Cleo: 2015 2015
DOI: 10.1364/cleo_si.2015.sm3n.2
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Picosecond Ionization Dynamics in Femtosecond Filaments at High Pressures

Abstract: We investigate the plasma dynamics inside a femtosecond-pulse-induced filament generated in an argon gas for a wide range of pressures up to 60 bar. At higher pressures, we observe ionization immediately following a pulse, with up to a threefold increase in the electron density within 30 ps after the filamentary propagation of a femtosecond pulse. Our study suggests that this picosecond evolution can be attributed to collisional ionization including Penning and associative ionizations and electron-impact ioniz… Show more

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Cited by 3 publications
(5 citation statements)
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“…As a consequence of this sequential coupling, avalanche ionization does not instantaneously follow the intensity, leading to memory or transient effects. As a related example exhibiting such memory effects, for a laser-produced high temperature plasma in air it has been shown both theoretically and experimentally that the plasma density can continue to increase well after the pulse has passed due to the high energy electrons in the tail of the Maxwell distribution that have enough energy for impact ionization of neutral atoms [27][28][29]. The distinction in the present case is that the mean kinetic energy of the freed electrons already is enough to produce impact ionization both during and after the pulse.…”
Section: Overview Of the Standard Modelmentioning
confidence: 99%
See 1 more Smart Citation
“…As a consequence of this sequential coupling, avalanche ionization does not instantaneously follow the intensity, leading to memory or transient effects. As a related example exhibiting such memory effects, for a laser-produced high temperature plasma in air it has been shown both theoretically and experimentally that the plasma density can continue to increase well after the pulse has passed due to the high energy electrons in the tail of the Maxwell distribution that have enough energy for impact ionization of neutral atoms [27][28][29]. The distinction in the present case is that the mean kinetic energy of the freed electrons already is enough to produce impact ionization both during and after the pulse.…”
Section: Overview Of the Standard Modelmentioning
confidence: 99%
“…This is correct and it is well known that impact excitation of excited atomic states can also occur and reduce the amount of ionization that occurs. To address this issue will require an extension of the current model to go beyond the freed electron density and allow for the excited state populations [29].…”
Section: Recurring Issuesmentioning
confidence: 99%
“…Studies of photoionization by strong optical fields have led to a number of interesting developments in physics, ranging from fundamental studies of ionization and subsequent plasma evolution [1][2][3] to applications such as high harmonic generation (HHG) [1] and the formation of plasma channels that can be used in particle acceleration and for the generation of coherent X-rays [4]. While these initial studies focused on low-density gases, recent research has explored the full nonlinear polarization of gases at atmospheric and higher pressures [5], as well as more exotic effects such as Kramers-Henneberger quasibound states [6], and avalanche ionisation by collisions of excited atoms in the absence of a laser pulse [7][8][9]. Understanding the dynamics of ionised gases at high pressures is also of great importance for HHG in the water window, a spectral region where phase-matching generally requires helium pressures of several atmospheres [10,11].…”
Section: Introductionmentioning
confidence: 99%
“…Such high-pressure (and multiply ionized) noble gases were used to achieve efficient ultrahigh-harmonic generation, in which case the combination of linear response of electron gas and nonlinear response of ions was shown to engineer phase matching with the driving UV laser pulse. 5,23,24 Most recently, timeresolved transverse interferometry and shadowgraphy was used to trace evolution of the electron density in the filament wake in a highpressure argon gas (60 bar) on picosecond time scale, 1 where an approximately 3-fold increase in the electron density was observed, saturating at about 30 picoseconds after the filamenting laser pulse.…”
mentioning
confidence: 99%
“…In this Communication, we investigate theoretically the evolution of a dense gas during interaction with an intense, ultrashort laser pulse. Similar to recent experimental work, 1 we assume an argon gas at a pressure of 60 atm. This gas interacts with a laser pulse at 800 nm, a duration of 70 fs (FWHM), and a focal-volume intensity in the range 0.5-1.0 × 10 14 W/cm 2 .…”
mentioning
confidence: 99%