Difference between revisions of "What is the Phenomenon That Keeps an Infinite Memory for the Fluctuactions in the Conduction Current"
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− | 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. | + | 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. |
− | [[Category:Electrodynamics]] | + | [[Category:Scientific Paper|phenomenon keeps infinite memory fluctuactions conduction current]] |
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+ | [[Category:Electrodynamics|phenomenon keeps infinite memory fluctuactions conduction current]] |
Latest revision as of 20:13, 1 January 2017
Scientific Paper | |
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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.