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Research article

A conserved Caginalp phase-field system with two temperatures and a nonlinear coupling term based on heat conduction

  • Received: 31 January 2023 Revised: 20 March 2023 Accepted: 29 March 2023 Published: 19 April 2023
  • MSC : 35B41, 35B45, 35K55

  • Our aim in this paper is to study generalizations of the Caginalp phase-field system based on a thermomechanical theory involving two temperatures and a nonlinear coupling. In particular, we prove well-posedness results. More precisely, the existence and uniqueness of solutions, the existence of the global attractor and the existence of an exponential attractor.

    Citation: Grace Noveli Belvy Louvila, Armel Judice Ntsokongo, Franck Davhys Reval Langa, Benjamin Mampassi. A conserved Caginalp phase-field system with two temperatures and a nonlinear coupling term based on heat conduction[J]. AIMS Mathematics, 2023, 8(6): 14485-14507. doi: 10.3934/math.2023740

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  • Our aim in this paper is to study generalizations of the Caginalp phase-field system based on a thermomechanical theory involving two temperatures and a nonlinear coupling. In particular, we prove well-posedness results. More precisely, the existence and uniqueness of solutions, the existence of the global attractor and the existence of an exponential attractor.



    Probability theory and uncertainty theory are two axiomatic mathematical systems that model uncertain phenomena. Probability theory is based on frequency. Traditionally, probability theory has been used to describe uncertain events, such as the price of the underlying asset in financial derivatives. If your distribution function is close enough to the frequency, using probability theory is fine. In fact, when we can only get small samples or no samples, the distribution function may deviate far from the real frequency. In this case, using probability theory may lead to counterintuitive results. The relevant content can be seen in Chapter 1 of [18]. Furthermore, as early as 1979, Kahneman and Tversky [12] pointed out that people always overestimate the probability of impossible events. Thus people always hope that experts in the field will give the belief degree of an event. In order to rationally deal with the belief degree, Liu [13] founded the uncertainty theory which is an axiomatic mathematical system based on normality, duality, subadditivity and product axioms in 2007. Nowadays uncertainty theory has become a branch of mathematics concerned with the analysis of belief degree. The forward development of a discipline is inseparable from the joint efforts of many scholars (see [4,13,14,15,16,28]).

    In 2009, Liu [15] introduced the uncertainty theory into the financial field and proposed an uncertain stock model that follows uncertain differential equations driven by the geometric Liu process. Peng and Yao [22] gave a class of uncertain stock models with mean reversion. Dai et al. [8] gave a nonlinear uncertain stock model. In addition, Yu [29] studied uncertain stock models with jumps and Chen et al. [] also proposed an uncertain stock model with periodic dividends. Many option pricing formulas have been obtained using the above uncertain stock models.

    In recent years, with the development of the financial market, hedging and avoiding financial risk have become more and more important, and various types of options have emerged. Default risk, also known as credit risk, comes from the possibility of the default of loan borrowers, bond issuers and derivative counterparties. In general, it has been assumed that options have no default risk when options are traded on an organized exchange. However, the rapid growth in the over-the-counter options has motivated increased attention to the implications of counterparty credit risk. The holders of over-the-counter options are exposed to potential credit risk due to the possibility of their counterparty being unable to make the necessary payments at the expiration date. In 1987, Johnson and Stulz [10] discussed the impact of credit default risk on option prices and called this option with credit risk a vulnerable option. In 2022, Xie and Deng [26] studied the pricing of European vulnerable options under the conditions of Heston stochastic volatility and a stochastic interest rate model. In 2021, Liang and Wang [21] proposed a closed-form hybrid credit risk model to price vulnerable options with stochastic volatility. In 2019, Zhou and Li [30] proposed a method to estimate the price of vulnerable options when the volatility of the underlying assets is within a small interval.

    For Cox-Ingersoll-Ross(CIR) interest rate models, most of the related research is carried out in the field of randomization. In 2022, Zheng [31] priced European export-oriented barrier options by using a CIR model. In 2020, Lei [20] studied the asset liability management problem with a CIR interest rate by using a Heston model. In 2019, Sun et al. [23] studied the Euler grid difference method and convergence analysis of CIR interest rate models under the conditions of a fractional jump diffusion environment. In 2018, Chen and Hsu [3] studied barrier option pricing and hedging by using a Markov-modulated double exponential jump diffusion-CIR model. Wu [25] discussed the application of a CIR model in the Chinese market under the condition of a stochastic field in 2017. More references can be seen in [7,9,24]. Although the CIR interest rate model has many applications in the field of randomness, CIR interest rate models have few applications in the field of uncertainty. In this paper, we get the solution of the CIR interest rate model in terms of distribution. Based on the CIR interest rate model, the pricing formulas of the European vulnerable call option and European vulnerable put option are obtained, and the related risks are analyzed.

    This paper gives the pricing formulas of vulnerable options as obtained by implementing the uncertain CIR interest rate model. The rest of the article is arranged as follows. In Section 2, we introduce some definitions and theorems that will be used in this article. In Section 3, the solution in terms of the distribution of an uncertain differential equation is given. Sections 4 and 5 give the pricing formulas of the European vulnerable call option and the European vulnerable put option based on a new uncertain vulnerable option pricing model, respectively. In Section 6, in order to obtain the numerical solution, two numerical algorithms are designed to calculate the prices of European vulnerable call options and European vulnerable put options, and numerical examples are given to verify the effectiveness of the numerical algorithm. Finally, a brief summary is given in Section 7.

    Definition 2.1. [13] Let Γ be a nonempty set and L be a σ-algebra on Γ. The set function M is called an uncertain measure if it satisfies the following axioms:

    Axiom 1. (Normality axiom) M{Γ}=1 for the universal set Γ.

    Axiom 2. (Duality axiom) M{Λ}+M{Λc}=1 for any ΛL.

    Axiom 3. (Subadditivity axiom) For every countable sequence Λ1,Λ2, in L, we have

    M{i=1Λi}i=1M{Λi}.

    The triplet (Γ,L,M) is called an uncertainty space. Moreover, the product uncertainty measure was defined by Liu [15] in 2009 as follows.

    Axiom 4. (Product axiom) Let (Γk,Lk,Mk) be uncertainty spaces for k=1,2,. The product uncertainty measure M is an uncertainty measure satisfying

    M{k=1Λk}=k=1Mk{Λk}

    where Λk denotes arbitrarily chosen events from Lk,k=1,2,.

    Definition 2.2. [13] Let ξ be a function from an uncertainty space (Γ,L,M) to the set of real numbers such that ξB is an event for any Borel set B of real numbers; then, the function ξ is called an uncertain variable.

    Theorem 2.1. [16] Let ξ1, ξ2, , ξn be independent uncertain variables with regular uncertainty distributions Φ1, Φ2, , Φn, respectively. If f(ξ1,ξ2,,ξn) is a strictly increasing function with respect to ξ1, ξ2, , ξm and a strictly decreasing function with respect to ξm+1, ξm+2, , ξn, then ξ=f(ξ1,ξ2,,ξn) has an inverse uncertainty distribution

    Ψ1(α)=f(Φ11(α),,Φ1m(α),Φ1m+1(1α),,Φ1n(1α)).

    Definition 2.3. [13] The expected value of an uncertain variable ξ is defined by

    E[ξ]=+0M{ξx}dx0M{ξx}dx

    provided that at least one of the two integrals exists.

    Theorem 2.2. [13] Let ξ be an uncertain variable with the uncertainty distribution Φ. Then

    E[ξ]=+0(1Φ(x))dx0Φ(x)dx.

    Theorem 2.3. [16] Let ξ be an uncertain variable with the regular uncertainty distribution Φ. Then

    E[ξ]=10Φ1(α)dα

    where Φ1(α) is the inverse uncertain distribution of the uncertain variable ξ.

    Theorem 2.4. [19] Let ξ1, ξ2, , ξn be independent uncertain variables with regular uncertainty distributions Φ1, Φ2, , Φn, respectively. If f(x1,x2,,xn) is a continuous, strictly increasing function with respect to x1, x2, , xm and a strictly decreasing function with respect to xm+1, xm+2, , xn, then the uncertain variable ξ=f(ξ1,ξ2,,ξn) has an expected value of

    E[ξ]=10f(Φ11(α),,Φ1m(α),Φ1m+1(1α),,Φ1n(1α))dα.

    Definition 2.4. [14] Let T be a totally ordered set (e.g. time) and let (Γ,L,M) be an uncertainty space. An uncertain process is a function Xt(γ) from T×(Γ,L,M) to the set of real numbers such that {XtB} is an event for any Borel set B of real numbers at each time t.

    Definition 2.5. [15] An uncertain process Ct is said to be a Liu process if

    (1) C0=0 and almost all sample paths are Lipschitz continuous;

    (2) Ct has stationary and independent increments;

    (3) every increments Ct+sCt is a normal uncertain variable with an expected value 0 and variance t2.

    It is very clear that a Liu process CtN(0,t2), that is, the uncertainty distribution of Ct is

    Φt(x)=(1+exp(πx3t))1,x.

    Definition 2.6. [14] Uncertain processes X1t,X2t,,Xnt are said to be independent if for any positive integer k and any times t1,t2,,tk, the uncertain vectors

    ξi=(Xit1,Xit2,,Xitk),i=1,2,,n

    are independent, i.e., for any Borel sets B1,B2,,Bn of k-dimensional real vectors, we have

    M{ni=1(ξξiBi)}=ni=1M{ξξiBi}.

    Definition 2.7. [17] The uncertainty distribution Φt(x) of an uncertain process Xt is defined by

    Φt(x)=M{Xtx}

    for any time t and any real number x.

    Definition 2.8. [17] Let Xt be an uncertain process with the regular uncertainty distribution Φt(x). Then the inverse function Φ1t(α) is called the inverse uncertainty distribution of Xt.

    Theorem 2.5. [27] Let Xt be a sample-continuous independent increment process with the regular uncertainty distribution Φt(x). Then for any time s>0, the time integral

    Ys=s0Xtdt

    has an inverse uncertainty distribution

    Ψ1s(α)=s0Φ1t(α)dt.

    Definition 2.9. [28] Let α be a number with 0<α<1. An uncertain differential equation

    dXt=f(t,Xt)dt+g(t,Xt)dCt

    is said to have an α-path Xαt if it solves the corresponding ordinary differential equation

    dXαt=f(t,Xαt)dt+|g(t,Xαt)|Φ1(α)dt

    where Φ1(α) is the inverse uncertainty distribution of standard normal uncertain variables, i.e.,

    Φ1(α)=3πlnα1α.

    Theorem 2.6. [28] Let Xt and Xαt be the solution and α-path of the uncertain differential equation

    dXt=f(t,Xt)dt+g(t,Xt)dCt

    respectively. Then the solution Xt has an inverse uncertain distribution

    Φ1t(α)=Xαt.

    Theorem 2.7. [27] Let Xt and Xαt be the solution and α-path of the uncertain differential equation

    dXt=f(t,Xt)dt+g(t,Xt)dCt

    respectively. Then for any time s>0 and a strictly increasing function J(x), the time integral s0J(Xt)dt has an inverse uncertainty distribution Ψ1s(α)=s0J(Xαt)dt.

    In 1985, the well-known interest rate model, the CIR model was proposed for probability theory [6]

    drt=(mart)dt+σrtdWt (3.1)

    where m>0, a0 and σ are constants, and Wt is Brownian motion. As its counterpart, Chen and Gao [2] proposed an uncertain interest model based on uncertainty theory in 2013. The interest rate rt follows the next uncertain differential equation driven by the Liu process

    drt=(mart)dt+σrtdC1t (3.2)

    where m>0, a0 and σ are constants, and C1t is the Liu process.

    Jiao and Yao [11] gave a numerical method of the uncertain interest model and obtained a formula to calculate the price of the zero coupon bond based on it.

    Next we will discuss the solution in terms of uncertainty distribution for the expression (3.2).

    Theorem 3.1. Let rt be the solution of the uncertain differential equation (3.2) with the inverse uncertainty distribution Ω1t(α). Then Ω1t(α) can be expressed in three forms with different values of Δ, where Δ=[σΦ1(α)]2+4am.

    Case I: Δ>0.

    A1ln(Ω1t(α)x1)+A2ln(Ω1t(α)x2)=t+A1ln(r0x1)+A2ln(r0x2)

    where A1=σΦ1(α)+ΔΔ, A2=σΦ1(α)+ΔΔ, x1=σΦ1(α)Δ2a and x2=σΦ1(α)+Δ2a.

    Case II: Δ=0.

    ln(Ω1t(α)σΦ1(α)a)σΦ1(α)aΩ1t(α)σΦ1(α)=12t+ln(r0σΦ1(α)a)σΦ1(α)ar0σΦ1(α).

    Case III: Δ<0.

    1aln(u2+p)σΦ1(α)a2parctanup=t1aln[(r0σΦ1(α)2a)2+p]σΦ1(α)a2parctanr0σΦ1(α)2ap

    where p=Δ4a2 and u=Ω1t(α)σΦ1(α)2a.

    Proof. From Definition 2.9, the uncertain differential equation

    drt=(mart)dt+σrtdC1t

    has the α-path

    drαt=(marαt)dt+σrαtΦ1(α)dt. (3.3)

    In order to obtain the solution of the differential equation (3.3), we divide it into three cases.

    Case I: Δ=[σΦ1(α)]2+4am>0. For the convenience of presentation, let

    A1=σΦ1(α)+ΔΔ,A2=σΦ1(α)+ΔΔ,x1=σΦ1(α)Δ2a,x2=σΦ1(α)+Δ2a.

    By solving Eq (3.3), we can get

    A1ln(rαtx1)+A2ln(rαtx2)=t+c

    where c is an arbitrary constant. Substituting the initial conditions rα0=r0 into the above equation, we get

    c=A1ln(r0x1)+A2ln(r0x2).

    Finally

    A1ln(rαtx1)+A2ln(rαtx2)=12t+A1ln(r0x1)+A2ln(r0x2).

    By Theorem 2.6, Case I is true.

    Case II: Δ=[σΦ1(α)]2+4am=0. For the convenience of presentation, let A1=1, A2=x1=x2=σΦ1(α)a.

    The general solution of Eq (3.3) is

    A1rαtx1+A2(rαtx1)2=12t+c

    where c is an arbitrary constant. From the initial value rα0=r0

    c=A1ln(r0x1)A21r0x1.

    Finally we get the special solution of Eq (3.3) as

    A1ln(rαtx1)A21rαtx1=12t+A1ln(r0x1)A21r0x1.

    By Theorem 2.6, the result of Case II be proved.

    Case III: Δ=[σΦ1(α)]2+4am<0. For the convenience of presentation, let p=Δ4a2, u=rαtσΦ1(α)2a.

    In this case, the general solution of Eq (3.3) is

    1aln(u2+p)σΦ1(α)a2parctanup=t+c

    where c is an arbitrary constant. By applying the initial value rα0=r0 we get the special solution of Eq (3.3) as

    1aln(u2+p)σΦ1(α)a2parctanup=t1aln[(r0σΦ1(α)a)2+p]σΦ1(α)a2parctanr0σΦ1(α)ap.

    From Theorem 2.6, the result of Case III is true.

    We have completed the proof of this theorem.

    As is well known, the European call option is a contract which gives the holder the right rather than the obligation to buy stocks at an expiration date T for a strike price K. The European vulnerable call option supposes that the value of a company is Zt at the time t. Then the option seller promises to give (YTK)+ to the option holder at the expiration date T. If the option seller cannot give (YTK)+ to the holder at the expiration date T, the option holder will immediately take over the company. In other words, the final payoff of the option holder at time T is min((YTK)+,ZT). We assume that the price of this European vulnerable call option is fc. According to the fair price principle, we can get the price of the European vulnerable call option

    fc=E[exp(T0rtdt)min((YTK)+,ZT)].

    In order to obtain the price of options, Liu [15] first modeled the change in financial asset price by using uncertain differential equations and proposed the Liu model, which is the counterpart of the famous B-S model [1]. From then on, based on the uncertainty theory, some scholars have put forward other uncertain financial derivatives models that are more suitable for market practice, such as the mean reversion stock model [22] and uncertain exponential Ornstein-Uhlenbeck model [8]. The above models always assume that the risk interest rate is a constant. However, in the real financial market, interest rates are often uncertain, so interest rates should follow an uncertain differential equation.

    In this paper, let rt, Yt and Zt be the interest rate, stock price and the company value at time t of a European vulnerable option, respectively, and they follow the uncertain differential equations

    {drt=(mart)dt+σrtdC1tdYt=e1Ytdt+σ1YtdC2tdZt=e2Ztdt+σ2ZtdC3t (4.1)

    where m>0, a0,e1,e2,σ,σ1 and σ2, are all constants and C1t, C2t and C3t are three independent Liu processes.

    Theorem 4.1. Assume that a European vulnerable call option satisfies the model (4.1) with a strike price K and an expiration date T; then, the price of the European vulnerable call option is

    fc=10Φ11T(α)(Υ11T(α)Ψ1T(α))dα (4.2)

    where Φ11T(α)=exp(T0Ω1t(1α)dt), Υ11T(α)=(Y0(e1T+3σ1Tπlnα1α)K)+ and Ψ1T(α)=Z0(e2T+3σ2Tπlnα1α).

    Proof. The inverse uncertainty distribution Ω1t(α) of rt has been obtained by Theorem 3.1.

    From Theorem 2.5, we can get the inverse uncertainty distribution Φ1T(α)=T0Ω1t(α)dt of T0rtdt. Since y=exp(x) is a decreasing function of x, from Theorem 2.1,

    exp(T0rtdt)

    has an inverse uncertainty distribution

    Φ11T(α)=exp(Φ1T(1α)). (4.3)

    Let Yαt be an α-path of the uncertain differential equation

    dYt=e1Ytdt+σ1YtdC2t.

    By solving the ordinary differential equation

    dYαt=e1Yαtdt+σ1YαtΦ1(α)dt,

    we can get

    Yαt=Y0(e1t+3σ1tπlnα1α).

    It follows from Theorem 2.6 that YT has an inverse uncertainty distribution

    Υ1T(α)=YαT. (4.4)

    Due to (YTK)+ being an increasing function with respect to YT, by Theorem 2.1, (YTK)+ has an inverse uncertainty distribution

    Υ11T(α)=(Υ1T(α)K)+.

    Similarly, we can get

    Zαt=Z0(e2t+3σ2tπlnα1α).

    Thus from Theorem 2.6, ZT has an inverse uncertainty distribution

    Ψ1T(α)=ZαT. (4.5)

    Following Theorem 2.1, the expression

    exp(T0rtdt)min((YTK)+,ZT)

    has an inverse uncertainty distribution

    Φ11T(α)(Υ11T(α)Ψ1T(α)).

    Thus according to Theorem 2.1 and Theorem 2.3, the price of the European vulnerable call option is shown as follows.

    fc=E[exp(T0rtdt)min((YTK)+,ZT)]=10Φ11T(α)(Υ11T(α)Ψ1T(α))dα.

    We have completed the proof of this theorem.

    In this section, we will give the pricing formulas of the European vulnerable put option. Note that rt, Yt and Zt are the same as in Theorem 4.1.

    The European put option is a contract which gives the holder the right rather than the obligation to sell stocks at an expiration date T for a strike price K.

    For the European vulnerable put option, the option seller promises to give (KYT)+ to the option holder at the expiration date T. If the option seller cannot give (KYT)+ to the holder at the expiration date T, the option holder will immediately take over the company. In other words, the final payoff of the option holder at time T is min((KYT)+,ZT). We assume that the price of this European vulnerable put option is fp.

    According to the fair price principle, we can get the price of the European vulnerable put option

    fp=E[exp(T0rtdt)min((KYT)+,ZT)].

    Theorem 5.1. Assume that a European vulnerable put option satisfies the uncertain stock model (4.1) with a strick K and an expiration date T; then, the price of the European vulnerable put option is

    fp=10Φ11T(α)(Υ12T(α)Ψ1T(α))dα (5.1)

    where Φ11T(α)=exp(T0Ω1t(1α)dt), Υ12T(α)=(KY0(e1T+3σ1Tπln1αα))+ and Ψ1T(α)=Z0(e2T+3σ2Tπlnα1α).

    Proof. Similar to the proof of Eqs (4.3)–(4.5) in Theorem 4.1, the inverse uncertainty distributions of exp(T0rtdt), YT and ZT are exp(Φ1T(1α)) Y_T^\alpha\triangleq \Upsilon_T^{-1}(\alpha) and Z_T^\alpha\triangleq \Psi_T^{-1}(\alpha) , respectively. Due to (K-Y_T)^+ being a decreasing function with respect to Y_T , by Theorem 2.1, (K-Y_T)^+ has an inverse uncertainty distribution

    \Upsilon_{2T}^{-1}(\alpha) = \left(K-\Upsilon_T^{-1}(1-\alpha)\right)^+.

    Following Theorem 2.1, the expression

    \exp \left(-\int_0^T r_t{{{\rm{d}}}} t\right)\min\left((K-Y_T)^+,Z_T\right)

    has an inverse uncertainty distribution

    \Phi_{1T}^{-1}(\alpha)\cdot\left(\Upsilon_{2T}^{-1}(\alpha)\wedge \Psi_T^{-1}(\alpha)\right).

    Thus according to Theorem 2.1 and Theorem 2.3, the price of the European vulnerable put option is shown as follows.

    \begin{align*} f_p & = E\left[\exp \left(-\int_0^T r_t{{{\rm{d}}}} t\right)\min\left((K-Y_T)^+,Z_T\right)\right]\\ & = \int_0^1 \Phi_{1T}^{-1}(\alpha)\cdot\left(\Upsilon_{2T}^{-1}(\alpha)\wedge \Psi_T^{-1}(\alpha)\right){{{\rm{d}}}} \alpha. \end{align*}

    We have completed the proof of this theorem.

    In this section, we design numerical algorithms to calculate the numerical solutions of the European vulnerable call option f_c and European vulnerable put option f_p , respectively.

    Step 0: Set the values of the corresponding parameters a, m, \sigma, Y_0, e_1, \sigma_1, Z_0, e_2, \sigma_2, T and K.

    Step 1: Choose two appropriate N and M values according to the required accuracy; set \alpha_i = i/N and t_j = jT/M , i = 1, 2, \cdots N-1 , j = 1, 2, \cdots, M.

    Step 2: Set i = 0 .

    Step 3: Set i = i+1 .

    Step 4: Set j = 0 .

    Step 5: Set j = j+1 .

    Step 6: For each \alpha_i , determine the value of \Delta = \left(\frac{\sqrt{3}\sigma}{\pi}\ln\frac{\alpha_i}{1-\alpha_i}\right)^2+4am.

    If \Delta > 0 , solve the following ordinary differential equation

    A_1\ln \left(\sqrt{\Omega_{t_j}^{-1}(1-\alpha_i)}-x_1\right)+A_2\ln \left(\sqrt{\Omega_{t_j}^{-1}(1-\alpha_i)}-x_2\right) = t_j+A_1\ln (\sqrt{r_0}-x_1)+A_2\ln (\sqrt{r_0}-x_2)

    where

    A_1 = \frac{-\sigma \Phi^{-1}(1-\alpha_i)+\sqrt {\left[\sigma \Phi^{-1}(1-\alpha_i)\right]^2+4am}}{\sqrt {\left[\sigma \Phi^{-1}(1-\alpha_i)\right]^2+4am}} , A_2 = \frac{\sigma \Phi^{-1}(1-\alpha_i)+\sqrt {\left[\sigma \Phi^{-1}(1-\alpha_i)\right]^2+4am}}{\sqrt {\left[\sigma \Phi^{-1}(1-\alpha_i)\right]^2+4am}} , x_1 = \frac{\sigma \Phi^{-1}(1-\alpha_i)-\sqrt{\left[\sigma \Phi^{-1}(1-\alpha_i)\right]^2+4am}}{2a} , x_2 = \frac{\sigma \Phi^{-1}(1-\alpha_i)+\sqrt {\left[\sigma \Phi^{-1}(1-\alpha_i)\right]^2+4am}}{2a} .

    Else if \Delta = 0 , solve the following ordinary differential equation

    \begin{equation} \nonumber \begin{aligned} &\ln \left(\sqrt{\Omega_{t_j}^{-1}(1-\alpha_i)}-\frac{\sigma \Phi^{-1}(1-\alpha_i)}{a}\right)-\frac{\sigma \Phi^{-1}(1-\alpha_i)}{a\sqrt{\Omega_{t_j}^{-1}(1-\alpha_i)}-\sigma \Phi^{-1}(1-\alpha_i)}\\ & = \frac{1}{2}t_j+\ln \left(\sqrt{r_0}-\frac{\sigma \Phi^{-1}(1-\alpha_i)}{a}\right)-\frac{}{}\frac{\sigma \Phi^{-1}(1-\alpha_i)}{a\sqrt{r_0}-\sigma \Phi^{-1}(1-\alpha_i)}. \end{aligned} \end{equation}

    Else if \Delta < 0 , solve the following ordinary differential equation

    \begin{equation} \nonumber \begin{aligned} &\frac{-1}{a}\ln \left(u^2+p\right)-\frac{\sigma \Phi^{-1}(1-\alpha_i)}{a^2\sqrt p}\arctan\frac{u}{\sqrt p}\\ & = t_j-\frac{1}{a}\ln\left[\left(\sqrt{r_0}-\frac{\sigma \Phi^{-1}(1-\alpha_i)}{2a}\right)^2+p\right]-\frac{\sigma \Phi^{-1}(1-\alpha_i)}{a^2\sqrt p}\arctan\frac{\sqrt{r_0}-\frac{\sigma \Phi^{-1}(1-\alpha_i)}{2a}}{\sqrt p} \end{aligned} \end{equation}

    where p = \frac{{\left[\sigma \Phi^{-1}(1-\alpha_i)\right]^2+4am}}{-4a^2} and u = \sqrt{\Omega_{t_j}^{-1}(1-\alpha_i)}-\frac{\sigma \Phi^{-1}(1-\alpha_i)}{2a}.

    If j < M , return to Step 5.

    Step 7: Calculate the discount rate

    \exp\left(-\int_0^T \Omega_{s}^{-1}(1-\alpha_i){{{\rm{d}}}} s \right) \rightarrow \exp\left(-\frac{T}{M}\sum\limits_{j = 1}^{M} \Omega_{t_j}^{-1}(1-\alpha_i)\right)

    and

    \Upsilon_{1T}^{-1}(\alpha_i) = \left(\Upsilon_T^{-1}(\alpha_i)-K\right)^+ = \max \left(Y_0\left(e_1T+\frac{\sqrt{3}\sigma_1 T}{\pi}\ln \frac{\alpha_i}{1-\alpha_i}\right)-K, 0\right).

    Step 8: It is obvious that

    \Psi_T^{-1}(\alpha_i) = Z_0\left(e_2T+\frac{\sqrt{3}\sigma_2 T}{\pi}\ln \frac{\alpha_i}{1-\alpha_i}\right).

    Step 9: Calculate

    \exp\left(-\int_0^T \Omega_{s}^{-1}(1-\alpha_i){{{\rm{d}}}} s \right)\min\left( \Upsilon_{1T}^{-1}(\alpha_i),\Psi_T^{-1}(\alpha_i)\right);

    if i < N-1 , return Step 3.

    Step 10: f_c \rightarrow \frac{1}{N-1} \sum_{i = 1}^{N-1}\exp\left(-\int_0^T \Omega_{s}^{-1}(1-\alpha_i){{{\rm{d}}}} s \right)\min\left(\Upsilon_{1T}^{-1}(\alpha_i), \Psi_T^{-1}(\alpha_i)\right).

    Example 6.1. For the European vulnerable call option pricing formula (6), we assume the M = 100, N = 100, a = 0.001, m = 0.002, \sigma = 5*10^{-5}, Y_0 = 5, e_1 = 0.1, \sigma_1 = \frac{\pi}{10\sqrt{3}}, Z_0 = 10, e_2 = 0.2, \sigma_2 = \frac{\pi}{8\sqrt{3}}, T = 5 and K = 3.6. Thus the European vulnerable call option price is f_c = 0.49944278. When the parameters aside from the parameter expiration date T remain unchanged, the relationship between the price of the European vulnerable call option f_c and the expiration date T is as shown in Figure 1. When all parameters except for the parameter volatility \sigma_1 remain unchanged, the relationship between the price of the European vulnerable call option f_c and volatility \sigma_1 is as shown in Figure 2. When all parameters except for the parameter log-drift e_1 remain unchanged, the relationship between the price of the European vulnerable call option f_c and the log-drift e_1 is as shown in Figure 3.

    Figure 1.  f_c versus the expiration date T .
    Figure 2.  f_c versus the volatility \sigma_1 .
    Figure 3.  f_c versus the log-drift e_1 .

    It can be seen in Figure 1 that with the increase of the expiration date T , the price of European vulnerable call options shows an overall upward trend. When the expiration date T is in the range of [0, 3], the price changes are not obvious, and the price shows a slow growth trend in the range of [3, 10]. Although the direction of time is deterministic, the trend of expiration T is still a focus of attention. As can be seen in Figure 2, with the increase of volatility \sigma_1 , the price of European vulnerable call options shows an overall upward trend. When the volatility is in the range of [0, 0.04], the option price is negative, indicating that the power of the sellers is far greater than that of the buyers. At this time, the investor should carefully consider the future prospect of this option according to their own risk preference. In the later period, with the increase of volatility \sigma_1 , the option price shows an upward trend. The slope of the figure represents the vega of the option price, which is the ratio of the change in the corresponding option price to the change in the volatility of the underlying asset. It can be seen in the figure that the vega presents a trend of first increasing and then decreasing under the conditions of this uncertain model. This indicates that the sensitivity of the European vulnerable call option price to volatility changes increases first and then decreases. At this time, it is best to frist buy and then sell the corresponding stock in the form of dynamic hedging, so as to ensure risk neutrality. It can be seen in Figure 3 that with the increase of log-drift e_1 , the price of European vulnerable call options shows an overall upward trend. When investing, investors should combine log-drift e_1 and other indicators to reasonably choose the time to buy and sell.

    The first six steps of the numerical algorithm for European vulnerable put options are the same as those for the European vulnerable call option.

    Step 7: Calculate the discount rate

    \exp\left(-\int_0^T \Omega_{s}^{-1}(1-\alpha_i){{{\rm{d}}}} s \right) \rightarrow \exp\left(-\frac{T}{M}\sum\limits_{j = 1}^{M} \Omega_{t_j}^{-1}(1-\alpha_i)\right)

    and

    \Upsilon_{2T}^{-1}(\alpha_i) = \left(K-\Upsilon_T^{-1}(1-\alpha_i)\right)^+ = \max \left(K-Y_0\left(e_1T+\frac{\sqrt{3}\sigma_1 T}{\pi}\ln \frac{1-\alpha_i}{\alpha_i}\right), 0\right).

    Step 8: It is obvious that

    \Psi_T^{-1}(\alpha_i) = Z_0\left(e_2T+\frac{\sqrt{3}\sigma_2 T}{\pi}\ln \frac{\alpha_i}{1-\alpha_i}\right).

    Step 9: Calculate

    \exp\left(-\int_0^T \Omega_{s}^{-1}(1-\alpha_i){{{\rm{d}}}} s \right)\min\left( \Upsilon_{2T}^{-1}(\alpha_i),\Psi_T^{-1}(\alpha_i)\right);

    if i < N-1 , return Step 3.

    Step 10: f_p \rightarrow \frac{1}{N-1} \sum_{i = 1}^{N-1}\exp\left(-\int_0^T \Omega_{s}^{-1}(1-\alpha_i){{{\rm{d}}}} s \right)\min\left(\Upsilon_{2T}^{-1}(\alpha_i), \Psi_T^{-1}(\alpha_i)\right).

    Example 6.2. For the European vulnerable put option pricing formula (7), we assume that M = 100, N = 100, a = 0.001, m = 0.002, \sigma = 5*10^{-5}, Y_0 = 5, e_1 = 0.1, \sigma_1 = \frac{\pi}{10\sqrt{3}}, Z_0 = 10, e_2 = 0.2, \sigma_2 = \frac{\pi}{8\sqrt{3}}, T = 5 and K = 3.6. Thus the European vulnerable put option price is f_p = 1.3576985. When all parameters except for the parameter expiration date T remain unchanged, the relationship between the price of the European vulnerable put option f_p and the expiration date T is as shown in Figure 4. When all parameters except for the parameter volatility \sigma_1 remain unchanged, the relationship between the price of the European vulnerable put option f_p and volatility \sigma_1 is as shown in Figure 5. When all parameters except for the parameter log-drift e_1 remain unchanged, the relationship between the price of the European vulnerable put option f_p and the log-drift e_1 is as shown in Figure 6.

    Figure 4.  f_p versus the expiration date T .
    Figure 5.  f_p versus the volatility \sigma_1 .
    Figure 6.  f_p versus the log-drift e_1 .

    It can be seen in Figure 4 that with the increase of the expiration date T , the price of the European vulnerable put option generally increases first and then decreases. When the expiration date T is in the range of [0, 1.6], the price gradually increases, and in the range of [1.6, 10], the price gradually decreases. As can be seen in Figure 5, with the increase of volatility \sigma_1 , the price of European vulnerable put options shows an overall upward trend. When the volatility is in the range of [0, 0.04], option prices are negative. In the range of [0.04, 0.45], with the increase of volatility \sigma_1 , the option prices show an upward trend. At this time, the vega is not very sensitive to changes in the current underlying asset, so there is no need to make significant adjustments. It can be seen in Figure 6 that with the increase of log-drift e_1 , the price of the European vulnerable put option shows a downward trend. When investing, investors should combine log-drift e_1 and other indicators to reasonably choose the time to buy and sell.

    In this paper, first, we obtained the solution in terms of the distribution of the uncertain CIR interest rate model. Second, we obtained the pricing formulas of the European vulnerable call option and European vulnerable put option in the model. Finally, according to the the above pricing formulas, the corresponding numerical algorithms and numerical examples were given to verify them.

    This work was supported by the Colleges and Universities in Hebei Province Science and Technology Research Project (ZD2019047) and the National Natural Science Foundation (61806133).

    The authors declare that they have no conflicts of interest.



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