A scheme for Sagnac-effect quantum enhancement with Fock state light input

doi:10.1088/1674-1056/26/9/094212

中国物理B ›› 2017, Vol. 26 ›› Issue (9): 94212-094212.doi: 10.1088/1674-1056/26/9/094212

• ELECTROMAGNETISM, OPTICS, ACOUSTICS, HEAT TRANSFER, CLASSICAL MECHANICS, AND FLUID DYNAMICS • 上一篇下一篇

A scheme for Sagnac-effect quantum enhancement with Fock state light input

Kun Chen(陈坤), Shu-Xin Chen(陈树新), De-Wei Wu(吴德伟), Chun-Yan Yang(杨春燕), Qiang Miao(苗强)

Information and Navigation College, Airforce Engineering University, Xi'an 710077, China

收稿日期:2016-12-19 修回日期:2017-05-23 出版日期:2017-09-05 发布日期:2017-09-05
通讯作者: Shu-Xin Chen E-mail:chenshuxin68@163.com
基金资助:
Project supported by the National Natural Science Foundation of China (Grant Nos. 61573372 and 61603413).

A scheme for Sagnac-effect quantum enhancement with Fock state light input

Kun Chen(陈坤), Shu-Xin Chen(陈树新), De-Wei Wu(吴德伟), Chun-Yan Yang(杨春燕), Qiang Miao(苗强)

Information and Navigation College, Airforce Engineering University, Xi'an 710077, China

Received:2016-12-19 Revised:2017-05-23 Online:2017-09-05 Published:2017-09-05
Contact: Shu-Xin Chen E-mail:chenshuxin68@163.com
Supported by:
Project supported by the National Natural Science Foundation of China (Grant Nos. 61573372 and 61603413).

摘要/Abstract

摘要： Sagnac effect enhancement can improve optical gyro precision. For a certain input intensity, we suggest that the other input port of beam splitter (BS) should be fed with some quantum light to break through shot noise limit (SNL) to improve Sagnac effect without increasing radiation-pressure noise (NRP). We design a Sagnac effect quantum enhancement criterion (SQEC) to judge whether some quantum light can enhance Sagnac effect and present a Sagnac effect enhancement scheme that utilizing Fock state light and parity measurement technique to extract the output phase. The results of the theoretical analysis show that the maximum sensitivity can be reached at θ = 0, and the phase precision can break through SNL and even achieve Heisenberg limit (HL). When the Fock state average photon number n is far less than coherent state, the minimum measurable angular rate is improved with √2n+1 times, which can deduce shot noise and increase NRP little.

关键词: optical gyro, radiation-pressure noise, parity measurement, Heisenberg limit

Abstract: Sagnac effect enhancement can improve optical gyro precision. For a certain input intensity, we suggest that the other input port of beam splitter (BS) should be fed with some quantum light to break through shot noise limit (SNL) to improve Sagnac effect without increasing radiation-pressure noise (NRP). We design a Sagnac effect quantum enhancement criterion (SQEC) to judge whether some quantum light can enhance Sagnac effect and present a Sagnac effect enhancement scheme that utilizing Fock state light and parity measurement technique to extract the output phase. The results of the theoretical analysis show that the maximum sensitivity can be reached at θ = 0, and the phase precision can break through SNL and even achieve Heisenberg limit (HL). When the Fock state average photon number n is far less than coherent state, the minimum measurable angular rate is improved with √2n+1 times, which can deduce shot noise and increase NRP little.

Key words: optical gyro, radiation-pressure noise, parity measurement, Heisenberg limit

中图分类号: (Quantum optics)

42.50.-p

06.20.-f (Metrology) 06.30.Gv (Velocity, acceleration, and rotation)

陈坤, 陈树新, 吴德伟, 杨春燕, 苗强. A scheme for Sagnac-effect quantum enhancement with Fock state light input[J]. 中国物理B, 2017, 26(9): 94212-094212.

Kun Chen(陈坤), Shu-Xin Chen(陈树新), De-Wei Wu(吴德伟), Chun-Yan Yang(杨春燕), Qiang Miao(苗强). A scheme for Sagnac-effect quantum enhancement with Fock state light input[J]. Chin. Phys. B, 2017, 26(9): 94212-094212.

参考文献 33

[1]	Joseph S 2014 Gen. Relativ. Gravit. 46 1710
[2]	Jing J, Li Y, Zhang Z C, Wu C X and Song N F 2016 Chin. Phys. B 25 084213
[3]	Wu Q, Yu J L, Wang J, Wang W R, Jia S, Huang G B, Hei K F and Li L J 2015 Acta Phys. Sin. 64 044205 (in Chinese)
[4]	Liu J, Zhang T E, Zhang W, Lei L H, Xue C Y, Zhang W D and Tang J 2015 Acta Phys. Sin. 64 107802 (in Chinese)
[5]	Luo C, Huang J, Zhang X and Lee C 2017 Phys. Rev. A 95 023608
[6]	Gauguet A, Canuel B, Leveque T, Chaibi W and Landragin A 2009 Phys. Rev. A 80 063604
[7]	Tackmann G, Berg P, Schubert C, Abend S, Gilowski M, Ertmer W and Rasel E M 2012 New J. Phys. 14 015002
[8]	Rico-Gutierrez L M, Spiller T P and Dunningham J A 2015 New J. Phys. 17 043022
[9]	Campbell W C and Hamilton P 2016 arXiv:1609.00659
[10]	Schreiber K U, Klugel T, Wells J P R, Hurst R B and Gebauer A 2011 Phys. Rev. Lett. 107 173904
[11]	Giovanetti V, Lloyd S and Maccone L 2011 Nat. Photon. 5 222
[12]	William N P and Jonathan P D 2010 New. J. Phys. 12 083014
[13]	Xiang G Y and Guo G C 2013 Chin. Phys. B 22 110601
[14]	Bertocchi G, Alibart O, Ostrowsky D B, Tanzilli S and Baldi P 2006 J. Phys. B 39 1011
[15]	Kolkiran and Agarwal G S 2007 Opt. Express 15 679
[16]	Caves C M 1981 Phys.Rev. D 23 1693
[17]	Chen K, Chen S X, Wu D W, Yang C Y and Wu H 2016 Acta Phys. Sin. 65 054203 (in Chinese)
[18]	Chen K, Chen S X, Wu D W, Yang C Y, Wang X, Li X, Wu H and Liu Z W 2016 Acta Phys. Sin. 65 194203 (in Chinese)
[19]	Barrett B, Geiger R and Dutta I 2014 C. R. Physique 15 875
[20]	Scully M O and Zubairy M S 1997 Quantum Optics (Cambridge: Cambridge University Press) pp. 101-106
[21]	Yurke B, McCall S L and Klauder J R 1986 Phys. Rev. A 33 4033
[22]	Alex M 2006 Phys. Rev. A 73 033821
[23]	Luca P and Augusto S 2014 arXiv: 1411.5164v1 [quant-ph]
[24]	Luca P and Augusto S 2013 Phys. Rev. Lett. 110 163604
[25]	Baune C, Gniesmer J, Schönbeck A, Vollmer C E, Fiurasek J and Schnabel R 2015 Opt. Express 23 16035
[26]	Jaewoo J, Kimin P, Hyunseok J, William J M, Kae N and Timothy P S 2012 Phys. Rev. A 86 043828
[27]	Gerry C C 2000 Phys. Rev. A 61 043811
[28]	Campos R A, Gerry C C and Benmoussa A 2003 Phys. Rev. A 68 023810
[29]	Hu L Y, Wei C P, Fang J, Huang J H and Liu C J 2014 Opt. Commun. 323 68
[30]	Xu X F and Fan H Y 2015 Chin. Phys. B 24 010301
[31]	Tan Q S, Liao J Q, Wang X G and Franco N 2014 Phys. Rev. A 89 053822
[32]	Luca P and Augusto S 2009 Phys. Rev. Lett. 102 100401
[33]	Windhagera A, Suda M, Pacher C, Peev M and Poppe A 2011 Opt. Commun. 284 1907

A scheme for Sagnac-effect quantum enhancement with Fock state light input

A scheme for Sagnac-effect quantum enhancement with Fock state light input

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