Third-order optical intensity correlation measurements of pseudo-thermal light

doi:10.1088/1674-1056/23/9/090701

›› 2014, Vol. 23 ›› Issue (9): 90701-090701.doi: 10.1088/1674-1056/23/9/090701

Third-order optical intensity correlation measurements of pseudo-thermal light

陈希浩^a, 吴炜^a, 孟少英^a, 李明飞^b

a College of Physics, Liaoning University, Shenyang 110036, China;
b Laboratory of Optical Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China

收稿日期:2014-01-15 修回日期:2014-03-10 出版日期:2014-09-15 发布日期:2014-09-15
基金资助:
Project supported by the National Natural Science Foundation of China (Grant Nos. 11204117 and 11005055), the China Postdoctoral Science Foundation of China (Grant No. 2013M540146), and the Education Department of Liaoning Province, China (Grant Nos. L2012001 and LJQ2011005).

Third-order optical intensity correlation measurements of pseudo-thermal light

Chen Xi-Hao (陈希浩)^a, Wu Wei (吴炜)^a, Meng Shao-Ying (孟少英)^a, Li Ming-Fei (李明飞)^b

a College of Physics, Liaoning University, Shenyang 110036, China;
b Laboratory of Optical Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China

Received:2014-01-15 Revised:2014-03-10 Online:2014-09-15 Published:2014-09-15
Contact: Meng Shao-Ying, Li Ming-Fei E-mail:mengshaoying@163.com;mf_li@sina.cn
Supported by:
Project supported by the National Natural Science Foundation of China (Grant Nos. 11204117 and 11005055), the China Postdoctoral Science Foundation of China (Grant No. 2013M540146), and the Education Department of Liaoning Province, China (Grant Nos. L2012001 and LJQ2011005).

摘要/Abstract

摘要： Third-order Hanbrury Brown-Twiss and double-slit interference experiments with a pseudo-thermal light are performed by recording intensities in single, double and triple optical paths, respectively. The experimental results verifies the theoretical prediction that the indispensable condition for achieving a interference pattern or ghost image in Nth-order intensity correlation measurements is the synchronous detection of the same light field by each reference detector, no matter the intensities recorded in one, or two, or N optical paths. It is shown that, when the reference detectors are scanned in the opposite directions, the visibility and resolution of the third-order spatial correlation function of thermal light is much better than that scanned in the same direction, but it is no use for obtaining the Nth-order interference pattern or ghost image in the thermal Nth-order interference or ghost imaging.

关键词: third-order intensity correlation, thermal double-slit interference, pseudo-thermal light

Abstract: Third-order Hanbrury Brown-Twiss and double-slit interference experiments with a pseudo-thermal light are performed by recording intensities in single, double and triple optical paths, respectively. The experimental results verifies the theoretical prediction that the indispensable condition for achieving a interference pattern or ghost image in Nth-order intensity correlation measurements is the synchronous detection of the same light field by each reference detector, no matter the intensities recorded in one, or two, or N optical paths. It is shown that, when the reference detectors are scanned in the opposite directions, the visibility and resolution of the third-order spatial correlation function of thermal light is much better than that scanned in the same direction, but it is no use for obtaining the Nth-order interference pattern or ghost image in the thermal Nth-order interference or ghost imaging.

Key words: third-order intensity correlation, thermal double-slit interference, pseudo-thermal light

中图分类号: (Image processing)

07.05.Pj

42.25.Hz (Interference) 42.25.Kb (Coherence)

陈希浩, 吴炜, 孟少英, 李明飞. Third-order optical intensity correlation measurements of pseudo-thermal light[J]. , 2014, 23(9): 90701-090701.

Chen Xi-Hao (陈希浩), Wu Wei (吴炜), Meng Shao-Ying (孟少英), Li Ming-Fei (李明飞). Third-order optical intensity correlation measurements of pseudo-thermal light[J]. Chin. Phys. B, 2014, 23(9): 90701-090701.

参考文献 37

[1]	Hanbury Brown R and Twiss R Q 1956 Nature 177 27
[2]	Hanbury Brown R and Twiss R Q 1956 Nature 178 1046
[3]	Strekalov D V, Sergienko A V, Klyshko D N and Shih Y H 1995 Phys. Rev. Lett. 74 3600
[4]	Gatti A, Brambilla E, Bache M and Lugiato L A 2004 Phys. Rev. Lett. 93 093602
[5]	Cheng J and Han S S 2004 Phys. Rev. Lett. 92 093903
[6]	Ferri F, Magatti D, Gatti A, Bache M, Brambilla E and Lugiato L A 2005 Phys. Rev. Lett. 94 183602
[7]	Cai Y J and Zhu S Y 2005 Phys. Rev. E 71 056607
[8]	Cao D Z and Wang K G 2005 Phys. Rev. A 71 013801
[9]	Xiong J, Cao D Z, Huang F, Li H G, Sun X J and Wang K G 2005 Phys. Rev. Lett. 94 173601
[10]	Valencia A, Scarcelli G, D'Angelo M and Shih Y 2005 Phys. Rev. Lett. 94 063601
[11]	Zhang D, Zhai Y H, Wu L A and Chen X H 2005 Opt. Lett. 30 2354
[12]	Zhai Y H, Chen X H, Zhang D and Wu L A 2005 Phys. Rev. A 72 043805
[13]	Zhai Y H, Chen X H and Wu L A 2006 Phys. Rev. A 74 053807
[14]	Scarcelli G, Berardi V and Shih Y H 2006 Appl. Phys. Lett. 88 061106
[15]	Scarcelli G, Berardi V and Shih Y H 2006 Phys. Rev. Lett. 96 063602
[16]	Shapiro J H 2008 Phys. Rev. A 78 061802
[17]	Chen X H, Liu Q, Luo K H and Wu L A 2009 Opt. Lett. 34 695
[18]	Liu Q, Chen X H, Luo K H, Wu W and Wu L A 2009 Phys. Rev. A 79 053844
[19]	Liu Q, Luo K H, Chen X H and Wu L A 2010 Chin. Phys. B 19 094211
[20]	Agafonov I N, Chekhova M V, Iskhakov T Sh and Penin A N 2008 Phys. Rev. A 77 053801
[21]	Agafonov I N, Chekhova M V, Iskhakov T Sh and Wu L A 2009 J. Mod. Opt. 56 422
[22]	Cao D Z, Xiong J, Zhang S H, Lin L F, Gao L and Wang K G 2008 Appl. Phys. Lett. 92 201102
[23]	Richter T 1990 Phys. Rev. A 42 1817
[24]	Richter T 1991 Quant. Opt. 3 115
[25]	Li H G, Zhang Y T, Cao D Z, Xiong J and Wang K G 2008 Chin. Phys. B 17 4510
[26]	Chen X H, Agafonov I N, Luo K H, Liu Q, Xian R, Chekhova M V and Wu L A 2010 Opt. Lett. 35 1166
[27]	Chen X H, Chen W, Meng S Y, Wu W, Wu L A and Zhai G J 2013 J. Opt. Soc. A 30 1422
[28]	Chan K W C, O'Sullivan M N and Boyd R W 2009 Opt. Lett. 34 3343
[29]	Cao B and Zhang C X 2010 Opt. Lett. 35 2091
[30]	Liu J B and Shih Y H 2009 Phys. Rev. A 79 023819
[31]	Li H, Chen Z P, Xiong J and Zeng G H 2012 Opt. Express 20 2956
[32]	Li H, Shi J H, Chen Z P and Zeng G H 2012 J. Opt. Soc. A 29 2256
[33]	Zhou Y, Simon J, Liu J B and Shih Y H 2010 Phys. Rev. A 81 043831
[34]	Zhou Y, Liu J B, Simon J and Shih Y H 2012 J.Opt. Soc. B 29 377
[35]	Bai Y F and Han S S 2007 Phys. Rev. A 76 043828
[36]	Ou L H and Kuang L M 2007 J. Phys. B 40 1833
[37]	Mandel L and Wolf E 1995 Optical Coherence and Quantum Optics (Cambridge: Cambridge University Press)

Third-order optical intensity correlation measurements of pseudo-thermal light

Third-order optical intensity correlation measurements of pseudo-thermal light

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