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Journal articles on the topic 'Electro-optic effect'

Author: Grafiati

Published: 4 June 2021

Last updated: 7 September 2023

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1

Long, X. ‐C, R. A. Myers, S. R. J. Brueck, R. Ramer, K. Zheng, and S. D. Hersee. "GaN linear electro‐optic effect." Applied Physics Letters 67, no. 10 (1995): 1349–51. http://dx.doi.org/10.1063/1.115547.

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2

Jamison, S. P., A. M. MacLeod, G. Berden, D. A. Jaroszynski, and W. A. Gillespie. "Temporally resolved electro-optic effect." Optics Letters 31, no. 11 (2006): 1753. http://dx.doi.org/10.1364/ol.31.001753.

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3

TAI REN-ZHONO, LU FU-YUN, YUAN SHU-ZHONG, GUAN XIN-AN, and LI BING. "ELECTRO-OPTIC EFFECT IN PESO ACOUSTO-OPTIC MODULATOR." Acta Physica Sinica 41, no. 6 (1992): 1012. http://dx.doi.org/10.7498/aps.41.1012.

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4

Li, Changsheng. "Proposal for electro-optic multiplier based on dual transverse electro-optic Kerr effect." Applied Optics 47, no. 30 (2008): 5701. http://dx.doi.org/10.1364/ao.47.005701.

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5

Liu, Zhaojun, Qingpu Wang, Xingyu Zhang, et al. "Investigation of the electro-optic activity and the electro-optic effect of La3Ga5SiO14crystal." physica status solidi (a) 203, no. 10 (2006): 2501–5. http://dx.doi.org/10.1002/pssa.200622178.

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6

Chang, Yia‐Chung, J. N. Schulman, and U. Efron. "Electro‐optic effect in semiconductor superlattices." Journal of Applied Physics 62, no. 11 (1987): 4533–37. http://dx.doi.org/10.1063/1.339045.

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7

WEGENER, M., A. WITT, C. KLINGSHIRN, D. GNASS, Y. IYECHIKA, and D. JÄGER. "CdS SELF-ELECTRO-OPTIC EFFECT DEVICE." Le Journal de Physique Colloques 49, no. C2 (1988): C2–109—C2–112. http://dx.doi.org/10.1051/jphyscol:1988224.

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8

OHKE, Shigeaki, Yoshio CHO, and Takahiro OKABE. "Electro-optic effect in zincblende crystals." Review of Laser Engineering 15, no. 1 (1987): 2–11. http://dx.doi.org/10.2184/lsj.15.2.

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9

Yang, Lie-Kun, Bing Liu, Pan-Yu Qiao, et al. "Measurement of the Quadratic Electro-Optic Coefficient of KTN Crystal with an Electro-Optic Modulation System in the Presence of Polar Nano-Regions." Crystals 11, no. 10 (2021): 1234. http://dx.doi.org/10.3390/cryst11101234.

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An electro-optic modulation system was adopted for measuring the quadratic electro-optic coefficient of KTN crystal. Theoretical analysis and experimental results verified the feasibility of this method. The quadratic electro-optic coefficient of a KTN crystal chip, which has a Curie temperature of 0 °C, was measured using this system in the temperature range of 2 °C to 18 °C (Tc = 0 °C). The influences of temperature, AC voltage and frequency on the quadratic electro-optic coefficient were discussed. It was found that the relaxation effect of PNRs (polar nano-regions) played an important role in the determination of the quadratic electro-optic coefficient of KTN crystal.

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10

Yang, Lie-Kun, Bing Liu, Pan-Yu Qiao, et al. "Measurement of the Quadratic Electro-Optic Coefficient of KTN Crystal with an Electro-Optic Modulation System in the Presence of Polar Nano-Regions." Crystals 11, no. 10 (2021): 1234. http://dx.doi.org/10.3390/cryst11101234.

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An electro-optic modulation system was adopted for measuring the quadratic electro-optic coefficient of KTN crystal. Theoretical analysis and experimental results verified the feasibility of this method. The quadratic electro-optic coefficient of a KTN crystal chip, which has a Curie temperature of 0 °C, was measured using this system in the temperature range of 2 °C to 18 °C (Tc = 0 °C). The influences of temperature, AC voltage and frequency on the quadratic electro-optic coefficient were discussed. It was found that the relaxation effect of PNRs (polar nano-regions) played an important role in the determination of the quadratic electro-optic coefficient of KTN crystal.

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11

Efremidis, Anastasios T., Nikolaos C. Deliolanis, Konstantinos Vyrsokinos, Constantinos Manolikas, Sotirios Ves, and Evaggelos D. Vanidhis. "Electro-optic and electro-gyration effects on light propagation in \bf \overline 4 2mpoint-group crystals." Journal of Applied Crystallography 44, no. 5 (2011): 1100–1110. http://dx.doi.org/10.1107/s0021889811028883.

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Several nonlinear crystals that are used in laser and optical signal processing technologies belong to the {\overline 4}2m point group. This group exhibits as primary effects natural birefringence, optical activity, linear and quadratic electro-optic effects, and linear and quadratic electro-gyration effects, and, as secondary effects, photo-elasticity and piezo-gyrationviathe inverse piezo-electric phenomenon. The combination of these effects makes the study of light propagation a complicated task. In this work, the influence of each of these effects on light propagation is analytically reviewed, and suitable configurations for the light propagation and applied electric field directions are identified, which decouple the contribution of the individual effects. It is found that the complete decoupling of the linear electro-gyration from the linear electro-optic effect is not possible for this symmetry, while the inverse is feasible, and that the separation of the quadratic from the linear electro-optic effect can be achieved. For the linear phenomena, index ellipsoid geometries and eingenpolarizations are calculated, and analytic expressions are derived for the intensity of a light beam propagating through a crystal followed by a polarizer, thus providing valuable information for the design of devices and/or measurements of corresponding coefficients.

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12

Jung, Hongsik. "Ti:LiNbO3Integrated Optic Electric-Field Sensors based on Electro-Optic Effect." Fiber and Integrated Optics 35, no. 4 (2016): 161–80. http://dx.doi.org/10.1080/01468030.2016.1198508.

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13

Patro, Y. G. K., and N. N. S. S. R. K. Prasad. "Self Electro-Optic Effect Device (S-SEED)." Journal of Optics 25, no. 4 (1996): 233–47. http://dx.doi.org/10.1007/bf03549772.

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14

Das, P., A. V. Scholtz, A. J. Urillo, D. M. Litynski, and D. Shklarsky. "Surface acoustic wave acousto‐electro‐optic effect." Applied Physics Letters 49, no. 16 (1986): 1016–18. http://dx.doi.org/10.1063/1.97457.

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15

Rubinger, R. M., A. G. de Oliveira, G. M. Ribeiro, J. C. Bezzera, M. V. B. Moreira, and H. Chacham. "Electro-optic recovery of the photoquenching effect." Applied Physics Letters 75, no. 9 (1999): 1252–54. http://dx.doi.org/10.1063/1.124658.

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16

Wahedy Zarch, AliAkbar, Hassan Kaatuzian, Ahmad Amjadi, and Ahmad Ajdarzadeh Oskouei. "A semiclassical approach for electro-optic effect." Optics Communications 281, no. 15-16 (2008): 4033–37. http://dx.doi.org/10.1016/j.optcom.2008.04.030.

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17

Nagata, T., A. Ashida, N. Fujimura, and T. Ito. "Electro-optic effect in ZnO:Mn thin films." Journal of Alloys and Compounds 371, no. 1-2 (2004): 157–59. http://dx.doi.org/10.1016/j.jallcom.2003.06.016.

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18

Fuflyigin, V., F. Wang, H. Jiang, J. Zhao, and P. Norris. "Electro-optic effect in Ba1−xPbxTiO3 films." Applied Physics Letters 76, no. 13 (2000): 1641–43. http://dx.doi.org/10.1063/1.126121.

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19

Yellampalle, Balakishore, Ki-Yong Kim, James H. Glownia, and Antoinette J. Taylor. "Comment on "Temporally resolved electro-optic effect"." Optics Letters 32, no. 10 (2007): 1341. http://dx.doi.org/10.1364/ol.32.001341.

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20

Ebbers, Chris A. "Linear electro‐optic effect in β‐BaB2O4". Applied Physics Letters 52, № 23 (1988): 1948–49. http://dx.doi.org/10.1063/1.99585.

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21

Nakatani, H., W. Bosenberg, L. K. Cheng, and C. L. Tang. "Linear electro‐optic effect in barium metaborate." Applied Physics Letters 52, no. 16 (1988): 1288–90. http://dx.doi.org/10.1063/1.99680.

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22

Mares, P. J., and S. L. Chuang. "Modeling of self‐electro‐optic‐effect devices." Journal of Applied Physics 74, no. 2 (1993): 1388–97. http://dx.doi.org/10.1063/1.354897.

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23

Adnan Hbeeb, Sadeq. "Improvement of Overlap for 2x2 MZI Electro-Optic Switch Based on Lithium Tantalite (LiTaO3)." Al-Nahrain Journal for Engineering Sciences 25, no. 2 (2022): 91–95. http://dx.doi.org/10.29194/njes.25020091.

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This research introduces a method of an electro-optic effect and electro-refractive effect that considers very imperative for high-speed optical communication systems. In this research, it presents way by a reduction the gap between the electrodes d, and this technique achieves to solve the problem of overlap for Mach-Zehnder interferometer MZI electro-optical switch base on lithium tantalite LiTaO3, also this technique suggests a model for analysis the effect parameters on the electro-optic overlap of the electro-optic switch as the ordinary positive changing of refractive index and a length of arm switch. This study achieves a better overlap by large positive changing refractive index with a suitable small length of arm about 8µm and low driving power at least 4V/µm. Also, for lithium tantalite LiTaO3, this research achieves a better performance for system using the near infrared wavelength.

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24

Takeda, Kotaro, Takuya Hoshina, Hiroaki Takeda, and Takaaki Tsurumi. "Electro-optic effect and photoelastic effect of feroelectric relaxors." Japanese Journal of Applied Physics 55, no. 10S (2016): 10TB05. http://dx.doi.org/10.7567/jjap.55.10tb05.

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25

Izdebski, Marek. "Precise Measurements of the Quadratic Electro-Optic Effect in KH2PO4 Crystals Using a Sénarmont-Type System." Materials 14, no. 18 (2021): 5435. http://dx.doi.org/10.3390/ma14185435.

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This paper presents precise measurements of the temperature dependencies of the quadratic electro-optic coefficients g1111−g1122 and ne3g3333−no3g1133 in KH2PO4 crystals. In addition to traditional electro-optic coefficients describing changes in the function of an applied electric field, intrinsic coefficients, defined in terms of induced polarization, are also considered. Both intrinsic coefficients decrease with increases in temperature, but the relative temperature changes are of different orders of magnitude: 10−4 and 10−3 K−1. A Sénarmont-type setup was used for the electro-optic measurements. To achieve the best accuracy, a new approach was developed, in which, instead of using only one specific point on the modulator’s transmission characteristic, the operating point is changed during the measurements.

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26

Satoh, Keisuke, Akio Sugama, Masatoshi Ishii, Masao Kondo, and Kazuaki Kurihara. "Crystal Phase and Orientation Dependence of Electro-Optic Effect in Epitaxial PLZT an PZT Films." Key Engineering Materials 350 (October 2007): 99–102. http://dx.doi.org/10.4028/www.scientific.net/kem.350.99.

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Lanthanum-modified lead zirconate titanate and lead zirconate titanate epitaxial films with (100) and (111) orientations were grown respectively on (100) and (111) niobium, lending conductivity to strontium titanate through chemical solution deposition. This study investigated changes in the ordinary and extraordinary refractive index no and ne induced in these films by an electric field using the prism-coupling method. In the (100) epitaxial PZT 30/70 film, anisotropic electro-optic effects arise from the Pockels effect. The isotropic electro-optic effect, which is no = ne , was achieved on (100) epitaxial PLZT 8/65/35 and PZT 70/30 films.

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27

Sun, Xiao-Qiang, Chang-Ming Chen, Xiao-Dong Li, et al. "Polymer Electro-optic Modulator Linear Bias Using the Thermo-optic Effect." Chinese Physics Letters 29, no. 1 (2012): 014212. http://dx.doi.org/10.1088/0256-307x/29/1/014212.

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28

Nakamura, Koichiro, Jun Miyazu, Yuzo Sasaki, Tadayuki Imai, Masahiro Sasaura, and Kazuo Fujiura. "Space-charge-controlled electro-optic effect: Optical beam deflection by electro-optic effect and space-charge-controlled electrical conduction." Journal of Applied Physics 104, no. 1 (2008): 013105. http://dx.doi.org/10.1063/1.2949394.

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29

Yilmaz, S., R. Gerhard-Multhaupt, W. A. Bonner, et al. "Electro-optic potassium-tantalate-niobate films prepared by pulsed laser deposition from segmented pellets." Journal of Materials Research 9, no. 5 (1994): 1272–79. http://dx.doi.org/10.1557/jmr.1994.1272.

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Thin films of potassium tantalate niobate (KTN) were prepared by means of pulsed excimer-laser deposition and investigated with a number of analytical techniques, including electrical and electro-optical measurements. For applications in longitudinal electro-optic modulators, a transparent electrode is required between substrate and electro-optic layers. Suitable electrode materials, which at the same time permit epitaxial growth of KTN, were identified and prepared. The resulting layered samples were not only of good epitaxial and optical quality, but also exhibited the expected maximum of the longitudinal electro-optic effect at temperatures between the phase transitions from cubic to tetragonal and from tetragonal to orthorhombic. However, the maximum achievable electro-optic phase shift was found to be limited to roughly τ/100 for KTN films in the thickness range around 1 μm. Therefore, much thicker films are probably necessary for most practical applications, which requires significant improvements in the long-term stability and homogeneity of the deposition process.

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30

Izdebski, Marek, Rafał Ledzion, and Włodzimierz Kucharczyk. "Precise Method for Measuring the Quadratic Electro-Optic Effect in Noncentrosymmetric Crystals in the Presence of Natural Birefringence." Materials 13, no. 18 (2020): 3942. http://dx.doi.org/10.3390/ma13183942.

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The application of the improved dynamic polarimetric method for the measurement of the quadratic electro-optic effect in NH4H2PO4 (ADP) crystal with the light beam propagating perpendicularly to its optical axis is presented. This technique can be applied in noncetrosymmetric crystals in the presence of natural birefringence even when the fast and slow rays diverge slightly, causing them to only partially interfere. The method allows for minor errors in cutting and orientation of the crystal samples, resulting in deviations from configurations in which the crystal symmetry vetoes the linear electro-optic effect. The occurring contribution of the linear effect, if it is not too large, not only does not exclude the measurement of the quadratic effect, but increases its accuracy. The method does not require any prior compensation for the natural birefringence. Its sensitivity allows for quadratic electro-optic effect measurements in ferroelectrics in temperatures significantly different from the phase transition temperature or in paraelectric crystals, for which this effect is relatively small.

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31

Hbeeb, Sadeq. "Estimation of analytical model for enhancement and implementation of an electro-optic switch." Iraqi Journal for Electrical and Electronic Engineering 13, no. 2 (2017): 166–72. http://dx.doi.org/10.37917/ijeee.13.2.3.

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This research presents a technique of an electro optic effect for enhancement the an accomplishment of an electro optics switch using Mat lab simulation program . this technique includes design a mathematical model for evaluate the effect of different parameters such as refractive index (n), distance of separation between waveguides (d), length of electrodes (L), relative refractive index (Δn), and switching voltage (V), on the DC bias voltage of an electro optics switch. In this work the investigation of performance of an electro optics switch by analysis of an effect of distance between waveguides and the changing of refractive index on the bias voltage (V), and which optimizes when the wavelength is from 1300 into 1550 nm. Finally, an electro-optic active switch is designed and optimized, using the analytical model and which considers important device in the modern optical communication system.

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32

Fuad, Sara. "Effect of Gold Nanoparticles on Dynamic Electro-optic Properties of Acrylate Liquid Crystal Polymers." Journal of Advanced Research in Dynamical and Control Systems 12, no. 3 (2020): 378–84. http://dx.doi.org/10.5373/jardcs/v12i3/20201204.

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33

Akishige, Yukikuni, and Etsuro Sawaguchi. "Electro-Optic Kerr Effect in Hexagonal Barium Titanate." Japanese Journal of Applied Physics 26, S2 (1987): 123. http://dx.doi.org/10.7567/jjaps.26s2.123.

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34

Zhou Fei, Cao Yuan, Yong Hai-Lin, Peng Cheng-Zhi, and Wang Xiang-Bin. "Photon frequency shift based on electro-optic effect." Acta Physica Sinica 63, no. 20 (2014): 204202. http://dx.doi.org/10.7498/aps.63.204202.

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35

Zhang, JianWei, XiaoPing Du, JiGuang Zhao, YongSheng Duan, Zhengjun liu, and Hang Chen. "Discrete electro-optic effect induced by multiscale nanoresonators." Optical Materials 127 (May 2022): 112271. http://dx.doi.org/10.1016/j.optmat.2022.112271.

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36

Morgan, Robert A., Gabriela Livescu, Leo M. F. Chirovsky, Marlin W. Focht, and Ronald E. Leibenguth. "Fabry–Perot-enhanced self-electro-optic-effect devices." Optics Letters 17, no. 6 (1992): 423. http://dx.doi.org/10.1364/ol.17.000423.

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37

Nazarenko, V. G., R. Klouda, and O. D. Lavrentovich. "Unipolar electro-optic effect in a nematic cell." Physical Review E 57, no. 1 (1998): R36—R38. http://dx.doi.org/10.1103/physreve.57.r36.

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38

Chang, Yun-Ching, Chao Wang, Shizhuo Yin, Robert C. Hoffman, and Andrew G. Mott. "Giant electro-optic effect in nanodisordered KTN crystals." Optics Letters 38, no. 22 (2013): 4574. http://dx.doi.org/10.1364/ol.38.004574.

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39

Tang, Xiao, Kenneth G. Irvine, Dongping Zhang, and Michael G. Spencer. "Linear electro‐optic effect in cubic silicon carbide." Applied Physics Letters 59, no. 16 (1991): 1938–39. http://dx.doi.org/10.1063/1.106165.

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40

Margulis, Vl A., E. E. Muryumin, and E. A. Gaiduk. "Quadratic electro-optic Kerr effect in doped graphene." Journal of Optics 19, no. 6 (2017): 065505. http://dx.doi.org/10.1088/2040-8986/aa6b6a.

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41

Nagata, Takahiro, Atsushi Ashida, Norifumi Fujimura, and Taichiro Ito. "Electro-Optic Effect in Epitaxial ZnO:Mn Thin Films." Japanese Journal of Applied Physics 41, Part 1, No. 11B (2002): 6916–18. http://dx.doi.org/10.1143/jjap.41.6916.

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42

Orihara, Hiroshi, Kiyomi Kawada, Naoshi Yamada, and Yoshihiro Ishibashi. "Electro-Optic Effect in an Antiferroelectric Liquid Crystal." Molecular Crystals and Liquid Crystals Science and Technology. Section A. Molecular Crystals and Liquid Crystals 303, no. 1 (1997): 159–64. http://dx.doi.org/10.1080/10587259708039420.

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43

Yu, Kuanxin, Shiya He, and Qida Zhao. "Two-dimensional acousto-electro-optic effect and device." Journal of Applied Physics 87, no. 11 (2000): 8204–5. http://dx.doi.org/10.1063/1.373521.

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44

Jin, Ru-Long, Yan-Hao Yu, Han Yang, et al. "Anomalous Electro-Optic Effect in Polar Liquid Films." IEEE Journal of Quantum Electronics 48, no. 10 (2012): 1310–13. http://dx.doi.org/10.1109/jqe.2012.2202636.

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45

Buckingham, A. D., and P. Fischer. "Linear electro-optic effect in optically active liquids." Chemical Physics Letters 297, no. 3-4 (1998): 239–46. http://dx.doi.org/10.1016/s0009-2614(98)01144-0.

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46

Simili, Deepak V., Michael Cada, and Jaromir Pistora. "Silicon Slot Waveguide Electro-Optic Kerr Effect Modulator." IEEE Photonics Technology Letters 30, no. 9 (2018): 873–76. http://dx.doi.org/10.1109/lpt.2018.2823080.

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47

Górski, P., D. Mik, W. Kucharczyk, and R. E. Raab. "On the quadratic electro-optic effect in KDP." Physica B: Condensed Matter 193, no. 1 (1994): 17–24. http://dx.doi.org/10.1016/0921-4526(94)90047-7.

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48

Meng, X. Y., Z. Z. Wang, and Chuangtian Chen. "Mechanism of the electro-optic effect in BaTiO3." Chemical Physics Letters 411, no. 4-6 (2005): 357–60. http://dx.doi.org/10.1016/j.cplett.2005.06.056.

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49

SAKAI, MASAMICHI. "NONLOCAL ELECTRO-OPTIC EFFECT IN SEMICONDUCTOR THIN FILMS." International Journal of Modern Physics B 15, no. 28n30 (2001): 3936–39. http://dx.doi.org/10.1142/s0217979201009049.

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Electroreflectance (ER) spectra of GaAs thin film/ Al 0.3 Ga 0.7 As -substrate systems are investigated theoretically by taking into account the nonlocal effect caused by the presence of a crystal surface. Calculations are carried out by following the previous work by DelSole but considering influence of film thickness and nonflat-band modulation of a static electric field. It is shown from thickness variation of ER spectra that the refractive indexes of the thin films are reduced by a factor of about 0.1 when the nonlocal effect is considered.

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50

Chen, P., D. G. Zhao, Y. H. Zuo, D. S. Jiang, Z. S. Liu, and Q. M. Wang. "Quadratic electro-optic effect in GaN-based materials." Applied Physics Letters 100, no. 16 (2012): 161901. http://dx.doi.org/10.1063/1.3703759.

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