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Optical resonator with high Q value can be used as a core component of the resonator optic gyro, with which the miniaturization and integration would be achieved. The coupling system composed of the disk cavity which is made by traditional micro-electro-mechanical system process and the tapered fiber which is drawn by melting method. When the disk cavity is coupled with the fiber at different places of the tapered region, by swapping input and output there is observed the deviation in the output transmission spectrum, also the resonant frequency, coupling efficiency and the Q value are changed, i.e., the non-reciprocity phenomenon appears. Then the distribution characteristics of the tapered fiber evanescent field are simulated with Rsoft software. The reason of the non-reciprocity is analyzed theoretically. According to the statistics of the output data when the disk cavity is coupled with the fiber at different places of the tapered region, it is found that the non-reciprocity can be eliminated effectively when the coupling happens at the center of the fiber tapered region. And this finding can be used to suppress the non-reciprocity noise produced by the coupling system composed of tapered fiber and resonant cavity in the resonator optic gyros application.
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Keywords:
- optical resonator /
- tapered fiber /
- non-reciprocity /
- resonator optic gyros
[1] Li Q, Eftekhar A A, Sodagar M, Xia Z, Atabaki A H, Adibi A 2013 Opt. Express 21 18236
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[9] Wang R M, Wang X P, Wu Z K, Yao X, Zhang Y Q, Zhang Y P 2014 Chin. Phys. B 23 054209
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[14] Yan Y Z, Zou C L, Yan S B, Sun F W, Ji Z, Liu J, Xiong J J 2011 Opt. Express 19 5753
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[16] Cai M, Painter O, Vahala K J 2000 Phys. Rev. Lett. 85 74
[17] Li J, Ji Z, Yan Y Z, Liu Z, Liu J, Yan S B 2011 Nano Tech. 2 33 (in Chinese) [李杰, 吉喆, 严英占, 刘正, 刘俊, 闫树斌 2011 纳米科技 2 33]
[18] Wang K, Feng L, Wang J, Lei M 2013 Appl. Opt. 52 1481
[19] Hong L F, Zhang C X, Feng L S, Yu H Y, Lei M 2012 Chin. Phys. Lett. 29 14211
[20] Yan Y Z, Ji Z, Wang B H, Yan S B, Xiong J J, Ma J 2010 Chin. J. Laser 7 1789 (in Chinese) [严英占, 吉喆, 王宝花, 闫树斌, 熊继军,马骏 2010 中国激光 7 1789]
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[1] Li Q, Eftekhar A A, Sodagar M, Xia Z, Atabaki A H, Adibi A 2013 Opt. Express 21 18236
[2] Bo F, Huang S H, Ozdemir S K, Zhang G, Xu J, Yang L 2013 Opt. Phys. 25 1311
[3] Zhai Y, Chen S W, Ren G H 2010 Chin. Phys. Lett. 27 104203
[4] Zhang L B, Chen S W, Fei Y H, Cao T T, Cao Y M, Lei X 2013 Acta Phys. Sin. 62 194201 (in Chinese) [张利斌, 陈少武, 费永浩, 曹彤彤, 曹严梅, 雷勋 2013 物理学报 62 194201]
[5] Lang J H 2011 Chin. Phys. Lett. 28 204210
[6] Matsko A B, Savchenkov A A, Yu N, Maleki L 2007 J. Opt. Soc. Am. B 24 1324
[7] Zhu J, Ozdemir S K, Xiao Y F, Li L, He L, Chen D R, Yang L 2010 Nat. Photon. 4 46
[8] Li J 2013 Ph. D. Dissertation (California: California Institute of Technology)
[9] Wang R M, Wang X P, Wu Z K, Yao X, Zhang Y Q, Zhang Y P 2014 Chin. Phys. B 23 054209
[10] DelHaye P, Herr T, Gavartin E, Gorodetsky M L, Holzwarth R, Kippenberg T J 2011 Phys. Rev. Lett. 107 063901
[11] Lee H, Chen T, Li J, Yang K Y, Jeon S, Painter O, Vahala K J 2012 Nat. Photon. 6 369
[12] Schell A W, Kaschke J, Fischer J, Henze R, Wolters J, Wegener M, Benson O 2013 Sci. Rep. 10 1038
[13] Monifi F, Odemir S K, Friedlein J, Yang L 2013 IEEE Photon. Tech. L 25 1458
[14] Yan Y Z, Zou C L, Yan S B, Sun F W, Ji Z, Liu J, Xiong J J 2011 Opt. Express 19 5753
[15] Niehusmann J, Vörckel A, Bolivar P H, Wahlbrink T, Henschel W, Kurz H 2004 Opt. Lett. 29 2861
[16] Cai M, Painter O, Vahala K J 2000 Phys. Rev. Lett. 85 74
[17] Li J, Ji Z, Yan Y Z, Liu Z, Liu J, Yan S B 2011 Nano Tech. 2 33 (in Chinese) [李杰, 吉喆, 严英占, 刘正, 刘俊, 闫树斌 2011 纳米科技 2 33]
[18] Wang K, Feng L, Wang J, Lei M 2013 Appl. Opt. 52 1481
[19] Hong L F, Zhang C X, Feng L S, Yu H Y, Lei M 2012 Chin. Phys. Lett. 29 14211
[20] Yan Y Z, Ji Z, Wang B H, Yan S B, Xiong J J, Ma J 2010 Chin. J. Laser 7 1789 (in Chinese) [严英占, 吉喆, 王宝花, 闫树斌, 熊继军,马骏 2010 中国激光 7 1789]
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