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Thematische Bibliographien / Cladding Magnets / Zeitschriftenartikel

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Zeitschriftenartikel zum Thema „Cladding Magnets“

Autor: Grafiati

Veröffentlicht am 25. Juni 2021

Zuletzt aktualisiert am 4. Februar 2022

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1

Jalas, Dirk, Alexander Petrov, Michael Krause, Jan Hampe, and Manfred Eich. "Integrated Non Reciprocal Ring Resonators." Advanced Materials Research 216 (March 2011): 533–38. http://dx.doi.org/10.4028/www.scientific.net/amr.216.533.

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We present the theoretical concept of an optical isolator based on a resonance splitting in a silicon ring resonators covered by a magneto-optical polymer cladding. A polymer magneto optical cladding causing a 0.01 amplitude of the off-diagonal element of the dielectric tensor is assumed. Using a perturbation method it is shown that the resonance splitting of the clockwise and counter-clockwise modes increases for smaller ring radii. For the ring with a radius of approximately 1.5μm a 29GHz splitting is demonstrated. An optical isolator is proposed based on a critically coupled ring resonator.

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2

Li Hongbo, 李洪波, 高强强 Gao Qiangqiang, 李康英 Li Kangying та 李班 Li Ban. "表面激光熔覆H13/NiCr-Cr3C2复合粉末熔覆层性能研究". Chinese Journal of Lasers 48, № 18 (2021): 1802017. http://dx.doi.org/10.3788/cjl202148.1802017.

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3

Chen, Qiuling, Hui Wang, Qingwei Wang, and Qiuping Chen. "Properties of tellurite core/cladding glasses for magneto-optical fibers." Journal of Non-Crystalline Solids 400 (September 2014): 51–57. http://dx.doi.org/10.1016/j.jnoncrysol.2014.05.001.

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4

Wang, Wei, Peng Qi, Guang Yang, et al. "Effects of Permanent Magnet Electromagnetic Stirring on TA15 Laser Metal Deposition." Materials Science Forum 723 (June 2012): 471–75. http://dx.doi.org/10.4028/www.scientific.net/msf.723.471.

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Electromagnetic stirring (EMS) is an important method to homogenize the hard phase of the cladding layer. Rotary Permanent magnet electromagnetic stirring (PEMS) is adopted during the experiment. The changes of heat affected zone, solidification character, microstructure and hardness of TA15 Laser Metal Deposition (LMD) based on PEMS have been researched during the experiment. The results show that the PEMS can refine the grain, homogenize the microstructure, eliminate the disfigurement and enhance the hardness.

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5

Mahmoud, Essam R. I., Vineet Tirth, Ali Algahtani, and Sohaib Z. Khan. "Microstructural characterization of different metal matrix composite claddings reinforced by TiC through YAG laser cladding." Materials Research Express 7, no. 6 (2020): 066407. http://dx.doi.org/10.1088/2053-1591/ab9bc4.

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6

Liu, Rui, Dapeng Yan, Ming Chen, Jianming Wang, Jianhong Shi, and Qixin Zhu. "Enhanced cladding pump absorption of ytterbium-doped double cladding fiber with internally modified cladding structures." Optical Materials Express 10, no. 1 (2019): 36. http://dx.doi.org/10.1364/ome.10.000036.

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7

Demirer, Figen Ece, Chris van den Bomen, Reinoud Lavrijsen, Jos J. G. M. van der Tol, and Bert Koopmans. "Design and Modelling of a Novel Integrated Photonic Device for Nano-Scale Magnetic Memory Reading." Applied Sciences 10, no. 22 (2020): 8267. http://dx.doi.org/10.3390/app10228267.

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Design and simulations of an integrated photonic device that can optically detect the magnetization direction of its ultra-thin (∼12 nm) metal cladding, thus ‘reading’ the stored magnetic memory, are presented. The device is an unbalanced Mach Zehnder Interferometer (MZI) based on InP Membrane on Silicon (IMOS) platform. The MZI consists of a ferromagnetic thin-film cladding and a delay line in one branch, and a polarization converter in the other. It quantitatively measures the non-reciprocal phase shift caused by the Magneto-Optic Kerr Effect in the guided mode which depends on the memory bit’s magnetization direction. The current design is an analytical tool for research exploration of all-optical magnetic memory reading. It has been shown that the device is able to read a nanoscale memory bit (400 × 50 × 12 nm) by using a Kerr rotation as small as 0.2∘, in the presence of a noise ∼10 dB in terms of signal-to-noise ratio. The device is shown to tolerate performance reductions that can arise during the fabrication.

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8

Agruzov, Petr M., Ivan V. Pleshakov, Efim E. Bibik, and Alexander V. Shamray. "Magneto-optic effects in silica core microstructured fibers with a ferrofluidic cladding." Applied Physics Letters 104, no. 7 (2014): 071108. http://dx.doi.org/10.1063/1.4866165.

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9

Kim, Yookyung, Byungrok Moon, Namhyun Kang, and Eun-Joon Chun. "Effect of Cladding Conditions on Solidification Cracking Behavior during Dissimilar Cladding of Inconel Alloy FM 52 and 308L Stainless Steel to Carbon Steel: Evaluation of Solidification Brittle Temperature Range by Transverse−Varestraint Test." Korean Journal of Metals and Materials 58, no. 6 (2020): 403–12. http://dx.doi.org/10.3365/kjmm.2020.58.6.403.

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In this study, solidification cracking behavior and susceptibility in dissimilar cladding of Inconel alloy FM 52, 308L stainless steel to carbon steel, was investigated by submerged arc welding and transverse−Varestraint testing with gas tungsten arc welding. The effect of cladding conditions on cracking behavior and susceptibility was extensively evaluated, and metallurgical factors affecting susceptibility were clarified. Depending on the cladding sequence (cladding combination A: Inconel 52→308L, cladding combination B: 308L→Inconel 52), opposite types of solidification cracking behavior were observed. Specifically, solidification cracking was observed only for cladding combination A. Using transverse−Varestraint tests, the solidification brittle temperature range (BTR) was determined to be 298 K for cladding combination A and 200 K for cladding combination B. The reason for solidification cracking in cladding combination A could be its higher solidification susceptibility (i.e., a larger BTR (298 K)) compared with cladding combination B (BTR: 200 K). To elucidate differences in solidification cracking susceptibility, a numerical simulation of non−equilibrium solidification segregation for impurity elements (P, S) was performed, based on velocity dependent solidification theories and the finite differential method. Different segregation behaviors were calculated upon the cladding combinations. The severe segregation of P and S during solidification was found to be one of the important metallurgical factors for the large BTR of cladding combination A, compared with cladding combination B.

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10

Guyard, Romain, Dominique Leduc, Cyril Lupi, and Yann Lecieux. "Critical cladding radius for hybrid cladding modes." Optics & Laser Technology 101 (May 2018): 116–26. http://dx.doi.org/10.1016/j.optlastec.2017.11.002.

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11

Kono, Naoya, and Masanori Koshiba. "Magneto-Photonic Crystal Slab Waveguides With Lower-Refractive-Index-Silica Claddings." IEEE Photonics Technology Letters 19, no. 5 (2007): 258–60. http://dx.doi.org/10.1109/lpt.2006.890042.

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12

Nielsen, M. L., M. O. Berendt, A. Bjarklev, and M. G. Dyndgaard. "Design of Matched Cladding Fiber with UV-Sensitive Cladding for Minimization of Cladding-Mode Losses in Fiber Bragg Gratings." Optical Fiber Technology 6, no. 1 (2000): 49–60. http://dx.doi.org/10.1006/ofte.1999.0309.

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13

Ji, Encai, Jie Shi, Congwen Zha, et al. "Ultimate capacity analysis of cladding-pumped 10/130 Tm:fiber laser." Chinese Optics Letters 18, no. 5 (2020): 051404. http://dx.doi.org/10.3788/col202018.051404.

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14

Hu, Junjiang, Liyan Zhang, Jiachuan Ni, et al. "Experimental investigation on residual reflectance of Nd:glass amplifier edge cladding." Chinese Optics Letters 18, no. 9 (2020): 091402. http://dx.doi.org/10.3788/col202018.091402.

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15

S. Baek, D. B. S. Soh, Y. Jeong, J. K. Sahu, J. Nilsson, and B. Lee. "A Cladding-Pumped Fiber Laser With Pump-Reflecting Inner-Cladding Bragg Grating." IEEE Photonics Technology Letters 16, no. 2 (2004): 407–9. http://dx.doi.org/10.1109/lpt.2003.823135.

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16

Sui, Guanghui, Huanhuan Liu, Fufei Pang, Jiajing Cheng, and Tingyun Wang. "Broadband Acoustic Vibration Sensor Based on Cladding-Mode Resonance of Double-Cladding Fiber." Photonic Sensors 9, no. 3 (2019): 230–38. http://dx.doi.org/10.1007/s13320-019-0548-7.

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17

Yoshida, Kazuaki, and Takayuki Morikawa. "Optical Fibers with Polygonal Cladding." Optical Fiber Technology 3, no. 3 (1997): 273–77. http://dx.doi.org/10.1006/ofte.1997.0222.

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18

Zhao, Yu, Chuang Guan, Liaoyuan Chen, Jiayu Sun, and Tianbiao Yu. "Effect of process parameters on the cladding track geometry fabricated by laser cladding." Optik 223 (December 2020): 165447. http://dx.doi.org/10.1016/j.ijleo.2020.165447.

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19

Grueninger, A., M. Hustedt, D. Herzog, et al. "Surface texturing by laser cladding." Journal of Laser Applications 23, no. 2 (2011): 022008. http://dx.doi.org/10.2351/1.3573371.

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20

Castano, Catalina Hurtado, Rodrigo Acuna Herrera, and Pedro I. Torres. "Modeling Nonlinear Acoustooptic Coupling in Fiber Optics Based on Refractive Index Variation due to Local Bending." Advances in Optical Technologies 2016 (September 18, 2016): 1–10. http://dx.doi.org/10.1155/2016/3696094.

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A detailed procedure is presented to compute analytically the acoustooptic coupling coefficient between copropagating core and lowest-order cladding modes in tapered fiber optics. Based on the effect of the local bending, the linear and nonlinear variations in the refractive index are modeled. A set of equations and parameters are presented in order to calculate the influence of acoustooptic effect in nonlinear pulse propagation. We will show that as the tapered fiber diameter decreases more energy can be transferred to the cladding and the nonlinear phenomena can compensate the coupling coefficients effects.

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21

Vekris, A., A. Royère, G. Campet, et al. "DNA Cladding with Inorganic Sulphide Nanoparticles." Active and Passive Electronic Components 21, no. 3 (1998): 183–87. http://dx.doi.org/10.1155/1998/21798.

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The formation of CdS and CoS2nanoparticles along the DNA strands have been studied. The systems DNA-Cdl2and DNA-CoCl2have been investigated in the solid state in order to form DNA-MX2complex salts used as precursors. They react with S2-ions giving birth to CdS and CoS2nanoparticles. A model describing the DNA-nanosulphide association is proposed.

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22

Chen, Na, Binfeng Yun, and Yiping Cui. "Cladding index modulated fiber grating." Optics Communications 259, no. 2 (2006): 587–91. http://dx.doi.org/10.1016/j.optcom.2005.09.017.

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23

Bashan, Gil, Yosef London, H. Hagai Diamandi, and Avi Zadok. "Distributed cladding mode fiber-optic sensor." Optica 7, no. 1 (2020): 85. http://dx.doi.org/10.1364/optica.377610.

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24

Weih, Robert, Adam Bauer, Martin Kamp, and Sven Höfling. "Interband cascade lasers with AlGaAsSb bulk cladding layers." Optical Materials Express 3, no. 10 (2013): 1624. http://dx.doi.org/10.1364/ome.3.001624.

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25

Wang Pengfei, 王鹏飞, 杨坤 Yang Kun, 陈明智 Chen Mingzhi та ін. "倾斜基板激光熔覆GH3536熔池形貌的仿真与实验研究". Chinese Journal of Lasers 48, № 10 (2021): 1002121. http://dx.doi.org/10.3788/cjl202148.1002121.

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26

Li Jinhua, 李金华, 安学甲 An Xuejia, 姚芳萍 Yao Fangping та 侯艳 Hou Yan. "H13钢激光熔覆Ni基涂层热应力循环的仿真研究". Chinese Journal of Lasers 48, № 10 (2021): 1002104. http://dx.doi.org/10.3788/cjl202148.1002104.

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27

Xu Yifei, 徐一飞, 孙耀宁 Sun Yaoning, 王国建 Wang Guojian та 贵永亮 Gui Yongliang. "高速激光熔覆铁基合金涂层的组织及性能研究". Chinese Journal of Lasers 48, № 10 (2021): 1002122. http://dx.doi.org/10.3788/cjl202148.1002122.

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28

Ju, Seongmin, Youngwoong Kim, Kadathala Linganna, Yune Hyoun Kim, and Won-Taek Han. "Effect of Temperature and Gamma-Ray Irradiation on Optical Characteristics of Fiber Bragg Grating Inscribed Radiation-Resistant Optical Fiber." Photonic Sensors 10, no. 1 (2019): 16–33. http://dx.doi.org/10.1007/s13320-019-0567-4.

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Abstract A new radiation-hard germano-silicate glass optical fiber with a pure silica glass buffer and a boron-doped silica glass inner cladding was fabricated for temperature sensor application based on the fiber Bragg grating (FBG) under γ-ray irradiation environment. The temperature dependences of optical attenuation at 1550.5 nm and Bragg reflection wavelength shift from 18 °C to 40 °C before the γ-ray irradiation were about 4.57×10−4 dB/ °C and 5.48 pm/ °C, respectively. The radiation-induced optical attenuation at 1550.5 nm and the radiation-induced Bragg reflection wavelength shift under the γ-ray irradiation with the total dose of 22.85kGy at 35 °C were about 0.03dB/m and 0.12nm, respectively, with the γ-ray irradiation sensitivity of 5.25×10−3 pm/Gy. The temperature and the γ-ray irradiation dependence of optical attenuation at 1550.5nm in the FBG written fiber with boron-doped silica glass inner cladding were about 6 times and 4 times lower than that in the FBG written fiber without boron-doped silica glass inner cladding under a temperature change from 18 °C to 40 °C and the γ-ray irradiation with the total dose of 22.85 kGy at 35 °C, respectively. Furthermore, the effect of temperature increase on the Bragg reflection wavelength of the FBG written fiber with boron-doped silica inner cladding was much larger about 1000 times than that of the γ-ray irradiation. However, no influence on the reflection power of the Bragg wavelengths and the full width at half maximum (FWHM) bandwidth under temperature and the γ-ray irradiation change was found. Also, after the γ-ray irradiation with the dose of 22.85kGy, no significant change in the refractive index was found but the residual stresses developed in the fiber were slightly relaxed or retained.

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29

Feng Tu, 涂峰, 刘德明 Deming Liu, 罗杰 Jie Luo, 钱新伟 Xinwei Qian, 杨晨 Chen Yang, and 邓涛 Tao Deng. "Low birefringence depressed cladding photosensitive fiber." Chinese Optics Letters 8, no. 1 (2010): 4–6. http://dx.doi.org/10.3788/col20100801.0004.

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30

Guo Yongli, 郭永利, 梁工英 Liang Gongying, and 李路 Li Lu. "Laser Cladding Reparation of Aluminum Alloy." Chinese Journal of Lasers 35, no. 2 (2008): 303–6. http://dx.doi.org/10.3788/cjl20083502.0303.

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31

Shen Bin, 沈斌, 闫广超 Yan Guangchao, and 吴钢 Wu Gang. "Laser Cladding on Complex Disc Cam." Chinese Journal of Lasers 36, no. 1 (2009): 244–48. http://dx.doi.org/10.3788/cjl20093601.0244.

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32

Yu-Hsin Su, Jyh-Shinn Yang, and Ching-Ray Chang. "Schwarz–Christoffel Transformation for Cladding Conducting Lines." IEEE Transactions on Magnetics 45, no. 10 (2009): 3800–3803. http://dx.doi.org/10.1109/tmag.2009.2022840.

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33

Valley, George C. "Modeling Cladding-Pumped Er/Yb Fiber Amplifiers." Optical Fiber Technology 7, no. 1 (2001): 21–44. http://dx.doi.org/10.1006/ofte.2000.0351.

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34

Doubenskaia, M., Ph Bertrand, and I. Smurov. "Optical monitoring of Nd:YAG laser cladding." Thin Solid Films 453-454 (April 2004): 477–85. http://dx.doi.org/10.1016/j.tsf.2003.11.184.

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35

Jing Ma, Jing Ma, Dongdong Liu Dongdong Liu, Jicheng Wang Jicheng Wang, and Zhengda Hu Zhengda Hu. "Plasmonic sensor with variable claddings based on metallic slit arrays." Chinese Optics Letters 16, no. 3 (2018): 032301. http://dx.doi.org/10.3788/col201816.032301.

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36

ZHU Hong-bo, 朱洪波, 张金胜 ZHANG Jin-sheng, 马军 MA Jun, 秦莉 QIN Li, 宁永强 NING Yong-qiang, and 王立军 WANG Li-jun. "10 kW CW diode laser cladding sources." Optics and Precision Engineering 21, no. 4 (2013): 829–34. http://dx.doi.org/10.3788/ope.20132104.0829.

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37

Kim, Jun Hwan, Hyeong Min Heo, and Sung Ho Kim. "Effect of an Intermediate Process on the Microstructure and Mechanical Properties of HT9 Fuel Cladding." Korean Journal Metals and Materials 51, no. 12 (2013): 893–900. http://dx.doi.org/10.3365/kjmm.2013.51.12.893.

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38

An Xianglong, 安相龙, 王玉玲 Wang Yuling, 姜芙林 Jiang Fulin, 张杰 Zhang Jie та 张金营 Zhang Jinying. "搭接率对42CrMo激光熔覆层温度场和残余应力分布的影响". Chinese Journal of Lasers 48, № 10 (2021): 1002110. http://dx.doi.org/10.3788/cjl202148.1002110.

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39

Zhu Ming, 朱明, 王博 Wang Bo, 颜步云 Yan Buyun, 杨骞 Yang Qian, 石玗 Shi Yu та 樊丁 Fan Ding. "激光熔覆过程预置粉末熔化行为的动态检测与分析". Chinese Journal of Lasers 48, № 14 (2021): 1402013. http://dx.doi.org/10.3788/cjl202148.1402013.

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40

Pekkarinen, Joonas, Antti Salminen, and Veli Kujanpää. "Laser cladding with scanning optics: Effect of scanning frequency and laser beam power density on cladding process." Journal of Laser Applications 26, no. 3 (2014): 032002. http://dx.doi.org/10.2351/1.4868895.

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41

Hou Shanglin, 侯尚林, 张书军 Zhang Shujun, 黎锁平 Li Suoping, 刘延君 Liu Yanjun, and 徐永钊 Xu Yongzhao. "Investigation on Transmission Characteristics of Doubly Cladding Fiber with an Inner Cladding Made of Negative Refractive-Index Material." Acta Optica Sinica 31, no. 5 (2011): 0506004. http://dx.doi.org/10.3788/aos201131.0506004.

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42

Wei, Wang, Hou Lan-Tian, Song Jun-Jie, and Zhou Gui-Yao. "Design of double cladding dispersion flattened photonic crystal fiber with deformation insensitive outer cladding air-holes." Optics Communications 282, no. 17 (2009): 3468–72. http://dx.doi.org/10.1016/j.optcom.2009.06.001.

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43

Fu, Xinghu, Yuepeng Zhang, Fan Liu, Guangwei Fu, and Weihong Bi. "A cascaded fiber sensor for measuring different curvature ranges based on the cladding mode resonance in double-cladding fiber." Optical Fiber Technology 50 (July 2019): 8–12. http://dx.doi.org/10.1016/j.yofte.2019.02.004.

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44

Korec, Joanna, Karol Antoni Stasiewicz, and Leszek Roman Jaroszewicz. "Temperature effect on the light propagation in a tapered optical fiber with a twisted nematic liquid crystal cladding." Photonics Letters of Poland 11, no. 1 (2019): 16. http://dx.doi.org/10.4302/plp.v11i1.881.

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This paper presents the influence of temperature on optical power spectrum propagated in a tapered optical fiber with twisted nematic liquid crystal cladding (TOF-TNLCC) modulated by an electric field. The measurements were performed for a liquid crystal cell with the twisted orientation of ITO layers, filled with E7 mixture. The induced reorientation of liquid crystal (LC) n-director was measured for visible and near-infrared wavelength range [550-1100 nm] at the electric field range of 0–160 V and temperature range of 20-60 °C. The relation between temperature and the optical power spectrum of the investigated device has been established. Full Text: PDF ReferencesV.J. Tekippe, "Passive fiber optic components made by the fused biconical taper process", Proc. SPIE 1085 (1990). CrossRef T. A. Birks, Y. W. Li, The shape of fiber tapers, Journal of Lightwave Technology 10, 4 (1992). CrossRef J. Korec, K. A. Stasiewicz, O. Strzeżysz, P. Kula, L. R. Jaroszewicz, Electro-Steering Tapered Fiber-Optic Device with Liquid Crystal Cladding, Journal of Sensors 2019: 1-11 (2019) CrossRef Ch. Veilleux, J. Lapierre, J. Bures, Liquid-crystal-clad tapered fibers, Opt. Lett. 11, 733-735 (1986) CrossRef J. F Henninot, D. Louvergneaux, N. Tabiryan, M. Warenghem, Controlled leakage of a tapered optical fiber with liquid crystal cladding, Molecular Crystals and Liquid Crystals, 282, 297-308. (1996). CrossRef Y. Wang, et.al., Tapered optical fiber waveguide coupling to whispering gallery modes of liquid crystal microdroplet for thermal sensing application, Opt. Express 25, 918-926 (2017) CrossRef J. Korec, K. A. Stasiewicz, O. Strzeżysz, P. Kula, L. R. Jaroszewicz, . E. Moś, Tapered fibre liquid crystal optical device, Proc. SPIE 10681 (2018) CrossRef G. Assanto, A. Picardi, R. Barboza, A. Alberucci, Electro-optic steering of Nematicons, Phot. Lett. Poland 4, 1 (2012). CrossRef A.Ghanadzadeh Gilani, M.S. Beevers, The Electro-optical kerr effect in eutectic nematic mixtures of E7 and E8,J ournal of Molecular Liquids, 92, 3 (2001). CrossRef E. C. Mägi, P. Steinvurzel, and B.J. Eggleton, Tapered photonic crystal fibers, Opt. Express 784, 12, 5 (2004). CrossRef Y. Li and J. Lit, Transmission properties of a multimode optical-fiber taper, J. Opt. Soc. Am. A 2, (1985). CrossRef J. Korec, K. A. Stasiewicz, and L. R. Jaroszewicz, Temperature influence on optical power spectrum of the tapered fiber device with a liquid crystal cladding, Proc. SPIE 11045, 110450I (2019) CrossRef L.M. Blinov, Liquid crystals: physical properties and their possibilities in application, Advances in Liquid Crystal Research and Applications, (1981). CrossRef

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Fujimura, Masatoshi, and Toshiaki Suhara. "Formation of MgO:LiNbO3 Domain-Inverted Gratings by Voltage Application under UV Light Irradiation at Room Temperature." Advances in OptoElectronics 2008 (October 30, 2008): 1–5. http://dx.doi.org/10.1155/2008/421054.

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MgO:LiNbO3 is an attractive nonlinear-optic crystal for quasiphasematched (QPM) nonlinear-optic devices. This paper reports a new formation method of domain-inverted gratings for QPM in MgO:LiNbO3. Domain inversion of MgO:LiNbO3 by voltage application under UV light was characterized, and reduction of the voltage required for inversion was demonstrated. Results of voltage application under periodic UV light suggested that suppression of excess lateral expansion of the domain inverted regions on −Z surface was crucial for domain-inverted grating formation. Voltage application to a crystal with a photoconductive cladding layer under periodic UV light was proposed. The cladding layer suppressed the expansion, and the domain-inverted gratings with period of 18 μm and area of 25×5 mm2 were obtained. The formation method does not require the photolithography process and allows the formation by voltage application at room temperature, and therefore, is quite simple and productive.

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Prabu, K., and R. Malavika. "Highly birefringent photonic crystal fiber with hybrid cladding." Optical Fiber Technology 47 (January 2019): 21–26. http://dx.doi.org/10.1016/j.yofte.2018.11.015.

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Sun Fujuan, 孙福娟, 胡芳友 Hu Fangyou, 黄旭仁 Huang Xuren, 王斌 Wang Bin, 卢常亮 Lu Changliang, and 胡滨 Hu Bin. "Fatigue Performance of Laser Cladding on LY12CZ." Chinese Journal of Lasers 35, no. 7 (2008): 1073–77. http://dx.doi.org/10.3788/cjl20083507.1073.

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Lin, Jehnming, and Bor-Chyang Hwang. "Coaxial laser cladding on an inclined substrate." Optics & Laser Technology 31, no. 8 (1999): 571–78. http://dx.doi.org/10.1016/s0030-3992(99)00116-4.

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Li, Hairong, Changjian Tang, and Pukun Liu. "Mode theory of the plasma cladding waveguide." Journal of Physics D: Applied Physics 40, no. 7 (2007): 2002–9. http://dx.doi.org/10.1088/0022-3727/40/7/023.

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50

Childs, Paul, Alessandro Candiani, and Stavros Pissadakis. "Optical Fiber Cladding Ring Magnetic Field Sensor." IEEE Photonics Technology Letters 23, no. 13 (2011): 929–31. http://dx.doi.org/10.1109/lpt.2011.2143397.

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