Back

Two-stream instability (1D PIC plasma)

What you are seeing: two counter-streaming beams of electrons in a 1D plasma. The configuration is unstable: any tiny perturbation in density grows exponentially, the beams form rolling vortices in phase space ("electron holes"), then trap each other, eventually settling into a single thermal distribution. This is the canonical kinetic plasma instability.

The top plot is the (x, v) phase space, sampled by 10000 macro-particles, drawn with persistence so the electron-hole vortices leave trails. The middle strip is the density-mode spectrogram (ρ^k|\hat\rho_k| for k=18k = 1\ldots 8 versus time): mode 1 dominates the linear phase, harmonics appear at saturation. The bottom trace is logρ^k=1\log|\hat\rho_{k=1}| with the dashed analytic reference of slope γ=ωp/(22)0.354\gamma = \omega_p/(2\sqrt 2)\approx 0.354 (plasma units): the measured slope tracks it in the linear regime, then the mode saturates. Default v0=0.6v_0 = 0.6 puts the fundamental near the peak-growth wavenumber.

Figure 1. 1D-1V particle-in-cell simulation of the two-stream instability. Method: NGP charge deposit, FFT Poisson solve, leapfrog particle push.
v_00.60
speed3

WHAT TO TRY

  • Vary each control and watch the rail readouts respond.
  • Compare the diagnostic plot against the live scene.