Relativistic pulse compression

Tunable radiation can be produced by Doppler upshifting light from a laser-generated moving ionization front. We analyze this technique as a method of generating ultrashort tunable light pulses in the UV to extreme UV (XUV) regions of the spectrum and demonstrate the possibility of generating subfemtosecond short-wavelength light pulses. Using realistic and technologically achievable experimental conditions and including dispersion of a pulse reflected from a finite-rise-time multiphoton-ionization-produced ionization front, we show that a single-cycle far-infrared (FIR) pulse can be compressed in time and frequency into a pulse substantially shorter than any light pulse demonstrated to date. We show that arbitrarily large upshifts are achievable using this technique, making it a potentially competitive way of producing tunable XUV radiation. The multiphoton ionization mechanism by which the ionization front is created is an important factor in determining the reflectivity of the ionization front.

[1]  Edward Ott,et al.  Interaction of electromagnetic waves with a moving ionization front , 1978 .

[2]  Eli Yablonovitch,et al.  Self-phase modulation and short-pulse generation from laser-breakdown plasmas , 1974 .

[3]  D. Marcuse,et al.  Pulse distortion in single-mode fibers. , 1980, Applied optics.

[4]  M. Fedorov,et al.  Field-induced effects of narrowing of photoelectron spectra and stabilisation of Rydberg atoms , 1988 .

[5]  Shelton Nonlinear-optical susceptibilities of gases measured at 1064 and 1319 nm. , 1990, Physical review. A, Atomic, molecular, and optical physics.

[6]  M. Nuss,et al.  Subpicosecond photoconducting dipole antennas , 1988 .

[7]  C. H. Brito Cruz,et al.  Phase correction of femtosecond optical pulses using a combination of prisms and gratings. , 1988, Optics letters.

[8]  William H. Carter,et al.  Anomalies in the field of a gaussian beam near focus , 1973 .

[9]  N. H. Burnett,et al.  Cold-plasma production for recombination extreme-ultraviolet lasers by optical-field-induced ionization , 1989 .

[10]  Xiang Zhang,et al.  Optically induced femtosecond electromagnetic pulses from GaSb/AlSb strained‐layer superlattices , 1990 .

[11]  J. Gersten,et al.  The shift of atomic states by laser fields , 1976 .

[12]  P. Becker,et al.  Compression of optical pulses to six femtoseconds by using cubic phase compensation. , 1987, Optics letters.

[13]  B. Hu,et al.  Subpicosecond electromagnetic pulses from large-aperture photoconducting antennas. , 1990, Optics letters.

[14]  J. Kuhl,et al.  Compression of femtosecond optical pulses with dielectric multilayer interferometers , 1986 .

[15]  Dörr,et al.  Tunneling ionization of atomic hydrogen by an intense low-frequency field. , 1990, Physical review letters.

[16]  Paul B. Corkum,et al.  Generation of 130-fsec Midinfrared Pulses , 1986 .

[17]  D. Meyerhofer,et al.  Tunneling ionization of noble gases in a high-intensity laser field. , 1989, Physical review letters.

[18]  W. H. Carter Electromagnetic Beam Fields , 1974 .

[19]  P. Corkum,et al.  Amplification of picosecond 10 µm pulses in multiatmosphere CO2lasers , 1985, IEEE Journal of Quantum Electronics.

[20]  C Rolland,et al.  High Energy Picosecond 10 µm Pulses , 1986, Other Conferences.

[21]  W. M. Wood,et al.  Tight focusing and blue shifting of millijoule femtosecond pulses from a conical axicon amplifier. , 1988, Optics letters.