Hostname: page-component-78c5997874-t5tsf Total loading time: 0 Render date: 2024-11-15T03:24:54.170Z Has data issue: false hasContentIssue false

Advanced 20 TW Ti:S laser system for X-ray laser and coherent XUV generation irradiated by ultra-high intensities

Published online by Cambridge University Press:  07 June 2005

HIROTO KURODA
Affiliation:
The Institute for Solid State Physics, The University of Tokyo, Chiba, Japan
MASAYUKI SUZUKI
Affiliation:
The Institute for Solid State Physics, The University of Tokyo, Chiba, Japan
RASHID GANEEV
Affiliation:
The Institute for Solid State Physics, The University of Tokyo, Chiba, Japan
JUN ZHANG
Affiliation:
The Institute for Solid State Physics, The University of Tokyo, Chiba, Japan
MOTOYOSHI BABA
Affiliation:
The Institute for Solid State Physics, The University of Tokyo, Chiba, Japan
TSUNEYUKI OZAKI
Affiliation:
Institut national de la recherche scientifique, Quebec, Canada
ZHI YI WEI
Affiliation:
Laboratory of Optical Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China
JIE ZHANG
Affiliation:
Laboratory of Optical Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China

Abstract

In order to develop a high repetition rate X-ray lasers, the longitudinal-pumped transient collisional excitation (TCE) X-ray laser is one of the most effective pumping schemes. The high directive Ni-like Mo 18.9 nm soft X-ray laser pumped by modest laser energy has already been demonstrated by using the tabletop size Ti:sapphire/Nd:glass laser system that delivering energy of 150 mJ in 475 fs at the center wavelength of 1054 nm. The total energy in the pre-pulse and the main pulse was 150 mJ, which will make possible multi-hertz operation. To pursue the high repetition rate of the laser-driven TCE X-ray laser, we have designed a new 20 TW Ti:Sapphire laser system (600 mJ, 30 fs, 10 Hz). Special attention was paid to improve the contrast ratio, control of pulse shape as well as phase by an acoustic optic programmable dispersive filter (AOPDF) and 1 kHz preamplifier. Preliminary data have shown good laser characteristics. As the preliminary experiments, we have investigated high order harmonics generation from low-density laser plasma by using the solid target irradiated by a femtosecond laser pulse. The highest order was the 51st. harmonic at wavelength of 15.61 nm.

Type
Research Article
Copyright
2005 Cambridge University Press

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

Footnotes

This paper was presented at the 28th ECLIM conference in Rome, Italy.

References

REFERENCES

Bellini, M., Cavalieri, S., Corsi, C.,et al. (2004). High resolution spectroscopy in the XUV with pairs of mutually coherent and time-delayed laser harmonics Laser Part. Beams 22, 199202.Google Scholar
Benware, B.R., Seminario, M., Lecher, A.L.,et al. (2001). Generation and application of a high-average-power polarized soft-X-ray laser beam. J. Opt. Soc. B. 18, 10411045.CrossRefGoogle Scholar
Földes, I.B., Kocsis, G., Racz, E.,et al. (2003). Generation of high harmonics in laser plasmas Laser Part. Beams 21, 517521.Google Scholar
Ganeev, R.A., Teruo, K., Ishizawa, A.,et al. (2004). Development and applications of a compact hybrid tabletop terawatt chirped-pulse amplification Ti:sapphire-Nd:glass for X-ray lasing and harmonic generation. Appl. Opt. 43, 13961403.CrossRefGoogle Scholar
Ishizawa, A., Ozaki, T., Ganeev, R.A. & Kuroda, H. (2002). Measurement of blue shifts due to collisionless absorption in harmonic generation from subpicosecond laser-produced plasmas. Phys. Rev. E 66, 026414.Google Scholar
Janulewicz, A., Nickles, P.V., King, R.E. & Pert, G.J. (2004). Influence of pump on a transient collisionally pumped Ni-like Ag X-ray laser. Phys. Rev. A. 70, 013804.CrossRefGoogle Scholar
Kanai, T., Yamamoto, K., Li, R. & Zhang, J. (2002a). Coherent short wavelength radiation via picosecond Nd : glass lasers. Laser Part. Beams 20, 5965.Google Scholar
Keenan, R., Dunn, J., Shlyaptsev, V.N.,et al. (2003). Efficient pumping schemes for high average brightness collisional X-ray lasers. SPIE 5197, 213219.Google Scholar
Kita, T., Harada, T., Nakano, N. & Kuroda, H. (1983). Mechanically ruled aberration-corrected concave gratings for a flat-field grazing-incidence spectrograph. Appl. Opt. 22, 512513.CrossRefGoogle Scholar
Kuroda, H., Ozaki, T., Ishizawa,et al. (2002b). Studies of advanced soft X-ray laser and coherent higher harmonic generation using intense subpicosecond laser produced high density plasma. J. Luminescence 100, 291300.Google Scholar
Li, R., Ozaki, T., Kanai, T. & Kuroda, H. (1998). Proposal of a longitudinally pumped saturated Ni-like Mo ion X-ray laser at 18.9 nm. Phys Rev. E. 57, 7093.CrossRefGoogle Scholar
Lan, K., Fill, E. & Meyer-Ter-Vehn, J. (2004). Photopumping of XUV lasers by XFEL radiation. Laser Part. Beams 22, 261266.CrossRefGoogle Scholar
Merdji, H., Hergott, J.F., Kovacev, M., Priori, E., Salieres, P. & Carra, B.. (2004). Manipulating intense XUV coherent light in the temporal domain. Laser Part. Beams 22, 275278.Google Scholar
Monmayrant, A., Joffre, M., Oksenhendler, T.,et al. (2003). Time dominant interferometric for direct electric-field reconstruction by use of an acousto-optic programmable filter and a two-photon detector. Opt. Lett. 28, 278280.CrossRefGoogle Scholar
Morlens, A.S, Zeitoun, P., Vanbostal, L., Mercere, P., Faivre, G., Hubert, S., Troussel, P., Remond, C., Marmoret, R., Delmotte, F., Ravet, M.F. & Rouillay, M. (2004). Study of XUV beam splitter flatness for use on a Michelson interferometer. Laser Part. Beams 22, 279284.Google Scholar
Neumayer, P., Bock, R., Borneis, S., Brambrink, E.,et al. (2005). Status of PHELIX laser and first experiments. Laser Part. Beams 23 (in print).CrossRefGoogle Scholar
Ozaki, T., Nakano, H. & Kuroda, H. (2002a). Prepulse-produced plasma waveguide for longitudinally pumped nickellike molybdenum X-ray lasers. J. Opt. Soc. B 19, 13351341.Google Scholar
Ozaki, T., Yamamoto, K., Kanai, T. & Kuroda, H. (2002b). Jetlike structure in the visible emission of plasma pumped by an obliquely incident picosecond laser. J. Phys. Soc. (Japan) 71, 29632968.Google Scholar
Ozaki, T., Ganeev, R.A., Ishizawa, A.,et al. (2002c). High Directive 18.9 nm Nickel-like Molybdenum X-ray Laser Operating at 150 mJ Pump Energy. Phys. Rev. Lett. 89, 253902.Google Scholar
Ozaki, T., Nakano, H. & Kuroda, H. (2002d). Effects of pump propagation and absorption on the gain distribution of longitudinally pumped Ni-like molybdenum X-ray lasers. Phys. Rev. E 66, 047402.Google Scholar
Ros, D., Jamelot, G., Carllon, A.,et al. (2002). State of the development of X-ray lasers and applications at LSAI. Laser Part. Beams 20, 2330.CrossRefGoogle Scholar
Sebban, S., Mocek, Ros, D.,et al. (2002). Demonstration of a Ni-like Kr Optical-Field-Ionization Collisional Soft X-ray Laser at 32.8 nm. Phys. Rev. Lett. 89, 253901.CrossRefGoogle Scholar