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Introduction to Plasma Physics

P. Gibbon

arXiv:1705.10529v1physics.acc-ph

TL;DR

Plasma physics requires a foundation in the definitions, properties, and processes governing collective charged-particle behavior. These notes develop that foundation through plasma classifications, response models, ionization, wave-propagation approaches, and relativistic thresholds, while identifying assumptions used in the models.

  • Problem

    A primer is needed to introduce plasma concepts that underpin contemporary plasma-based accelerator schemes.

  • Method

    The notes develop plasma physics from definitions and applications through two-fluid modeling, wave-propagation analysis, plasma creation, and nonlinear and relativistic descriptions.

  • Results

    The notes establish that overdense plasmas make electromagnetic waves evanescent, while nonlinear wakes exhibit spiked density profiles, sawtooth electric fields, and longer wavelengths.

  • Takeaways & Limitations

    These plasma properties and response regimes provide foundational concepts for applications including nonlinear refractive behavior, high-field generation, and particle acceleration.

  • Takeaways & Limitations

    The treatment uses idealized assumptions including cold immobile ions for nonlinear analysis and collisionless, non-relativistic finite-temperature fluids elsewhere.

Abstract

from arXiv · show

These notes are intended to provide a brief primer in plasma physics, introducing common definitions, basic properties, and typical processes found in plasmas. These concepts are inherent in contemporary plasma-based accelerator schemes, and thus provide a foundation for the more advanced expositions that follow in this volume. No prior knowledge of plasma physics is required, but the reader is assumed to be familiar with basic electrodynamics and fluid mechanics.

1 Plasma types and definitions

Plasmas are quasi-neutral gases of charged particles whose collective electromagnetic behavior distinguishes them from ordinary matter. Their Debye shielding, collision regime, oscillation timescale, creation mechanisms, and relativistic response underpin plasma accelerator applications.

  • Definitions: A plasma is a quasi-neutral gas of charged particles exhibiting collective behavior through long-range electromagnetic interactions.Charge imbalance produces electric fields, while moving charges produce currents and magnetic fields that govern plasma dynamics.
  • Plasma types and applications: Plasmas occur across astrophysical and terrestrial environments, including stars, the ionosphere, fusion devices, lighting, industrial systems, lightning, and particle accelerators.Approximately 99% of the visible universe is in a plasma state.
  • Debye shielding and ideality: Debye shielding restores quasi-neutrality after a charge disturbance, with the Debye length setting the characteristic screening scale and many particles per Debye sphere required for collective behavior.When the plasma parameter indicates few particles per Debye sphere, screening is reduced and collisions dominate particle dynamics.
  • Plasma classification: Accelerator plasmas occupy an intermediate density–temperature regime, with roughly atmospheric-pressure densities and temperatures of a few eV produced by field ionization.The classification is illustrated in the density–temperature plane.
  • Plasma oscillations: Displacing an electron layer creates capacitor-like charge separation and a restoring electric field, producing plasma oscillations at the electron plasma frequency.The response time for recovering quasi-neutrality is related to the Debye length divided by the electron thermal velocity.
  • Plasma oscillations: For a 100 fs interaction at ne = 10^17 cm^-3, ωpτint = 1.8, so the plasma response must be considered on the interaction timescale.This collective response is relevant to plasma applications including high-field generation and particle acceleration.

2 Wave propagation in plasmas

Plasma wave propagation is analyzed with fluid models and linearized wave equations, covering longitudinal, electromagnetic, and nonlinear modes. Dispersion relations identify propagation behavior, including evanescence in overdense plasmas and qualitatively distinct nonlinear wakes.

  • Modeling approaches: Four theoretical approaches span plasma-wave modeling: N-body dynamics, phase-space methods, two-fluid equations, and magnetohydrodynamics.First-principles modeling is computationally prohibitive for large laboratory plasmas, motivating more tractable fluid descriptions.
  • Modeling approaches: The two-fluid model describes each charged species as a fluid coupled through electric and magnetic fields, under stated temperature, collision, and velocity assumptions.The baseline formulation assumes finite temperature, negligible ion-electron collisions, and non-relativistic fluid velocities.
  • Linear wave propagation: Linearization treats small perturbations by neglecting products of perturbations, yielding tractable equations for longitudinal and transverse waves.The longitudinal analysis produces the Bohm–Gross dispersion relation, while electromagnetic analysis uses transverse plane-wave solutions and Maxwell’s equations.
  • Linear wave propagation: Dispersion relations chart permitted propagation modes across wavelength limits for Langmuir, electromagnetic, and ion-acoustic waves.The electromagnetic analysis assumes E1 ⊥ k and a cold plasma with vp, vg ≫ vte.
  • Electromagnetic waves: In overdense plasmas, ne > nc, the refractive index becomes imaginary and electromagnetic waves become evanescent rather than propagating.The decay length is set by the collisionless skin depth c/ωp.
  • Nonlinear wave propagation: Nonlinear wave propagation requires retaining effects excluded by linearization and is characterized by spiked density, sawtooth electric fields, and longer wavelengths.The nonlinear treatment uses the electron Lorentz equation and Maxwell’s equations with immobile singly charged ions and negligible thermal motion.

A Useful constants and formulae

The appendix provides reference tables for commonly used physical constants, SI and cgs formulae, and practical formulae using plasma and laser units.

  • Table A.1 lists commonly used physical constants.
  • Table A.2 collects formulae expressed in SI and cgs units.
  • Table A.3 gives useful formulae with Te in eV, ne and ni in cm−3, and λL in µm.
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