PhysicsLogic / Landau 1946

Phase Mixing and Recoverable Information

A nearly homogeneous density can retain phases that a velocity reversal refocuses.

Definitions and assumptions

Scope and physical limitations

The independent example has two equal dynamical populations of opposite charge, a positive Gaussian-modulated distribution, and zero electric potential. It solves the actual nonlinear collisionless kinetic equation and Poisson closure. Its number-density contrast decays uniformly in position, while each velocity-mode modulus persists. An ideal externally imposed reversal v -> -v leaves the instantaneous number density unchanged; subsequent forward streaming restores the initial modulation. For every positive tolerance there is a positive reversal time with smaller initial contrast but recovered contrast 1/2. The reversal is an external operation, not autonomous recurrence, a collision process, entropy production, or a nonlinear plasma-echo experiment. The example is not Landau's fixed-ion electric-field damping solution. His separate conditional source argument retains the contour asymptotics and a nonzero residue; a pole location alone does not supply persistent amplitude.

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Examples and distinctions

Constructed examples of this model; each answer includes the Lean statement.

Exact root statement

∀ (epsilon : ℝ),
  0 < epsilon →
    ∃ turn,
      0 < turn ∧
        (∀ (elapsed position : ℝ), (reversedPair turn).NonvacuousVlasovPoissonAt elapsed position) ∧
          (∀ (position : ℝ), |(∫ (velocity : ℝ), afterVelocityReversal turn 0 position velocity) - 1| < epsilon) ∧
            (∀ (position velocity : ℝ),
                afterVelocityReversal turn turn position velocity =
                  PlasmaPhysics.phaseSpaceDensity 0 position velocity) ∧
              |(∫ (velocity : ℝ), afterVelocityReversal turn turn 0 velocity) - 1| = 1 / 2
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