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Generation of rf radiation by low-intensity laser pulse trains in air

Gavin Blair and Phillip Sprangle
Phys. Rev. E 108, 015203 – Published 14 July 2023

Abstract

In this paper, we analyze and numerically simulate mechanisms for generating directed rf radiation by a low-intensity laser pulse train (LPT) propagating in air. The LPT ionizes the air, forming a plasma filament. The ionization process relies on the background level of radioactivity which plays an important role in initiating a collisional ionization process. In our model a low-intensity LPT photoionizes background negative ions (produced by ambient ionizing radiation) and provides the seed electrons necessary to initiate collisional ionization. The intensity of the LPT is far below tunneling ionization levels. The ponderomotive forces associated with the LPT and self-fields drive plasma oscillations predominately in the radial direction. The driven radial electron currents in turn generate directed rf radiation. As the plasma density builds up on axis, the later portion of the LPT can defocus and limit the interaction length. The spectrum of the rf radiation consists of the fundamental frequency associated with the pulse separation time as well as harmonics. The rf generation mechanism is analyzed using fluid equations which incorporate, among other things, the effects of background radioactivity, photoionization, collisional ionization, ponderomotive and space-charge effects, and electron attachment–recombination processes. As an example, for a specific set of parameters, the rf spectrum and intensity are compared to experimental data.

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  • Received 15 February 2023
  • Revised 13 April 2023
  • Accepted 9 June 2023

DOI:https://doi.org/10.1103/PhysRevE.108.015203

©2023 American Physical Society

Physics Subject Headings (PhySH)

Plasma PhysicsAtomic, Molecular & Optical

Authors & Affiliations

Gavin Blair and Phillip Sprangle

  • Department of Physics, University of Maryland, College Park, Maryland 20742, USA;
  • Department of Electrical and Computer Engineering, University of Maryland, College Park, Maryland 20742, USA; and Institute for Research in Electronics and Applied Physics, University of Maryland, College Park, Maryland 20740, USA

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Issue

Vol. 108, Iss. 1 — July 2023

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Images

  • Figure 1
    Figure 1

    Schematic overview of LPT generating a plasma filament in air by a combination of photoionization of background negative ions and collisional ionization processes. Radial plasma currents induced by ponderomotive LPT fields generate rf radiation in forward and backward directions.

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  • Figure 2
    Figure 2

    LPT intensity ILPT vs ρ/ρ0 and τ=tz/vG. Parameters for this plot are Ipeak=4×1015W/m2, τL=100ps, Tp=0.65ns, ρ0=100µm, and Np=15.

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  • Figure 3
    Figure 3

    Configuration used in evaluation of rf intensity. Localized current and charge density are confined to region with dotted red curve.

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  • Figure 4
    Figure 4

    Electron density as a function of time in laser pulse frame for a LPT with 25 micropulses. Peak laser intensity is I0=4×1015W/m2. (a) Logarithmic plot of electron density along axis of propagation. (b) Electron density as a function of time and radius, normalized to spot size, from axis of propagation.

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  • Figure 5
    Figure 5

    Radial electron current density for a LPT of 25 micropulses having a peak intensity of I0=4×1015W/m2. (a) Radial current density as a function of radius, normalized to spot size, and time in laser pulse frame. (b) Radial electron current density as a function of time in laser pulse frame at ρ=0.5ρ0.

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  • Figure 6
    Figure 6

    Calculated and experimental spectra of the rf in arb. units. (a) Calculated spectrum from a LPT with 40 micropulses and (b) experimentally measured spectrum. Fundamental peak is at 1.6GHz in both spectra. Note that harmonics are not shown in experimental spectrum since receiving antenna was tuned to only a narrow range of frequencies. Harmonics, however, have been measured experimentally (private communications with V. Markov at AS&T, Inc. [13]).

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  • Figure 7
    Figure 7

    Polar plots showing dependence of strength of rf signal on angle θ for various plasma filament lengths: (a) 3 mm and (b) 3 cm.

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