Journal of Mathematical Finance, 2011, 1, 83-89
doi:10.4236/jmf.2011.13011 Published Online November 2011 (http://www.SciRP.org/journal/jmf)
Copyright © 2011 SciRes. JMF
The Markovian Regime-Switching Risk Model with
Constant Dividend Barrier under Absolute Ruin
Wenguang Yu1, Yujuan Huang2
1School of Statistics and Mathematics, Shandong Economic University, Jinan, China
2Departme n t of Mathematics and Physics, Shandong Jiaotong University, Jinan, China
E-mail: yuwg@mail.sdu.edu.cn
Received July 26, 2011; revised September 8, 2011; accepted September 22, 2011
Abstract
In this paper, we consider the dividend payments prior to absolute ruin in a Markovian regime-switching risk
process in which the rate for the Poisson claim arrivals and the distribution of the claim amounts are driven
by an underlying Markov jump process. A system of integro-differential equations with boundary conditions
satisfied by the moment-generating function, the n th moment of the discounted dividend payments prior to
absolute ruin and the expected discounted penalty function, given the initial environment state, are derived.
Then, the matrix form of systems of integro-differential equations satisfied by the discounted penalty func-
tion are presented. Finally, we obtain the integro-differential equations satisfied by the time to reach the
dividend barrier.
Keywords: Absolute Ruin, Debit Interest, Moment-Generating Function, Markovian Regime-Switching Risk
Model, Dividend Barrier, Integro-Differential Equation
1. Introduction
In recent years, ruin theory under regime-switching mo-
del is becoming a popular topic. This model is proposed
in Reinhard [1] and Asmussen [2]. Asmussen calls it a
Markov-modulated risk model. The purpose for this ge-
neralization is to enhan ce the flexibility of the model pa-
rameter settings for the classical risk process. This model
can capture the feature that insurance policies may need
to change if economical or political env ironment chan ges.
There are many papers published on ruin probabilities and
the related problems under the Markov regime-switching
risk model. For example, Lu and Li [3] study ruin prob-
abilities under this model. Ng and Yang [4] obtain an up-
per bound for the joint distribution of surplus before and
at ruin under the regime-switching model by using a mar-
tingale approach. Ng and Yang [5] present some explicit
results for the joint distribution of surplus before and at
ruin under this model in the cases of zero initial surplus
and phase type claim size distributions, respectively. Li
and Lu [6] investigate the moments of the dividend pay-
ments and related problems in a Markov-modulated risk
model. Lu and Li [7] and Liu et al. [8] consider a regime-
switching risk model with a threshold dividend strategy.
Zhu and Yang [9] study a more general Markovian re-
gime-switching risk model in which the premium, the
claim intensity, the claim amount, the dividend payment
rate and the dividend threshold level are influenced by an
external Markovi an environm ent process. Wei et al. [10] con-
sider the Markov-modulated insurance risk model with tax.
However, there is no work that deals with the absolute
ruin in a regime-switching risk model. This motivates us
to investigate such a risk model in th is work.
Due to its practical importance, the issue of absolute
ruin problem has received attention in risk theory. Zhou
and Zhang [11] got the explicit expression of the absolu te
ruin probability for the classical risk model with expo-
nential individual claim by using the Markov property.
Cai [12] defined Gerber-Shiu function at absolute ruin
and derived a system of the integro-differential equations
satisfied by the Gerber-Shiu function. Yuan and Hu [13]
investigate the absolute ruin in the compound Poisson
risk model with nonnegative interest and a constant di-
vidend barrier. Wang and Yin [14] studied the dividend
payments in the classical risk model under absolute ruin
with debit interest. Wang et al. [15] considered the divi-
dend payments in a compound Poisson risk model with
credit and debit interest under absolute ruin.
Now denote by
(); 0Jt tthe external environment
process, and suppose that it is a homogeneous, irreduci-
ble and recurrent Markov process with a finite state space
W. G. YU ET AL.
84
1,2,3,,Em
and intensity matrix
,1
m
ij ij
 ,
where

iii for i. Let be the number of
claims occurring in E

Nt
0,t. If
J
si for allin a small
interval s
,tt h
Nt
, then the number of claims occurring in
that interval, , is assumed to follow a

h N

t
Poisson distribution with parameter , and the n
th claim amounts n
0
i
X
have distribution ()
i
x with
density function
i
f
xand finite mean
i
uiE

. More-
over, We assume that the process and the

;0Jt t
process has independent increments. Then

;0Nt t


Pr1, , 
Nt hnNtnJsi
for

i
tsth hoh
 .
The process is called a Markov-modu

;0Nt t
lated Poisson process, which is a special case of Cox
processes. It also can be seen as a Poisson process with
the parameter driven by an external environment process

;0Jt t.
In this paper, we consider a regime-switching risk mo-
del with debit interest and constant dividend barrier. In
this model, the insurer could borrow an amount of money
equal to the deficit at a debit interest force
when the
surplus is negative. Meanwh ile, the insurer will repay the
debts con tinuously from his premium income. The nega-
tive su rplus may return to a p osit ive leve l. Ho wev er, when
the negative surplus attains the level c
or is below
c
, the surplus is no longer able to be positive, be-
cause the deb ts of the insurer at this time are greater than
or equal to c
, which is the present value at that time
for all premium income available after that point. Abso-
lute ruin occurs at this moment. Moreover, When the
surplus exceeds the constant barrier , dividends
are paid continuously so the surplus stays at the level b
until a new claim occurs. The corresponding sur- plus
process is given by
b
u

;0
b
Utt
 

1
d
d
b
Nt
k
k
Utc UtIUtt
X
 



0d
u
(1.1)
where is the initial surplus and

0U

I
B means
the indicator function of an event B.
Let be the cumulative amount of dividends paid
out up to timetand

Dt
0
the force of interest, then

,0ed
b
Tt
ub
D
Dt (1.2)
is the present value of all dividends until time of ruin ,
b
T
where denoted by
b
T


inf 0:
bb
TtUtc
  is
the time of absolute ruin.
In the sequel we will be interested in the momentgen-
erating function
 
,
,,e0,
ub
yD
i
M
uybEJi i E



,
and the n th moment func tion
 
,,
;0
,
n
ni ub
Vub EDJi
nNiE




,
,
with
0, ;
iub
V1
, and the expected discounted pen-
alty function, for iE



 
,
e, 0,
b
i
Tb
bbbb b
ub
EUTTITUuJ
U
0i

(1.3)
where,
bb
UT
is the surplus prior to absolute ruin
and
bb
UT is the deficit at absolute ruin. The penalty
function
11
,
x
x
is an arbitrary nonnegative measure
able function defined on
,,cc

 . Throu-
ghout this paper we assume that

,,
i
M
uyb,
,;
ni
Vub
and
,
iub are sufficiently smooth functions in u and
, respectively.
yThen the expected present value of the total dividend
payments until ruin in the stationary case is given by
 
1
,,
m
ii
i
VubVub

where
1,,
 m is the stationary initial distribu-
tion of process
;0tJt .
The rest of the paper is organized as follows. In Sec-
tion 2, we obtain the integro-differential equations for the
moment-generating function and boundary conditions in
a regime-switching risk model. In Section 3, the integro–
differential equations satisfied by higher moment of the
dividend payments and boundary conditions are derived.
In the last section, we get the systems of integro-differential
equations for
,
iub
and it’s matrix form.
2. Moment-Generating Function of Du.b
We now derive the systems of integro-differential equa-
tions satisfied by
,,
i
M
uyb
i
, for . Clearly, the mo-
ment-generating function iE

,;
M
uyb behaves differently,
depending on whether its initial surplusuis below zero or
above the barrier level b. He nce, we write
1,;
i
M
uyb for
0ub
and
2,;
i
M
uyb for 0uc
.
Theorem 2.1
For 0ub
,
Copyright © 2011 SciRes. JMF
85
W. G. YU ET AL.
  



 
11
1
1
0
2
0
1
1
,;,; ,;
,; d
,; d
,; ,
ii
ii
u
ii i
c
u
ii i
m
iiik k
k
M uybM uyb
cy Mu
uy
MuxybFx
MuxybFx
yb
F
ucM uyb
iE








(2.1)
and, for 0cu
,

 
 



22
2
2
0
2
1
,; ,;
,;
,;
,;
ik
ii
ii ii
c
u
ii i
m
k
k
Muyb Muyb
uc y
uy
Muyb Fuc
M
uxybdFx
Muyb
iE







(2.2)
with boundary conditions, for , iE

11
,; ,;
ii
ub
Muyb yMby b
u
(2.3)
2,; 1
i
Mcyb
(2.4)
Proof. Considering a small time interval
0,t
tb
, with
being sufficiently small that , there
are four possible events regarding the occurrence of the
claim and the change of the environment:
0tt
uc
1) No claim and no change of environment occur in
0,t;
2) A claim occurs in
0,t (it can either cause the
absolute ruin or not);
3) The environment changes in
0,t;
4) Two or more events occur in
0,t.
In view of the strong Markov property of the surplus
process , we have


,0
b
Utt
 
,;,e;
t
iib
M
uybEMUt yb


. (2.5)
Conditioning on the event occurring in the interval
0,t, we have










11
1
0
2
1
1,
,;1,e ;
,e; d
,e; d
,e ;.
t
iiii
uct t
ii i
c
uct t
ii
uct
ii
mt
ik k
kki
Muybt tMuctyb
tMuctxybFx
tMuctxybF
tF uctc
tMuctybot




 




i
x
(2.6)
Taylor’s expansion gives




11
1
1
,; ,;
,;
,;
.
t
ii
i
i
Muctb Muyb
ye
M
uyb
ct u
M
uyb
yt u
ot

(2.7)
Substituting (2.7) into (2.6), dividing both sides by t,
and letting , we obtain (2.1).
0t
Similarly, when 0cu
, we still consider a small
time interval
0,t, with
0ttbeing sufficiently small
so that the surplus will not reach 0 in the time interval.
Let t0 be the solution to

,e e1
tt
hut uc

0

then
,hut
is the surplus at time 0 if no claim
occurs prior to time t0. We assume 0. So condition-
ing on the time and the amount of the first claim, we
have
tt
tt











22
(,)
2
0
2
1,
,;1, ,e;
,,e;d
,
,,e;
t
iiii
c
hut t
ii
ii
mt
ik k
kki
MuybttMhutyb
tMhutxybF
tFhutc
tMhutybot



 



i
x
(2.8)
By Taylor’s expansion




22
2
2
,,e; ,;
,;
,;
t
ii
i
i
Mhutyb Muyb
M
uyb
uctu
Muyb
yto t
y


(2.9)
Copyright © 2011 SciRes. JMF
W. G. YU ET AL.
86
Substituting (2.9) into (2.8), dividing both sides by t, and
letting , we obtain (2.2) .
0t
When the initial surplus is b, we obtain










11
1
0
2
1
1,
,;1e,e;
,e; d
,e;d
e
e,e;
yct t
iiii
b
yct t
iii
c
b
yct t
ii
b
yct
ii
m
yct t
ik k
kki
Mbybt tMbyb
teMbx ybFx
teMbxybFx
tFbc
tMbybo



 




i
t
(2.10)
Using Taylor’s expansion and noting that ii
,
we have, for ,
iE










11
1
0
2
1
1,
,; ,;
,e; d
,e; d
,e ;
iii
bt
ii i
c
bt
ii i
b
ii
mt
ik k
kki
Mbyb
ycyMbyb
y
Mbxy bFx
M
bxy bFx
Fb c
M
byb ot








(2.11)
Letting in (2.1) and comparing it with (2.11),
we obtain (2.3).
ub
When uc
 , absolute ruin is immediate. Thus, no
dividend is paid. So we obtain (2.4). Theorem 2.1 is
proved.
Theorem 2.2 For , iE

12
0,; 0,;
ii
M
yb Myb  (2.12)
Proof. For 0cu
, letting 0
be the time that the
surplus reach 0 for the first time from and using
the Markov property of the surplus process, we obtain
0u



 








,
,
0
0
0
20
0
00
0
0
0
0
10
,; e
e
expe d
expee d
0, ;
ub
i
ub
i
b
i
b
i
yD
u
ib
yD
ub
T
ut
b
b
T
ut
b
b
ib
Muyb EIT
EI T
EI TyDt
PT
EI TyDt
PT
MybP T









 









(2.13)
Similarly, we obtain










,
,
0
0
0
2000
0
10
0
110
()10
,;, e
e
0, ;e,
0, ;e
e0,;
ub
i
ub
i
i
yD
u
ib
yD
u
ib
u
ib
b
ib
tib
Muyb EITt
EI T
00
0
M
yb EITt
PT
M
ybPT tPT
MybPT


















(2.14)
where is the time of the first claim.
1
T
When 0u
, we notice that 0
and both go into
zero. Letting
0
t
0u
in (2.13) and (2.14) and in view of
0
0
lim 0
b
uPT

we obtain (2.12). Theorem 2.2 is proved.
3. Higher Moment of the Dividend Payments
By the definitions of
,;
M
uyb and , we ob-
tain, for
,Vub
iE
,

1,
1
,; 1,
!
n
i
n
y
1,n
i
M
uybV ub
n

(3.1)
2
1
(,;) 1,
!
n
i
n
y
,2,n
i
M
uybVub
n

(3.2)
where


,1,
,
,2,
;,0
;;, /0
ni
ni
ni
Vub ub
Vub Vub cu


Substituting (3.1) and (3.2) into (2.1) and (2.2), respec-
tively, and comparing the coefficients of yn yield the fol-
lowing integro-differential equations:





,1, ,1,
,1,
0
,2,
,1,
1
,,
,d
,d
,
nii ni
u
inii
c
u
ini i
u
m
ik n k
k
cVubnVub
VuxbFx
VuxbFx
Vub




(3.3)
for 0ub
, and for 0cu
,




,2, ,2,
,2,
0
,2,
1
,,
,d
,



nii ni
c
u
ini i
m
ik nk
k
ucVubnV ub
VuxbFx
Vub
(3.4)
Copyright © 2011 SciRes. JMF
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W. G. YU ET AL.
Substituting (3.1) into (2.3), similarly, we obt ain
,1, 1,1,
,| ,
niubn i
VubnVbb

(3.5)
thus, is an obvious result since

1,1, ,
i
Vbb1
0,1,i,1Vbb.
Substituting (3.1) and (3.2) into (2.4) and (2.12), we
obtain, for
nN

,2, ,
ni
Vcb
0
b
b
(3.6)

,1, ,2,
0, 0,
nin i
VbV  (3.7)
Letting in (3.3) and in (3.4) and using (3.7),
we obtain, for
0u0u
nN

,1, ,2,
0, 0,
nin i
VbV

  (3.8)
4. Expected Discounted Penalty Function
In this section, we derive integro-differential equations
for the expected discounted penalty function. For iE
,
define
 

1
2
,,0
,,, 0
i
i
i
ubu b
ub ubc u



Theorem 4.1 For , 0ub






 
1, 1,
1,
0
2,
1,
1
,,
,d
,d
,,
iii
u
ii i
c
u
iii
u
m
ikki i
k
cub ub
uxbFx
uxbFx
ubA uiE





 
(4.1)
and, for 0cu
,





 
2, 2,
2,
0
2,
1
,,
,d
,,
iii
c
u
iii
m
iiik i
k
u cubub
uxbFx
A
uub




 
iE
(4.2)
with boundary conditions
1, ,
ibb
0
b
b
(4.3)
 
1, 2,
0, 0,
ii
b (4.4)
 
1, 2,
0, 0,
ii
b

 (4.5)
where
 
,d
c
ii
u
A
uuxuF

x
Proof. For and . Similar to argument
as in Section 2, we condition on the events that can occur
in the small time interval
iE0ub
0,t.








11
1
0
2
1
1,
,(1 )e,
e,
e,
e,d
e,
t
iiii
uct
t
ii i
c
uct
t
ii
uct
tc
ii
u
m
tik k
kki
ubttu ctb
tuctxbF
tuctxb
tuxuFx
tuctb
ot









d
d
i
x
Fx
(4.6)
Since
e1
thoh

we then get






11
1
0
2
1
1,
,1 ,
,d
,d
,d
,
iiii
uct
ii i
c
uct
ii
uct
c
ii
u
m
ik k
kki
ubtuctb
tuctxbFx
tuctxbF
tuxuFx
tuctbo











i
x
t
(4.7)
Equation (4.7) can be rewritten as









11
1
1
0
2
1
1,
,,
,
,d
,d
,d
,
ii
ii i
uct
ii i
c
uct
ii i
uct
c
ii
u
m
ik k
kki
uctb ub
t
uctb
uctxbFx
uctxbFx
uxuFx
ot
uctb t




 





(4.8)
Letting in (4.8) and noting that 0tii i
, we
obtain (4.1).
For iE
and 0cu
, we have











22
(,)
2
0
(,)
2
1,
,1 e,,
e,,d
e,,,
e,,
t
iiii
c
hut
t
ii i
tc
ii
hut
m
tik k
kki
ubtthub b
thubxbF
th ubxh ubFx
thubbot







 
d
x
(4.9)
By Taylor’s expansion
Copyright © 2011 SciRes. JMF
W. G. YU ET AL.
88




22 2
,, ,,
ii i
hubbubuctub ot

1,2
(4.10)
Substituting (4.10) into (4.9), dividing both sides by t,
and letting , we obtain (4.2). Theorem 4.1 is proved.
0t
Integro-differential Equations (4.1) and (4.2) can easily
be rewritten in matrix form.
Let .

T
1
,,,,(,), 
jj jm
ubububjΦ
“T” denoting transpose. Then the vectors of the expected
discounted penalty function
1,ubΦ and
2,ubΦ sat-
isfy the following integro-differential equations
 
 
 

111
11
0
12
1
,,
,d
,d
,0
u
c
u
u
ub ub
x
uxbx
x
uxbx
uub



P
G
G
A

 
 

222
22
0
2
,(),
,d
,/0


c
u
ubuub
x
uxbx
uc u

P
G
A
where

11
diag,,mc
 



P



21
diag,,
 



m
uu
Pc
 

111
diag, ,

 mm
x
fxf xcG
 



11
2diag ,...,



 



mm
f
xf
xuc uc
Gx
are all matrices, and and defined
b
y
mm

1uA

2uA

11
,dx
c
u
uuuxIxAG
 
22
,d

c
u
uuxuxAGxI
are all -dimensional vector, in whichm

1,1, ,1
I

2,ub
is
an column vector. The continuity condition and
derivative condit i on for and is
1m
1,ub
12
0, 0, bbΦ
 
12
0, 0,

 bb
5. Time to Reach the Dividend Barrier
In this section, we consider how long it takes for the surplus
process to reach the dividend barrier b from the initial
surplus u without ruin occurring. We define b
to be the
first time that the surplus reaches b, and for 0
,
iE
and cub
, define
 
,|0
b
ibb
LubEeIT UuJi

,0

(5.1)
,
i
Lub can be interpreted as the expected present va-
lue of one dollar payable at the time of reaching the bar-
rier b without ruin occurring, given that the initial envi-
ronment state is i and the initial surplus is u. Alterna-
tively, it can be viewed as the Laplace transform of the
time to reach the dividend barrier b without ruin occur-
ring with respect to the parameter
.
We define
 

1,
2,
;0
;;0
i
i
i
Lubub
Lub Lub c u


(5.2)
Using the same arguments as in Section 2, we can eas-
ily show that
,
i
Lub satisfies the following integro-
differential equations :





1, 1,
1,
0
2,
1,
1
,,
,d
,d
,
iii
u
ii i
c
u
iii
u
m
ik k
k
cL ubL ub
LuxbFx
LuxbFx
Lub




(5.3)
for 0ub
, and for 0cu
,




2, 2,
2,
0
2,
1
,,
,)d
,
iii
c
u
iii
m
ik k
k
ucL ubLub
LuxbFx
Lub



(5.4)
with boundary conditions
1, ;1
iub
Lub

1, 2,
0; 0;
ii
LbL
b


1, 2,
0; 0;
ii
LbL

b

6. Acknowledgements
We would like to thank the anonymous referee who gave
us many insightful suggestions and valuable comments
on the previous version of this paper. This work is sup-
ported by Humanities and Social Sciences Project of the
Ministry Education of China (No. 09YJC910004, No.
10YJC630092) and Natural Science Foundation of
Shandong Province (No. ZR2010GL013) and Research
Program of Higher Education of Shandong Province (No.
J10WF84) and Natural Science Foundation of Shandong
Jiaotong University (No. Z201 031).
Copyright © 2011 SciRes. JMF
W. G. YU ET AL.
Copyright © 2011 SciRes. JMF
89
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