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Degenerate parabolic stochastic partial differential equations

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M. Hofmanová / Stochastic Processes and their Applications 123 (2013) 4294–4336 4311<br />

Moreover, by (14),<br />

t <br />

−E g i (y, y, s) Dσ i (y)z · (∇ϱ)(z) dz dy ds<br />

0 (T N )<br />

2 t <br />

= E g i (y, y, s)div σ i (y) dy ds<br />

0 T N<br />

and accordingly (21) follows.<br />

The last term K is, due to (3), bounded as follows<br />

K ≤ L t<br />

<br />

2 E ϱ τ (x − y)|x − y|<br />

0<br />

(T 2 ψ δ (ξ − ζ ) dν 1<br />

N ) 2 R 2 x,s (ξ) dν2 y,s (ζ ) dx dy ds<br />

+ L t <br />

<br />

2 E ϱ τ (x − y) ψ δ (ξ − ζ )|ξ − ζ |h(|ξ − ζ |)dν 1<br />

0 (T N ) 2 R 2 x,s (ξ)dν2 y,s (ζ )dxdyds<br />

≤ Lt <br />

|x − y| 2 ϱ τ (x − y) dx dy + LtC <br />

ψh(δ)<br />

ϱ τ (x − y) dx dy<br />

2δ (T N ) 2 2 (T N ) 2<br />

≤ Lt<br />

2 δ−1 τ 2 + LtC ψh(δ)<br />

,<br />

2<br />

where C ψ = sup ξ∈R |ξψ(ξ)|. Finally, we set δ = τ 4/3 , let τ → 0 and deduce<br />

<br />

<br />

E f<br />

T ± N 1 (t) f ¯ ± 2 (t) dξ dx ≤ E f 1,0 f¯<br />

2,0 dξ dx.<br />

T<br />

R N<br />

R<br />

Let us now consider f 1 = f 2 = f . Since f 0 = 1 u0 >ξ we have the identity f 0 f¯<br />

0 = 0 and<br />

therefore f ± (1 − f ± ) = 0 a.e. (ω, x, ξ) and for all t. The fact that f ± is a kinetic function and<br />

Fubini’s theorem then imply that, for any t ∈ [0, T ], there exists a set Σ t ⊂ Ω × T N of full<br />

measure such that, for (ω, x) ∈ Σ t , f ± (ω, x, t, ξ) ∈ {0, 1} for a.e. ξ ∈ R. Therefore, there exist<br />

u ± : Ω × T N × [0, T ] → R such that f ± = 1 u ± >ξ for a.e. (ω, x, ξ) and all t. In particular,<br />

u ± = R ( f ± − 1 0>ξ )dξ for a.e. (ω, x) and all t. It follows now from Proposition 3.1 and the<br />

identity<br />

<br />

|α − β| = |1 α>ξ − 1 β>ξ | dξ, α, β ∈ R,<br />

R<br />

that u + = u − = u for a.e. t ∈ [0, T ]. Since<br />

<br />

1 u<br />

±<br />

1 >ξ 1 u ± 2 >ξ dξ = (u± 1 − u± 2 )+<br />

R<br />

we obtain the comparison property<br />

E u ± 1 (t) − u± 2 (t) + <br />

L 1 (T N ) ≤ E (u 1,0 − u 2,0 ) + <br />

L 1 (T N ) .<br />

□<br />

As a consequence of Theorem 3.3, namely from the comparison property (19), the uniqueness<br />

part of Theorem 2.10 follows. Furthermore, we obtain the continuity of trajectories in L p (T N ).<br />

Corollary 3.4 (Continuity in Time). Let u be a kinetic solution to (1). Then there exists a<br />

representative of u which has almost surely continuous trajectories in L p (T N ), for all p ∈<br />

[1, ∞).

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