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Einstein's Diffusion and Probability-Wave Equations of Random ...

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Gauge Institute Journal,<br />

H. Vic Dannon<br />

<strong>and</strong> writes his integral as<br />

Δ=∞ Δ=∞ 2<br />

Δ=∞<br />

f<br />

1 f<br />

2<br />

fxt (,) δ ∂<br />

( ) d ( ) d ( ) d ..<br />

x<br />

δ ∂<br />

∫ Δ Δ + Δ Δ Δ + Δ<br />

2!<br />

δ Δ Δ +<br />

∂<br />

∫ ∫<br />

2<br />

∂x<br />

Δ=−∞ Δ=−∞ Δ=−∞<br />

He observes that the odd integrals vanish<br />

Δ=∞<br />

∫ Δδ( Δ) dΔ = 0,<br />

Δ=−∞<br />

Δ=∞<br />

∫<br />

Δ=−∞<br />

Δ 3 δ( Δ) dΔ = 0<br />

………………………<br />

He only misses that the even integrals vanish as well.<br />

Indeed, the sifting by<br />

δ( Δ)<br />

, gives<br />

k<br />

Δ = 0 .<br />

Δ= 0<br />

In particular, his Drift Coefficient, which is [p.131]<br />

D<br />

Δ=∞<br />

∫<br />

2ϕ( ) dΔ,<br />

Δ=−∞<br />

1<br />

= Δ Δ<br />

2τ<br />

vanishes,<br />

<strong>and</strong> his <strong>Diffusion</strong> Equation [equation 18, p. 132]<br />

collapses to<br />

2<br />

∂f<br />

∂ f<br />

= D<br />

∂t<br />

2<br />

∂x<br />

∂ f =<br />

∂t<br />

0 .<br />

,<br />

6

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