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According to the mechanism of nearly degeneration four-wave mixing that occurs in a sufficiently nonlinear resonant gaseous medium caused by phase-modulated laser beam, the electromagnetism excitation and dynamic evolvement of modulation transfer spectroscopy(MTS) technique is studied theoretically, and then mathematic models of dispersion spectrum and absorption spectrum of MTS are established too. The results show that when the frequency of modulation signal source is equal to 0.72 times the linewidth of absorption line approximatively, the intensity of dispersion signal reaches a maximum value; it can obtain a better frequency-stabilization result when modulation factor is set to be nearly 0.3; the instability of demodulation phase has a big effect on the absorption spectrum, but on dispersion spectrum, the effect is tiny when the demodulation phase fluctuates near 90.
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Keywords:
- optical frequency standard /
- modulation transfer spectroscopy /
- frequency stabilization /
- optimizing electro-optical parameter
[1] Hall J L, Hollberg L, Baer T, Robinson H G 1981 Appl. Phys. Lett. 39 680
[2] [3] Arie A, Byer R L 1993 Appl. Opt. 32 7382
[4] [5] Bruner A, Arie A, Arbore M A, Fejer M M 1998 Appl. Opt. 37 1049
[6] Guo R, Hong F L, Onae A, Bi Z Y, Matsumoto H 2004 Opt. Lett. 29 1733
[7] [8] [9] Drever R W P, Hall J L, Kowalski F V, Hough J, Ford G M, Munley A J, Ward H 1983 Appl. Phys. 31 97
[10] Bjorklund G C 1980 Opt. Lett. 5 15
[11] [12] Shirley J H 1982 Opt. Lett. 7 537
[13] [14] [15] Yoshitake S, Akiyama K, Iritani M, Murayama H 1992 Proc. SPIE 1837 124
[16] [17] Pisani M, Sassi M P, Zucco M 1995 IEEE Trans. Instrum. Meas. 44 159
[18] [19] Ye J, Ma L S, Hall J L 1998 Proc. SPIE 3270 85
[20] [21] Galzerano G, Svelto C, Bava E, Bertinetto F 1999 Appl. Opt. 38 6962
[22] [23] Leonhardt V, Camp J B 2006 Appl. Opt. 45 4142
[24] [25] Galzerano G, Laporta P 2007 IEEE Trans. Instrum. Meas. 56 365
[26] Bjorklund G C, Levenson M D 1981 Phys. Rev. A 24 166
[27] [28] Ma L S, Hall J L 1990 IEEE J. Quantum Electron. 26 2006
[29] -
[1] Hall J L, Hollberg L, Baer T, Robinson H G 1981 Appl. Phys. Lett. 39 680
[2] [3] Arie A, Byer R L 1993 Appl. Opt. 32 7382
[4] [5] Bruner A, Arie A, Arbore M A, Fejer M M 1998 Appl. Opt. 37 1049
[6] Guo R, Hong F L, Onae A, Bi Z Y, Matsumoto H 2004 Opt. Lett. 29 1733
[7] [8] [9] Drever R W P, Hall J L, Kowalski F V, Hough J, Ford G M, Munley A J, Ward H 1983 Appl. Phys. 31 97
[10] Bjorklund G C 1980 Opt. Lett. 5 15
[11] [12] Shirley J H 1982 Opt. Lett. 7 537
[13] [14] [15] Yoshitake S, Akiyama K, Iritani M, Murayama H 1992 Proc. SPIE 1837 124
[16] [17] Pisani M, Sassi M P, Zucco M 1995 IEEE Trans. Instrum. Meas. 44 159
[18] [19] Ye J, Ma L S, Hall J L 1998 Proc. SPIE 3270 85
[20] [21] Galzerano G, Svelto C, Bava E, Bertinetto F 1999 Appl. Opt. 38 6962
[22] [23] Leonhardt V, Camp J B 2006 Appl. Opt. 45 4142
[24] [25] Galzerano G, Laporta P 2007 IEEE Trans. Instrum. Meas. 56 365
[26] Bjorklund G C, Levenson M D 1981 Phys. Rev. A 24 166
[27] [28] Ma L S, Hall J L 1990 IEEE J. Quantum Electron. 26 2006
[29]
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