. Grünberg. "Surface Magneto-optic Kerr Effect Studies of p(1x1) Fe/Au(100)." In Springer Proceedings in Physics, 70–74. Berlin, Heidelberg: Springer Berlin Heidelberg, 1986. http://dx.doi.org/10.1007/978-3-642-71012-4_9.

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Grünberg, P. "Magneto-Optic Kerr Effect and Lightscattering from Spinwaves: Probes of Layered Magnetic Structures." In Thin Film Growth Techniques for Low-Dimensional Structures, 487–505. Boston, MA: Springer US, 1987. http://dx.doi.org/10.1007/978-1-4684-9145-6_27.

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O’Connor, Charles J. "The Photomagnetic and Magneto-Optic Effects." In Molecular Magnetism: From Molecular Assemblies to the Devices, 521–52. Dordrecht: Springer Netherlands, 1996. http://dx.doi.org/10.1007/978-94-017-2319-0_20.

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Eremenko, V. V., Yu G. Litvinenko, N. K. Kharchenko, and V. M. Naumenko. "Magneto-Optic Effects in Non-Centroantisymmetrical Antiferromagnetic Crystals." In Magneto-Optics and Spectroscopy of Antiferromagnets, 1–66. New York, NY: Springer New York, 1992. http://dx.doi.org/10.1007/978-1-4612-2846-2_1.

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Fratello, V. J., I. Mnushkina, and S. J. Licht. "Anisotropy Effects in the Growth of Magneto-Optic Indicator Films." In Magneto-Optical Imaging, 311–18. Dordrecht: Springer Netherlands, 2004. http://dx.doi.org/10.1007/978-94-007-1007-8_40.

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Lange, W., K. H. Drake, and J. Mlynek. "Nonlinear Magneto-Optic Effects in a J=1 to J’=0 Transition." In Laser Spectroscopy VIII, 300–301. Berlin, Heidelberg: Springer Berlin Heidelberg, 1987. http://dx.doi.org/10.1007/978-3-540-47973-4_89.

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Newnham, Robert E. "Magneto-optics." In Properties of Materials. Oxford University Press, 2004. http://dx.doi.org/10.1093/oso/9780198520757.003.0033.

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The magneto-optic properties of interest are the Faraday Effect, Kerr Rotation, and the Cotton–Mouton Effect. In 1846, Michael Faraday discovered that when linearly polarized light passes through glass in the presence of a magnetic field, the plane of polarization is rotated. The Faraday Effect is now used in a variety of microwave and optical devices. Normally the Faraday experiment is carried out in transmission, but rotation also occurs in reflection, the so-called Kerr Rotation that is used in magneto-optic disks with Mbit storage capability. Other magneto-optic phenomena of less practical interest include the Cotton– Mouton Effect, a quadratic relationship between birefringence and magnetic field, and magnetic circular dichroism that is closely related to the Faraday Effect. A number of nonlinear optical effects of magnetic or magnetoelectric origin are also under study. Almost all these magnetooptical effects are caused by the splitting of electronic energy levels by a magnetic field. This splitting was first discovered by the Dutch physicist Zeeman in 1896, and is referred to as the Zeeman Effect. When linearly polarized light travels parallel to a magnetic field, the plane of polarization is rotated through an angle ψ. It is found that the angle of rotation is given by . . . ψ(ω) = V(ω)Ht, . . . where H is the applied magnetic field, t is the sample thickness, ω is the angular frequency of the electromagnetic wave, and V(ω) is the Verdet coefficient. Faraday rotation is observed in nonmagnetic materials as well as in ferromagnets. The Verdet coefficient of a commercial one-way glass is plotted as a function of wavelength in Fig. 31.1(a). Corning 8363 is a rare earth borate glass developed to remove reflections from optical systems. A polarized laser beam is transmitted through the glass parallel to the applied magnetic field. The plane of polarization is rotated 45◦ by the Faraday Effect. The transmitted beam passes through the analyzer that is set at 45◦ to the polarizer. But the reflected waves coming from the surface of the glass and from the analyzer are rotated another 45◦ as they return toward the laser.
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Conference papers on the topic "Magneto-optic effect"

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Semchuk, A. Y. "Magneto-optic Effect In Ferromagnetic Semiconductors." In 1993 Digests of International Magnetics Conference. IEEE, 1993. http://dx.doi.org/10.1109/intmag.1993.642226.

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Oliver, Steven A., Charles A. DiMarzio, Aniruddha B. Kale, Scott C. Lindberg, and Stephen W. McKnight. "Magneto-optic Kerr effect sensors for fiber optic applications." In Optical Tools for Manufacturing and Advanced Automation, edited by Ramon P. DePaula. SPIE, 1994. http://dx.doi.org/10.1117/12.169948.

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Shoji, Yuya, Hideki Yokoi, and Tetsuya Mizumoto. "Enhancement of Magneto-Optic Effect in Magneto-Optic Waveguide with Low Refractive Index Undercladding Layer." In 2003 International Conference on Solid State Devices and Materials. The Japan Society of Applied Physics, 2003. http://dx.doi.org/10.7567/ssdm.2003.a-5-5.

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Feng, Guobing, Zhengfu Li, Xiaoming Wang, Qunshu Wang, and Changan Liu. "Fiber optic pulsed magnetic-field sensor based on magneto-optic effect." In International Conference on Sensing units and Sensor Technology, edited by Yikai Zhou and Shunqing Xu. SPIE, 2001. http://dx.doi.org/10.1117/12.440226.

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Karthick, R., K. Ramachandran, and R. Srinivasan. "Study of magneto-optic effect on Mn1-xZnxFe2O4 nanoferrofluids." In DAE SOLID STATE PHYSICS SYMPOSIUM 2015. Author(s), 2016. http://dx.doi.org/10.1063/1.4948160.

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Choi, Jeongyong, Giwan Seo, Yong Wook Lee, Bong-Jun Kim, Sungyoul Choi, Hyun-Tak Kim, and Sunglae Cho. "Magneto-optic Kerr effect of ferromagnetic semiconducting MnGeP2 thin films." In 2012 Opto-Electronics and Communications Conference (OECC). IEEE, 2012. http://dx.doi.org/10.1109/oecc.2012.6276772.

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Iskandar, Alexander A., and M. Reza Nurrahman. "Enhancement of Magneto-Optic Kerr Effect (MOKE) by Backscattering Suppression." In Conference on Lasers and Electro-Optics/Pacific Rim. Washington, D.C.: OSA, 2020. http://dx.doi.org/10.1364/cleopr.2020.p4_9.

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Waring, Mark. "Polarized Beam Splitting Effect In Heterogeneously Magnetized Magneto-Optic Films." In 33rd Annual Techincal Symposium, edited by Bahram Javidi. SPIE, 1990. http://dx.doi.org/10.1117/12.962256.

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Silva, Thomas J., and A. B. Kos. "Dependence of contrast on probe/sample spacing with the magneto-optic Kerr effect scanning near-field magneto-optic microscope (MOKE-SNOM)." In SPIE's 1995 International Symposium on Optical Science, Engineering, and Instrumentation, edited by Michael A. Paesler and Patrick J. Moyer. SPIE, 1995. http://dx.doi.org/10.1117/12.218702.

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Gibson, Ursula, Patrick Cantwell, and H. Angus Macleod. "Antireflection Coatings for Improvement of Longitudinal Magneto-Optic Kerr Effect Contrast." In Optical Interference Coatings. Washington, D.C.: OSA, 2007. http://dx.doi.org/10.1364/oic.2007.thd7.

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Reports on the topic "Magneto-optic effect"

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Lawrence, Andrew. Development of a Hybrid Atomic Force and Scanning Magneto-Optic Kerr Effect Microscope for Investigation of Magnetic Domains. Portland State University Library, January 2000. http://dx.doi.org/10.15760/etd.147.

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