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Lévy integrals and the stationarity of generalised Ornstein–Uhlenbeck processes
The generalised Ornstein–Uhlenbeck process constructed from a bivariate Lévy process ( ξ t , η t ) t ⩾ 0 is defined as V t = e - ξ t ∫ 0 t e ξ s - d η s + V 0 , t ⩾ 0 , where V 0 is an independent starting random variable. The stationarity of the process is closely related to the convergence or dive...
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Published in: | Stochastic processes and their applications 2005-10, Vol.115 (10), p.1701-1722 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | The generalised Ornstein–Uhlenbeck process constructed from a bivariate Lévy process
(
ξ
t
,
η
t
)
t
⩾
0
is defined as
V
t
=
e
-
ξ
t
∫
0
t
e
ξ
s
-
d
η
s
+
V
0
,
t
⩾
0
,
where
V
0
is an independent starting random variable. The stationarity of the process is closely related to the convergence or divergence of the Lévy integral
∫
0
∞
e
-
ξ
t
-
d
η
t
. We make precise this relation in the general case, showing that the conditions are not in general equivalent, though they are for example if
ξ
and
η
are independent. Characterisations are expressed in terms of the Lévy measure of
(
ξ
,
η
)
. Conditions for the moments of the strictly stationary distribution to be finite are given, and the autocovariance function and the heavy-tailed behaviour of the stationary solution are also studied. |
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ISSN: | 0304-4149 1879-209X |
DOI: | 10.1016/j.spa.2005.05.004 |