2016
DOI: 10.1103/physreva.94.033824
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Optimal laser-pulse energy partitioning for air ionization

Abstract: We investigate the pulse partitioning of a 6.3-mJ, 450-fs pulse at 1030 nm to produce plasma channels. At such moderate energies, splitting the energy into several subpulses reduces the ionization efficiency and thus does not extend the plasma lifetime. We numerically show that when sufficient energy to produce multifilamentation is available, splitting the pulse temporally in a pulse train increases the gas temperature compared to a filament bundle of the same energy. This could improve the mean free path of … Show more

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Cited by 12 publications
(16 citation statements)
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References 39 publications
(63 reference statements)
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“…More ionization simultaneously implies more free charges and more energy deposition, hence a lower air density, and finally less efficient attachment to neutral molecules and therefore a longer plasma lifetime. The plasma evolution model, described in [28] confirms this interpretation. Indeed, simulations show that for picosecond pulses at 1030 nm the tunnel ionization term widely dominates over the multiphoton ionization, described by the Perelomov-Popov-Terent'ev (PPT) model.…”
Section: Discussionsupporting
confidence: 64%
See 2 more Smart Citations
“…More ionization simultaneously implies more free charges and more energy deposition, hence a lower air density, and finally less efficient attachment to neutral molecules and therefore a longer plasma lifetime. The plasma evolution model, described in [28] confirms this interpretation. Indeed, simulations show that for picosecond pulses at 1030 nm the tunnel ionization term widely dominates over the multiphoton ionization, described by the Perelomov-Popov-Terent'ev (PPT) model.…”
Section: Discussionsupporting
confidence: 64%
“…Another approach consists in re-detaching and/or re-heating the free electrons by subsequent laser pulses. On one hand, multiple ultrashort pulses [28,29,30] increased the free electron lifetime over a duration similar to the pulse train.…”
Section: Introductionmentioning
confidence: 99%
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“…The subsequent evolution of the charges relied on the plasma model of [44]. The results are displayed in Fig.…”
Section: Comparison With a Filament Propagation Modelmentioning
confidence: 99%
“…The lifetime of the plasma is in the range of nanoseconds to tens of nanoseconds for the free electrons [25] and in the microsecond range for the ions. The speed of the guided discharge propagation amounts to -10 m s 5 1 for a leader regime in gaps or 3-7 m [13], and -10 m s 6 1 in a streamer regime for a shorter gap of 2 m [26].…”
Section: Introductionmentioning
confidence: 99%