Beam-Plasma Collective Oscillations in Intense Charged-Particle Beams: Dielectric Response Theory, Langmuir Wave Dispersion, and Unsupervised Detection via Prometheus
Brandon Yee, Wilson Collins, Michael Iofin, Jiayi Fu

TL;DR
This paper develops a theoretical framework for beam-plasma oscillations in intense charged-particle beams, deriving dispersion relations and validating predictions with simulations, revealing signatures observable at current facilities.
Contribution
It introduces a kinetic field theory for beam-plasma oscillations, deriving dielectric functions and validating them with machine learning on simulation data, including detection of collective modes.
Findings
Existence of undamped Langmuir wave modes above a critical density
Validation of plasma frequency and dispersion relations via simulations
Detection of Friedel oscillations and Kohn anomaly in structure factor data
Abstract
We develop a theoretical and computational framework for beam-plasma collective oscillations in intense charged-particle beams at intermediate energies (10-100 MeV). In Part I, we formulate a kinetic field theory governed by the Vlasov-Poisson system, deriving the Lindhard dielectric function and random phase approximation (RPA) polarization tensor for three beam distribution functions. We prove via the dielectric function epsilon(omega,q)=0 the existence of undamped Langmuir wave modes above a critical beam density n_c, obtain explicit beam-plasma dispersion relations, and show that Landau damping vanishes above the particle-hole continuum. The plasma frequency Omega_p^2 = ne^2/(m*epsilon_0) is fixed by the f-sum rule independently of distribution shape; higher dispersion coefficients depend on velocity moments. Space charge effects drive anomalous beam broadening with sqrt(n-n_c)…
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