Efficient multi-keV x-ray sources from Ti-doped aerogel targets

We have measured the production of hν equal to or greater than 4.5 keV x-rays from low-density Ti-doped aerogel targets at the OMEGA laser facility (University of Rochester). The targets were 2.2 mm long by 2 mm diameter beryllium cylinders filled with Ti-doped (3 atomic percent) SiO2 foam. The doped-foam density was ≈ 3 mg/cc. Forty beams of the OMEGA laser (λ = 351 nm) illuminated the two cylindrical faces of the target with a total power that ranged from 7 to 14 TW. The laser interaction fully ionizes the target (formula available in paper), and allows the laser-bleaching wave to excite, supersonically, the high-Z emitter ions in the sample. The heating of the target was imaged with a gated (200 ps time resolution) x-ray framing camera filtered to observe > 4 keV. 2-D radiative-hydrodynamic calculations predict rapid and uniform heating over the whole target volume with minimal energy losses into hydrodynamic motion. An x-ray streak camera, also filtered to observe > 4 keV, was used to measure the rate of heat propagation in the target. Ti K-shell x-ray emission was spectrally resolved with a two-channel crystal spectrometer and also with a set of filtered aluminum x-ray diodes, both instruments provide absolute measurement of the multi-keV x-ray emission. Back-scattered laser energy is observed to be minimal. We find between 100 to 400 J of output with 4.67 equal to or less than hv equal to or less than 5.0 keV, predicted target performance is a factor of 2 - 3 too low in this range.

[1]  K B Fournier,et al.  Spectroscopy of heliumlike argon resonance and satellite lines for plasma temperature diagnostics. , 2002, Physical review. E, Statistical, nonlinear, and soft matter physics.

[2]  J. D. Kilkenny,et al.  Observation of enhanced x‐ray emission from long‐pulse‐width laser‐produced plasmas , 1989 .

[3]  Takayasu Mochizuki,et al.  Soft x‐ray emission from ω0, 2ω0, and 4ω0 laser‐produced plasmas , 1986 .

[4]  J. D. Moody,et al.  Time-resolved x-ray imaging of high-power laser-irradiated underdense silica aerogels and agar foams , 1995 .

[5]  Christopher E. Clayton,et al.  Experimental studies of Raman scattering from foam targets using a 0.35 μm laser beam , 1987 .

[6]  Hammel,et al.  Accuracy of K-shell spectra modeling in high-density plasmas , 2000, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[7]  R. S. Craxton,et al.  Brillouin scattering, two‐plasmon decay, and self‐focusing in underdense ultraviolet laser‐produced plasmas , 1985 .

[8]  O. L. Landen,et al.  Ablation Front Rayleigh- Taylor Growth Experiments in Spherically Convergent Geometry , 2000 .

[9]  B. L. Henke,et al.  High-energy x-ray response of photographic films: models and measurement , 1986 .

[10]  Dennis L. Matthews,et al.  Characterization of laser‐produced plasma x‐ray sources for use in x‐ray radiography , 1983 .

[11]  G. A. Kyrala,et al.  X-ray yield scaling studies performed on the OMEGA laser , 2000 .

[12]  Nigel Woolsey,et al.  Kilovolt x-ray scattering from a plasma , 1998 .

[13]  O. Landen,et al.  Efficient multi-keV underdense laser-produced plasma radiators. , 2001, Physical review letters.

[14]  Robert P. Weaver,et al.  Shock structuring due to fabrication joints in targets , 1999 .

[15]  Martin Richardson,et al.  Self-Focusing in Underdense Ultraviolet Laser-Produced Plasmas , 1984 .

[16]  J. A. Cobble,et al.  X-ray Generation by High Irradiance Subpicosecond Lasers , 1992, Short-Wavelength Coherent Radiation: Generation and Application.

[17]  Donald W. Phillion,et al.  Laser ionization and heating of gas targets for long‐scale‐length instability experiments , 1994 .

[18]  Michael H. Key,et al.  AN INVESTIGATION OF THE X-RAY POINT-SOURCE BRIGHTNESS FOR A SHORT-PULSE LASER PLASMA , 1990 .

[19]  J. M. Soures,et al.  High X-ray conversion efficiency with target irradiation by a frequency tripled Nd : Glass laser , 1981 .

[20]  Phillion Dw,et al.  Brightness and duration of x-ray line sources irradiated with intense 0.53- microm laser light at 60 and 120 ps pulse width. , 1986 .

[21]  Y. T. Lee A model for ionization balance and L-shell spectroscopy of non-LTE plasmas. , 1987 .