1966
DOI: 10.1103/physrev.143.1
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Multiphoton Ionization of Hydrogen and Rare-Gas Atoms

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Cited by 432 publications
(95 citation statements)
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“…It has been established [3][4][5][6][7][8][9][10][11] that the threshold photon flux density or equivalently the threshold power density for MPI varies with P −1/n , where P is the gas pressure and n is the number of simultaneously absorbed photons. Therefore, MPI predicts a very weak dependence of the threshold power density on pressure.…”
Section: Optical Breakdown Threshold Intensities For Omentioning
confidence: 99%
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“…It has been established [3][4][5][6][7][8][9][10][11] that the threshold photon flux density or equivalently the threshold power density for MPI varies with P −1/n , where P is the gas pressure and n is the number of simultaneously absorbed photons. Therefore, MPI predicts a very weak dependence of the threshold power density on pressure.…”
Section: Optical Breakdown Threshold Intensities For Omentioning
confidence: 99%
“…Measurements of the emission spectra revealed a highly ionized plasma which expanded somewhat like a blast wave into the surrounding medium. Since the first observations of LIB in gases [2], the phenomenon has been studied extensively, both theoretically and experimentally [3][4][5][6][7][8][9][10][11]. Among the various diagnostic techniques which are convenient tools for detecting various transient species from UV up to IR spectral regions, optical emission spectroscopy (OES) has definite advantages pertaining to high spatial and temporal resolution without perturbation of the laser-induced plasma.…”
Section: Introductionmentioning
confidence: 99%
“…Bebb and Gold [60][61][62] concluded that although multiphoton ionization may supply the initial electrons, it does not account entirely for the breakdown phenomenon, except possibly at very low pressures when the formation of an electron cascade is inhibited. Moreover, it has been established [60][61][62] that the threshold photon flux density F th or, equivalently, the threshold power density J th for multiphoton ionization varies with P −1/n , where P is the gas pressure and n is the number of simultaneously absorbed photons. Therefore, multiphoton ionization predicts a very weak dependence of J th on P for trisilane.…”
Section: F Laser-induced Breakdown Mechanism In Trisilanementioning
confidence: 99%
“…primarily with the phenomenon of laser-induced gas breakdown (Bebb andGold 1966, Morton 1967). For the treatment of processes associated with very high light intensities, the perturbation treatment of the interaction between the atomic system and the radiation field is not valid; and other more suitable methods have been proposed (Reiss 1970, Faisal 1972.…”
Section: Some Investigations Of Multiphoton Ionization Have Been Concmentioning
confidence: 99%