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Hindawi Publishing Corporation
Discrete Dynamics in Nature and Society
Volume 2013, Article ID 128796, 8 pages
http://dx.doi.org/10.1155/2013/128796
Research Article
Studies on a Double Poisson-Geometric Insurance Risk
Model with Interference
Yujuan Huang1 and Wenguang Yu2
1
2
School of Science, Shandong Jiaotong University, Jinan 250023, China
School of Insurance, Shandong University of Finance and Economics, Jinan 250014, China
Correspondence should be addressed to Yujuan Huang; yujuanh518@163.com
Received 11 January 2013; Accepted 5 March 2013
Academic Editor: Hua Su
Copyright © 2013 Y. Huang and W. Yu. This is an open access article distributed under the Creative Commons Attribution License,
which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
This paper mainly studies a generalized double Poisson-Geometric insurance risk model. By martingale and stopping time
approach, we obtain adjustment coefficient equation, the Lundberg inequality, and the formula for the ruin probability. Also the
Laplace transformation of the time when the surplus reaches a given level for the first time is discussed, and the expectation and its
variance are obtained. Finally, we give the numerical examples.
1. Introduction
In insurance mathematics, the classical risk model has been
the center of focus for decades [1–3]. The surplus π‘ˆ(𝑑) in the
classical model at time 𝑑 can be expressed as
𝑁1 (𝑑)
π‘ˆ (𝑑) = 𝑒 + 𝑐𝑑 − ∑ π‘Œπ‘– ,
(1)
𝑖=1
where 𝑒 = π‘ˆ(0) > 0 is the initial capital, 𝑐 > 0 is the constant
rate of premium, and {𝑁1 (𝑑), 𝑑 ≥ 0} is a Poisson process, with
Poisson rate πœ† 1 > 0 denoting the number of claims up to
time 𝑑. The individual claim sizes π‘Œ1 , π‘Œ2 , . . ., independent of
{𝑁1 (𝑑), 𝑑 ≥ 0}, are independent and identically distributed
nonnegative random variables with common distribution
function 𝐹(𝑦) with mean πœ‡π‘Œ , variance πœŽπ‘Œ2 , and moment
generating function π‘€π‘Œ (π‘Ÿ) = 𝐸[π‘’π‘Ÿπ‘Œ ].
But in the Poisson process, the expectation and variance
are equal. This is obviously not consistent with actual situation. So recently there is a huge amount of literature devoted
to the generalization of the classical model in different ways.
Lu and Li [4] consider a Markov-modulated risk model in
which the claim interarrivals, claim sizes, and premiums are
influenced by an external Markovian environment process.
Tan and Yang [5] discuss the compound binomial risk model
with an interest on the surplus under a constant dividend
barrier and periodically paying dividends. Vellaisamy and
Upadhye [6] study the convolution of compound negative
binomial distributions with arbitrary parameters. The exact
expression and also a random parameter representation are
obtained. Cossette et al. [7] present a compound Markov
binomial model, which is an extension of the compound
binomial model. The compound Markov binomial model is
based on the Markov Bernoulli process which introduces
dependency between claim occurrences. Recursive formulas
are provided for the computation of the ruin probabilities
over finite- and infinite-time horizons. A Lundberg exponential bound is derived for the ruin probability, and numerical
examples are also provided. Yang and Zhang [8] investigate
a Sparre Andersen risk model in which the inter-claim times
are generalized Erlang(n) distributed. Czarna and Palmowski
[9] focus on a general spectrally negative Levy insurance
risk process. For this class of processes, they analyze the socalled Parisian ruin probability, which arises when the surplus
process stays below 0 longer than a fixed amount of time 𝑑 > 0.
In this paper, we will consider a double PoissonGeometric risk model with diffusion in which the arrival
of policies is a Poisson-Geometric process and the claims
process follows the compound Poisson-Geometric process.
For more details and new developments on the PoissonGeometric risk model, the interested readers can refer to [10–
13].
The rest of the paper is organized as follows. In Section 2,
the risk model is introduced. In Section 3, we obtain the
2
Discrete Dynamics in Nature and Society
adjustment coefficient equation and the formula of ruin probability. Then we present the effect of the related parameters on
the adjustment coefficient. In Section 4, using the martingale
method, the time when the surplus reaches a level firstly is
considered, and the expectation and its variance are obtained.
Numerical illustrations are also given.
For the risk model (3), the time to ruin, denoted by 𝑇, is
defined as
𝑇 = inf {𝑑 ≥ 0 | π‘ˆ (𝑑) < 0} .
(7)
And define the ruin probability with an initial surplus 𝑒 > 0
by πœ“(𝑒), namely,
2. The Risk Model
πœ“ (𝑒) = Pr (𝑇 < ∞ | π‘ˆ (0) = 𝑒) .
Definition 1 (see [10]). A distribution is said to be PoissonGeometric distributed, denoted by 𝑃𝐺(πœ†, 𝜌), if its generating
function is
πœ† (𝑑 − 1)
},
exp {
(2)
1 − πœŒπ‘‘
3. The Ruin Probability
Define the profits process by {𝑆(𝑑); 𝑑 ≥ 0}; that is,
𝑁3 (𝑑)
where πœ† > 0, 0 ≤ 𝜌 < 1. Note that if 𝜌 = 0, then
the Poisson-Geometric distribution degenerates into Poisson
distribution.
Definition 2 (see [10]). Let πœ† > 0 and 0 ≤ 𝜌 < 1, then
{𝑁(𝑑), 𝑑 ≥ 0} is said to be a Poisson-Geometric process with
parameters πœ†, 𝜌 if it satisfies
(1) 𝑁(0) = 0;
(2) {𝑁(𝑑), 𝑑 ≥ 0} has stationary and independent increments;
(3) for all 𝑑 > 0, 𝑁(𝑑) is a Poisson-Geometric distributed
with parameters πœ†, 𝜌, and 𝐸[𝑁(𝑑)] = πœ†π‘‘/(1 −
𝜌), Var[𝑁(𝑑)] = πœ†π‘‘(1 + 𝜌)/(1 − 𝜌)2 .
𝑆 (𝑑) = 𝑐𝑁2 (𝑑) − ∑ π‘Œπ‘˜ + πœŽπ‘Š (𝑑) .
Obviously we have
𝐸 [𝑆 (𝑑)] = [
πœ† πœ‡
πœ†2𝑐
− 3 π‘Œ ] 𝑑,
1 − 𝜌2 1 − 𝜌3
Var [𝑆 (𝑑)] = 𝑐2 Var [𝑁2 (𝑑)] + Var [𝑁3 (𝑑)] ⋅ 𝐸2 [π‘Œπ‘˜ ]
+ 𝐸 [𝑁3 (𝑑)] ⋅ Var [π‘Œπ‘˜ ] + 𝜎2 Var [π‘Š (𝑑)]
= [
πœ† 2 𝑐2 (1 + 𝜌2 )
2
(1 − 𝜌2 )
+
+
πœ† 3 (1 + 𝜌3 ) πœ‡π‘Œ2
(10)
2
(1 − 𝜌3 )
πœ† 3 πœŽπ‘Œ2
+ 𝜎2 ] 𝑑.
1 − 𝜌3
Let
𝑁3 (𝑑)
(3)
𝛼=
πœ† πœ‡
πœ†2𝑐
− 3 π‘Œ,
1 − 𝜌2 1 − 𝜌3
πœ† 2 𝑐2 (1 + 𝜌2 )
πœ† 3 (1 + 𝜌3 ) πœ‡π‘Œ2
π‘˜=1
where 𝑁2 (𝑑) is the number of premium up to time 𝑑 and
follows a Poisson-Geometric distribution with parameters πœ† 2
and 𝜌2 ; 𝑁3 (𝑑) is the number of claims up to time 𝑑 and follows
a Poisson-Geometric distribution with parameters πœ† 3 and 𝜌3 .
π‘Š(𝑑) is the standard Brownian motion and 𝜎 is a constant,
representing the diffusion volatility parameters. Throughout
this paper, we assume that 𝑁2 (𝑑), 𝑁3 (𝑑), π‘Š(𝑑), and {π‘Œπ‘˜ } are
mutually independent.
In order to ensure the insurance company’s stable operation, we assume
𝑁3 (𝑑)
𝐸 [𝑐𝑁2 (𝑑) − ∑ π‘Œπ‘˜ + πœŽπ‘Š (𝑑)] > 0,
(9)
π‘˜=1
The corresponding moment generating function of 𝑁(𝑑)
is 𝑀𝑁(𝑑) (π‘Ÿ) = exp[πœ†π‘‘(π‘’π‘Ÿ − 1)/(1 − πœŒπ‘’π‘Ÿ )].
Then the double Poisson-Geometric risk model with
interference is defined as
π‘ˆ (𝑑) = 𝑒 + 𝑐𝑁2 (𝑑) − ∑ π‘Œπ‘˜ + πœŽπ‘Š (𝑑) ,
(8)
(4)
π‘˜=1
𝛽=
2
(1 − 𝜌2 )
+
2
(1 − 𝜌3 )
πœ† 𝜎2
+ 3 π‘Œ + 𝜎2 .
1 − 𝜌3
(11)
Then
𝐸 [𝑆 (𝑑)] = 𝛼𝑑,
Var [𝑆 (𝑑)] = 𝛽𝑑.
(12)
Lemma 3. The profits process {𝑆(𝑑); 𝑑 ≥ 0} has the following
properties:
(1) 𝑆(0) = 0;
which implies
πœ† πœ‡
πœ†2𝑐
− 3 π‘Œ > 0.
1 − 𝜌2 1 − 𝜌3
(5)
Let
πœ† πœ‡
πœ†2𝑐
= (1 + πœƒ) 3 π‘Œ .
1 − 𝜌2
1 − 𝜌3
Then πœƒ > 0 is the relative security loading factor.
(6)
(2) {𝑆(𝑑); 𝑑 ≥ 0} has stationary and independent increments.
Theorem 4. For the profits process {𝑆(𝑑); 𝑑 ≥ 0}, there is a
function 𝑔(π‘Ÿ) such that
𝐸 [𝑒−π‘Ÿπ‘†(𝑑) ] = 𝑒𝑑𝑔(π‘Ÿ) .
(13)
Discrete Dynamics in Nature and Society
3
0.855
0.164
0.85
0.162
0.845
𝑅
0.16
𝑅 0.84
0.158
0.835
0.83
0.156
0.825
0.154
0.47
0.48
0.49
0.5
0.51 0.52
𝑐
0.53
0.54
0.55
0.56
0.82
0.36
0.37
Figure 1: The impact of 𝑐 on 𝑅.
0.89
−π‘Ÿπ‘†(𝑑)
0.88
] = 𝐸 {exp [−π‘Ÿπ‘π‘2 (𝑑)]} ⋅ 𝐸
0.41
πœ†2
0.42
0.43
0.44
0.45
0.24
0.25
0.86
× {exp [π‘Ÿ ∑ π‘Œπ‘˜ ]} ⋅ 𝐸 {exp [−π‘ŸπœŽπ‘Š (𝑑)]}
π‘˜=1
0.85
(14)
πœ† 2 (𝑒−π‘Ÿπ‘ − 1)
1 − 𝜌2 𝑒−π‘Ÿπ‘
+πœ† 3
0.4
0.87
𝑁3 (𝑑)
= exp {𝑑 [
0.39
Figure 2: The impact of πœ† 2 on 𝑅.
Proof. Consider
𝐸 [𝑒
0.38
𝑅 0.84
0.83
0.82
π‘€π‘Œ (π‘Ÿ) − 1
1
+ 𝜎2 π‘Ÿ2 ] } .
1 − 𝜌3 π‘€π‘Œ (π‘Ÿ) 2
0.81
0.8
Let
𝑔 (π‘Ÿ) =
πœ† 2 (𝑒−π‘Ÿπ‘ − 1)
π‘€π‘Œ (π‘Ÿ) − 1
1
+ 𝜎2 π‘Ÿ2 .
+ πœ†3
1 − 𝜌2 𝑒−π‘Ÿπ‘
1 − 𝜌3 π‘€π‘Œ (π‘Ÿ) 2
(15)
0.79
0.16
0.17
0.18
0.19
0.2
0.21
0.22
0.23
πœ†3
Then we obtain (13).
Figure 3: The impact of πœ† 3 on 𝑅.
Theorem 5. Equation
𝑔 (π‘Ÿ) = 0
(16)
has a unique positive solution π‘Ÿ = 𝑅 > 0, and (16) is said to
be an adjustment coefficient equation of the risk model (3) and
𝑅 > 0 is said to be an adjustment coefficient.
Proof. From (15), we have 𝑔(0) = 0, and since
𝑔󸀠 (π‘Ÿ) =
𝑔󸀠󸀠 (π‘Ÿ) =
−π‘Ÿπ‘
π‘πœ† 2 𝑒
(𝜌2 − 1)
(1 − 𝜌2
2
𝑒−π‘Ÿπ‘ )
π‘Ÿπ‘Œ
+
πœ† 3 (1 − 𝜌3 ) 𝐸 [π‘Œπ‘’ ]
2
(1 − 𝜌3 π‘€π‘Œ (π‘Ÿ))
+ 𝜎2 π‘Ÿ,
𝑐2 πœ† 2 𝑒−π‘Ÿπ‘ (1 − 𝜌2 ) (1 + 𝜌2 𝑒−π‘Ÿπ‘ )
3
(1 − 𝜌2 𝑒−π‘Ÿπ‘ )
+
πœ† 3 (1 − 𝜌3 ) [1 − 𝜌3 π‘€π‘Œ (π‘Ÿ)]
[1 − 𝜌3 π‘€π‘Œ (π‘Ÿ)]
4
2
× {(1− 𝜌3 π‘€π‘Œ (π‘Ÿ)) 𝐸 [π‘Œ2 π‘’π‘Ÿπ‘Œ ]+ 2𝜌[𝐸 (π‘Œπ‘’π‘Ÿπ‘Œ )] }+𝜎2 ,
(17)
which imply
𝑔󸀠 (0) = −
πœ† πœ‡
πœ† πœ‡
πœ†2𝑐
+ 3 π‘Œ = −πœƒ 3 π‘Œ < 0.
1 − 𝜌2 1 − 𝜌3
1 − 𝜌3
(18)
It is easy to see that the moment generating function
π‘€π‘Œ (π‘Ÿ) is an increasing function. Due to 0 < 𝜌3 < 1, there
exists an π‘Ÿ1 such that π‘€π‘Œ (π‘Ÿ1 ) = 1/𝜌3 ; that is, 1 − 𝜌3 π‘€π‘Œ (π‘Ÿ) > 0
when 0 < π‘Ÿ < π‘Ÿ1 . So when 0 < π‘Ÿ < π‘Ÿ1 , 𝑔󸀠󸀠 (π‘Ÿ) > 0 and
𝑔(π‘Ÿ) is a convex function with limπ‘Ÿ → +∞ 𝑔(π‘Ÿ) = +∞. Then
it can be shown that 𝑔(π‘Ÿ) has a unique positive solution on
(0, +∞).
Example 6. Suppose 𝑐 = 0.5, πœ† 2 = 0.4, πœ† 3 = 0.2, 𝜌2 = 0.9, and
𝜌3 = 0.6, 𝛼 = 0.9, 𝜎 = 1.4. By (16), we obtain the adjustment
coefficient 𝑅 = 0.158. Moreover, we give the effect of related
parameters on adjustment coefficient 𝑅; see Figures 1, 2, 3, 4,
5, 6, and 7.
For the profits process {𝑆(𝑑); 𝑑 ≥ 0}, let 𝐹𝑑𝑠 = 𝜎{𝑆(V); V ≤ 𝑑}.
4
Discrete Dynamics in Nature and Society
0.86
0.846
0.855
0.844
0.842
0.85
0.84
𝑅 0.845
𝑅 0.838
0.84
0.836
0.834
0.835
0.83
0.88
0.832
0.89
0.9
0.91
𝜌2
0.92
0.93
0.94
0.95
0.83
0.86 0.87
Figure 4: The impact of 𝜌2 on 𝑅.
0.88
0.89
0.9
𝛼
0.91
0.92
0.93
0.94
0.95
Figure 6: The impact of 𝛼 on 𝑅.
0.86
0.87
0.855
0.86
0.85
0.85
0.845
𝑅 0.84
𝑅 0.84
0.835
0.83
0.83
0.82
0.825
0.82
0.57
0.58
0.59
0.6
𝜌3
0.61
0.62
0.81
1.36
0.63
Proof. Consider
1.4
1.41
1.42
1.43
1.44
1.45
Proof. Consider
𝐸 [𝑒−π‘Ÿπ‘†(𝑑)−𝑑𝑠 | 𝐹V𝑠 ] = 𝐸 [𝑒−π‘Ÿπ‘†(𝑑)−𝑑𝑔(π‘Ÿ) | 𝐹V𝑠 ]
= 𝐸 [𝑒−π‘Ÿπ‘†(V)−𝑑𝑔(π‘Ÿ)−π‘Ÿ[𝑆(𝑑)−𝑆(V)]−(𝑑−V)𝑔(π‘Ÿ) | 𝐹V𝑠 ]
𝑒−π‘Ÿ(𝑒+𝑆(𝑑))
𝐸 [𝐻𝑒 (𝑑) | 𝐹V𝑠 ] = 𝐸 [ 𝑑𝑔(π‘Ÿ) | 𝐹V𝑠 ]
𝑒
= 𝐻𝑒 (V) 𝐸 [
1.39
Figure 7: The impact of 𝜎 on 𝑅.
Theorem 7. {𝐻𝑒 (𝑑); 𝐹𝑑𝑠 ; 𝑑 ≥ 0} is a martingale, where 𝐻𝑒 (𝑑) =
𝑒−π‘Ÿ(𝑒+𝑆(𝑑)) /𝑒𝑑𝑔(π‘Ÿ) .
𝑒−π‘Ÿ(𝑒+𝑆(V)) 𝑒−π‘Ÿ(𝑆(𝑑)−𝑆(V))
| 𝐹V𝑠 ]
𝑒V𝑔(π‘Ÿ)
𝑒(𝑑−V)𝑔(π‘Ÿ)
1.38
𝜎
Figure 5: The impact of 𝜌3 on 𝑅.
= 𝐸[
1.37
= 𝑒−π‘Ÿπ‘†(V)−𝑑𝑔(π‘Ÿ) ⋅ 𝐸 [𝑒−π‘Ÿ[𝑆(𝑑)−𝑆(V)]−(𝑑−V)𝑔(π‘Ÿ) | 𝐹V𝑠 ]
= 𝑒−π‘Ÿπ‘†(V)−𝑑𝑠 .
(19)
𝑒−π‘Ÿ(𝑆(𝑑)−𝑆(V))
| 𝐹V𝑠 ]
𝑒(𝑑−V)𝑔(π‘Ÿ)
= 𝐻𝑒 (V) .
Theorem 8. If π‘Ÿ and 𝑠 satisfy the equation 𝑔(π‘Ÿ) = 𝑠, then the
surplus {𝑒−π‘Ÿπ‘†(𝑑)−𝑑𝑠 ; 𝑑 ≥ 0} is a martingale.
(20)
Lemma 9. The ruin time 𝑇 is the stopping time of 𝐹𝑑𝑠 .
Theorem 10. For for all π‘Ÿ, the ultimate ruin probability satisfies
πœ“ (𝑒) ≤ 𝑒−π‘Ÿπ‘’ 𝐡 (π‘Ÿ) ,
where 𝐡(π‘Ÿ) = 𝐸[sup𝑑≥0 {exp[𝑑𝑔(π‘Ÿ)]}].
(21)
Discrete Dynamics in Nature and Society
5
500
1
0.9
480
0.8
0.7
460
𝐸[𝜏]
πœ“(𝑒)
0.6
0.5
0.4
440
420
0.3
0.2
400
0.1
0
0
2
4
𝑒
6
8
380
0.4
10
0.45
0.5
0.55
𝜌3
0.6
0.65
0.7
0.75
Figure 10: The impact of 𝜌3 on 𝐸[𝜏].
𝑅 = 0.2
𝑅 = 0.3
𝑅 = 0.4
900
Figure 8: The impact of 𝑅 on ruin probability πœ“(𝑒).
800
700
𝐸[𝜏]
900
800
700
600
500
𝐸[𝜏]
600
400
500
300
0.55
400
0.6
0.65
0.7
300
0.8
0.85
0.9
0.95
1
πœ†2
Figure 11: The impact of πœ† 2 on 𝐸[𝜏].
200
100
0.65
0.75
0.7
0.75
0.8
0.85
0.9
𝜌2
which implies
Figure 9: The impact of 𝜌2 on 𝐸[𝜏].
Pr (𝑇 ≤ 𝑑0 ) =
Proof. For a fixed time 𝑑0 , 𝑑0 ∧ 𝑇 is a bounded stopping time;
using the theorem of martingale and stopping time, we have
+ 𝐸 [𝐻𝑒 (𝑑) | 𝑇 > 𝑑0 ] Pr (𝑇 > 𝑑0 )
≥ 𝐸 [𝐻𝑒 (𝑇) | 𝑇 ≤ 𝑑0 ] Pr (𝑇 ≤ 𝑑0 ) ,
= 𝑒−π‘Ÿπ‘’ sup {exp [𝑑𝑔 (π‘Ÿ)]} ,
0≤𝑑≤𝑑0
(23)
by expectation on both sides of (23), and letting 𝑑0 → +∞,
we can obtain (21).
𝑒−π‘Ÿπ‘’ = 𝐸 [𝐻𝑒 (0)] = 𝐸 [𝐻𝑒 (𝑇 ∧ 𝑑0 )]
= 𝐸 [𝐻𝑒 (𝑇) | 𝑇 ≤ 𝑑0 ] Pr (𝑇 ≤ 𝑑0 )
𝑒−π‘Ÿπ‘’
𝑒−π‘Ÿπ‘’
≤
𝐸 [𝐻𝑒 (𝑇) | 𝑇 < 𝑑0 ] inf 0≤𝑑≤𝑑0 exp [−𝑑𝑔 (π‘Ÿ)]
Theorem 11. The probability of the risk model (3) is
(22)
πœ“ (𝑒) =
𝑒−𝑅𝑒
.
𝐸 [𝑒−π‘…π‘ˆ(𝑇) | 𝑇 < ∞]
(24)
6
Discrete Dynamics in Nature and Society
1000
12000
900
10000
8000
700
Var [𝜏]
𝐸[𝜏]
800
600
6000
4000
500
2000
400
300
0
0.2
0.4
0.6
0.8
0
0.65
1
0.7
0.75
0.8
𝜌2
πœ†3
0.85
0.9
Figure 15: The impact of 𝜌2 on Var[𝜏].
Figure 12: The impact of πœ† 3 on 𝐸[𝜏].
3500
1000
900
3000
800
Var [𝜏]
𝐸[𝜏]
700
600
2500
2000
500
1500
400
300
0
0.2
0.4
0.6
0.8
1000
0.4
1
0.45
0.5
0.55
πœ‡π‘Œ
1000
12000
900
10000
800
0.65
0.7
0.75
8000
Var [𝜏]
700
𝐸[𝜏]
0.6
Figure 16: The impact of 𝜌3 on Var[𝜏].
Figure 13: The impact of πœ‡π‘Œ on 𝐸[𝜏].
600
500
6000
4000
400
2000
300
200
𝜌3
0.7
0.8
0.9
1
1.1
1.2
1.3
𝑐
Figure 14: The impact of 𝑐 on 𝐸[𝜏].
1.4
1.5
0
0.55
0.6
0.65
0.7
0.75
0.8
0.85
0.9
πœ†2
Figure 17: The impact of πœ† 2 on Var[𝜏].
0.95
1
Discrete Dynamics in Nature and Society
7
×104
2.5
12000
10000
2
Var [𝜏]
8000
Var [𝜏]
1.5
6000
1
4000
0.5
2000
0
0
0
0.2
0.4
0.6
0.8
1
0.7
0.8
0.9
1
1.1
1.2
1.3
1.4
1.5
𝑐
Figure 20: The impact of 𝑐 on Var[𝜏].
Figure 18: The impact of πœ† 3 on Var[𝜏].
3700
×10
3
4
3600
2.5
Var (𝜏)
3500
Var [𝜏]
2
3400
1.5
3300
1
3200
0.5
0
3100
0.4
0.8
1
1.2
1.4
1.6
1.8
2
𝜎
0
0.2
0.4
πœ‡π‘Œ
0.6
0.8
1
Figure 19: The impact of πœ‡π‘Œ on Var[𝜏].
−π‘Ÿπ‘’
(25)
𝑒
= 𝐸 [𝑒
(28)
lim 𝐸 [𝑒−π‘…π‘ˆ(𝑇) | 𝑇 > 𝑑0 ] Pr (𝑇 > 𝑑0 ) = 0,
(a.s.) .
(29)
Corollary 12. Consider
| 𝑇 ≤ 𝑑0 ] Pr (𝑇 ≤ 𝑑0 )
−π‘…π‘ˆ(𝑇)
+ 𝐸 [𝑒
0 ≤ 𝑒−π‘…π‘ˆ(𝑑0 ) 𝐼 (π‘ˆ (𝑑0 ) ≥ 0) ≤ 1,
Then when 𝑑0 → ∞ in (26), we can obtain (24).
Let π‘Ÿ = 𝑅, we have
−π‘…π‘ˆ(𝑇)
(27)
Since
𝑑0 → ∞
+ 𝐸 [𝐻𝑒 (𝑇 ∧ 𝑑0 ) | 𝑇 > 𝑑0 ] Pr (𝑇 > 𝑑0 ) .
−𝑅𝑒
= 𝐸 [𝑒−π‘…π‘ˆ(𝑇) 𝐼 (𝑇 > 𝑑0 )] ≤ 𝐸 [𝑒−π‘…π‘ˆ(𝑑0 ) 𝐼 (π‘ˆ (𝑑0 ) ≥ 0)] .
by the law of large numbers, when 𝑑0 → ∞, π‘ˆ(𝑑0 ) → ∞
(a.s.). By dominated convergence theorem, we have
= 𝐻𝑒 (0) = 𝐸 [𝐻𝑒 (𝑇 ∧ 𝑑0 )]
= 𝐸 [𝐻𝑒 (𝑇 ∧ 𝑑0 ) | 𝑇 ≤ 𝑑0 ] Pr (𝑇 ≤ 𝑑0 )
Figure 21: The impact of 𝜎 on Var[𝜏].
0 ≤ 𝐸 [𝑒−π‘…π‘ˆ(𝑇) | 𝑇 > 𝑑0 ] Pr (𝑇 > 𝑑0 )
Proof. 𝑇 is a ruin time and for a fixed time 𝑑0 , 𝑇𝑒 ∧ 𝑑0 is a
bounded stopping time. Using the theorem of martingale and
stopping time, we have
𝑒
0.6
| 𝑇 > 𝑑0 ] Pr (𝑇 > 𝑑0 ) .
(26)
If 𝐼(𝐴) is an indicator function of the event 𝐴, we get
πœ“ (𝑒) ≤ 𝑒−𝑅𝑒 .
(30)
Example 13. Suppose 𝑅 = 0.2, 𝑅 = 0.3, and 𝑅 = 0.4. By (30),
we give the effect of adjustment coefficient 𝑅 on the upper
bound of the ruin probability; see Figure 8.
8
Discrete Dynamics in Nature and Society
4. The Time to Reach a Given Level
Acknowledgments
Let
Y. Huang thanks the three anonymous referees for the
thoughtful comments and suggestions that greatly improved
the presentation of this paper. This work was supported by
the National Natural Science Foundation of China (Grant
no. 11171187, Grant no. 10921101), National Basic Research
Program of China (973 Program, Grant no. 2007CB814906),
Natural Science Foundation of Shandong Province (Grant
no. ZR2012AQ013, Grant no. ZR2010GL013), Humanities and
Social Sciences Project of the Ministry Education of China
(Grant no. 10YJC630092, Grant no. 09YJC910004), and 2013
Major Project Cultivation Plan of Shandong Jiaotong University.
𝜏 = inf {𝑑 ≥ 0 | π‘ˆ (𝑑) = π‘₯} .
(31)
Then 𝜏 is the time when the surplus reaches a given level
firstly.
Theorem 14. The Laplace transform of 𝜏 is
𝐸 [𝑒−π‘ πœ ] = π‘’π‘Ÿπ‘₯ ,
(32)
𝑔 (π‘Ÿ) = 𝑠.
(33)
where π‘Ÿ and 𝑠 satisfy
Proof. For the surplus process {π‘ˆ(𝑑); 𝑑 ≥ 0}, using the
theorem of martingale and stopping time, we see that 𝜏 is a
stopping rime of 𝐹𝑑𝑠 . Let 𝑄(𝑑) = 𝑒−π‘Ÿπ‘ˆ(𝑑)−𝑑𝑠 . By Theorem 8, the
surplus process {𝑄(𝑑); 𝑑 ≥ 0} is a martingale; hence, we have
𝐸 [𝑄 (𝜏)] = 𝐸 [𝑄 (0)] ,
(34)
𝐸 [𝑒−π‘Ÿπ‘ˆ(𝑑)−𝑑𝑠 ] = 1.
(35)
implying that
Since π‘ˆ(𝑑) = π‘₯, so we get
𝐸 [𝑒−π‘ πœ ] = π‘’π‘Ÿπ‘₯ .
(36)
Theorem 15. The expectation and variance of 𝜏 satisfy
π‘₯
𝐸 [𝜏] = ,
𝛼
(37)
π‘₯𝛽
.
𝛼3
Proof. Let πœ‘(𝑠) = ln 𝐸[𝑒−π‘ πœ ]. Using Theorem 11, we have
πœ‘(𝑠) = π‘Ÿπ‘₯. Then
Var [𝜏] =
π‘‘πœ‘ (𝑠) π‘‘πœ‘ (𝑠) π‘‘π‘Ÿ π‘‘πœ‘ (𝑠)
1
π‘₯
,
=
⋅
=
⋅
=
𝑑𝑠
π‘‘π‘Ÿ
𝑑𝑠
π‘‘π‘Ÿ
𝑑𝑔 (π‘Ÿ) /π‘‘π‘Ÿ 𝑔󸀠 (π‘Ÿ)
𝑑2 πœ‘ (𝑠) π‘‘πœ‘σΈ€  (𝑠) π‘‘πœ‘σΈ€  (𝑠) π‘‘π‘Ÿ π‘‘πœ‘σΈ€  (𝑠)
1
=
=
⋅
=
⋅
2
𝑑𝑠
𝑑𝑠
π‘‘π‘Ÿ
𝑑𝑠
π‘‘π‘Ÿ
𝑑𝑔 (π‘Ÿ) /π‘‘π‘Ÿ
=−
π‘₯𝑔󸀠󸀠 (π‘Ÿ)
2
[𝑔󸀠 (π‘Ÿ)]
⋅
𝑔󸀠
π‘₯𝑔󸀠󸀠 (π‘Ÿ)
1
=−
.
3
(π‘Ÿ)
[𝑔󸀠 (π‘Ÿ)]
(38)
Let 𝑠 = π‘Ÿ = 0. We have
𝐸 [𝜏] = −
π‘‘πœ‘ (𝑠) 󡄨󡄨󡄨󡄨
π‘₯
π‘₯
= ,
󡄨󡄨 = − σΈ€ 
𝑑𝑠 󡄨󡄨𝑠=0
𝑔 (0) 𝛼
󡄨
π‘₯𝛽
𝑑2 πœ‘ (𝑠) 󡄨󡄨󡄨
󡄨󡄨
=
.
Var [𝜏] = −
𝑑𝑠2 󡄨󡄨󡄨𝑠=π‘Ÿ=0 𝛼3
(39)
Example 16. Suppose 𝜌2 = 0.75, 𝜌3 = 0.75, πœ† 2 = 0.75, πœ† 3 =
0.5, πœ‡π‘Œ = 0.5, πœŽπ‘Œ = 0.5, 𝜎 = 1, and 𝑐 = 1. By (37), we give the
effect of related parameters on 𝐸[𝜏] and Var[𝜏]; see Figures 9,
10, 11, 12, 13, 14, 15, 16, 17, 18, 19, 20, and 21.
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