Quasilinear SPDEs via Rough Paths
We are interested in (uniformly) parabolic PDEs with a nonlinear dependence of the leading-order coefficients, driven by a rough right hand side. For simplicity, we consider a space-time periodic setting with a single spatial variable: ∂ 2 u - P ( a ( u ) ∂ 1 2 u + σ ( u ) f ) = 0 , where P is the p...
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Veröffentlicht in: | Archive for rational mechanics and analysis 2019-05, Vol.232 (2), p.873-950 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | We are interested in (uniformly) parabolic PDEs with a nonlinear dependence of the leading-order coefficients, driven by a rough right hand side. For simplicity, we consider a space-time periodic setting with a single spatial variable:
∂
2
u
-
P
(
a
(
u
)
∂
1
2
u
+
σ
(
u
)
f
)
=
0
,
where
P
is the projection on mean-zero functions, and
f
is a distribution which is only controlled in the low regularity norm of
C
α
-
2
for
α
>
2
3
on the parabolic Hölder scale. The example we have in mind is a random forcing
f
and our assumptions allow, for example, for an
f
which is white in the time variable
x
2
and only mildly coloured in the space variable
x
1
; any spatial covariance operator
(
1
+
|
∂
1
|
)
-
λ
1
with
λ
1
>
1
3
is admissible. On the deterministic side we obtain a
C
α
-estimate for
u
, assuming that we control products of the form
v
∂
1
2
v
and
vf
with
v
solving the constant-coefficient equation
∂
2
v
-
a
0
∂
1
2
v
=
f
. As a consequence, we obtain existence, uniqueness and stability with respect to
(
f
,
v
f
,
v
∂
1
2
v
)
of small space-time periodic solutions for small data. We then demonstrate how the required products can be bounded in the case of a random forcing
f
using stochastic arguments. For this we extend the treatment of the singular product
σ
(
u
)
f
via a space-time version of Gubinelli’s notion of controlled rough paths to the product
a
(
u
)
∂
1
2
u
, which has the same degree of singularity but is more nonlinear since the solution
u
appears in both factors. In fact, we develop a theory for the linear equation
∂
t
u
-
P
(
a
∂
1
2
u
+
σ
f
)
=
0
with rough but given coefficient fields
a
and
σ
and then apply a fixed point argument. The PDE ingredient mimics the (kernel-free) Safonov approach to ordinary Schauder theory. |
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ISSN: | 0003-9527 1432-0673 |
DOI: | 10.1007/s00205-018-01335-8 |