Terahertz Waveforms Manipulation by Two Orthogonal-Polarized Femtosecond Pulses
LI De-Hua1,2**, MA Jian-Jun1,2, ZHOU Wei1,2, LIU Sheng-Gang3
1Terahertz Science and Technology Research Center, Shandong University of Science and Technology, Qingdao 266510 2Qingdao Key Laboratory of Terahertz Technology, Qingdao 266510 3Terahertz Science and Technology Research Center, University of Electronic Science and Technology of China, Chengdu 610054
Terahertz Waveforms Manipulation by Two Orthogonal-Polarized Femtosecond Pulses
LI De-Hua1,2**, MA Jian-Jun1,2, ZHOU Wei1,2, LIU Sheng-Gang3
1Terahertz Science and Technology Research Center, Shandong University of Science and Technology, Qingdao 266510 2Qingdao Key Laboratory of Terahertz Technology, Qingdao 266510 3Terahertz Science and Technology Research Center, University of Electronic Science and Technology of China, Chengdu 610054
摘要We present a method of terahertz generation in which both the amplitude and polarity of the terahertz pulse can be manipulated. A pair of temporally separated and orthogonally polarized collinear propagating femtosecond pulses with the same central frequencies are focused onto a (110) oriented ZnTe crystal. By adjusting the relative time delay between the pulses, the amplitude and polarity of the generated terahertz pulse based on difference frequency generation can be controlled. Theoretical derivation and simulation based on the one-dimensional propagation equation of the terahertz wave are carried out under simplified conditions of perfect phase matching, plane-wave approximation and no absorption.
Abstract:We present a method of terahertz generation in which both the amplitude and polarity of the terahertz pulse can be manipulated. A pair of temporally separated and orthogonally polarized collinear propagating femtosecond pulses with the same central frequencies are focused onto a (110) oriented ZnTe crystal. By adjusting the relative time delay between the pulses, the amplitude and polarity of the generated terahertz pulse based on difference frequency generation can be controlled. Theoretical derivation and simulation based on the one-dimensional propagation equation of the terahertz wave are carried out under simplified conditions of perfect phase matching, plane-wave approximation and no absorption.
[1] Weiner A M, Heritage J P and Salehi J A 1995 Opt. Lett. 13 300
[2] White W E, Patterson F G, Combs R L, Price D F and Shepherd R L 1993 Opt. Lett. 18 1343
[3] Lee Y S, Norris T B, Maslov A, Citrin D S, Prineas J, Khitrova G and Gibbs H M 2001 Appl. Phys. Lett. 78 3941
[4] Broers B, Noordam L D and van Linden van den Heuvell H B 1992 Phys. Rev. 46 2749
[5] Rice S A Science 1992 258 412
[6] Ahn J, Efimov A, Averitt R and Taylor A J 2003 Opt. Exp. 11 2486
[7] Liu Y Q, Park S G and Weiner A M 1996 Opt. Lett. 21 1762
[8] Lee Y S, Amer N and Hurlbut W C 2003 Appl. Phys. Lett. 82 170
[9] Liu Y Q, Park S G and Weiner A M 1996 IEEE J. Sel. Top. Quantum Electron. 2 709
[10] Hurlbut W C, Norton B J, Amer N and Lee Y S 2006 J. Opt. Soc. Am. B 23 90
[11] Dai J, Karpowicz N and Zhang X C 2009 Phys. Rev. Lett. 103 023001
[12] Manceau J M, Massaouti M and Tzortzakis S 2010 Opt. Exp. 18 18894
[13] Boyd R W 1992 Nonlinear Optics (New York: Academic Press) chap 1 p 67
[14] Sutherland R L 1996 Handbook of nonlinear optics (New York: Routledge) chap 2 p 17
[15] Hebling J, Yeh K L, Hoffmann M C, Bartal B and Nelson K A 2008 J. Opt. Soc. Am. B 25 6
[16] Lee Y S 2009 Principles of Terahertz Science and Technology (New York: Springer) chap 3 p 51
[17] Nahata A, Weling A S and Heinz T F 1996 Appl. Phys. Lett. 69 2321
[18] Gaivoronsky V Y, Nazarov M M, Sapozhnikov D A, Shepelyavyi E V, Shkel'nyuk S A, Shkurinov A P and Shuvaev A V 2005 Quantum Electron. 35 407