1964
DOI: 10.1016/0031-9163(64)90465-2
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Experimental and theoretical studies of air breakdown by intense pulse of light

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1966
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Cited by 29 publications
(8 citation statements)
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“…2. When the target is exposed to the extremely high irradiance (typical pulse duration is less than 1 sec μ and fluence rate is more than 10 10 W/cm 2 ), a phenomenon called optical breakdown occurs [5,[28][29][30]. The laser creates numerous ionized molecules and free electrons.…”
Section: Plasma-induced Ablationmentioning
confidence: 99%
See 1 more Smart Citation
“…2. When the target is exposed to the extremely high irradiance (typical pulse duration is less than 1 sec μ and fluence rate is more than 10 10 W/cm 2 ), a phenomenon called optical breakdown occurs [5,[28][29][30]. The laser creates numerous ionized molecules and free electrons.…”
Section: Plasma-induced Ablationmentioning
confidence: 99%
“…When a nanosecond pulse interacts with a target, the photon energy is converted to the kinetic energy of electrons (macroscopically, the heat energy) and subsequently, a number of thermions are emitted. During the interaction between the Q-switched nanosecond pulse and targets, such as tissue or industrial material, the plasma is initiated by means of a thermionic process [29][30][31]. Usually, thermal and mechanical damage accompany this process.…”
Section: Thermionic Emissionmentioning
confidence: 99%
“…[3][4][5] During the past century, extensive efforts have been taken on the study of laser induced gas breakdown with various laser wavelengths [6][7][8], laser pulse widths, [9,10] focal areas [11], pressures [12], and gas media [13]. The combination of all these factors determines the gas breakdown energy threshold and electron number denisty.…”
Section: Introductionmentioning
confidence: 99%
“…The interaction of the intense light radiation with the targeted material leads to the generation of free electrons and to the formation of a plasma volume. Particularly in gases and liquids, the plasma formation is followed by a rapid thermoelastic expansion and successive collapse of the ionized volume, leading to the emission of an acoustic pulse 14 , 15 . Figure 1 shows a conceptual diagram of the physical processes behind laser-induced breakdown (LIB) in gases.…”
Section: Introductionmentioning
confidence: 99%