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Estimation optimale du gradient du semi-groupe de la chaleur sur le ...

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D. Brydges, A. Ta<strong>la</strong>rczyk / Journal of Functional Analysis 236 (2006) 682–711 699<br />

Proposition 4.1. Assume that L>0, d 1, B =∇, and Λ is some boun<strong>de</strong>d open set in R d ,<br />

such that the set Λ−2L ={x ∈ Λ: dist(x, ∂Λ) > 2L} is nonempty. If y ∈ Λ−2L then ALϕ(y) =<br />

d<br />

R hL(y − x)ϕ(x)dx, where<br />

hL(x) =<br />

1<br />

|B|L 2 |x| d<br />

<br />

∂BL<br />

2x · z −|x| 2 1|x−z|LσL(dz), (4.2)<br />

where σL <strong>de</strong>notes the <strong>sur</strong>face mea<strong>sur</strong>e (normalized to 1) on a sphere of radius L. In the case<br />

d = 1, σL(dx) = 1<br />

2 (δ−L(dx) + δL(dx)) where δt(dx) <strong>de</strong>notes a unit point mass at x = t.<br />

Notice that since σL is a uniform mea<strong>sur</strong>e on the sphere ∂BL the value of hL(x) <strong>de</strong>pends only<br />

on |x|.<br />

Proof. From Theorem 2.8 and Lemma 2.11, for ϕ ∈ H+(Λ) and y ∈ Λ−2L we have<br />

By trans<strong>la</strong>tion invariance,<br />

ALϕ(y) = 1<br />

|BL|<br />

ALϕ(y) = 1<br />

|BL|<br />

<br />

y+BL<br />

<br />

y+BL<br />

where ϕx(z) = ϕ(x + z).<br />

Recall the well-known formu<strong>la</strong> for the Poisson kernel of the ball BL<br />

<br />

PBLϕ(y) =<br />

∂BL<br />

Px+BL ϕ(y)dx. (4.3)<br />

PBL ϕx(y − x)dx, (4.4)<br />

Ld−2 (L2 −|y| 2 )<br />

|y − z| d<br />

ϕ(z)σL(dz).<br />

Note that this is valid also for d = 1. Applying this to (4.4), then changing the or<strong>de</strong>r of integration<br />

and substituting x = x ′ − z we obtain<br />

ALϕ(y) = 1<br />

<br />

|BL|<br />

∂BL<br />

= 1<br />

<br />

|BL|<br />

= 1<br />

|BL|<br />

<br />

=<br />

R d<br />

∂BL<br />

<br />

<br />

<br />

∂BL<br />

1x∈y+BL<br />

1x∈z+y+BL<br />

1z∈x−y+BL<br />

hL(y − x)ϕ(x)dx<br />

Ld−2 (L2 −|y − x| 2 )<br />

|y − x − z| d<br />

ϕ(x + z) dx σL(dz)<br />

Ld−2 (L2 −|y − x + z| 2 )<br />

|y − x| d<br />

ϕ(x)dx σL(dz)<br />

Ld−2 (L2 −|y − x + z| 2 )<br />

|y − x| d<br />

σL(dz)ϕ(x) dx

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