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Journal articles on the topic 'Polarization modulator'

Author: Grafiati

Published: 4 June 2021

Last updated: 1 February 2022

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1

Xu, Yin, Feng Li, Zhe Kang, Dongmei Huang, Xianting Zhang, Hwa-Yaw Tam, and P. Wai. "Hybrid Graphene-Silicon Based Polarization-Insensitive Electro-Absorption Modulator with High-Modulation Efficiency and Ultra-Broad Bandwidth." Nanomaterials 9, no. 2 (January 27, 2019): 157. http://dx.doi.org/10.3390/nano9020157.

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Polarization-insensitive modulation, i.e., overcoming the limit of conventional modulators operating under only a single-polarization state, is desirable for high-capacity on-chip optical interconnects. Here, we propose a hybrid graphene-silicon-based polarization-insensitive electro-absorption modulator (EAM) with high-modulation efficiency and ultra-broad bandwidth. The hybrid graphene-silicon waveguide is formed by leveraging multi-deposited and multi-transferred methods to enable light interaction with graphene layers in its intense field distribution region instead of the commonly used weak cladding region, thus resulting in enhanced light–graphene interaction. By optimizing the dimensions of all hybrid graphene-silicon waveguide layers, polarization-insensitive modulation is achieved with a modulation efficiency (ME) of ~1.11 dB/µm for both polarizations (ME discrepancy < 0.006 dB/µm), which outperforms that of previous reports. Based on this excellent modulation performance, we designed a hybrid graphene-silicon-based EAM with a length of only 20 µm. The modulation depth (MD) and insertion loss obtained were higher than 22 dB and lower than 0.23 dB at 1.55 µm, respectively, for both polarizations. Meanwhile, its allowable bandwidth can exceed 300 nm by keeping MD more than 20 dB and MD discrepancy less than 2 dB, simultaneously, and its electrical properties were also analyzed. Therefore, the proposed device can be applied in on-chip optical interconnects.

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2

Zou, Xinhai, Yujia Zhang, Zhihui Li, Yiwei Yang, Shangjian Zhang, Zhiyao Zhang, Yali Zhang, and Yong Liu. "Polarization-Insensitive Phase Modulators Based on an Embedded Silicon-Graphene-Silicon Waveguide." Applied Sciences 9, no. 3 (January 28, 2019): 429. http://dx.doi.org/10.3390/app9030429.

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A polarization-insensitive phase modulator concept is presented, based on an embedded silicon-graphene-silicon waveguide. Simulation results show that the effective mode index of both transverse electric (TE) and transverse magnetic (TM) modes in the silicon-graphene-silicon waveguide undergoes almost the same variations under different biases across a broad wavelength range, in which the real-part difference is less than 1.2 × 10−3. Based on that, a polarization-insensitive phase modulator is demonstrated, with a 3-dB modulation bandwidth of 135.6 GHz and a wavelength range of over 500 nm. Moreover, it has a compact size of 60 μm, and a low insertion loss of 2.12 dB. The proposed polarization-insensitive waveguide structure could be also applied to Mach-Zehnder modulators and electro-absorption modulators.

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3

Yang, D., J. C. Canit, and E. Gaignebet. "Photoelastic modulator: polarization modulation and phase modulation." Journal of Optics 26, no. 4 (July 1995): 151–59. http://dx.doi.org/10.1088/0150-536x/26/4/002.

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4

Liu, Qiushi, and Ming Liu. "Circular-polarization modulator." Nature Photonics 11, no. 10 (September 29, 2017): 614–16. http://dx.doi.org/10.1038/s41566-017-0015-1.

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5

Feng, Li Shuang, Bo Hao Yin, Zhen Zhou, Jia Wei Sui, and Chen Long Li. "Design and Simulation of a Polarization-Independent Active Metamaterial Terahertz Modulator." Applied Mechanics and Materials 455 (November 2013): 167–72. http://dx.doi.org/10.4028/www.scientific.net/amm.455.167.

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The design and simulation of a polarization-independent active metamaterial terahertz modulator is presented in this work. The device incorporates an array of gold triple SRRs on an n-doped gallium arsenide layer to create an active metamaterial terahertz modulator with a high modulation depth, a high modulation speed and an especial polarization-independent performance for use in terahertz communication, imaging and sense.We established the theoretical model and simulatedthe key performances of the device with Ansoft HFSS.The results showed that the device exhibits a polarization-insensitivebehavior with a maximum amplitude modulation depth of 71% and a modulation rate of3.2Mbps at the resonance frequency of0.86 THz.

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6

Zhao, Feng, Jianjun Yu, and Jingling Li. "Dual-services generation using an integrated polarization multiplexing modulator." Chinese Optics Letters 18, no. 11 (2020): 110601. http://dx.doi.org/10.3788/col202018.110601.

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7

Jullien, Aurélie. "Spatial light modulators." Photoniques, no. 101 (March 2020): 59–64. http://dx.doi.org/10.1051/photon/202010159.

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Spatial Light Modulators (SLMs) are quasiplanar devices, allowing for the modulation of the amplitude, phase and polarization, or a combination of these parameters of an incident light beam according to the two spatial dimensions of the modulator. SLMs are employed in many different fields and are the subject of continuous technological development.

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8

Wan, Yuhang, Mengxuan Cheng, Zheng Zheng, and Kai Liu. "Polarization-Modulated, Goos–Hanchen Shift Sensing for Common Mode Drift Suppression." Sensors 19, no. 9 (May 5, 2019): 2088. http://dx.doi.org/10.3390/s19092088.

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A polarization-modulation-based Goos–Hanchen (GH) sensing scheme leveraging the polarization-dependence of the Bloch surface wave enhanced GH shift is proposed and experimentally demonstrated. Based on a simple setup utilizing a liquid crystal modulator to switch the polarization state of the input beam periodically, the alternating positions of the reflected beam for both polarizations are monitored by a lock-in amplifier to handily retrieve the GH shift signal. The conventional direct measurement of the beam position for the target state of polarization is vulnerable to instabilities in the optomechanical setup and alignment. Our proposed scheme provides a sensitive yet robust GH shift-sensing setup where the common mode drift and noise could be suppressed to ensure better system stability.

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9

Maeda, Shiro, Kazuhiro Nakae, and Yohji Shindo. "High-Performance Photoelastic Modulator for Polarization Modulation Spectrometer." Enantiomer: A Journal of Sterochemistry 7, no. 4-5 (July 2002): 175–83. http://dx.doi.org/10.1080/10242430212885.

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10

Hu, Xiao, and Jian Wang. "Design of graphene-based polarization-insensitive optical modulator." Nanophotonics 7, no. 3 (February 23, 2018): 651–58. http://dx.doi.org/10.1515/nanoph-2017-0088.

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AbstractBy exploiting the electroabsorption effect of graphene, we present a graphene-based polarization-insensitive optical modulator. The waveguide structure consists of a silica substrate, high-index silicon strip waveguide, Si3N4dielectric spacer, two graphene layers, and two metal electrodes. The modulator performance is comprehensively studied in terms of attenuation, insertion loss, modulation depth, and bandwidth. We achieve broadband >16 dB attenuation graphene-based optical modulator over a 35 nm wavelength range (covering C band) with an imbalance of no >1 dB and insertion loss of <2 dB for transverse magnetic and transverse electric polarized modes. Moreover, the electrical properties such as energy per bit consumption (Ebit) are also studied.

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11

Yanbing Jin, Yanbing Jin, Erwin H. W. Chan Erwin H. W. Chan, Xinhuan Feng Xinhuan Feng, Xudong Wang Xudong Wang, and Bai-ou Guan Bai-ou Guan. "Tunable negative coefficient microwave photonic filter based on a polarization modulator and a polarization beam interferometer." Chinese Optics Letters 13, no. 5 (2015): 050601–50603. http://dx.doi.org/10.3788/col201513.050601.

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12

Yang, Zhixian, Kun Qu, and Xiang Liu. "Frequency-Octupling Millimeter-Wave Optical Vector Signal Generation via an I/Q Modulator-Based Sagnac Loop." Symmetry 11, no. 1 (January 14, 2019): 84. http://dx.doi.org/10.3390/sym11010084.

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A new method for generating frequency-octupling millimeter-wave (mm-wave) vector signals in optical fields via a Sagnac loop is proposed. In this scheme, two orthogonally polarized fourth order sidebands can be obtained through an integrated dual-polarization quadrature phase shift keying (DP-QPSK) modulator. The two optical sidebands are sent into an I/Q modulator-based Sagnac loop. The I/Q modulator is modulated by a 16QAM baseband signal. In the Sagnac loop, one of the sidebands is modulated by the baseband vector signal along one direction, and the other sideband is unmodulated along the opposite direction because the I/Q modulator has the traveling-wave nature. Thanks to this modulation property and the symmetrical structure of the Sagnac loop, a frequency-octupling mm-wave vector signal that is free from interband beating and fiber chromatic dispersion interference can be generated by the photodetector (PD). After simulating a 20 km single-mode fiber (SMF) transmission, the generated frequency-octupling vector signal was good in function.

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13

Canit, J. C., M. Nerozzi, and Jacques Badoz. "Monomode all-fiber polarization modulator." Applied Optics 26, no. 15 (August 1, 1987): 2966. http://dx.doi.org/10.1364/ao.26.002966.

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14

Kotov, O. I., A. V. Khlybov, S. I. Markov, and A. V. Kudryashov. "Effective fiber-optic polarization modulator." Technical Physics Letters 30, no. 4 (April 2004): 262–64. http://dx.doi.org/10.1134/1.1748594.

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15

Chen, Wei, Yan Xu, Yang Gao, Lanjing Ji, Xibin Wang, Xiaoqiang Sun, and Daming Zhang. "A Broadband Polarization-Insensitive Graphene Modulator Based on Dual Built-in Orthogonal Slots Plasmonic Waveguide." Applied Sciences 11, no. 4 (February 21, 2021): 1897. http://dx.doi.org/10.3390/app11041897.

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A broadband polarization-insensitive graphene modulator has been proposed. The dual built-in orthogonal slots waveguide allows polarization independence for the transverse electric (TE) mode and the transverse magnetic (TM) mode. Due to the introduction of metal slots in both the vertical and horizontal directions, the optical field as well as the electro-absorption of graphene are enhanced by the plasmonic effect. The proposed electro-optic modulator shows a modulation depth of 0.474 and 0.462 dB/μm for two supported modes, respectively. An ultra-low effective index difference of 0.001 can be achieved within the wavelength range from 1100 to 1900 nm. The 3 dB-bandwidth is estimated to be 101 GHz. The power consumption is 271 fJ/bit at a modulation length of 20 μm. The proposed modulator provides high speed broadband solutions in microwave photonic systems.

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16

Rexwinkel, R. B., P. Schakel, S. C. J. Meskers, and H. P. J. M. Dekkers. "Time-Resolved Polarization of Luminescence Spectroscopy: An Accurate and Versatile Digital Instrument for the Sub-μs Time Domain." Applied Spectroscopy 47, no. 6 (June 1993): 731–40. http://dx.doi.org/10.1366/0003702934067063.

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An instrument is described for the measurement of circular and linear polarizations of the luminescence with a time resolution up to 50 ns. The spectrometer, which makes use of a 50-kHz photoelastic modulator and a differential photon-counting technique, is accurate and absolute and is capable of detecting small degrees of polarization. Making use of excitation light pulses which lie randomly in the modulator's duty cycle, the instrument can be readily interfaced with a variety of externally triggered or free running pulsed light sources.

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17

Malon, Petr, and Timothy A. Keiderling. "Spinning Quarter-Wave Plate Polarization Modulator: Test of Feasibility for Vibrational Circular Dichroism Measurements." Applied Spectroscopy 50, no. 5 (May 1996): 669–74. http://dx.doi.org/10.1366/0003702963905844.

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A novel polarization modulator design based on a rotating quarter-wave plate and preliminary results of its application for vibrational circular dichroism (VCD) are presented. The device permits quarter-wave retardation in the infrared with alternating senses so that the resultant components of circular polarization can be modulated at frequencies on the order of 100 Hz. We have been able to apply this device to measure VCD with a step-scan FT-IR spectrometer by incorporating a stressed ZnSe optical element as the rotating quarter-wave plate. VCD of α-pinene and camphor were obtained. While these test spectra were of low signal-to-noise ratio (S/N), they exhibited the correct VCD spectral features for these chiral molecules. While not yet of competitive, practical utility, this design is potentially adaptable to extension into the far-IR with alternative optical elements, permits variable-frequency polarization modulation, and should be capable of improved S/N with modifications to increase rotation frequency.

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18

Dorjgotov, Enkh-Amgalan, Achintya K. Bhowmik, Douglas Bryant, Liang-Chy Chien, and Philip J. Bos. "Polarization-independent liquid-crystal-etalon modulator." Journal of the Society for Information Display 17, no. 12 (2009): 1015. http://dx.doi.org/10.1889/jsid17.12.1015.

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19

He, Jingwen, Zhenwei Xie, Sen Wang, Xinke Wang, Qiang Kan, and Yan Zhang. "Terahertz polarization modulator based on metasurface." Journal of Optics 17, no. 10 (September 22, 2015): 105107. http://dx.doi.org/10.1088/2040-8978/17/10/105107.

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20

Donval, A., E. Toussaere, R. Hierle, and J. Zyss. "Polarization insensitive electro-optic polymer modulator." Journal of Applied Physics 87, no. 7 (April 2000): 3258–62. http://dx.doi.org/10.1063/1.372333.

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21

Yang, J., Q. Zhou, X. Jiang, M. Wang, and R. T. Chen. "Polymer-Based Electrooptical Circular-Polarization Modulator." IEEE Photonics Technology Letters 16, no. 1 (January 2004): 96–98. http://dx.doi.org/10.1109/lpt.2003.820455.

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22

Hutchinson, Meredith N., Nicholas J. Frigo, and Vincent J. Urick. "Procedure for aligning polarization modulator link for amplitude modulation applications." Optics Express 22, no. 20 (October 3, 2014): 24859. http://dx.doi.org/10.1364/oe.22.024859.

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23

Ahmad, H., H. S. Lim, M. Z. MatJafri, Y. Q. Ge, H. Zhang, and Z. C. Tiu. "All-fiber optical polarization modulation system using MoS2 as modulator." Infrared Physics & Technology 102 (November 2019): 103002. http://dx.doi.org/10.1016/j.infrared.2019.103002.

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24

Belhassen, Jérémy, Zeev Zalevsky, and Avi Karsenty. "Optical Polarization Sensitive Ultra-Fast Switching and Photo-Electrical Device." Nanomaterials 9, no. 12 (December 7, 2019): 1743. http://dx.doi.org/10.3390/nano9121743.

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Ultra-fast electrical switches activated with an optical-polarized light trigger, also called photo-polarized activated electrical switches, are presented. A set of new transistor circuits is switched by light from above, illuminating deep V-grooves, whose angle is sensitive to the polarization of the incident. Thus, this application may serve for encryption/decryption devices since the strongest electrical responsivity is only obtained for very specific spatial polarization directions of the illumination beam. When this V-groove is sufficiently narrow, the device mainly responds to one polarization and not to the other. In such a way, electrons are generated only for one specific polarization. While the nature of the data remains electronic, the modulation control is optic, creating a photo-induced current depending on the polarization direction. This coupled device acts as a polarization modulator as well as an intensity modulator. The article focuses on the integration of several devices in different configurations of circuitry: dual, triple, and multi-element. Case studies of several adjacent devices are presented with varying critical variables, such as the V-groove aperture dimensions. Analytical models and complementary numerical analyses are presented for the future smooth integration into Complementary Metal-Oxide-Semiconductor (CMOS) technology.

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25

Xu, Lei, Jin Nan Zhang, Yan Gan Zhang, and Mi Lin. "Application of a Novel Modulation Scheme of PS-RZ-QPSK Signal in High-Speed Optical Transmission System." Applied Mechanics and Materials 347-350 (August 2013): 1879–83. http://dx.doi.org/10.4028/www.scientific.net/amm.347-350.1879.

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Modulation principle of dual-polarization quadratu-re phase shift keying signal and polarization-switched QPSK signal are demonstrated and advantages of PS-QPSK are proved in theoretically. A novel modulation scheme of PS-RZ-QPSK signal is proposed in this paper. The scheme reduces transmitter cost by less use of Mach-Zehnder modulator, but also presents similar performance as traditional structure for PS-RZ-QPSK. The simulate result indicates PS-RZ-QPSK can achieve a better transmission performance than DP-RZ-QPSK at the same bit rate (84Gb/s) and baud rate (28GBd), and proves showing the feasibility of novel modulation scheme.

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26

Min-Cheol Oh and Sang-Yung Shin. "Polymeric polarization-independent modulator incorporating twisted optic-axis waveguide polarization converters." IEEE Photonics Technology Letters 8, no. 11 (November 1996): 1483–85. http://dx.doi.org/10.1109/68.541557.

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27

Xu, Zhongyang, Hongxiang Zhang, Kai Chen, and Shilong Pan. "Compact All-Fiber Polarization Coherent Lidar Based on a Polarization Modulator." IEEE Transactions on Instrumentation and Measurement 69, no. 5 (May 2020): 2193–98. http://dx.doi.org/10.1109/tim.2019.2921053.

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28

MOROHASHI, Isao, Takahide SAKAMOTO, Masaaki SUDO, Atsushi KANNO, Akito CHIBA, Junichiro ICHIKAWA, and Tetsuya KAWANISHI. "Synthesis of 16 Quadrature Amplitude Modulation Using Polarization-Multiplexing QPSK Modulator." IEICE Transactions on Communications E94-B, no. 7 (2011): 1809–14. http://dx.doi.org/10.1587/transcom.e94.b.1809.

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29

WANG Zhi-bin, 王志斌, 张瑞 ZHANG Rui, 赵冬娥 ZHAO Dong-e, 陈友华 CHEN You-hua, and 魏海潮 WEI Hai-chao. "Photoelastic-modulator-based differential frequency polarization modulation measurement and error analysis." Optics and Precision Engineering 21, no. 4 (2013): 876–83. http://dx.doi.org/10.3788/ope.20132104.0876.

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30

Qi, Bing, Lei-Lei Huang, Hoi-Kwong Lo, and Li Qian. "Polarization insensitive phase modulator for quantum cryptosystems." Optics Express 14, no. 10 (2006): 4264. http://dx.doi.org/10.1364/oe.14.004264.

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31

Campillo, A. L. "Polarization-based single-sideband suppressed carrier modulator." IEEE Photonics Technology Letters 18, no. 16 (August 2006): 1780–82. http://dx.doi.org/10.1109/lpt.2006.880768.

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32

Xue-Feng, Huang, Yu Guo-Xian, and Zhang Hai-Ting. "Interferometric waveguide modulator with polarization-independent operation." Microwave and Optical Technology Letters 2, no. 3 (March 1989): 101–3. http://dx.doi.org/10.1002/mop.4650020308.

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33

He, Xiaoying, Jiale Su, and Lan Rao. "Controllable polarization electro-optic absorption graphene modulator." Engineering Research Express 2, no. 4 (December 18, 2020): 045033. http://dx.doi.org/10.1088/2631-8695/abd1e5.

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34

Tsai, Tsung-Han, Xin Yuan, and David J. Brady. "Spatial light modulator based color polarization imaging." Optics Express 23, no. 9 (April 28, 2015): 11912. http://dx.doi.org/10.1364/oe.23.011912.

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35

Chuss, David T., Edward J. Wollack, Ross Henry, Howard Hui, Aaron J. Juarez, Megan Krejny, S. Harvey Moseley, and Giles Novak. "Properties of a variable-delay polarization modulator." Applied Optics 51, no. 2 (January 10, 2012): 197. http://dx.doi.org/10.1364/ao.51.000197.

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36

Spickermann, R., M. G. Peters, and N. Dagli. "A polarization independent GaAs-AlGaAs electrooptic modulator." IEEE Journal of Quantum Electronics 32, no. 5 (May 1996): 764–69. http://dx.doi.org/10.1109/3.492998.

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37

Khaleque, Abdul, and Haroldo T. Hattori. "Plasmonic electro-absorption modulator and polarization selector." Journal of Modern Optics 64, no. 12 (December 12, 2016): 1164–74. http://dx.doi.org/10.1080/09500340.2016.1267814.

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38

Hsu, Chia-Wei, Chih-Fan Huang, Wan-Shao Tsai, and Way-Seen Wang. "Lithium Niobate Polarization-Independent Modulator Using Integrated Polarization Splitters and Mode Converters." Journal of Lightwave Technology 35, no. 9 (May 1, 2017): 1663–69. http://dx.doi.org/10.1109/jlt.2016.2642203.

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39

Hua, Chu Yi, Menke Neimule, Jie Zhou, Chen Zhang, and Peng Wang. "Theoretical Simulation and Preparation of Magneto-Optical Modulator." Advanced Materials Research 403-408 (November 2011): 2368–73. http://dx.doi.org/10.4028/www.scientific.net/amr.403-408.2368.

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Magneto-Optical modulation technology has become key component in many optical information systems. However, due to the abstract theoretical knowledge, many textbooks do not introduce the properties of circular anisotropy, so it is difficult for most students to understand the polarization properties of light accurately and in depth. In this paper, the processes of Magneto-Optical modulation are Three-Dimensionally dynamically simulated by using MATLAB software first. These simulations make the complex and abstract light propagation processes become visual, which are effective aids for optics’ teaching. These simulations can enhance the understanding of the concept and the interactions with media of polarized lights and the principles of Magneto-Optical modulation. Second, a magnetic rotation glass is used to produce Magneto-Optical modulator, and finally the optical communication simulation experiment is realized and the effect is good. Experimental results show that the magneto-optical modulator has advantages like low power requirements, low modulation voltage, simple device, flexible, long life-time and small affect to the external temperature etc.

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40

Chen, Zhen, Bo Liu, Shengjie Wang, and Enhai Liu. "Polarization-modulated three-dimensional imaging using a large-aperture electro-optic modulator." Applied Optics 57, no. 27 (September 12, 2018): 7750. http://dx.doi.org/10.1364/ao.57.007750.

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41

Liu, Xinkai, Wei Pan, Xihua Zou, Lianshan Yan, Bin Luo, and Bing Lu. "Investigation on Tunable Modulation Index in the Polarization-Modulator-Based Optoelectronic Oscillator." IEEE Journal of Quantum Electronics 50, no. 2 (February 2014): 68–73. http://dx.doi.org/10.1109/jqe.2013.2294378.

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42

Ciddor, P. E., and Hariharan P. "Broad-band polarization-insensitive optical-path-length modulator." Journal of Modern Optics 48, no. 1 (January 20, 2001): 15–19. http://dx.doi.org/10.1080/09500340119001.

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43

Chen, Tien-Kjng, Jer-Mlng Hsu, and Shu-Hsia Chen. "In-Line Fiber Polarization Selector and Intensity Modulator." Molecular Crystals and Liquid Crystals Science and Technology. Section A. Molecular Crystals and Liquid Crystals 304, no. 1 (September 1997): 415–21. http://dx.doi.org/10.1080/10587259708046990.

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44

Jung, H. S., H. F. Taylor, and O. Eknoyan. "Interferometric polarization-independent modulator in LiTaO/sub 3/." Journal of Lightwave Technology 8, no. 10 (1990): 1452–55. http://dx.doi.org/10.1109/50.59180.

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45

Fuller, Gerald G., and Kirk J. Mikkelsen. "Note: Optical Rheometry Using a Rotary Polarization Modulator." Journal of Rheology 33, no. 5 (July 1989): 761–69. http://dx.doi.org/10.1122/1.550064.

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46

Jen, Yi-Jun. "Near-perfect modulator for polarization state of light." Journal of Nanophotonics 2, no. 1 (November 1, 2008): 029504. http://dx.doi.org/10.1117/1.3039081.

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47

Schaal, Frederik, Michael Rutloh, Susanne Weidenfeld, Joachim Stumpe, Peter Michler, Christof Pruss, and Wolfgang Osten. "Optically addressed modulator for tunable spatial polarization control." Optics Express 26, no. 21 (October 12, 2018): 28119. http://dx.doi.org/10.1364/oe.26.028119.

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48

Chen, Zi-Yu, and Alexander Pukhov. "Plasma-based polarization modulator for high-intensity lasers." Physics of Plasmas 23, no. 12 (December 2016): 123107. http://dx.doi.org/10.1063/1.4971232.

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49

Stubbe, R., G. Edwall, B. Sahlgren, L. Svahn, P. Granestrand, and L. Thylen. "Polarization selective phase modulator in LiNbO/sub 3/." IEEE Photonics Technology Letters 2, no. 3 (March 1990): 187–90. http://dx.doi.org/10.1109/68.50885.

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50

Kashyap, R., C. S. Winter, and B. K. Nayar. "Polarization-desensitized liquid-crystal overlay optical-fiber modulator." Optics Letters 13, no. 5 (May 1, 1988): 401. http://dx.doi.org/10.1364/ol.13.000401.

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