Phase-dependent double optomechanically induced transparency in a hybrid optomechanical cavity system with coherently mechanical driving
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摘要
We propose a scheme that can generate tunable double optomechanically induced transparency in a hybrid optomechanical cavity system.In this system, the mechanical resonator of the optomechanical cavity is coupled with an additional mechanical resonator and the additional mechanical resonator can be driven by a weak external coherently mechanical driving field.We show that both the intensity and the phase of the external mechanical driving field can control the propagation of the probe field, including changing the transmission spectrum from double windows to a single-window.Our study also provides an effective way to generate intensity-controllable, narrow-bandwidth transmission spectra, with the probe field modulated from excessive opacity to remarkable amplification.
We propose a scheme that can generate tunable double optomechanically induced transparency in a hybrid optomechanical cavity system.In this system, the mechanical resonator of the optomechanical cavity is coupled with an additional mechanical resonator and the additional mechanical resonator can be driven by a weak external coherently mechanical driving field.We show that both the intensity and the phase of the external mechanical driving field can control the propagation of the probe field, including changing the transmission spectrum from double windows to a single-window.Our study also provides an effective way to generate intensity-controllable, narrow-bandwidth transmission spectra, with the probe field modulated from excessive opacity to remarkable amplification.
We propose a scheme that can generate tunable double optomechanically induced transparency in a hybrid optomechanical cavity system.In this system, the mechanical resonator of the optomechanical cavity is coupled with an additional mechanical resonator and the additional mechanical resonator can be driven by a weak external coherently mechanical driving field.We show that both the intensity and the phase of the external mechanical driving field can control the propagation of the probe field, including changing the transmission spectrum from double windows to a single-window.Our study also provides an effective way to generate intensity-controllable, narrow-bandwidth transmission spectra, with the probe field modulated from excessive opacity to remarkable amplification.
引文
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[2]Andrews R W, Peterson R W, Purdy T P, Cicak K, Simmonds R W,Regal C A and Lehnert K W 2014 Nat.Phys.10 321
[3]Verhagen E, Delaiaeglise S, Weis S, Schliesser A and Kippenberg T J2012 Nature 482 63
[4]Bochmann J, Vainsencher A, Awschalom D D and Cleland A N 2013Nat.Phys.9 712
[5]Balram K C, Davanco M I, Song J D and Srinivasan K 2016 Nat.Photon.10 346
[6]Jing C, Cui Y S, Liu H X, Li X W and Chen G B 2018 Chin.Phys.B27 24204
[7]Liu Y L, Wang C, Zhang J and Liu Y X 2018 Chin.Phys.B 27 24204
[8]Wu S C, Qin L G, Jing J, Yang G H and Wang Z Y 2016 Chin.Phys.B25 54203
[9]Aspelmeyer M, Kippenberg T J and Marquardt F 2014 Rev.Mod.Phys.86 1391
[10]Fan L, Fong K Y, Poot M and Tang H X 2015 Nat.Commun.6 5850
[11]Weis S, Riviere R, Deleglise S, Gavartin E, Arcizet O, Schliesser A and Kippenberg T J 2010 Science 330 1520
[12]Xiao Y, Yu Y F and Zhang Z M 2014 Opt.Express 22 17979
[13]Jinag C, Cui Y S, Zhai Z Y, Yu H L, Li X W and Chen G B 2018 Opt.Express 26 28834
[14]Yang Q, Hou B P and Lai D G 2017 Opt.Express 25 9697
[15]Xiong H and Wu Y 2018 Appl.Phys.Rev.5 031305
[16]Lin Q, Rosenberg J, Chang D, Camacho R, Eichenfield M, Vahala K J and Painter O 2010 Nat.Photon.4 236
[17]Ma P C, Zhang J Q, Xiao Y, Feng M and Zhang Z M 2014 Phys.Rev.A 90 043825
[18]Regal C, Teufel J and Lehnert K 2008 Nat.Phys.4 555
[19]Sanchez D G, Daiaeleglise S, Thomas J L, Atkinson P, Lagoin C and Perrin B 2016 Phys.Rev.A 94 033813
[20]Balram K C, Davanco M I, Ilic B R, Kyhm J H, Song J D and Srinivasan K 2017 Phys.Rev.Appl.7 024008
[21]Zhang J Q, Li Y, Feng M and Xu Y 2012 Phys.Rev.A 86 053806
[22]Gaidarzhy A, Zolfagharkhani G, Badzey R L and Mohanty P 2005Phys.Rev.Lett.94 030402
[23]Xue F, Wang Y D, Sun C P, Okamoto H, Yamaguchi H and Semba K2007 New J.Phys.9 35
[24]Wang Q, Zhang J Q, Ma P C, Yao C M and Feng M 2015 Phys.Rev.A91 063827
[25]Zhang H, Saif F, Jiao Y and Jing H 2018 Opt.Express 26 25199
[26]Agarwal G S and Huang S 2010 Phys.Rev.A 81 041803
[27]Xiang Z L, Ashhab S, You J Q and Nori F 2013 Rev.Mod.Phys.85 623
[28]Safavi-Naeini A H, Alegre T M, Chan J, Eichenfield M, Winger M, Lin Q, Hill J T, Chang D E and Painter O 2011 Nat.(London)472 69
[29]Jia W Z, Wei L F, Li Y and Liu Y X 2015 Phys.Rev.A 91 043843
[30]Harris S E 1997 Phys.Today 50 36
[31]Boller K J, Imamoglu A and Harris S E 1991 Phys.Rev.Lett.66 2593
[32]Xu J and Huang G 2013 Opt.Express 25 33575
[33]Cheng H, Wang H M, Zhang S S, Xin P P, Luo J and Liu H P 2017 Opt.Express 472 69
[34]Bienert M and Blostein P B 2015 Phys.Rev.A 91 023818
[35]Zhang S, Zhang J Q, Zhang J, Wu C W, Wu W and Chen P X 2014 Opt.Express 22 28118
[36]Akram M J, Khan M M and Saif F 2015 Phys.Rev.A 92 023846
[37]Jiang C, Liu H, Cui Y, Li X, Chen G and Chen B 2013 Opt.Express 2112165
[38]Stannigel K, Rabl P, Sorensen A S, Lukin M D and Zoller P 2011 Phys.Rev.A 84 042341
[39]Mcgeev S A, Meiser D, Regal C A, Lehnert K W and Holland M J 2013Phys.Rev.A 87 053818
[40]Wu Q, Zhang J Q, Wu J H, Feng M and Zhang Z M 2015 Opt.Express23 18534
[41]Li L C, Shi R, Xu J and Hu X M 2015 Chin.Phys.B 24 054205
[42]Wang H, Gu X, Liu Y X, Miranowicz A and Nori F 2014 Phys.Rev.A90 023817
[43]Qu K and Agarwal G S 2013 Phys.Rev.A 87 031802
[44]Gu W G and Yi Z 2014 Opt.Commun.333 261
[45]Wu S C, Qin L G, Jing J, Yan T M, Lu J and Wang Z Y 2018 Phys.Rev.A 98 013807
[46]Harris S E and Yamamoto Y 1998 Phys.Rev.Lett.81 3611
[47]Yan M, Rickey E G and Zhu Y 2001 Opt.Lett.26 548
[48]Barzanjeh S and Vitali D 2016 Phys.Rev.A 93 033846
[49]Xu X W, Liu Y, Sun C P and Li Y 2015 Phys.Rev.A 92 013852
[50]Santos E G, Ramos D, Pini V, Calleja M and Tamayo J 2011 Appl.Phys.Lett.98 123108
[51]Luo G, Zhang Z Z, Deng G W, Li H O, Cao G, Xiao M, Guo G C, Tian L and Guo G P 2018 Nat.Commun.9 383
[52]Karabalin R B, Cross M C and Roukes M L 2009 Phys.Rev.B 79165309
[53]Huang P, Wang P F, Zhou J W, Wang Z X, Ju C Y, Wang Z M, Yang S,Duan C K and Du J F 2013 Nat.Phys.9 480
[54]Okamoto H, Gourgout A, Chang C Y, Onomitsu K, Mahboob I, Chang E Y and Yamaguchi H 2013 Nat.(London)472 69
[55]Zou C L, Han X, Jiang L and Tang H X 2016 Phys.Rev.A 94 013812
[56]Han X, Zou C L and Tang H X 2016 Phys.Rev.Lett.117 123603
[57]Cleland A N and Geller M R 2004 Phys.Rev.Lett.93 070501
[58]Oaarconnell A D, Hofheinz M, Ansmann M, Bialczak R C, Lenander M, Lucero E, Neeley M, Sank D, Wang H and Weides M 2010 Nature464 697
[59]Xu X W and Li Y 2015 Phys.Rev.A 92 69
[60]Si L G, Xiong H, Zubairy M S and Wu Y 2017 Phys.Rev.A 95 033803
[61]Ma J, You C, Si L G, Xiong H, Li J, Yang X and Wu Y 2015 Sci.Rep.5 11278
[62]Barzanjeh S, Vitali D, Tombesi P and Milburn G J 2011 Phys.Rev.A84 042342
[63]Huang S and Agarwal G S 2011 Phys.Rev.A 83 023823
[64]Cleland A 2009 Nat.Phys.5 458
[65]Alotaibi H M M and Sanders B C 2014 Phys.Rev.A 89 021802
[66]Simon G, Klemens H, Vanner M R and Markus A 2009 Nat.(London)460 724
[67]Yan M, Rickey E G and Zhu Y 2001 Phys.Rev.A 64 041801
[68]Li S, Yang X, Cao X, Zhang C, Xie C and Wang H 2008 Phys.Rev.Lett.101 073602
[69]Balic V, Braje D A, Kolchin P, Yin G Y and Harris S E 2005 Phys.Rev.Lett.94 183601
[70]Kumar P and Dasgupta S 2016 Phys.Rev.A 94 023851
[71]Harris S E and Hau L V 1999 Phys.Rev.Lett.82 4611