STAPRO: 8203 Model 3G pp. 1–9 (col. fig: nil)
Please cite this article in press as: Boufoussi B., Hajji S., Transportation inequalities for stochastic heat equations. Statistics and Probability Letters (2018),
https://doi.org/10.1016/j.spl.2018.03.012.
Statistics and Probability Letters xx (xxxx) xxx–xxx
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Statistics and Probability Letters
journal homepage: www.elsevier.com/locate/stapro
Transportation inequalities for stochastic heat equations
Brahim Boufoussi
a
, Salah Hajji
b,
*
a
Department of Mathematics, Faculty of Sciences Semlalia, Cadi Ayyad University, 2390 Marrakesh, Morocco
b
Department of Mathematics, Regional Center for the Professions of Education and Training, Marrakesh, Morocco
article info
Article history:
Received 18 November 2017
Received in revised form 6 March 2018
Accepted 16 March 2018
Available online xxxx
MSC:
60H15
Keywords:
Stochastic heat equation
White noise
Fractional noise
Girsanov transformation
Transportation inequality
abstract
Using the method of Girsanov transformation, we establish the transportation inequalities,
on the continuous paths space with respect to the L
2
metric, for the law of the solution
of stochastic heat equation driven by space–time white noise. The case of stochastic heat
equations driven by fractional noise is also investigated.
© 2018 Elsevier B.V. All rights reserved.
1. Introduction 1
Let (E , d) be a metric space equipped with σ -field B such that d(.,.) is B × B measurable. Given p ≥ 1 and two probability 2
measures μ and ν on E , we define the Wasserstein distance of order p between μ and ν by 3
W
d
p
(μ,ν ) = inf
π ∈Π(μ,ν)
(∫
E×E
d(x, y)
p
dπ (x, y)
)
1/p
, 4
where Π (μ,ν ) is the set of all probability measures on the product space E × E with marginals μ and ν . The relative entropy 5
of ν with respect to μ is defined as 6
H(ν/μ) =
⎧
⎨
⎩
∫
E
log
dν
dμ
dν, if ν ≪ μ
+∞ otherwise.
7
The probability measure μ satisfies the L
p
− transportation inequality on (E , d) if there exists a constant C ≥ 0 such that 8
for any probability measure ν , 9
W
d
p
(μ,ν ) ≤
√
2CH(ν/μ). 10
We shall write μ ∈ T
p
(C ) for this relation. 11
*
Corresponding author.
E-mail addresses: boufoussi@ucam.ac.ma (B. Boufoussi), hajjisalahe@yahoo.fr (S. Hajji).
https://doi.org/10.1016/j.spl.2018.03.012
0167-7152/© 2018 Elsevier B.V. All rights reserved.