Development of Brillouin-enhanced four-wave mixing

Yang Jun; He Weiming; Ding Yingchun

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Volume 26 Issue 5

Sep. 2013

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Article Navigation > LASER TECHNOLOGY > 2002 > 26(5): 394-397

Citation:

Development of Brillouin-enhanced four-wave mixing

1.
Institute of Opto Electronics, Harbin Institute of Technology, Harbin, 150001

Received Date: 2002-01-08
Accepted Date: 2002-03-13

Abstract

When a Brillouin-shifted signal interacts with two strong counterpropagating pump beams in a Brillouin active medium,a conjugate field will grow exponentially in time until it depletes the power of the pump beams. This technique can be used to conjugate very weak signals or alternatively a large fraction of the pump power can be transferred into the conjugate beam.
- Brillouin-enhanced four-wave mixing,
- pump beam,
- conjugate beam

References

[1]	Bespalov V I,Matveev A Z,Pasmanik G A.Radiophys and Quantum Electron,1987,29:818～830.
[2]	Scott A M,Ridley K D.IEEE J Q E,1989,25:438～459.
[3]	Scott A M,Waggott P.IEEE J Q E,1990,26:631～632.
[4]	Holmes R E.IEEE J Q E,1990,26:1980～1989.
[5]	Chio B I,Nam C H.Appl Phys,1999,B69(1):450～453.
[6]	敖发良,黄红刚,李思敏.桂林电子工业学院学报,1999,19(1):12～15.
[7]	Scott A M,Hazell M S.IEEE J Q E,1986,QE22:1248～1257.
[8]	Yung-Sheng K,Yu-Chue F.Opt Commun,1993,97:228～232.
[9]	Chio B I,Jo M S.Opt Commun,1994,107:425～431.
[10]	Bowers M W,Boyd R W. Opt Lett,1997,22:360～362.
[11]	Bowers M W,Boyd R W.IEEE J Q E,1998,34:634～644.
[12]	Taylor F.J Modern Optics,1997,44(4):731～738.
[13]	Matthews S C,Rockwell D A.IEEE NLO'94:415～417.
[14]	何伟明,吕志伟,王琪 et al.中国激光,1997,24(8):721～724.
[15]	Syed K S,Crofts G J. J O S A,1997,B14:2067～2078.

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通讯作者: 陈斌, bchen63@163.com

1.
沈阳化工大学材料科学与工程学院沈阳 110142

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Development of Brillouin-enhanced four-wave mixing

1. Institute of Opto Electronics, Harbin Institute of Technology, Harbin, 150001

Received Date: 2002-01-08
Accepted Date: 2002-03-13
Available Online: 2002-09-25

Abstract: When a Brillouin-shifted signal interacts with two strong counterpropagating pump beams in a Brillouin active medium,a conjugate field will grow exponentially in time until it depletes the power of the pump beams. This technique can be used to conjugate very weak signals or alternatively a large fraction of the pump power can be transferred into the conjugate beam.

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Reference (15)

[1]	Bespalov V I,Matveev A Z,Pasmanik G A.Radiophys and Quantum Electron,1987,29:818～830.
[2]	Scott A M,Ridley K D.IEEE J Q E,1989,25:438～459.
[3]	Scott A M,Waggott P.IEEE J Q E,1990,26:631～632.
[4]	Holmes R E.IEEE J Q E,1990,26:1980～1989.
[5]	Chio B I,Nam C H.Appl Phys,1999,B69(1):450～453.
[6]	敖发良,黄红刚,李思敏.桂林电子工业学院学报,1999,19(1):12～15.
[7]	Scott A M,Hazell M S.IEEE J Q E,1986,QE22:1248～1257.
[8]	Yung-Sheng K,Yu-Chue F.Opt Commun,1993,97:228～232.
[9]	Chio B I,Jo M S.Opt Commun,1994,107:425～431.
[10]	Bowers M W,Boyd R W. Opt Lett,1997,22:360～362.
[11]	Bowers M W,Boyd R W.IEEE J Q E,1998,34:634～644.
[12]	Taylor F.J Modern Optics,1997,44(4):731～738.
[13]	Matthews S C,Rockwell D A.IEEE NLO'94:415～417.
[14]	何伟明,吕志伟,王琪 et al.中国激光,1997,24(8):721～724.
[15]	Syed K S,Crofts G J. J O S A,1997,B14:2067～2078.

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Development of Brillouin-enhanced four-wave mixing

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通讯作者: 陈斌, bchen63@163.com

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