A deep-UV optical frequency comb at 205 nm.

By frequency quadrupling a picosecond pulse train from a Ti:sapphire laser at 820 nm we generate a frequency comb at 205 nm with nearly bandwidth-limited pulses. The nonlinear frequency conversion is accomplished by two successive frequency doubling stages that take place in resonant cavities that are matched to the pulse repetition rate of 82 MHz. This allows for an overall efficiency of 4.5 % and produces an output power of up to 70 mW for a few minutes and 25 mW with continuous operation for hours. Such a deep UV frequency comb may be employed for direct frequency comb spectroscopy in cases where it is less efficient to convert to these short wavelengths with continuous wave lasers.

[1]  T. Hänsch,et al.  Two-photon frequency comb spectroscopy of the 6s-8s transition in cesium. , 2007, Optics letters.

[2]  Erich P. Ippen,et al.  Astigmatically compensated cavities for CW dye lasers , 1972 .

[3]  Arlee V. Smith How to select nonlinear crystals and model their performance using SNLO software , 2000, LASE.

[4]  Allister I. Ferguson,et al.  Two-photon spectroscopy of laser-cooled Rb using a mode-locked laser , 1996 .

[5]  F Noack,et al.  Tunable femtosecond pulses in the near vacuum ultraviolet generated by frequency conversion of amplified Ti:sapphire laser pulses. , 1993, Optics letters.

[6]  John L. Hall,et al.  Laser phase and frequency stabilization using an optical resonator , 1983 .

[7]  Chuangtian Chen,et al.  Recent advances in deep and vacuum-UV harmonic generation with KBBF crystal , 2004 .

[8]  R. Beigang,et al.  External frequency conversion of cw mode-locked Ti:Al(2)O(3) laser radiation. , 1991, Optics letters.

[9]  T. Hänsch,et al.  Laser frequency stabilization by polarization spectroscopy of a reflecting reference cavity , 1980 .

[10]  F. Nez,et al.  Analysis and observation, on an atomic resonance, of the frequency shift due to the length modulation of an optical cavity. , 2002, Applied optics.

[11]  J. K. Shaw,et al.  Analysis of cross correlation, phase velocity mismatch and group velocity mismatches in sum-frequency generation , 1993 .

[12]  R. Beigang,et al.  Tunable picosecond pulses below 200 nm by external frequency conversion of cw modelocked Ti:Al2O3 laser radiation , 1992 .

[13]  A. Clairon,et al.  Metrology of the hydrogen and deuterium atoms: Determination of the Rydberg constant and Lamb shifts , 2000 .

[14]  Yelena Isyanova,et al.  A quasi-continuous-wave deep ultraviolet laser source , 2003 .

[15]  François Nez,et al.  Ultra-violet light generation at 205 nm by two frequency doubling steps of a cw titanium-sapphire laser , 1997 .

[16]  V. Chebotayev,et al.  Narrow resonances of two-photon absorption of super-narrow pulses in a gas , 1977 .

[17]  T. Hänsch,et al.  Optical frequency metrology , 2002, Nature.

[18]  Direct frequency comb measurements of absolute optical frequencies and population transfer dynamics. , 2005, Physical review letters.

[19]  A. Dubietis,et al.  Highly efficient subpicosecond pulse generation at 211 nm , 2000 .

[20]  F. Rotermund,et al.  Generation of the fourth harmonic of a femtosecond Ti:sapphire laser. , 1998, Optics Letters.

[21]  J. Sakuma,et al.  High-power CW deep-UV coherent light sources around 200 nm based on external resonant sum-frequency mixing , 2004, IEEE Journal of Selected Topics in Quantum Electronics.

[22]  Catherine Schwob,et al.  Towards an absolute measurement of the 1S-3S line in atomic hydrogen , 2005 .

[23]  G. Boyd,et al.  Parametric Interaction of Focused Gaussian Light Beams , 1968 .

[24]  Baichang Wu,et al.  Design and synthesis of an ultraviolet-transparent nonlinear optical crystal Sr2Be2B2O7 , 1995, Nature.