By F.B. Dunning and Randall G. Hulet (Eds.)
Mixed with Volumes 29A and 29B, this quantity is a complete remedy of the most important experimental tools of atomic, molecular, and optical physics, in addition to an outstanding experimental instruction manual for the sector. Thewide availability of tunable lasers long ago numerous years has revolutionized the sector and bring about the advent of many new experimental equipment which are coated in those volumes. conventional tools also are incorporated to make sure that the volumes could be an entire reference resource for the sector.
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Additional resources for Atomic, Molecular, and Optical Physics: Electromagnetic Radiation
Am. B 8,2437. 64. Murnane, M. , Kapteyn, H. , Gordon, S. , and Glytsis, E. N. (1993). Appl. Phys. Lett. 62, 1068. 65. Silfvast, W. , Richardson, M. , and Thorp, J. (1992). J. Vac. Sci. Technol. B 10,3 126. 66. Bortz, M. , and French, R. H. (1989). Appl. Phys. Lett. 55, 1955. 67. Powell, F. , Vedder, P. , Lindblom, J. , and Powell, S. F. (1990). Opt. Eng. 29, 614. 68. Catura, R. , Joki, E. , Roethig, D. , and Brookover, W. J. (1987). Appl. Opt. 26, 1563. 69. Ginter, M. J. (1988). Appl. Opt. 27, 885.
Mayer, F. , Tarvin, J. , Busch, G. , Matthews, D. , and Kippel, L. (1981). “Laser-Heated Gas Jet: A Soft X-Ray Source,” in Low Energy X-Ray Diagnostics-1981, AIP Conference Proceedings, No. 75, D. T. Attwood and B. L. ), pp. 270-274, American Institute of Physics, New York. 56. , Bartnik, A,, and Patron, Z. (1993). Appl. Phys. Lett. 62, 2778. 57. , Chin, C. , Herman, P. , Budnik, F. , and Majoribanks, R. S. ( 1993). “Extreme-Ultraviolet Laser Photo-Pumped by a Self-Healing Hg Target,” in Applications of Laser Plasma Radiation, Vol.
Field to the plasma. The conditions under which resonance absorption or other higher-order processes are important are generally present only in laser inertial confinement fusion plasmas and will not be considered here. The plasma electron temperature is determined by a balance between the absorbed laser energy and the loss of energy from the plasma. The primary loss mechanism is the conduction of energy to the colder, higher-density regions of the plasma near the target, which cannot be heated directly by the laser light.
Atomic, Molecular, and Optical Physics: Electromagnetic Radiation by F.B. Dunning and Randall G. Hulet (Eds.)