By M. D. Perry, B. C. Stuart, D. Pennington, G. Tietbohl, J. Britten, C. Brown, S. Herman (auth.), Louis DiMauro, Margaret Murnane, Anne L’Huillier (eds.)
The Optical Society of the US convention on functions of excessive Fields and brief Wavelength assets, held in Santa Fe, New Mexico, united states, from March 20-22, 1997, was once an incredibly intriguing convention. This convention used to be the 7th in a chain of topical con ferences, held each years, that are dedicated to the new release and alertness of excessive box and brief wavelength resources. The assembly used to be actually overseas in scope, with equivalent participation from either inside of and outdoors of the U.S.. some time past years, there was dramatic development in either laser and x-ray coher ent assets, either primary and utilized. The 1997 assembly highlighted those advances, that are summarized in sections 1 and a pair of of this quantity. Terawatt-class lasers at the moment are avail capable within the UV or at excessive repetition premiums. Michael Perry (LLNL) provided a keynote speak on petawatt type lasers and their functions in inertial confinement fusion, whereas Jorge Rocca (Colorado country college) offered a keynote speak on tabletop soft-x-ray lasers. Genera tion and dimension strategies have gotten very refined during the UV and x ray sector of the spectrum, and coherent assets were prolonged to wavelengths lower than 30A. section keep an eye on within the x-ray sector is additionally now attainable, and new phase-matching schemes within the UV were experimentally confirmed. it's transparent new box of x-ray nonlin ear optics will deveiop speedily over the following couple of years.
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The data corresponding to 37 kA discharges through 4-mm diameter. 8 em long capillary channels. b) Variation of the integrated intensity of the J= 0-1 line ofNe-like sulfur as a function of the discharge current on the same capillary. The pressure was maintained constant at about 470 mTorr in all the shots. The change in the integrated laser line intensity was also measured as a function of the amplitude of the fast current pulse and the sulfur filling pressure. Figure 9a shows the dependence of the intensity of the lasing line as a function of filling pressure for discharge shots with a current of 37± I kA.
Assuming a pulse shape of the (sech)2 form, we obtain a pulse duration tFWHM (full width at half maximum) of 50 femtoseconds. The obtained pulse duration is in good agreement with simulations taking into account group velocity and phase mismatch in the doubling crystal. We also studied the second harmonic of an amplified CPM dye laser working at 615 nm with an energy of 2 mJ per pulse and pulse durations as short as 80 femtoseconds. It was obtained with a KDP crystal (100 Jlm thickness) yielding 10 111 per pulse in the UV.
35 Under optimized conditions, strong lasing can be expected to occur in the 3s 1P01 - 3p 1So line, as is the case in the Switch discharge pumped Ne-Iike Ar laser. S4 run in spectra obtained from laser-created sulfur plasmas 27 , and has recently been observed to lase in laser-created plasmas generated using the Sulfur channel Asterix iodine laser facility at the Max Planck Institute for Quantum Optics28 . 2 run using a tin filter. S em long channel filled with 460 mTorr of sulfur vapor. 015 run.
