Abstract

The intensities of the higher frequency anti-Stokes components of resonantly pumped Raman scattering are observed to be greatly enhanced as a result of minimizing dispersion when focusing into a hollow fiber, as compared to their intensities at higher pressures. As well, the significant spectral broadening of these Raman orders in the absence of any such broadening on the pump beams suggests the synthesis of a short temporal structure as a result of a the decreased dispersion.

© 2008 Optical Society of America

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References

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2007 (1)

F. C. Turner, A. Trottier, L. L. Losev, and D. Strickland, Opt. Commun. 270, 419 (2007).
[CrossRef]

2005 (2)

M. Y. Shverdin, D. R. Walker, D. D. Yavuz, G. Y. Yin, and S. E. Harries, Phys. Rev. Lett. 94, 033904 (2005).
[CrossRef] [PubMed]

E. Sali, P. Kinsler, G. H. C. New, K. J. Mendham, T. Halfmann, J. W. G. Tisch, and J. P. Marangos, Phys. Rev. A 72, 013813 (2005).
[CrossRef]

2004 (1)

2003 (1)

V. P. Kalosha and J. Herrmann, Phys. Rev. A 68, 023812 (2003).
[CrossRef]

2002 (3)

L. L. Losev, J. Song, J. F. Xia, D. Strickland, and V. V. Brukhanov, Opt. Lett. 27, 2100 (2002).
[CrossRef]

A. Nazarkin, G. Korn, M. Wittmann, and T. Elsaesser, Phys. Rev. A 65, 041802(R) (2002).
[CrossRef]

N. Zhavoronkov and G. Korn, Phys. Rev. Lett. 88, 203901 (2002).
[CrossRef] [PubMed]

2000 (2)

1998 (1)

S. E. Harris and A. V. Sokolov, Phys. Rev. Lett. 81, 2894 (1998).
[CrossRef]

1995 (1)

1994 (1)

1987 (1)

N. J. Everall, J. P. Partanen, J. R. M. Barr, and M. J. Shaw, Opt. Commun. 64, 393 (1987).
[CrossRef]

1964 (1)

E. A. J. Marcatili and R. A. Schmeltzer, Bell Syst. Tech. J. 43, 1783 (1964).

Bell Syst. Tech. J. (1)

E. A. J. Marcatili and R. A. Schmeltzer, Bell Syst. Tech. J. 43, 1783 (1964).

Opt. Commun. (2)

F. C. Turner, A. Trottier, L. L. Losev, and D. Strickland, Opt. Commun. 270, 419 (2007).
[CrossRef]

N. J. Everall, J. P. Partanen, J. R. M. Barr, and M. J. Shaw, Opt. Commun. 64, 393 (1987).
[CrossRef]

Opt. Lett. (5)

Phys. Rev. A (3)

V. P. Kalosha and J. Herrmann, Phys. Rev. A 68, 023812 (2003).
[CrossRef]

E. Sali, P. Kinsler, G. H. C. New, K. J. Mendham, T. Halfmann, J. W. G. Tisch, and J. P. Marangos, Phys. Rev. A 72, 013813 (2005).
[CrossRef]

A. Nazarkin, G. Korn, M. Wittmann, and T. Elsaesser, Phys. Rev. A 65, 041802(R) (2002).
[CrossRef]

Phys. Rev. Lett. (4)

S. E. Harris and A. V. Sokolov, Phys. Rev. Lett. 81, 2894 (1998).
[CrossRef]

V. P. Kalosha and J. Herrmann, Phys. Rev. Lett. 85, 1226 (2000).
[CrossRef] [PubMed]

M. Y. Shverdin, D. R. Walker, D. D. Yavuz, G. Y. Yin, and S. E. Harries, Phys. Rev. Lett. 94, 033904 (2005).
[CrossRef] [PubMed]

N. Zhavoronkov and G. Korn, Phys. Rev. Lett. 88, 203901 (2002).
[CrossRef] [PubMed]

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Figures (3)

Fig. 1
Fig. 1

Comparison between halving energy and pressure: (a) 3 atm , 0.4 mJ in each pump; (b) 3 atm , 0.2 mJ in each pump; and (c) 1.5 atm , 0.4 mJ in each pump.

Fig. 2
Fig. 2

Pressure scan with 0.4 mJ pump pulses: (a) 3, (b) 2.33, (c) 1.67, and (d) 1 atm .

Fig. 3
Fig. 3

Intensity scan with a gas pressure of 1.1 atm . Total energy in the two pump pulses are (a) 0.45, (b) 0.68, (c) 0.9, (d) 1.12, and (e) 1.35 mJ .

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