Hindawi Publishing Corporation Journal of Applied Mathematics Volume 2013, Article ID 621371, 9 pages http://dx.doi.org/10.1155/2013/621371 Research Article Pricing Options with Credit Risk in Markovian Regime-Switching Markets Jinzhi Li1 and Shixia Ma2 1 2 College of Sciences, Minzu University of China, Beijing 100081, China College of Sciences, Hebei University of Technology, Tianjin 300401, China Correspondence should be addressed to Jinzhi Li; lijinzhi118@gmail.com Received 16 February 2013; Revised 16 May 2013; Accepted 20 May 2013 Academic Editor: Shan Zhao Copyright © 2013 J. Li and S. Ma. 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 investigates the valuation of European option with credit risk in a reduced form model when the stock price is driven by the so-called Markov-modulated jump-diffusion process, in which the arrival rate of rare events and the volatility rate of stock are controlled by a continuous-time Markov chain. We also assume that the interest rate and the default intensity follow the Vasicek models whose parameters are governed by the same Markov chain. We study the pricing of European option and present numerical illustrations. 1. Introduction Pricing options with credit risk is an important topic in finance from both theoretical and practical perspectives. Credit risk refers to an investor’s risk that a borrower will default on making payments as promised. There are basically two kinds of models to describe the default: structural models and reduced form models. The structural approach was firstly introduced by Merton [1] who investigated European option pricing for modeling single corporate default. The approach is further extended by recent literature: see Ammann [2] and Klein and Inglis [3]. Another tractable approach is called reduced form model, which models the intensity of arrival of default events directly. The reduced form models can be seen in Artzner and Freddy [4], Duffie and Singleton [5], Duffie and GaΜrleanu [6], and Leung and Kwok [7] and are developed extensively by Su and Wang [8]. Recently, Markovian regime-switching models have attracted attention among researchers and practitioners in economics and mathematics. Elliott et al. [9] introduce a self-calibrating model for short-term interest rate by assuming that the short rate is governed by a finite state space Markov process. Elliott et al. [10] and Elliott and Osakwe [11] use Markov-modulated market parameters to capture the time inhomogeneity generated by the financial market. Elliott et al. [12] perform the valuation of option under a generalized Markov-modulated jump-diffusion model. Siu et al. [13] consider the pricing currency options under two-factor Markov-modulated stochastic volatility models. Bo et al. [14] derive the valuation of currency option when the spot foreign exchange rates follow Markov-modulated jump-diffusion model. In this paper, we investigate the valuation of European option with credit risk in a reduced form model in Markovian regime-switching markets. We assume that the recovery rate is constant; that is, when the writer of the option defaults, a specified constant fraction times the payoff will be paid at maturity. In order to incorporate both rare events and time-inhomogeneity in finance market, we model the stock price by the so-called Markov-modulated jump-diffusion process, in which rare events are described as a compound Poisson process and the arrival rate of Poisson process and the volatility rate of stock are governed by a continuous-time Markov chain. The states of Markov chain can be interpreted as the states of the market. The transitions of the states of the market may describe changes of economy, finance, business cycles, and other conditions. In addition, we assume that the interest rate and the default intensity both follow the Vasicek models and the parameters of models are correlated with the same Markov chain. By the method of changing measures, 2 Journal of Applied Mathematics we obtain the closed form formula for the valuation of the European option. The rest of this paper is organized as follows. Section 2 presents the model description. In Section 3, by applying Girsanov’s measure changing theorem, we derive the formula of the pricing of European-style call option. We provide numerical analysis in Section 4. The concluding remarks are contained in Section 5. 2. The Model Description Let (Ω, F, π) be a complete probability space, where π is a neutral-risk probability measure. Define π = {ππ‘ , π‘ ≥ 0} on (Ω, F, π) as a continuous-time, finite state Markov chain with π-state space πΈ. We interpret the state of π as the states of the economy as follows (Elliott et al. [10] and Elliott and Osakwe [11]). Without loss of generality, we take the state space of π to be a finite set of unite vectors {π1 , π2 , . . . , ππ } with ππ = (0, . . . , 1, . . . , 0) ∈ π π . And π has the following semimartingale representation: πππ‘ = πππ‘ ππ‘ + πππ‘ , (1) where π = (πππ )π,π=1,2,...,π is π-matrix of π and π = {ππ‘ }0≤π‘≤π is an π π -valued martingale with respect to the filtration generated by {ππ‘ , 0 ≤ π‘ ≤ π} under π. Suppose that the stock price ππ‘ and interest rate ππ‘ satisfy the following stochastic differential equations (SDE): πππ‘ = (ππ‘ − π]π‘ ) ππ‘ + π1π‘ ππ1π‘ + (πππ‘− − 1) ππ (π‘) , ππ‘− (2) where π3π‘ is standard Brownian motion and π3π‘ is the stochastic volatility of default intensity. π3π‘ , πΌπ‘ , and π½π‘ are also controlled by ππ‘ and satisfy πΌπ‘ = β¨πΌ, ππ‘ β©, πΌ = (πΌ1 , πΌ2 , . . . , πΌπ ) ∈ (0, ∞)π , π½π‘ = β¨π½, ππ‘ β©, π½ = (π½1 , π½2 , . . . , π½π ) ∈ (0, ∞)π . 1 π12 π13 (π12 1 π23 ) π‘. π13 π23 1 3. Pricing Options with Credit Risk We consider the case of a European call option with credit risk. Assume that the recovery rate is a constant π€. When the seller of option defaults, the payoff is given by π€ times the payoff of the default-free option at maturity. Therefore, by the risk neutral pricing theorem, the valuation of the European call option at time π‘, with strike price πΎ and maturity π, is given by πΆ (π‘, π) π = πΈ [π− ∫π‘ π1 = (π11 , π12 , . . . , π1π ) ∈ (0, ∞) , π2π‘ = β¨π2 , ππ‘ β©, π2 = (π21 , π22 , . . . , π2π ) ∈ (0, ∞)π , π ]π‘ = β¨], ππ‘ β©, ] = (]1 , ]2 , . . . , ]π ) ∈ (0, ∞) , ππ‘ = β¨π, ππ‘ β©, π = (π1 , π2 , . . . , ππ ) ∈ (0, ∞)π , ππ‘ = β¨π, ππ‘ β©, π = (π1 , π2 , . . . , ππ ) ∈ (0, ∞)π , + (π€(ππ − πΎ) 1(π≤π) + (ππ − πΎ) 1(π>π) ) | Fπ‘ ] ππ ππ (π€(ππ −πΎ) +(1−π€) (ππ −πΎ) 1(π>π) ) | Fπ‘ ] . + + Following Lando [15], π πΈ [π− ∫π‘ ππ ππ + (ππ − πΎ) 1(π>π) | Fπ‘ ] π − ∫π‘ (ππ +π π )ππ = 1(π>π‘) πΈ [π (8) + (ππ − πΎ) | Fπ‘ ] . We can obtain the following expression: π πΆ (π‘, π) = π€πΈ [π− ∫π‘ ππ ππ (3) + (ππ − πΎ) | Fπ‘ ] π + (1 − π€) 1(π>π‘) πΈ [π− ∫π‘ (ππ +π π )ππ + (ππ − πΎ) | Fπ‘ ] = πΌ1 + πΌ2 . where β¨⋅, ⋅β© denotes the inner product in π π . Let π denote the default time of the writer of the option with default intensity process π π‘ , and π π‘ is given by ππ π‘ = (πΌπ‘ − π½π‘ π π‘ ) ππ‘ + π3π‘ ππ3π‘ , + ππ ππ (7) π π1π‘ = β¨π1 , ππ‘ β©, (6) The filtration Fπ‘ is generated by Fπ‘ = Fππ‘ ∨Fππ‘ ∨Fππ‘ ∨Fππ ∨ Hπ‘ , where Fππ‘ = π(ππ , 0 ≤ π ≤ π‘), Fππ‘ = π(ππ , 0 ≤ π ≤ π‘), Fππ‘ = π(π π , 0 ≤ π ≤ π‘), Fππ‘ = π(ππ , 0 ≤ π ≤ π‘), and Hπ‘ = π(1(π≤π ) , π ≤ π‘). π where π1π‘ , π2π‘ are standard Brownian motions and π1π‘ , π2π‘ are the stochastic volatility of the stock and the interest rate, respectively. {ππ‘ }0≤π‘≤π is Poisson process with the stochastic jump intensity {]π‘ }0≤π‘≤π , and the jump amplitude is controlled by {ππ‘ }. ππ and ππ‘ for π =ΜΈ π‘ independently identify distribution, and write π = πΈπππ − 1. Moreover, ππ‘ , ππ‘ are assumed to be mutually independent. π1π‘ , π2π‘ , Vπ‘ , ππ‘ , ππ‘ are controlled by ππ‘ , that is, (5) Moreover, we assume that ππ‘ , ππ‘ are independent of π1π‘ , π2π‘ , and π3π‘ and the covariance matrix of the Brownian motion (π1π‘ , π2π‘ , π3π‘ ) is = πΈ [π− ∫π‘ πππ‘ = (ππ‘ − ππ‘ ππ‘ ) ππ‘ + π2π‘ ππ2π‘ , π3 = (π31 , π32 , . . . , π3π ) ∈ (0, ∞)π , π3π‘ = β¨π3 , ππ‘ β©, (4) (9) Next, we calculate πΌ1 and πΌ2 , respectively. For π > π‘, we have π π π π π ππ = π− ∫π‘ ππ’ ππ’ ππ‘ + ∫ π− ∫V ππ’ ππ’ πV πV + ∫ π− ∫V ππ’ ππ’ π2V ππ2V . π‘ π‘ (10) Journal of Applied Mathematics 3 Integrated from π‘ to π in both sides of (10), Thus, we can define the probability measure π by π π π π‘ π‘ π π π π‘ V exp {− ∫π‘ (ππ + π π ) ππ } ππ σ΅¨σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ = ππ σ΅¨σ΅¨Fπ‘ πΈ [exp {− ∫π (π + π ) ππ } | F ] π π π‘ π‘ π ∫ ππ ππ = ∫ π− ∫π‘ ππ’ ππ’ ππ ππ‘ + ∫ πV πV ∫ π− ∫V ππ’ ππ’ ππ π π π‘ V π − ∫V ππ’ ππ’ + ∫ π2V ππ2V ∫ π π − ∫π π₯π’ ππ’ π¦ Let π(π₯, π¦, π) = ∫π¦ π (11) 1 π 2 2 = exp {− ∫ π2π’ π (π, π’, π) ππ’ 2 π‘ ππ . 1 π 2 2 − ∫ π3π’ π (π½, π’, π) ππ’} 2 π‘ π ππ ; then × exp {−π23 ∫ π2π’ π3π’ π (π, π’, π) π (π½, π’, π) ππ’} π‘ π π π π‘ π‘ × exp {− ∫ π2V π (π, V, π) ππ2V π‘ ∫ ππ ππ = π (π, π‘, π) ππ‘ + ∫ πV π (π, V, π) πV π π (12) − ∫ π3V π (π½, V, π) ππ3V } . π‘ + ∫ π2V π (π, V, π) ππ2V . (15) π‘ By Girsanov’s theorem, Similarly, ππ2π‘π = ππ2π‘ + π2π‘ π (π, π‘, π) ππ‘ + π23 π3π‘ π (π½, π‘, π) ππ‘, ππ3π‘π = ππ3π‘ + π3π‘ π (π½, π‘, π) ππ‘ + π23 π2π‘ π (π, π‘, π) ππ‘, π π π‘ π‘ ππ1π‘π = ππ1π‘ + π12 π1 (π‘) ππ‘ + π13 π2 (π‘) ππ‘, ∫ π π ππ = π (π½, π‘, π) π π‘ + ∫ πΌV π (π½, V, π) πV π (13) + ∫ π3V π (π½, V, π) ππ3V . (16) where π‘ π1 (π‘) = π2π‘ π (π, π‘, π) + π23 π3π‘ π (π½, π‘, π) , π2 (π‘) = π3π‘ π (π½, π‘, π) + π23 π2π‘ π (π, π‘, π) . From (12) and (13), we have that (17) π1π‘π, π2π‘π, and π3π‘π are standard Brownian motions under probability measure π, and (π1π‘π, π2π‘π, π3π‘π) has the same covariance matrix as (π1π‘ , π2π‘ , π3π‘ ). Therefore, π π (π‘, π) := πΈ [exp {− ∫ (ππ + π π ) ππ } | Fπ‘ ] π‘ π πΈ [π− ∫π‘ = exp {−π (π, π‘, π) ππ‘ − π (π½, π‘, π) π π‘ (ππ +π π )ππ + (ππ − πΎ) | Fπ‘ ] + π (18) = π (π‘, π) πΈ ((ππ − πΎ) | Fπ‘ ) . π − ∫ ππ’ π (π, π’, π) ππ’ π‘ In addition, π + πΈπ ((ππ − πΎ) | Fπ‘ ) − ∫ πΌπ’ π (π½, π’, π) ππ’} π‘ = πΈπ (ππ 1(ππ ≥πΎ) | Fπ‘ ) − πΎπΈπ (1(ππ ≥πΎ) | Fπ‘ ) . 1 π 2 2 π (π, π’, π) ππ’ × exp { ∫ π2π’ 2 π‘ By the solution of SDE (2), 1 π 2 2 + ∫ π3π’ π (π½, π’, π) ππ’} 2 π‘ π 1 2 ππ = ππ‘ exp {∫ (ππ − π]π − π1π ) ππ 2 π‘ π × exp {π23 ∫ π2π’ π3π’ π (π, π’, π) π (π½, π’, π) ππ’} . π‘ (19) (14) π π π‘ π‘ + ∫ π1π ππ1π + ∫ ππ − πππ } . (20) 4 Journal of Applied Mathematics Under π, πΈ(⋅) is the expectation of ππ under π, and π(⋅) is distribution function of standard normal distribution. On the other hand, let π ππ = ππ‘ exp {Λ (π‘, π) + ∫ π1π ππ1π π π‘ +∫ π π‘ π2π π (π, π , π) ππ2π π (21) π + ∫ ππ − πππ } , L (π‘, π) := πΈπ (ππ | Fπ‘ ) π‘ 1 π 2 1 π 2 2 ππ + ∫ π2π π (π, π , π) ππ } = ππ‘ πΛ(π‘,π) exp { ∫ π1π 2 π‘ 2 π‘ where 1 2 Λ (π‘, π) = − ∫ (π]π + π1π ) ππ + π (π, π‘, π) ππ‘ 2 π‘ π π π π‘ π‘ × exp {π12 ∫ π1π π2π π (π, π , π) ππ + π ∫ ]π ππ } . π π 2 + ∫ ππ π (π, π , π) ππ − ∫ π2π π2 (π, π , π) ππ π‘ π‘ π π π‘ π‘ − π12 ∫ π1π π1 (π ) ππ − π13 ∫ π1π π2 (π ) ππ π − π23 ∫ π2π π3π π (π, π , π) π (π½, π , π) ππ . π‘ (22) We can define the probability measure π as follows: ππ ππ σ΅¨σ΅¨σ΅¨σ΅¨ σ΅¨ = ππ σ΅¨σ΅¨σ΅¨Fπ‘ πΈπ (ππ | Fπ‘ ) π π π‘ π‘ = exp {∫ π1π ππ1π π + ∫ π2π π (π, π , π) ππ2π π 1 π 2 − ∫ π1π ππ } 2 π‘ So, π (ππ ≥ πΎ | Fπ‘ ) π π π‘ π‘ = ππ (∫ π1π ππ1π π + ∫ π2π π (π, π , π) ππ2π π π −π12 ∫ π1π π2π π (π, π , π) ππ } π‘ π ≥ ln (πΎ/ππ‘ ) − Λ (π‘, π) − ∫ ππ πππ ) ∫π‘ π1π ππ1π π + π ∫π‘ π2π π (π, π , π) ππ2π π π π π‘ π‘ × exp {∫ ππ πππ − π ∫ ]π ππ } . π‘ π (26) 1 π 2 2 π (π, π , π) ππ × exp {− ∫ π2π 2 π‘ π = ππ ( (25) (23) √Δ By Girsanov’s theorem, we have that π ≤ π ∞ =∑ ln (ππ‘ /πΎ) + Λ (π‘, π) + ∫π‘ ππ πππ (∫π‘ ]π ππ ) π=0 π! √Δ ππ1π‘π = ππ1π‘π − π1π‘ ππ‘ − π12 π2π‘ π (π, π‘, π) ππ‘, ) ππ2π‘π = ππ2π‘π − π2π‘ π (π, π‘, π) ππ‘ − π12 π1π‘ ππ‘, π π π− ∫π‘ ]π ππ πΈ (π (π1 )) , where, under π , π1π‘π , π2π‘π are standard Brownian motions and their correlation coefficient is π12 , ππ‘ is Poisson process with intensity (π + 1)]π‘ , and the density function of π1 is ππ¦ π(π¦)/(π + 1), where π(⋅) is the density function of π1 under π. Since, under π , where π π 2 2 Δ = ∫ π1π ππ + ∫ π2π π2 (π, π , π) ππ π‘ π‘ π π + 2π12 ∫ π1π π2π π (π, π , π) ππ , (24) π‘ π1 = ln (ππ‘ /πΎ) + Λ (π‘, π) + ∑ππ=1 ππ √Δ (27) . ππ = ππ‘ exp {Λ (π‘, π) + Δ + ∫ π1π ππ1π π π‘ π π π‘ π‘ + ∫ π2π π (π, π , π) ππ2π π + ∫ ππ − πππ } , (28) Journal of Applied Mathematics 5 Denote by π(π‘, π) the value at time π‘ of a π maturity zero coupon bond whose face value is 1. Then then πΈπ (ππ 1(ππ ≥πΎ) | Fπ‘ ) π π (π‘, π) = πΈ [π− ∫π‘ = L (π‘, π) ππ (ππ ≥ πΎ | Fπ‘ ) π π π‘ π‘ = L (π‘, π) ππ (∫ π1π ππ1π π + ∫ π2π π (π, π , π) ππ2π π ≥ ln ( π = L (π‘, π) π ( ∫π‘ π1π ππ1π π + π π‘ π ∫π‘ π2π π (π, π , π) ππ2π π 1 2 π2 (π, V, π) πV} , + ∫ π2V 2 π‘ ln (ππ‘ /πΎ) + Λ (π‘, π) + Δ + ∫π‘ ππ πππ π ∞ = L (π‘, π) ∑ (∫π‘ ]π ππ ) π! π=0 (34) π √Δ √Δ (33) π (π‘, π) = exp {−π (π, π‘, π) ππ‘ − ∫ πV π (π, V, π) πV ππ (π‘, π) = ππ‘ ππ‘ − π (π, π‘, π) π2π‘ ππ2π‘ . π (π‘, π) π ≤ | Fπ‘ ] . From (12), π πΎ ) − Λ (π‘, π) − Δ − ∫ ππ πππ ) ππ‘ π‘ π ππ ππ ) (35) Define the Radon-Nikodym derivative given by π π − ∫π‘ ]π ππ π πΈπ (π (π2 )) , π πππ π− ∫π‘ ππ ππ = π ππ πΈ [π− ∫π‘ ππ ππ | Fπ‘ ] (29) where π π2 = ln (ππ‘ /πΎ) + Λ (π‘, π) + Δ + ∑ππ=1 ππ √Δ π‘ 1 π 2 2 − ∫ π2V π (π, V, π) πV} , 2 π‘ (30) = π1 + √Δ and πΈπ (⋅) is the expectation of ππ under π . By (23) and (29), we have the following lemma. and by Girsanov’s theorem, under ππ , π ππ2π‘π = ππ2π‘ + π2π‘ π (π, π‘, π) ππ‘ Lemma 1. Consider the Following: π − ∫π‘ (ππ +π π )ππ πΈ [π π ππ1π‘π + (ππ − πΎ) | Fπ‘ ] ×∑ (37) = ππ1π‘ + π12 π2π‘ π (π, π‘, π) ππ‘. Thus ππ can be rewritten as = π (π‘, π) ∞ (36) = exp {− ∫ π (π, V, π) π2V ππ2V π (∫π‘ ]π ππ ) π π π! π=0 π‘ π − ∫π‘ ]π ×π π π ππ = ππ‘ exp {A (π‘, π) + ∫ π (π, V, π) π2V ππ2V ππ π ππ ππ ππ ππ ππ 1(ππ ≥πΎ) | Fπ‘ ] π − ∫π‘ ππ ππ − πΎπΈ [π = πΌ3 − πΌ4 . 1(ππ ≥πΎ) | Fπ‘ ] (38) π‘ π‘ π 1 2 A (π‘, π) = − ∫ (π]π + π1π ) ππ + π (π, π‘, π) ππ‘ 2 π‘ + π π where (ππ − πΎ) | Fπ‘ ] = πΈ [π− ∫π‘ π π + ∫ π1V ππ1V + ∫ ππ − πππ } , [L (π‘, π) πΈπ (π (π2 )) − πΎπΈ (π (π1 ))] . (31) In the following; in order to calculate πΌ1 , we write πΈ [π− ∫π‘ π (32) π π π‘ π‘ 2 + ∫ ππ π (π, π , π) ππ − ∫ π2π π2 (π, π , π) ππ π − π12 ∫ π1π π2π π (π, π , π) ππ . π‘ (39) 6 Journal of Applied Mathematics and, under ππ , ππ‘ is Poisson process with intensity (π + 1)]π‘ , and the density function of π1 is ππ¦ π(π¦)/(π + 1), where π(⋅) is the density function of π1 under π. Since, under ππ , Then π ππ (ππ ≥ πΎ | Fπ‘ ) π π π π π = ππ (∫ π1π ππ1π π + ∫ π2π π (π, π , π) ππ2π π π‘ π π‘ π πΎ ≥ ln ( ) − A (π‘, π) − ∫ ππ − πππ ) ππ‘ π‘ π ππ =π ( π ∫π‘ π1π ππ1π π + +∫ √Δ ∞ =∑ π=0 √Δ π π ) π π! π π πΈ (π (π3 )) , ln (ππ‘ /πΎ) + A (π‘, π) + ππ . =π (41) ππ ( ∞ π = πΎπ (π‘, π) ∑ ln (ππ‘ /πΎ) + A (π‘, π) + Δ + ∫π‘ ππ − πππ √Δ (1(ππ ≥πΎ) | Fπ‘ ) (∫π‘ ]π ππ ) π! π=0 π √Δ ≤ π π π ∫π‘ π1π ππ1π π + ∫π‘ π2π π (π, π , π) ππ2π π Therefore, πΌ4 = πΎπ (π‘, π) πΈ π πΎ ) − A (π‘, π) − Δ − ∫ ππ − πππ ) ππ‘ π‘ π ∑ππ=1 √Δ ππ π π‘ ≥ ln ( where πΈ(⋅) is the expectation of ππ under π, π3 = π π = ππ (∫ π1π ππ1π π + ∫ π2π π (π, π , π) ππ2π π π‘ π π‘ ππ (ππ ≥ πΎ | Fπ‘ ) π − ∫π‘ ]π ππ + ∫ ππ − πππ } , then ln (ππ‘ /πΎ) + A (π‘, π) + ∫π‘ ππ − πππ (∫π‘ ]π ππ ) (46) π ππ π1V ππ1V (40) π ≤ π π‘ π π ∫π‘ π2π π (π, π , π) ππ2π π π π ππ = ππ‘ exp {A (π‘, π) + Δ + ∫ π (π, V, π) π2V ππ2V π‘ π π − ∫π‘ ]π ππ π π (∫π‘ ]π ππ ) ∞ (42) =∑ πΈ (π (π3 )) . π! π=0 ) π π π− ∫π‘ ]π ππ π πΈ (π (π4 )) , (47) Finally, let π π΄ (π‘, π) := πΈ (π− ∫π‘ ππ ππ where πΈπ (⋅) is the expectation of ππ under ππ , ππ | Fπ‘ ) π 1 2 = ππ‘ exp {− ∫ (π]π + π1π ) ππ 2 π‘ π π4 = (43) π 1 2 ππ + π ∫ ]π ππ } . + ∫ π1π 2 π‘ π‘ ln (ππ‘ /πΎ) + A (π‘, π) + Δ + ∑ππ=1 ππ √Δ (48) = π3 + √Δ. From (42) and (33), we can conclude the following lemma. We define π Lemma 2. Consider the following: π− ∫π‘ ππ ππ ππ πππ = π ππ πΈ [π− ∫π‘ ππ ππ ππ | Fπ‘ ] π = exp {∫ π1V ππ1V − π‘ π 1 π 2 ∫ π πV 2 π‘ 2V π πΈ [π− ∫π‘ (44) π =∑ π=0 + ∫ ππ − ππ (π ) − π ∫ ]π ππ } , π‘ + (ππ − πΎ) | Fπ‘ ] (∫π‘ ]π ππ ) ∞ π π‘ ππ ππ π! π × π− ∫π‘ π and by Girsanov’s theorem, under π , π ]π ππ [π΄ (π‘, π) πΈπ (π (π4 ))−πΎπ (π‘, π) πΈ (π (π3 ))] . (49) π ππ1π‘π = ππ1π‘ − π1π‘ ππ‘ π ππ2π‘π = ππ2π‘ − π12 π1π‘ ππ‘, (45) Combined with the previous lemmas, the price of European call option at time π‘ is given by the following theorem. Journal of Applied Mathematics 7 28 Table 1: The parameter values. 26 Value in state π1 Value in state π2 Volatility of π Jump intensity Speed of reversion of π Long-term average of π Volatility of π Speed of reversion of π Long-term average of π Volatility of π Initial stock price π11 = 0.2 ]1 = 15 π1 = 2 π1 /π1 = 0.04 π21 = 0.15 π½1 = 1.5 πΌ1 /π½1 = 0.01 π31 = 0.25 π0 = 100 Initial interest rate π0 = 0.04 Initial default intensity π 0 = 0.5 π12 = 0.4 ]2 = 30 π2 = 1 π2 /π2 = 0.02 π22 = 0.3 π½2 = 2 πΌ2 π½2 = 0.02 π32 = 0.45 24 22 Option price Parameter name 16 14 12 10 0.8 0.9 0.95 π = 0.4 π = 0.6 ππ½ = 0.1 1 1.05 1.1 1.15 1.2 1.25 π = 0.8 π=1 Figure 1: The option price with different recovery rate for π = 1, π12 = 0.7, π13 = 0.5, and π23 = 0.6. πΆ (π‘, π) 30 π (∫π‘ ]π ππ ) π 25 π! π × π− ∫π‘ ]π ππ [π€ (π΄ (π‘, π) πΈπ (π (π4 )) − πΎπ (π‘, π) πΈ (π (π3 ))) (50) + (1 − π€) 1(π>π‘) π (π‘, π) Option price π=0 0.85 π0 /πΎ Theorem 3. The price of European call option with credit risk at time π‘ is ∞ 18 ππ½ = 0 Mean jump size Standard deviation of jump size =∑ 20 20 15 10 π × (L (π‘, π) πΈ (π (π2 )) 5 0.8 − πΎπΈ (π (π1 )))] . 4. Numerical Analysis In this section, we will employ Monte Carlo simulation and perform a numerical analysis for European-style call option with credit risk under the Markov-modulated jump-diffusion model. We consider that the Markov chain π has two states, which means that macroeconomic shifts between the two states: π1 (“boom” or “good”) and π2 (“recession” or “bad”). We assume that the current economy is in boom and that the transition probability matrix of the two-state Markov chain π is given by ( 0.7 0.3 π11 π12 )=( ). π21 π22 0.2 0.8 (51) Assume that ππ‘ is normally distributed with mean ππ½ and standard deviation ππ½ . We will adopt the specimen values for the model parameters as Table 1. We consider a range of spot-to-strike ratios π0 /πΎ from 0.8 to 1.2 and assume that one year has 252 trading days. We perform 10 000 simulations for computing the option price. 0.85 0.9 0.95 1 1.05 π0 /πΎ 1.1 1.15 1.2 1.25 π = 0.5 π=1 π = 1.5 Figure 2: The option price with different maturity π for π = 0.4, π12 = 0.7, π13 = 0.5, and π23 = 0.6. For each π = 0.4, 0.6, 0.8, 1, we consider the impact of the spot-to-strike ratio on the option price. From Figure 1, we observe that the option price increases as the spot-to-strike ratio increases. We can also see that the greater the π, the greater the option price. When π = 1, it follows that there is not default risk. It is a result of the fact that the payoff at the maturity will increase as the recovery rate increases. Figure 2 depicts the plot of the option price against the spotto-strike ratio for each maturity π = 0.5, 1, 1.5. From these plots, we find that the longer the maturities, the greater the option price. In the following, we compare the option price with different correlation coefficients for fixed maturity π = 1 8 Journal of Applied Mathematics 24 25 22 20 18 Option price Option price 20 16 14 15 12 10 8 0.8 0.85 0.9 0.95 1 1.05 1.1 1.15 1.2 10 0.8 1.25 0.85 0.9 0.95 1 1.05 1.1 1.15 1.2 1.25 π0 /πΎ π0 /πΎ 1 = 10, 2 = 20 1 = 15, 2 = 30 1 = 20, 2 = 40 π12 = 0.7 π12 = −0.7 π12 = −0.9 Figure 3: The option price with different correlation coefficients π12 for π = 1, π = 0.4, π13 = 0.5, and π23 = 0.6. Figure 5: The option price with different ] for π = 0.4, π12 = 0.7, π13 = 0.5, and π23 = 0.6. 35 25 30 25 Option price Option price 20 20 15 15 10 10 0.8 0.85 0.9 0.95 1 1.05 π0 /πΎ 1.1 1.15 1.2 1.25 π13 = 1 π13 = 0.5 π13 = −0.5 Figure 4: The option price with different correlation coefficients π13 for π = 1, π = 0.4, π12 = 0.7, and π23 = 0.6. and recovery rate π = 0.4. Figure 3 illustrates that option price increases as correlation coefficient π12 increases. From Figure 4, we can also see that option price decreases as correlation coefficient π13 increases. In Figure 5, we present how the option prices vary with the changes of the annual jump intensity ]. Figure 5 displays a large change in the option price due to the variation of the jump intensity. The option price increases as jump intensity increases. 5 0.8 0.85 0.9 0.95 1 1.05 π0 /πΎ 1.1 1.15 1.2 1.25 Markov-modulated model Non-Markov-modulated model for a good economy Non-Markov-modulated model for a bad economy Figure 6: The option price in Markov-modulated model and nonMarkov-modulated models. Finally, we investigate the difference of the option price in Markov-modulated model and non-Markov-modulated models. From Figure 6, we can observe that the call option price in good economy is lower than that in bad economy. The reason is that when economy is bad, the volatility of the risky asset is great so that the option price is higher. In our model, we assume that the current economy is good, so Markovmodulated model is close to the model for a good economy, while the two plots and the model for a bad economy are relatively far apart. In Markov-modulated model, we take into Journal of Applied Mathematics consideration the changes of the state of the economy, so Markov-modulated model is more in accord with the reality for the pricing of the defaultable options. 5. Conclusion The pricing of European option with credit risk in a reduced form model was studied, while the stock price was driven by Markov-modulated jump-diffusion models. The interest rate and the default intensity followed the Vasicek models, and the parameters were also controlled by the same Markov chain. Compared with most of the credit risk models, the main advantage is that we incorporated Markov-modulated rates into the models. We applied Girsanov’s theorem to obtain the equivalent martingale measure and derived the closed form formula for the valuation of the European option. Finally, from the numerical illustrations, we obtain the effects of the recovery rate, the maturity, the correlation coefficients, and the jump intensity of stock on the option price. Acknowledgments The authors would like to thank the referee for many helpful and valuable comments and suggestions. Jinzhi Li would like to acknowledge the National Commission of Ethnic Affair (no. 12ZYZ003) and the Ministry of Education of Humanities and Social Sciences Project (no. 11YJC790102). References [1] R. Merton, “On the pricing of corporate debt: the risk structure of interest rates,” The Journal of Finance, vol. 29, no. 2, pp. 449– 470, 1974. [2] M. Ammann, Credit Risk Valuation: Methods, Models, and Applications, Springer, New York, NY, USA, 2nd edition, 2001. [3] P. Klein and M. 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