Difference between revisions of "What is the Phenomenon That Keeps an Infinite Memory for the Fluctuactions in the Conduction Current"

From Natural Philosophy Wiki
Jump to navigation Jump to search
(Imported from text file)
(Imported from text file)
 
Line 14: Line 14:
 
[[Category:Scientific Paper|phenomenon keeps infinite memory fluctuactions conduction current]]
 
[[Category:Scientific Paper|phenomenon keeps infinite memory fluctuactions conduction current]]
  
[[Category:Electrodynamics]]
+
[[Category:Electrodynamics|phenomenon keeps infinite memory fluctuactions conduction current]]

Latest revision as of 20:13, 1 January 2017

Scientific Paper
Title What is the Phenomenon That Keeps an Infinite Memory for the Fluctuactions in the Conduction Current
Author(s) Gianfranco Spavieri, Giancarlo Cavalleri, Francesco Barbero, Ernesto Tonni, Leonardo Bosi
Keywords Magnetic Memory
Published 2008
Journal None
No. of pages 6

Abstract

If the electron acceleration aZPF due to the nonrenormalized zero-point field (ZPF) of stochastic electrodynamics (SED) is introduced in the Fokker-Planck equation accounting for electron-electron acceleration (e ? e FP), there is always a small interval dv of speed v starting from v1 where the two collision frequencies n1(v) and n2(v) appearing in the e ? e FP are both proportional to 1/v, corresponding to the threshold of runaways. Both diffusion and drift in the v space almost vanish in the small dv where n2(v) = Bn1(v) = BK/v. The Green's solution p0(v,t | v1) [or a pimple on p0(v,t ? ?) is almost crystallized, being ? t ?e  with 0.003 ? e ? 0.007. There is therefore a process of reconstruction of a fluctuaction occurring in dv, and that fluctuaction decays with a power law with such a small exponent that its memory is practically infinite.