2016
DOI: 10.1063/1.4948431
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Quantitative measurement of electron number in nanosecond and picosecond laser-induced air breakdown

Abstract: Here we present quantitative measurements of total electron numbers in laser-induced air breakdown at pressures ranging from atmospheric to 40 barg by 10 ns and 100 ps laser pulses. A quantifiable definition for the laser-induced breakdown threshold is identified by a sharp increase in the measurable total electron numbers via dielectric-calibrated coherent microwave scattering. For the 10 ns laser pulse, the threshold of laser-induced breakdown in atmospheric air is defined as the total electron number of ∼10… Show more

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Cited by 27 publications
(23 citation statements)
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“…A 10-dBm tunable microwave source (HP 8350B sweep oscillator, set at ~10 GHz) was split into two channels [22,24]. One of the channels was used to illuminate the plasma by employing a microwave horn (WR75, 15-dB gain).…”
Section: Coherent Microwave Scattering Systemmentioning
confidence: 99%
See 2 more Smart Citations
“…A 10-dBm tunable microwave source (HP 8350B sweep oscillator, set at ~10 GHz) was split into two channels [22,24]. One of the channels was used to illuminate the plasma by employing a microwave horn (WR75, 15-dB gain).…”
Section: Coherent Microwave Scattering Systemmentioning
confidence: 99%
“…Microwave scattering can measure the total electron number evolution with a temporal resolution of ~3 nanoseconds (ns). Note that plasma expansion leads to a critical electron number density beyond the microwave penetration depth, which causes the microwave signal to decrease after peak [22]. A variable zoom camera lens was used to relay the plasma emissions into the threechannel MUSIC apparatus, as shown in Fig.…”
Section: Imaging Targetmentioning
confidence: 99%
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“…A careful understanding of electromagnetic-plasma and scattering interactions is essential for the proper extraction of information on total electron numbers and subsequent derivable quantities (e.g., the electron number density ) from CMS. Vast historical art exists for weakly-ionized, strongly collisional microplasmas in which electron motion is restricted by electron-neutral collisions 4 , 5 , 9 , 10 . However, application of the diagnostic to collisionless plasmas has remained relatively unexplored (no N e correspondence is given by 11 , 13 , 18 )—despite garnering some attention in recent years 19 due to a prevalence in studies on electric propulsion devices 20 , photoionization in low-pressure conditions 21 , 22 , etc.…”
Section: Introductionmentioning
confidence: 99%
“…16 In traditional ns-LIBS, the plasma results from a few seed electrons being generated via multiphoton ionization at a high-intensity focus of the laser beam; these seed electrons are then accelerated by the pervading laser field to liberate more electrons. 3,4,17,18 This process, termed avalanche ionization, leads to a strong plasma with continuum radiation dominating the early emission and atomic emission emerging as the plasma rapidly expands and cools down. The continuum radiation, a trademark of the avalanche ionization process, is generally problematic for accurate measurements of equivalence ratio.…”
Section: Introductionmentioning
confidence: 99%