2014
DOI: 10.1111/stan.12021
|View full text |Cite
|
Sign up to set email alerts
|

Limit theorems for reflected Ornstein–Uhlenbeck processes

Abstract: This paper studies one-dimensional Ornstein-Uhlenbeck processes, with the distinguishing feature that they are reflected on a single boundary (put at level 0) or two boundaries (put at levels 0 and d>0). In the literature they are referred to as reflected OU (ROU) and doubly-reflected OU (DROU) respectively. For both cases, we explicitly determine the decay rates of the (transient) probability to reach a given extreme level. The methodology relies on sample-path large deviations, so that we also identify the a… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
19
0

Year Published

2017
2017
2023
2023

Publication Types

Select...
4
2

Relationship

1
5

Authors

Journals

citations
Cited by 10 publications
(19 citation statements)
references
References 16 publications
0
19
0
Order By: Relevance
“…Let us briefly summarize the result in HUANG et al (). In that paper, the object of study was a doubly reflected (at the lower bound zero and an upper bound d ) OU process Z , satisfying the SDE dZt=(αγZt)dt+σdWt+dLtdUt. For a twice continuously differentiable function h on double-struckR, by Itô's formula, we have dh(Zt)=((αγZt)h(Zt)+σ22h(Zt))dt+σh(Zt)dWt+h(Zt)dLth(Zt)dUt. On the basis of the key properties of L (e.g., Equation ) and U (which takes care of the reflection at the upper level d ), this reduces to normaldh(Zt)=1.19em(αγZt)h(Zt)+σ22h(...…”
Section: A Previous Resultsmentioning
confidence: 81%
See 3 more Smart Citations
“…Let us briefly summarize the result in HUANG et al (). In that paper, the object of study was a doubly reflected (at the lower bound zero and an upper bound d ) OU process Z , satisfying the SDE dZt=(αγZt)dt+σdWt+dLtdUt. For a twice continuously differentiable function h on double-struckR, by Itô's formula, we have dh(Zt)=((αγZt)h(Zt)+σ22h(Zt))dt+σh(Zt)dWt+h(Zt)dLth(Zt)dUt. On the basis of the key properties of L (e.g., Equation ) and U (which takes care of the reflection at the upper level d ), this reduces to normaldh(Zt)=1.19em(αγZt)h(Zt)+σ22h(...…”
Section: A Previous Resultsmentioning
confidence: 81%
“…Indeed, with this choice of h , we have dh(Zt)=σh(Zt)dWt(dUtqUdt). Boundedness of h ( Z t )( Z is a bounded process) combined with a central limit theorem for the martingale 0·σh(Zt)normaldWt was central in the proof of the central limit theorem for U t ; see HUANG et al () for further details. In the present paper, we deal with the one‐sided reflected process Y and with a twice differential function h one obtains normaldh(Yt)=(scriptLh)(Yt)normaldt+σh(Yt)normaldWt+h(0)normaldLt. Two facts obstruct a direct application of the method earlier: (i) the process h ( Y t ) is not bounded, and (ii) we cannot immediately apply Lemma to obtain a proper choice of h .…”
Section: A Previous Resultsmentioning
confidence: 99%
See 2 more Smart Citations
“…> α N +1 are the roots of the polynomial P , due to Lemma 3.1, and where β k is defined in (27). Finally, after straightforward calculations one obtains the expression (25).…”
Section: Analysis Of the Modelmentioning
confidence: 99%