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(π‘) in the classical model at time π‘ can be expressed as π1 (π‘) π (π‘) = π’ + ππ‘ − ∑ ππ , (1) π=1 where π’ = π(0) > 0 is the initial capital, π > 0 is the constant rate of premium, and {π1 (π‘), π‘ ≥ 0} is a Poisson process, with Poisson rate π 1 > 0 denoting the number of claims up to time π‘. The individual claim sizes π1 , π2 , . . ., independent of {π1 (π‘), π‘ ≥ 0}, are independent and identically distributed nonnegative random variables with common distribution function πΉ(π¦) with mean ππ , variance ππ2 , and moment generating function ππ (π) = πΈ[πππ ]. 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 π‘ > 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 π, is defined as π = inf {π‘ ≥ 0 | π (π‘) < 0} . (7) And define the ruin probability with an initial surplus π’ > 0 by π(π’), namely, 2. The Risk Model π (π’) = Pr (π < ∞ | π (0) = π’) . Definition 1 (see [10]). A distribution is said to be PoissonGeometric distributed, denoted by ππΊ(π, π), if its generating function is π (π‘ − 1) }, exp { (2) 1 − ππ‘ 3. The Ruin Probability Define the profits process by {π(π‘); π‘ ≥ 0}; that is, π3 (π‘) where π > 0, 0 ≤ π < 1. Note that if π = 0, then the Poisson-Geometric distribution degenerates into Poisson distribution. Definition 2 (see [10]). Let π > 0 and 0 ≤ π < 1, then {π(π‘), π‘ ≥ 0} is said to be a Poisson-Geometric process with parameters π, π if it satisfies (1) π(0) = 0; (2) {π(π‘), π‘ ≥ 0} has stationary and independent increments; (3) for all π‘ > 0, π(π‘) is a Poisson-Geometric distributed with parameters π, π, and πΈ[π(π‘)] = ππ‘/(1 − π), Var[π(π‘)] = ππ‘(1 + π)/(1 − π)2 . π (π‘) = ππ2 (π‘) − ∑ ππ + ππ (π‘) . Obviously we have πΈ [π (π‘)] = [ π π π2π − 3 π ] π‘, 1 − π2 1 − π3 Var [π (π‘)] = π2 Var [π2 (π‘)] + Var [π3 (π‘)] ⋅ πΈ2 [ππ ] + πΈ [π3 (π‘)] ⋅ Var [ππ ] + π2 Var [π (π‘)] = [ π 2 π2 (1 + π2 ) 2 (1 − π2 ) + + π 3 (1 + π3 ) ππ2 (10) 2 (1 − π3 ) π 3 ππ2 + π2 ] π‘. 1 − π3 Let π3 (π‘) (3) πΌ= π π π2π − 3 π, 1 − π2 1 − π3 π 2 π2 (1 + π2 ) π 3 (1 + π3 ) ππ2 π=1 where π2 (π‘) is the number of premium up to time π‘ and follows a Poisson-Geometric distribution with parameters π 2 and π2 ; π3 (π‘) is the number of claims up to time π‘ and follows a Poisson-Geometric distribution with parameters π 3 and π3 . π(π‘) is the standard Brownian motion and π is a constant, representing the diffusion volatility parameters. Throughout this paper, we assume that π2 (π‘), π3 (π‘), π(π‘), and {ππ } are mutually independent. In order to ensure the insurance company’s stable operation, we assume π3 (π‘) πΈ [ππ2 (π‘) − ∑ ππ + ππ (π‘)] > 0, (9) π=1 The corresponding moment generating function of π(π‘) is ππ(π‘) (π) = exp[ππ‘(ππ − 1)/(1 − πππ )]. Then the double Poisson-Geometric risk model with interference is defined as π (π‘) = π’ + ππ2 (π‘) − ∑ ππ + ππ (π‘) , (8) (4) π=1 π½= 2 (1 − π2 ) + 2 (1 − π3 ) π π2 + 3 π + π2 . 1 − π3 (11) Then πΈ [π (π‘)] = πΌπ‘, Var [π (π‘)] = π½π‘. (12) Lemma 3. The profits process {π(π‘); π‘ ≥ 0} has the following properties: (1) π(0) = 0; which implies π π π2π − 3 π > 0. 1 − π2 1 − π3 (5) Let π π π2π = (1 + π) 3 π . 1 − π2 1 − π3 Then π > 0 is the relative security loading factor. (6) (2) {π(π‘); π‘ ≥ 0} has stationary and independent increments. Theorem 4. For the profits process {π(π‘); π‘ ≥ 0}, there is a function π(π) such that πΈ [π−ππ(π‘) ] = ππ‘π(π) . (13) Discrete Dynamics in Nature and Society 3 0.855 0.164 0.85 0.162 0.845 π 0.16 π 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 π 0.53 0.54 0.55 0.56 0.82 0.36 0.37 Figure 1: The impact of π on π . 0.89 −ππ(π‘) 0.88 ] = πΈ {exp [−πππ2 (π‘)]} ⋅ πΈ 0.41 π2 0.42 0.43 0.44 0.45 0.24 0.25 0.86 × {exp [π ∑ ππ ]} ⋅ πΈ {exp [−πππ (π‘)]} π=1 0.85 (14) π 2 (π−ππ − 1) 1 − π2 π−ππ +π 3 0.4 0.87 π3 (π‘) = exp {π‘ [ 0.39 Figure 2: The impact of π 2 on π . Proof. Consider πΈ [π 0.38 π 0.84 0.83 0.82 ππ (π) − 1 1 + π2 π2 ] } . 1 − π3 ππ (π) 2 0.81 0.8 Let π (π) = π 2 (π−ππ − 1) ππ (π) − 1 1 + π2 π2 . + π3 1 − π2 π−ππ 1 − π3 ππ (π) 2 (15) 0.79 0.16 0.17 0.18 0.19 0.2 0.21 0.22 0.23 π3 Then we obtain (13). Figure 3: The impact of π 3 on π . Theorem 5. Equation π (π) = 0 (16) has a unique positive solution π = π > 0, and (16) is said to be an adjustment coefficient equation of the risk model (3) and π > 0 is said to be an adjustment coefficient. Proof. From (15), we have π(0) = 0, and since πσΈ (π) = πσΈ σΈ (π) = −ππ ππ 2 π (π2 − 1) (1 − π2 2 π−ππ ) ππ + π 3 (1 − π3 ) πΈ [ππ ] 2 (1 − π3 ππ (π)) + π2 π, π2 π 2 π−ππ (1 − π2 ) (1 + π2 π−ππ ) 3 (1 − π2 π−ππ ) + π 3 (1 − π3 ) [1 − π3 ππ (π)] [1 − π3 ππ (π)] 4 2 × {(1− π3 ππ (π)) πΈ [π2 πππ ]+ 2π[πΈ (ππππ )] }+π2 , (17) which imply πσΈ (0) = − π π π π π2π + 3 π = −π 3 π < 0. 1 − π2 1 − π3 1 − π3 (18) It is easy to see that the moment generating function ππ (π) is an increasing function. Due to 0 < π3 < 1, there exists an π1 such that ππ (π1 ) = 1/π3 ; that is, 1 − π3 ππ (π) > 0 when 0 < π < π1 . So when 0 < π < π1 , πσΈ σΈ (π) > 0 and π(π) is a convex function with limπ → +∞ π(π) = +∞. Then it can be shown that π(π) has a unique positive solution on (0, +∞). Example 6. Suppose π = 0.5, π 2 = 0.4, π 3 = 0.2, π2 = 0.9, and π3 = 0.6, πΌ = 0.9, π = 1.4. By (16), we obtain the adjustment coefficient π = 0.158. Moreover, we give the effect of related parameters on adjustment coefficient π ; see Figures 1, 2, 3, 4, 5, 6, and 7. For the profits process {π(π‘); π‘ ≥ 0}, let πΉπ‘π = π{π(V); V ≤ π‘}. 4 Discrete Dynamics in Nature and Society 0.86 0.846 0.855 0.844 0.842 0.85 0.84 π 0.845 π 0.838 0.84 0.836 0.834 0.835 0.83 0.88 0.832 0.89 0.9 0.91 π2 0.92 0.93 0.94 0.95 0.83 0.86 0.87 Figure 4: The impact of π2 on π . 0.88 0.89 0.9 πΌ 0.91 0.92 0.93 0.94 0.95 Figure 6: The impact of πΌ on π . 0.86 0.87 0.855 0.86 0.85 0.85 0.845 π 0.84 π 0.84 0.835 0.83 0.83 0.82 0.825 0.82 0.57 0.58 0.59 0.6 π3 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 πΈ [π−ππ(π‘)−π‘π | πΉVπ ] = πΈ [π−ππ(π‘)−π‘π(π) | πΉVπ ] = πΈ [π−ππ(V)−π‘π(π)−π[π(π‘)−π(V)]−(π‘−V)π(π) | πΉVπ ] π−π(π’+π(π‘)) πΈ [π»π’ (π‘) | πΉVπ ] = πΈ [ π‘π(π) | πΉVπ ] π = π»π’ (V) πΈ [ 1.39 Figure 7: The impact of π on π . Theorem 7. {π»π’ (π‘); πΉπ‘π ; π‘ ≥ 0} is a martingale, where π»π’ (π‘) = π−π(π’+π(π‘)) /ππ‘π(π) . π−π(π’+π(V)) π−π(π(π‘)−π(V)) | πΉVπ ] πVπ(π) π(π‘−V)π(π) 1.38 π Figure 5: The impact of π3 on π . = πΈ[ 1.37 = π−ππ(V)−π‘π(π) ⋅ πΈ [π−π[π(π‘)−π(V)]−(π‘−V)π(π) | πΉVπ ] = π−ππ(V)−π‘π . (19) π−π(π(π‘)−π(V)) | πΉVπ ] π(π‘−V)π(π) = π»π’ (V) . Theorem 8. If π and π satisfy the equation π(π) = π , then the surplus {π−ππ(π‘)−π‘π ; π‘ ≥ 0} is a martingale. (20) Lemma 9. The ruin time π is the stopping time of πΉπ‘π . Theorem 10. For for all π, the ultimate ruin probability satisfies π (π’) ≤ π−ππ’ π΅ (π) , where π΅(π) = πΈ[supπ‘≥0 {exp[π‘π(π)]}]. (21) Discrete Dynamics in Nature and Society 5 500 1 0.9 480 0.8 0.7 460 πΈ[π] π(π’) 0.6 0.5 0.4 440 420 0.3 0.2 400 0.1 0 0 2 4 π’ 6 8 380 0.4 10 0.45 0.5 0.55 π3 0.6 0.65 0.7 0.75 Figure 10: The impact of π3 on πΈ[π]. π = 0.2 π = 0.3 π = 0.4 900 Figure 8: The impact of π on ruin probability π(π’). 800 700 πΈ[π] 900 800 700 600 500 πΈ[π] 600 400 500 300 0.55 400 0.6 0.65 0.7 300 0.8 0.85 0.9 0.95 1 π2 Figure 11: The impact of π 2 on πΈ[π]. 200 100 0.65 0.75 0.7 0.75 0.8 0.85 0.9 π2 which implies Figure 9: The impact of π2 on πΈ[π]. Pr (π ≤ π‘0 ) = Proof. For a fixed time π‘0 , π‘0 ∧ π is a bounded stopping time; using the theorem of martingale and stopping time, we have + πΈ [π»π’ (π‘) | π > π‘0 ] Pr (π > π‘0 ) ≥ πΈ [π»π’ (π) | π ≤ π‘0 ] Pr (π ≤ π‘0 ) , = π−ππ’ sup {exp [π‘π (π)]} , 0≤π‘≤π‘0 (23) by expectation on both sides of (23), and letting π‘0 → +∞, we can obtain (21). π−ππ’ = πΈ [π»π’ (0)] = πΈ [π»π’ (π ∧ π‘0 )] = πΈ [π»π’ (π) | π ≤ π‘0 ] Pr (π ≤ π‘0 ) π−ππ’ π−ππ’ ≤ πΈ [π»π’ (π) | π < π‘0 ] inf 0≤π‘≤π‘0 exp [−π‘π (π)] Theorem 11. The probability of the risk model (3) is (22) π (π’) = π−π π’ . πΈ [π−π π(π) | π < ∞] (24) 6 Discrete Dynamics in Nature and Society 1000 12000 900 10000 8000 700 Var [π] πΈ[π] 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 π2 π3 0.85 0.9 Figure 15: The impact of π2 on Var[π]. Figure 12: The impact of π 3 on πΈ[π]. 3500 1000 900 3000 800 Var [π] πΈ[π] 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 ππ 1000 12000 900 10000 800 0.65 0.7 0.75 8000 Var [π] 700 πΈ[π] 0.6 Figure 16: The impact of π3 on Var[π]. Figure 13: The impact of ππ on πΈ[π]. 600 500 6000 4000 400 2000 300 200 π3 0.7 0.8 0.9 1 1.1 1.2 1.3 π Figure 14: The impact of π on πΈ[π]. 1.4 1.5 0 0.55 0.6 0.65 0.7 0.75 0.8 0.85 0.9 π2 Figure 17: The impact of π 2 on Var[π]. 0.95 1 Discrete Dynamics in Nature and Society 7 ×104 2.5 12000 10000 2 Var [π] 8000 Var [π] 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 π Figure 20: The impact of π on Var[π]. Figure 18: The impact of π 3 on Var[π]. 3700 ×10 3 4 3600 2.5 Var (π) 3500 Var [π] 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 π 0 0.2 0.4 ππ 0.6 0.8 1 Figure 19: The impact of ππ on Var[π]. −ππ’ (25) π = πΈ [π (28) lim πΈ [π−π π(π) | π > π‘0 ] Pr (π > π‘0 ) = 0, (a.s.) . (29) Corollary 12. Consider | π ≤ π‘0 ] Pr (π ≤ π‘0 ) −π π(π) + πΈ [π 0 ≤ π−π π(π‘0 ) πΌ (π (π‘0 ) ≥ 0) ≤ 1, Then when π‘0 → ∞ in (26), we can obtain (24). Let π = π , we have −π π(π) (27) Since π‘0 → ∞ + πΈ [π»π’ (π ∧ π‘0 ) | π > π‘0 ] Pr (π > π‘0 ) . −π π’ = πΈ [π−π π(π) πΌ (π > π‘0 )] ≤ πΈ [π−π π(π‘0 ) πΌ (π (π‘0 ) ≥ 0)] . by the law of large numbers, when π‘0 → ∞, π(π‘0 ) → ∞ (a.s.). By dominated convergence theorem, we have = π»π’ (0) = πΈ [π»π’ (π ∧ π‘0 )] = πΈ [π»π’ (π ∧ π‘0 ) | π ≤ π‘0 ] Pr (π ≤ π‘0 ) Figure 21: The impact of π on Var[π]. 0 ≤ πΈ [π−π π(π) | π > π‘0 ] Pr (π > π‘0 ) Proof. π is a ruin time and for a fixed time π‘0 , ππ’ ∧ π‘0 is a bounded stopping time. Using the theorem of martingale and stopping time, we have π 0.6 | π > π‘0 ] Pr (π > π‘0 ) . (26) If πΌ(π΄) is an indicator function of the event π΄, we get π (π’) ≤ π−π π’ . (30) Example 13. Suppose π = 0.2, π = 0.3, and π = 0.4. By (30), we give the effect of adjustment coefficient π 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. π = inf {π‘ ≥ 0 | π (π‘) = π₯} . (31) Then π is the time when the surplus reaches a given level firstly. Theorem 14. The Laplace transform of π is πΈ [π−π π ] = πππ₯ , (32) π (π) = π . (33) where π and π satisfy Proof. For the surplus process {π(π‘); π‘ ≥ 0}, using the theorem of martingale and stopping time, we see that π is a stopping rime of πΉπ‘π . Let π(π‘) = π−ππ(π‘)−π‘π . By Theorem 8, the surplus process {π(π‘); π‘ ≥ 0} is a martingale; hence, we have πΈ [π (π)] = πΈ [π (0)] , (34) πΈ [π−ππ(π‘)−π‘π ] = 1. (35) implying that Since π(π‘) = π₯, so we get πΈ [π−π π ] = πππ₯ . (36) Theorem 15. The expectation and variance of π satisfy π₯ πΈ [π] = , πΌ (37) π₯π½ . πΌ3 Proof. Let π(π ) = ln πΈ[π−π π ]. Using Theorem 11, we have π(π ) = ππ₯. Then Var [π] = ππ (π ) ππ (π ) ππ ππ (π ) 1 π₯ , = ⋅ = ⋅ = ππ ππ ππ ππ ππ (π) /ππ πσΈ (π) π2 π (π ) ππσΈ (π ) ππσΈ (π ) ππ ππσΈ (π ) 1 = = ⋅ = ⋅ 2 ππ ππ ππ ππ ππ ππ (π) /ππ =− π₯πσΈ σΈ (π) 2 [πσΈ (π)] ⋅ πσΈ π₯πσΈ σΈ (π) 1 =− . 3 (π) [πσΈ (π)] (38) Let π = π = 0. We have πΈ [π] = − ππ (π ) σ΅¨σ΅¨σ΅¨σ΅¨ π₯ π₯ = , σ΅¨σ΅¨ = − σΈ ππ σ΅¨σ΅¨π =0 π (0) πΌ σ΅¨ π₯π½ π2 π (π ) σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ = . Var [π] = − ππ 2 σ΅¨σ΅¨σ΅¨π =π=0 πΌ3 (39) Example 16. Suppose π2 = 0.75, π3 = 0.75, π 2 = 0.75, π 3 = 0.5, ππ = 0.5, ππ = 0.5, π = 1, and π = 1. By (37), we give the effect of related parameters on πΈ[π] and Var[π]; see Figures 9, 10, 11, 12, 13, 14, 15, 16, 17, 18, 19, 20, and 21. References [1] J. Grandell, Aspects of Risk Theory, Springer, New York, NY, USA, 1991. [2] H. U. Gerber, An Introduction to Mathematical Risk Theory, vol. 8 of S.S. Heubner Foundation Monograph Series, Huebner Foundation, Philadelphia, Pa, USA, 1979. [3] S. Asmussen, Ruin Probabilities, vol. 2, World Scientific Publishing Co. Inc., River Edge, NJ, USA, 2000. [4] Y. Lu and S. Li, “On the probability of ruin in a Markovmodulated risk model,” Insurance: Mathematics & Economics, vol. 37, no. 3, pp. 522–532, 2005. [5] J. Tan and X. 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Liu, “A risk model and ruin probability with a compound Poisson-geometric process,” Acta Mathematicae Applicatae Sinica, vol. 28, no. 3, pp. 419–428, 2005. [11] Z. C. Mao and J. E. Liu, “The expression of ruin probability under claim numbers with compound Poisson-Geometric process,” Chinese Journal of Management Science, vol. 15, no. 5, pp. 23–28, 2007. [12] J. D. Liao, R. Z. Gong, Z. M. Liu, and J. Z. Zou, “The GeberShiu discounted penalty function in the Poisson geometric risk model,” Acta Mathematicae Applicatae Sinica, vol. 30, no. 6, pp. 1076–1085, 2007. [13] X. Lin and N. Li, “Ruin probability, optimal investment and reinsurance strategy for an insurer with compound Poissongeometric risk process,” Mathematica Applicata. Yingyong Shuxue, vol. 24, no. 1, pp. 174–180, 2011. 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