
In this work, we mainly focused on the pricing formula for fractal barrier options where the underlying asset followed the sub-mixed fractional Brownian motion with jump, including the down-and-out call option, the down-and-out put option, the down-and-in call option, the down-and-in put option, and so on. To start, the fractal Black-Scholes type partial differential equation was established by using the fractal Itô's formula and a self-financing strategy. Then, by transforming the partial differential equation to the Cauchy problem, we obtained the explicit pricing formulae for fractal barrier options. Finally, the effects of barrier price, fractal dimension, Hurst index, jump intensity, and volatility on the value of fractal barrier options were exhibited through numerical experiments.
Citation: Chao Yue, Chuanhe Shen. Fractal barrier option pricing under sub-mixed fractional Brownian motion with jump processes[J]. AIMS Mathematics, 2024, 9(11): 31010-31029. doi: 10.3934/math.20241496
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In this work, we mainly focused on the pricing formula for fractal barrier options where the underlying asset followed the sub-mixed fractional Brownian motion with jump, including the down-and-out call option, the down-and-out put option, the down-and-in call option, the down-and-in put option, and so on. To start, the fractal Black-Scholes type partial differential equation was established by using the fractal Itô's formula and a self-financing strategy. Then, by transforming the partial differential equation to the Cauchy problem, we obtained the explicit pricing formulae for fractal barrier options. Finally, the effects of barrier price, fractal dimension, Hurst index, jump intensity, and volatility on the value of fractal barrier options were exhibited through numerical experiments.
Barrier option is a European option contract in which the value depends not only on the price of the underlying asset on the expiration date of the option, but also on whether the underlying asset price reaches a specified level (barrier) during the entire option validity period. It is cheaper than ordinary European options, and therefore attracts more attention from investors in the financial market. Barrier option also contributes to the research of many structured financial products, so barrier option pricing has always been a hot topic [1,2,3,4].
Merton [5] proposed a closed solution for European options, which was later extended by Reiner and Rubinstein [6] to pricing formulas for other European barrier options. However, these studies were carried out under the Black-Scholes (B-S) model [7] in which the underlying asset price assumed to obey the logarithmic normal distribution. However, later, a large number of subsequent financial empirical studies [8,9] revealed that financial assets have self-similarity and long-term dependence, which is inconsistent with the B-S model. To deal with this, subsequently following Kolmogorov's theory [10] that assets price is driven by fractional Brownian motion (fBm), many option pricing models with fBm have been extensively studied [11,12,13,14]. However, we can apply Wick-self-financing strategies to explore the fBm [15,16], but its application has tiny economic significance, which severely placed restrictions on its applicability in the financial market. As a result, alternative models have been suggested to account for the variation in financial assets, including the subfractional Brownian motion (sub-fBm) [17] and the sub-mixed fractional Brownian motion (sub-mixed fBm) [18].
The sub-fBm is similar to the fBm in most respects, but it differs in that it possesses a non-stationary second-order moment increment and converges more quickly [19]. Additionally, the sub-mixed fBm is a hybrid of the Brownian motion and the sub-fBm. The sub-mixed fBm transforms into a semi-martingale that is equivalent to the Brownian motion when the Hurst index H∈[0.75,1)[20]. Meanwhile, enlightened by Merton [21] and some recent studies [22,23,24,25], this article considers jump diffusion processes to describe asset price jump points caused by some unsystematic risk factors, which are often overlooked in the pricing of barrier options.
Nowadays, the fractional calculus has extensive applications in mathematical finance [26,27] and other problems [28,29,30,31,32]. Considering the fractal structure of financial markets, [33] addressed a double-barrier-option pricing problem under the time-fractional B-S framework and presented a robust second-order numerical scheme to solve the discretely monitored double-barrier time-fractional B-S partial differential equation. However, the barrier options studied in this paper did not involve jump processes. The authors [34] investigated the methodology for hedging an up-out put lookback-barrier option with the floating strike price, taking into account the dynamics of the underlying asset as modeled within a framework based on mixed fBm. The conclusion section of this article mentioned that future work would focus on developing a jump-diffusion version of the mixed fBm model, which can accurately describe the leptokurtosis phenomenon and infinite small jump behaviors of asset return distribution. In view of this, we introduce fractal derivatives into barrier options to study its pricing in the sub-mixed fBm with jump environment.
The paper is organized as follows. In Section 2, we introduce the definitions, properties, and formulae of the sub-mixed fBm and fractal derivative. Section 3 presents the fractal Itô's formula of the asset price driven by the sub-mixed fBm with jump, as well as the explicit solution of underlying asset price. In Section 4, we obtain the fractal B-S PDE and the closed-form solutions of barrier options. Section 5 is devoted to discussing the influences of some parameters on barrier options. Section 6 concludes the paper.
Definition 2.1. The sub-mixed fBm ζHt={ζHt(a,b)}t≥0 of parameters a,b and H, is a linear combination of the Brownian motion {Bt}t≥0 and the sub-fBm {BHt}t≥0, defined on the probability space {Ω,F,P} by
ζHt(a,b)=aBt+bBHt,∀t≥0, |
where {Bt}t≥0 and {BHt}t≥0 are independent of each other.
Some properties of the sub-mixed fBm ζHt={ζHt(a,b)}t≥0 are presented as
(1) ζHt is a central Gaussian process.
(2) ζH0(a,b)=aB0+bBH0=0,t=0.
(3) The covariance of ζHt(a,b) and ζHs(a,b) is
Cov(ζHt(a,b),ζHs(a,b))=a2(t∧s)+b22(t2H+s2H−∣t−s∣2H), |
where t∧s=12(t+s−∣t−s∣),∀t,s≥0.
(4) E((ζHt(a,b))2)=a2t+b2(2−22H−1)t2H),∀t≥0.
Definition 2.2. The fractal derivative with respect to t is defined as [35,36,37]:
∂u∂tα(t0,x)=Γ(1+α)limt−t0→ΔtΔt≠0u(t,x)−u(t0,x)(t−t0)α, | (2.1) |
where Δt is the smallest timescale, and α is the fractal dimension.
The following rules and formulae are very useful for practical applications:
(1) The chain rules:
∂∂tα(∂u∂tβ)=∂∂tβ(∂u∂tα), | (2.2) |
∂∂tα[ϕ(u)]=∂ϕ∂u(∂u∂tα). | (2.3) |
(2) The differential and integration formulae:
∂tm∂tα=mαtm−α, | (2.4) |
∫tα1tα0tmdtα=αm+α[tα(m+α)1−tα(m+α)0]. | (2.5) |
In this article, we combine classical financial stochastic analysis theory and fractal derivative knowledge to extend the B-S model. In addition, the following assumptions hold:
(1) There are two types of assets in the financial market: Risk-free assets (bonds) and risky assets (stocks).
(2) We suppose that the dynamics of stock price St is driven by the fractal sub-mixed fBm with jump:
dαSt=(μ−q)Stdtα+StdζHt(σ1,σ2)+σ3StdJt=(μ−q)Stdtα+σ1StdBt+σ2StdBHt+σ3StdJt, | (3.1) |
where μ represents the instantaneous expected return rate of the stock, q represents the stock dividend rate, σi(i=1,2,3) are the volatility of stock price, {Jt}t≥0 is a compensated Poisson process with intensity λ, and {Bt}t≥0, {BHt}t≥0 and {Jt}t≥0 are independent of each other.
(3) The return of risk-free assets in time period t are presented as follows:
dαMt=rMtdtα, | (3.2) |
where constant r presents the risk-free interest rate.
(4) All assets can be freely and continuously traded without the need to pay transaction costs and taxes.
(5) There is no arbitrage opportunity in the financial market.
(6) Short selling is unrestricted.
(7) The option can only be exercised at maturity.
Theorem 3.1. Suppose the initial value of ξt=ζHt(σ1,σ2)+σ3Jt is zero, and f(t,ξt) is second-order differentiable. Hence, the fractal Itô's formula of the sub-mixed fBm with jump can be given as:
f(t,ξt)=f(0,0)+∫tα0(∂f∂s−λσ3∂f∂ξ)dsα+∫tα0[σ212+(2−22H−1)Hσ22s2H−1]∂2f∂ξ2dsα+σ1∫tα0∂f∂ξdBs+σ2∫tα0∂f∂ξdBHs+∑s≤t[f(s,ξs)−f(s−,ξs−)]=f(0,0)+∫tα0{∂f∂s+[σ212+λσ312+(2−22H−1)Hσ22s2H−1]∂2f∂ξ2dsα+σ1∫tα0∂f∂ξdBs+σ2∫tα0∂f∂ξdBHs+σ3∫tα0∂f∂ξdJs. |
Proof. Based on the Itô's formula of the sub-mixed fBm [18], the jump process analysis method [38], and fractal derivative knowledge, we obtain
f(t,ξt)=f(0,0)+∫tα0∂f∂sdsα+∫tα0∂f∂Sdξcs+12∫tα0∂2f∂S2d(ξcs)2+∑s≤t[f(s,ξs)−f(s−,ξs−)]=f(0,0)+∫tα0(∂f∂s−λσ3∂f∂ξ)dsα+∫tα0[σ212+(2−22H−1)Hσ22s2H−1]∂2f∂ξ2dsα+σ1∫tα0∂f∂ξdBs+σ2∫tα0∂f∂ξdBHs+∑s≤t[f(s,ξs)−f(s−,ξs−)]. | (3.3) |
Take advantage of the identities:
dξct=σ1dBt+σ2dBHt−λσ3dtα, |
(dξct)2=[σ21+2(2−22H−1)Hσ22t(2H−1)α]dtα, |
where ξct=σ1Bt+σ2BHt−λσ3tα represents the continuous part of ξt.
Provided that u(x) is second-order differentiable and the Poisson process {Nt}t≥0 possesses second-order moment increment <dNt,dNt>=λdtα, the generalized fractal Itô's formula gives
∑s≤t[u(Ns)−u(us−)]=∫tα0∂u∂NdNs+λ2∫tα0∂2u∂N2dsα. |
Coupling ξt=ζHt(σ1,σ2)+σ3Jt=σ1Bt+σ2BHt+σ3Nt−λσ3tα, we have
∑s≤t[f(s,ξs)−f(s−,ξs−)]=σ3∫tα0∂f∂ξdNs+λσ232∫tα0∂2f∂ξ2dsα. | (3.4) |
Inserting (3.4) into (3.3), we arrive at
f(t,ξt)=f(0,0)+∫tα0{∂f∂s+[σ212+λσ312+(2−22H−1)Hσ22s2H−1]∂2f∂ξ2}dsα+σ1∫tα0∂f∂ξdBs+σ2∫tα0∂f∂ξdBHs+σ3∫tα0∂f∂ξdJs. |
Theorem 3.2. The explicit solution of the stock price (3.1) is given by:
St=S0exp[(μ−q−σ212−λσ312)tα−(1−22H−2)σ22t2Hα+σ1Bt+σ2BHt+σ3Jt]. |
Proof. Suppose f(t,ξt)=S0exp[(μ−q−σ212−λσ312)tα−(1−22H−2)σ22t2Hα+ξt],
then by use of Theorem 3.1, we obtain
df(t,ξt)={∂f∂tα+[σ212+λσ312+(2−22H−1)Hσ22t(2H−1)α]∂2f∂ξ2}dtα+∂f∂ξdξt=(μ−q)f(t,ξt)dtα+f(t,ξt)dξt=(μ−q)f(t,ξt)dtα+f(t,ξt)dζHt(σ1,σ2)+σ3f(t,ξt)dJt, | (3.5) |
where
∂f∂tα=[μ−q−σ212−λσ312−(2−22H−1)Hσ22t(2H−1)α]f(t,ξt),∂f∂ξ=f(t,ξt),∂2f∂ξ2=f(t,ξt). |
Comparing (3.1) with (3.5), we have dSt=df(t,ξt), where f(0,ξ0)=S0. Thence,
St=S0exp[(μ−q−σ212−λσ312)tα−(1−22H−2)σ22t2Hα+σ1Bt+σ2BHt+σ3Jt]. |
In this section, we will derive the pricing formula for fractal battier options with the help of the explicit solution of stock price St.
Theorem 4.1. Suppose that the underlying asset price St complies with (3.1), then the value of contingent claims Wt=W(t,St) is presented as:
∂W∂tα−(r−q)St∂W∂S+[σ212+λσ232+(2−22H−1)Hσ22t(2H−1)α]S2t∂2W∂S2−rWt=0. |
Proof. Applying self-financing strategy νt=(ν1t,ν2t), we hold many ν1t bonds and ν2t stocks to construct the wealth process, and its value at time t is given as
Wt=ν1tMt+ν2tSt. | (4.1) |
Using (3.1) and (3.2), we have
dWt=ν1tdMt+ν2tdSt+ν2tqStdtα=(rν1tMt+μν2tSt)dtα+ν2tSt(σ1dBt+σ2dBHt+σ3dJt). | (4.2) |
Meanwhile, combining Theorems 3.1 and 3.2, we obtain
dWt=∂W∂tαdtα+∂W∂SdSt+12∂2W∂S2(dSt)2={∂W∂tα+(μ−q)St∂W∂S+[σ212+λσ232+(2−22H−1)Hσ22t(2H−1)α]S2t∂2W∂S2}dtα+St∂W∂S(σ1dBt+σ2dBHt+σ3dJt), | (4.3) |
where (dSt)2=S2t[σ21+λσ23+(4−4H)Hσ22t(2H−1)α]dtα.
By using (4.2) and (4.3), ν1t and ν2t are presented as
{ν1t=(rMt)−1{∂W∂tα−qSt∂W∂S+[σ212+λσ232+(2−22H−1)Hσ2t(2H−1)α]S2t∂2W∂S2},ν2t=∂W∂S. | (4.4) |
In addition, according to formula (4.1), we have
ν1t=Wt−ν2tStMt, | (4.5) |
then combining (4.4) and (4.5) yields the result.
Theorem 4.2. Consider that the underlying asset price St complies with (3.1), then the value of the down-and-out call option Vdo(t,St) at time t, with the fixed strike price K, the fixed barrier R, and the maturity time T, is expressed as follows:
Vdo(t,St)=Ste−q(Tα−tα2)N(l1)−Ke−r(Tα−tα2)N(l2)−(StR)h(t)[R2Ste−q(Tα−tα2)N(l3)−Ke−r(Tα−tα2)N(l4)], |
where N(⋅) stands for the cumulative probability of standard normal distribution, and
l1=lnStK+(r−q+σ212+λσ232)(Tα−tα2)+σ22(1−22H−2)(T2Hα−t2Hα2)√(σ21+λσ23)(Tα−tα2)+σ22(2−22H−1)(T2Hα−t2Hα2),l2=l1−√(σ21+λσ23)(Tα−tα2)+σ22(2−22H−1)(T2Hα−t2Hα2),l3=lnR2KSt+(r−q+σ212+λσ232)(Tα−tα2)+σ22(1−22H−2)(T2Hα−t2Hα2)√(σ21+λσ23)(Tα−tα2)+σ22(2−22H−1)(T2Hα−t2Hα2),l4=l3−√(σ21+λσ23)(Tα−tα2)+σ22(2−22H−1)(T2Hα−t2Hα2),h(t)=1−2(r−q)(Tα−tα2)(σ21+λσ23)(Tα−tα2)+σ22(2−22H−1)(T2Hα−t2Hα2). |
Proof. For convenience, let Wt(t,St)=Vdo(t,St)=Vdo, then in terms of Theorem 4.1, the value of the down-and-out call option Vdo(t,St) is expressed as follows
∂Vdo∂tα+(r−q)St∂Vdo∂S+[σ212+λσ232+(2−22H−1)Hσ22t(2H−1)α]S2t∂2Vdo∂S2−rVdo=0, |
along with the initial condition Vdo(T,ST)=(ST−K)+,R<St<+∞, as well as the boundary condition Vdo(t,R)=0,0≤t≤T.
Suppose
x=lnStR,Vdo(t,St)=RˆV(t,x). | (4.6) |
We have
∂Vdo∂tα=R∂ˆV∂tα,∂Vdo∂S=R∂ˆV∂x∂x∂S=RSt∂ˆV∂x,∂2Vdo∂S2=RS2t(∂2ˆV∂x2−∂ˆV∂x). |
Then, we obtain
∂ˆV∂tα+(r−q)∂ˆV∂x+[σ212+λσ232+(2−22H−1)Hσ22t(2H−1)α](∂2ˆV∂x2−∂ˆV∂x)−rˆV=0, |
along with the initial condition ˆV(T,lnSTR)=(ex−KR)+,0<x<+∞, as well as the boundary condition ˆV(0,t)=0,0≤t≤T.
Furthermore, we let
δ(ρ,ι)=ˆV(x,t)ek2(t),ρ=k3(t),ι=x+k1(t), | (4.7) |
where ki(t)(i=1,2,3) are functions to be determined about t. Then we have
∂ˆV∂tα=e−k2(t)[dk1(t)dtα∂δ∂ι+dk3(t)dtα∂δ∂ρ−dk2(t)dtαδ], |
∂ˆV∂x=e−k2(t)∂δ∂ι,∂2ˆV∂x2=e−k2(t)∂2δ∂ι2 |
and
dk3(t)dtα∂δ∂ρ+κ(t)∂2δ∂ι2+[r−q+dk1(t)dtα−κ(t)]∂ˆV∂x−[r+dk1(t)dtα]δ=0, | (4.8) |
where κ(t)=σ212+λσ232+(2−22H−1)Hσ22t(2H−1)α.
In order to find the solution, let
{dk3(t)dtα+κ(t)=0,r−q+dk1(t)dtα−κ(t)=0,r+dk2(t)dtα=0,k1(T)=k2(T)=k3(T)=0, | (4.9) |
to transform (4.8) into the heat equation. According to (4.9), ki(t)(i=1,2,3) are presented as
{k1(t)=∫Ttαr−q−κ(s)dsα=(r−q−σ212−λσ232)(Tα−tα2)−σ22(1−22H−2)(T2Hα−t2Hα2),k2(t)=∫Ttαrdsα=r(Tα−tα2),k3(t)=∫Ttακ(s)dsα=(σ212+λσ232)(Tα−tα2)+σ22(1−22H−2)(T2Hα−t2Hα2). | (4.10) |
Inserting (4.10) into (4.8), we obtain the value of the down-and-out call option Vdo(t,St) presented by
∂δ∂ρ=∂2δ∂ι2, | (4.11) |
along with the initial condition δ(0,ι)=(eι−K)+,0<ι<+∞, and the boundary condition δ(ρ,k1(t))=0,0≤t≤T.
To begin, considering the above equation with initial condition, we obtain the following solution through Poisson formula
δ(ρ,ι)=12√πρ∫+∞−∞φ(y)e−(ι−y)24ρdy. | (4.12) |
Next, we handle the boundary conditions and let Φ(y)=φ(y)e−[k1(t)−y]24ι(y>0), Then Φ(y) is extended to an odd function in the entire real field
Φ(y)={φ(y)e−[k1(t)−y]24ι,y>0,−φ(−y)e[k1(t)+y]24ι,y≤0. |
Consider the above equation and the original initial condition in (4.11), then the extended initial condition, including the boundary condition, can be presented as follows:
φ(y)={(ey−KR)+,y>0,−(e−y−KR)+e−k1(t)yι,y≤0. |
Then, (4.6) becomes a Cauchy problem
∂δ∂ρ=∂2δ∂ι2, | (4.13) |
along with the initial condition δ(0,ι)=φ(ι),0<ι<+∞.
In terms of (4.12), we have
δ(ρ,ι)=12√πρ∫+∞−∞φ(y)e−(ι−y)24ρdy.=12√πρ∫+∞lnKR(ey−KR)e−(ι−y)24ρdy−12√πρ∫−lnKR−∞(e−y−KR)e−(ι−y)2+4k1(t)y4ρdy=12√πρ∫+∞lnKRey−(ι−y)24ρdy−12√πρKR∫+∞lnKLe−(ι−y)24ρdy−12√πρ∫+∞lnKRey−(ι+y)2−4k1(t)y4ρdy+12√πρKR∫+∞lnKRe(ι+y)2−4k1(t)y4ρdy=A1+A2+A3+A4. |
Consider A1,
A1=12√πρ∫+∞lnKRey−(ι−y)24ρdy=eρ+ι12√πρ∫+∞lnKRe−(y−ι−2ρ)24ρdy. |
Now, let t=y−ι−2ρ√2ρ, then we obtain
A1=eρ+ι1√2π∫+∞lnKR−ι−2ρ√2ρe−t22dt=eρ+ιN(l1), |
where N(⋅) stands for the cumulative probability of standard normal distribution, and l1=ι+2ρ−lnKR√2ρ.
Then, in the similar way, denote t=y−ι√2ρ, and we have
A2=−12√πρKR∫+∞lnKRe−(ι−y)24ρdy=−KR1√2π∫+∞lnKR−ι√2ρe−t22dt=−KRN(l2), |
where l2=ι−lnKR√2ρ=l1−√2ρ.
For A3,
A3=−12√πρ∫+∞lnKRey−(ι+y)2−4k1(t)y4ρdy=−e[ρ+k1(t)][ρ+k1(t)−ι]ρ12√πρ∫+∞lnKRe−[y+ι−2k1(t)−2ρ]24ρdy. |
Making the change of variable t=y+ι−2k1(t)−2ρ√2ρ,
A3=−e[ρ+k1(t)][ρ+k1(t)−ι]ρ1√2π∫+∞lnKR+ι−2k1(t)−2ρ√2ρe−t22dt=−e[ρ+k1(t)][ρ+k1(t)−ι]ρN(l3), |
with l3=2k1(t)+2ρ−ι−lnKR√2ρ.
We put t=y+ι−2k1(t)√2ρ, then
A4=12√πρKR∫+∞lnKRe−(ι+y)2−4k1(t)y4ρdy=KRek1(t)[k1(t)−ι]ρ12√πρ∫+∞lnKRe[y+ι−2k1(t)]24ρdy=ek1(t)[k1(t)−ι]ρ1√2π∫+∞lnKR+ι−2k1(t)√2ρKRe−t22dt=KRek1(t)[k1(t)−ι]ρN(l4), |
where l4=2k1(t)−ι−lnKR√2ρ=l3−√2ρ.
Insert (4.6) and (4.7) into them, we have
A1=StRe(r−q)(Tα−tα2)N(l1),A2=−KRN(l2),A3=−e(r−q)(Tα−tα2)(ρ−lnStR)ρN(l3)=−e(r−q)(Tα−tα2)+[1−(r−q)(Tα−tα2)ρ]lnStR−lnStRN(l3)=−e(r−q)(Tα−tα2)(StR)1−(r−q)(Tα−tα2)ρRStN(l3),A4=KRe[ρ−(r−q)(Tα−tα2)]lnStRρN(l4)=KR(StR)1−(r−q)(Tα−tα2)ρN(l4). |
By using Ai(i=1,2,3,4), one has
Vdo(t,St)=RˆV(t,x)=Re−r(Tα−tα2)δ(ρ,ι)=Re−r(Tα−tα2)(A1+A2+A3+A4)=Ste−q(Tα−tα2)N(l1)−Ke−r(Tα−tα2)N(l2)−(StR)h(t)[R2Ste−q(Tα−tα2)N(l3)−Ke−r(Tα−tα2)N(l4)], |
where h(t)=1−2(r−q)(Tα−tα2)(σ21+λσ23)(Tα−tα2)+σ22(2−22H−1)(T2Hα−t2Hα2).
Corollary 4.1. Assuming that the underlying asset price St meets (3.1), we have the value of the vanilla call option Vvanilla(t,St) at time t, along with a fixed strike price K and the maturity time T as follows:
Vvanilla(t,St)=Ste−q(Tα−tα2)N(l1)−Ke−r(Tα−tα2)N(l2), |
among them, N(⋅),l1, and l2 are the same as Theorem 4.2.
Proof. We can prove it using a process similar to Theorem 4.2. Let
ˉx=lnStR,Vvanilla(t,St)=RˉV(t,ˉx). |
ˉδ(ˉρ,ˉι)=ˉV(t,ˉx)ek2(t),ˉρ=k3(t),ˉι=ˉx+k1(t), |
where ki(t)(i=1,2,3) are shown in (4.10).
Then, we can obtain the value of vanilla call option Vvanilla(t,St) by analyzing the Cauchy problem below
∂ˉδ∂ˉρ=∂2ˉδ∂ˉι2, |
along with the initial condition ˉδ(0,ˉι)=(eˉι−K)+,0<ˉι<+∞. Then, we can use a process similar to (4.13) to prove the subsequent parts of this corollary.
Corollary 4.2. Assuming that the underlying asset price St meets (3.1), we obtain the value of the vanilla put option Gvanilla(t,St) at time t, along with a fixed strike price K and the maturity time T
Gvanilla(t,St)=Ke−r(Tα−tα2)N(−l2)−Ste−q(Tα−tα2)N(−l1), |
among them, N(⋅),l1, and l2 are presented in Theorem 4.2.
Proof. The remaining proof process is similar to Corollary 4.1 after changing the condition to (K−ST)+.
Theorem 4.3. Consider that the underlying asset price St complies with (3.1). If the options possess the same fixed strike price K, fixed barrier R, and maturity time T, then at time t, there exists the parity formula between the value of the down-and-out call option Vdo(t,St) and the value of the down-and-out put option Gdo(t,St) as follows:
Vdo(t,St)+Ke−r(Tα−tα2)[N(l6)−(StR)h(t)N(l8)]=Gdo(t,St)+Ste−q(Tα−tα2)[N(l5)−(StR)h(t)−2N(l7)], |
where N(⋅) stands for the cumulative probability of standard normal distribution, and
l5=lnStR+(r−q+σ212+λσ232)(Tα−tα2)+σ22(1−22H−2)(T2Hα−t2Hα2)√(σ21+λσ23)(Tα−tα2)+σ22(2−22H−1)(T2Hα−t2Hα2),l6=l5−√(σ21+λσ23)(Tα−tα2)+σ22(2−22H−1)σ22(T2Hα−t2Hα2),l7=lnRSt+(r−q+σ212+λσ232)(Tα−tα2)+σ22(1−22H−2)σ22(T2Hα−t2Hα2)√(σ21+λσ23)(Tα−tα2)+σ22(2−22H−1)(T2Hα−t2Hα2),l8=l7−√(σ21+λσ23)(Tα−tα2)+σ22(2−22H−1)σ22(T2Hα−t2Hα2),h(t)=1−2(r−q)(Tα−tα2)(σ21+λσ23)(Tα−tα2)+σ22(2−22H−1)(T2Hα−t2Hα2). |
Proof. To start, let
Cdo(t,St)=Vdo(t,St)−Gdo(t,St), | (4.14) |
which denotes the difference between the value of Vdo(t,St) and Gdo(t,St) at time t and meets
∂Cdo∂tα+(r−q)St∂Cdo∂S+[σ212+λσ232+(2−22H−1)Hσ22t(2H−1)α]S2t∂2Cdo∂S2−rCdo=0, |
along with the initial condition Cdo(T,ST)=(ST−K),R<St<+∞, as well as the boundary condition Cdo(t,R)=0,0≤t≤T.
Similar to the solving process of (4.11), we can obtain
Cdo(t,St)=Ste−q(Tα−tα2)N(l5)−Ke−r(Tα−tα2)N(l6)−(StR)h(t)[R2Ste−q(Tα−tα2)N(l7)−Ke−r(Tα−tα2)N(l8)], |
then combining the above result and (4.14) yields the Theorem 4.3.
Theorem 4.4. Consider that the underlying asset price St complies with (3.1), then the value of the down-and-out put option Gdo(t,St) at time t, with the fixed strike price K, the fixed barrier R, and the maturity time T, is expressed as follows:
Gdo(t,St)=Ste−q(Tα−tα2)[N(l1)−N(l5)]−Ke−r(Tα−tα2)[N(l2)−N(l6)]−(StR)h(t){R2Ste−q(Tα−tα2)[N(l3)−N(l7)]−Ke−r(Tα−tα2)[N(l4)−N(l8)]}, |
where N(⋅),li(i=1,2,…,8), and h(t) are presented in Theorems 4.2 and 4.3.
Proof. Theorem 4.4 can be easily proved by using Theorems 4.2 and 4.3.
Theorem 4.5. Consider that the underlying asset price St complies with (3.1), then the value of the down-and-in call option Vdi(t,St) and the value of the down-and-in put option Gdi(t,St) at time t, with the fixed strike price K, the fixed barrier R, and the maturity time T, is
Vdi(t,St)=(StR)h(t)[R2Ste−q(Tα−tα2)N(l3)−Ke−r(Tα−tα2)N(l4)], |
Gdi(t,St)=Ke−r(Tα−tα2)N(−l6)−Ste−q(Tα−tα2)N(−l5)]+(StR)h(t){R2Ste−q(Tα−tα2)[N(l3)−N(l7)]−Ke−r(Tα−tα2)[N(l4)−N(l8)]}, |
where N(⋅),li(i=3,4,…,8) and h(t) are shown in Theorems 4.2 and 4.3.
Proof. Investment portfolio with both out option and corresponding in option tend to always perform one of their option rights when other conditions are the same. In this case, it is equivalent to a vanilla option
Wvanilla(t,St)=Wdo(t,St)+Wdi(t,St)=Wuo(t,St)+Wui(t,St), |
where Wvanilla(t,St) means the European option, and Wdo(t,St),Wdi(t,St),Wuo(t,St), and Wui(t,St) stand for the value of the down-and-out option, the down-and-in option, the up-and-out option, and the up-and-in option. Then, we have
Vdi(t,St)=Vvanilla(t,St)−Vdo(t,St),Gdi(t,St)=Gvanilla(t,St)−Gdo(t,St). |
Combining Corollaries 4.1 and 4.2 and Theorems 4.2 and 4.4, Theorem 4.5 is proved.
So far, we have obtained the pricing formulas for all four fractal downward barrier options. Of course, using a similar process, pricing formulas corresponding to the four fractal upward barrier options can also be derived. Obviously, the aforementioned are closed-form solutions of barrier options. Due to the difficulty in obtaining general analytical expressions for barrier options under the jump-diffusion framework, a significant amount of work has focused on numerical or the Monte Carlo simulation algorithm. For example, S. A. Metwally and A. F. Atiya [39] put forward a fast and unbiased Monte Carlo approach for pricing barrier options when the underlying security adheres to a simple jump-diffusion process with constant parameters and a continuously monitored barrier. Two algorithms were founded on the Brownian bridge concept. Both methods remarkably reduced bias and accelerated convergence compared to the standard Monte Carlo simulation approach. Based on this comparative analysis approach, we will discuss the impact of different parameter values on barrier options under sub-mixed fBm in three different cases in the next section.
In this section, we take the down-and-out call option as an example to discuss the impacts of the fractal dimension α, the barrier price R, the Hurst index H, the jump intensity λ, and volatility σ1,σ2,σ3 on barrier options.
Case 1. Numerical analysis of barrier prices under different fractal dimensions
According to Theorem 4.2, assume that the parameter selection is as follows:
t=0,T=0.5,K=100,H=0.95,σ1=σ2=σ3=0.4,λ=1. |
Then the trend of option value Vdo(t,St) affected by different barrier prices R=60,65,…,115, and different stock prices S=80,90,…,120, with different fractal dimensions α=1, 0.9, 0.8 is given in Figure 1(a)–(d), respectively.
From Figure 1, it can be seen that when the stock price is fixed, the relationships between the value of down-and-out call option and the barrier price is always negative as fractal dimension α changes. Under other unchanged conditions, as the barrier price rises, the possibility of down-and-out call option termination due to the option hitting the barrier price during its validity period will increase, and therefore the value of the option will continue to decline. Especially when the barrier price rises to the initial stock price, the option will be knocked out immediately, which means it no longer has value. On the other hand, for each fixed stock price and barrier price, the value of down-and-out call option increases with the decrease of fractal dimension, and the larger the stock price, the greater the difference in option value corresponding to the same barrier price.
Case 2. Numerical comparisons for different Hurst index and jump intensity values under different fractal dimensions.
In order to analyze the impact of the fractal dimension α, the Hurst index H, and the jump intensity λ on the option price, some parameters are chosen as follows:
t=0,T=0.5,S0=85,K=100,R=70,σ1=σ2=σ3=0.4. |
Figure 2(a) shows the variation of the value of down-and-out call option with the different Hurst index and jump intensity when α=1. As the Hurst index rises, the value of the down-and-out call option continues to decline. This change is mainly due to the fact that a larger Hurst index represents a smoother and more stable price of the underlying asset, which means that its price fluctuation will also be smaller, ultimately resulting in a smaller corresponding option value. In addition, it can be seen that the value of options and the jumps intensity vary in the same direction. The jump intensity reflects the unsystematic risk. As it increases, the underlying asset will experience more drastic fluctuations, which implies higher upper limit and a constant lower limit. Hence, the value of options will increase. Figure 2(b)–(d) depicts the trend of the value of down-and-out call option affected by different fractal dimensions α=0.9,0.8, and 0.7, respectively. From Figure 2(a)–(d), it can be seen that under the same other conditions, the value of down-and-out call option gradually increases as the fractal dimension α decreases, which indicates a negative correlation between them.
Case 3. Numerical results of different volatilities and fractal dimensions.
The parameter values are given as
t=0,T=0.5,R=70,K=100,H=0.95,λ=2,α=1. |
Set ˉσ=(σ1,σ2,σ3), let ˉσ1=(0.1,0.15,0.2),ˉσ2=(0.2,0.25,0.3),ˉσ3=(0.3,0.35,0.4),ˉσ4=(0.4,0.45,0.5). In terms of Theorem 4.2, we present the results for a comparison of the value of down-and-out call option under different volatility across different S0 between 75 and 120 in Table 1. It can be clearly seen that the value of the down-and-out call option increases with the growth of the volatility, which is consistent with the fact.
S | ˉσ1=(0.1,0.15,0.2) | ˉσ2=(0.2,0.25,0.3) | ˉσ3=(0.3,0.35,0.4) | ˉσ4=(0.4,0.45,0.5) |
75 | 0.9617 | 2.8239 | 3.7386 | 11.8228 |
80 | 1.6937 | 5.4347 | 10.5512 | 21.4360 |
85 | 2.1655 | 8.1616 | 19.1924 | 31.2478 |
90 | 2.3682 | 15.3213 | 27.9598 | 41.2370 |
95 | 6.6820 | 22.5143 | 36.8354 | 51.3861 |
100 | 11.5698 | 29.7287 | 45.8048 | 61.6805 |
105 | 16.4553 | 36.9562 | 54.8566 | 72.1077 |
110 | 21.3405 | 44.1912 | 63.9814 | 82.6571 |
115 | 26.2281 | 51.4299 | 73.1715 | 93.3198 |
120 | 31.1214 | 58.6699 | 82.4206 | 104.0877 |
In addition, let
t=0,T=0.5,R=70,K=100,H=0.95,λ=2,ˉσ1=(0.1,0.15,0.2). |
Table 2 shows that the value of the down-and-out call option is decreasing as the fractal dimension increasing with other parameters remains unchanged, which means a negative relationship between them.
S | α=0.9 | α=0.8 | α=0.7 | α=0.6 |
75 | 1.0735 | 1.1924 | 1.3187 | 1.4523 |
80 | 1.8954 | 2.1100 | 2.3378 | 2.5789 |
85 | 2.4341 | 2.7199 | 3.0232 | 3.3443 |
90 | 2.6809 | 3.0137 | 3.3668 | 3.7405 |
95 | 7.3313 | 8.0241 | 8.7620 | 9.5467 |
100 | 12.5828 | 13.6637 | 14.8154 | 16.0409 |
105 | 17.8296 | 19.2957 | 20.8582 | 22.5214 |
110 | 23.0736 | 24.9227 | 26.8935 | 28.9916 |
115 | 28.3184 | 30.5486 | 32.9256 | 35.4567 |
120 | 33.5677 | 36.1775 | 38.9595 | 41.9220 |
Considering that the price change of the underlying is regarded as a fractal transmission system, the fractal derivative is introduced into the barrier option under sub-mixed fBm with jump to try to achieve the ideal expectation of market justice. This paper mainly investigates the pricing formula for fractal barrier options under sub-mixed fBm with jump, including the down-and-out call option, the down-and-out put option, the down-and-in call option, the down-and-in put option, and so on. To start, the B-S type PDE is established by using the fractal Itô's formula and a self-financing strategy. Then, by transforming the PDE to the Cauchy problem, we obtain the explicit pricing formulae for fractal barrier options. Besides, the value of the fractal vanilla call option, the value of the fractal vanilla put option, and the parity formula between fractal barrier call option and fractal barrier put option are obtained by a similar method. Finally, taking the down-and-out call option as an example, numerical experiments show that barrier price, fractal dimension, and Hurst index are negatively correlated with the value of down-and-out call option, while jump intensity and volatility are positively correlated with it. In numerical experiments, using real data and achieving the calibration of the model to real-time market data will be an important topic of future research. This is beneficial in enhancing the degree of fit between the model and the actual market and providing directions for model improvement, so as to help investors analyze and control the risks associated with barrier options more intuitively and effectively and enrich the research content of barrier options.
Chao Yue: Conceptualization, formal analysis, methodology, software, resources, writing-original draft; Chuanhe Shen: Funding acquisition, investigation, supervision, validation, visualization, editing. All authors have read and agreed to the published version of the manuscript.
This work was supported by the Natural Science Foundation of Shandong Province (No.ZR2022MG045), the High-level Talent Introduction Scientific Research Project of Shandong Women's University(No.2022RCYJ01)
The authors declare no conflicts of interest.
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S | ˉσ1=(0.1,0.15,0.2) | ˉσ2=(0.2,0.25,0.3) | ˉσ3=(0.3,0.35,0.4) | ˉσ4=(0.4,0.45,0.5) |
75 | 0.9617 | 2.8239 | 3.7386 | 11.8228 |
80 | 1.6937 | 5.4347 | 10.5512 | 21.4360 |
85 | 2.1655 | 8.1616 | 19.1924 | 31.2478 |
90 | 2.3682 | 15.3213 | 27.9598 | 41.2370 |
95 | 6.6820 | 22.5143 | 36.8354 | 51.3861 |
100 | 11.5698 | 29.7287 | 45.8048 | 61.6805 |
105 | 16.4553 | 36.9562 | 54.8566 | 72.1077 |
110 | 21.3405 | 44.1912 | 63.9814 | 82.6571 |
115 | 26.2281 | 51.4299 | 73.1715 | 93.3198 |
120 | 31.1214 | 58.6699 | 82.4206 | 104.0877 |
S | α=0.9 | α=0.8 | α=0.7 | α=0.6 |
75 | 1.0735 | 1.1924 | 1.3187 | 1.4523 |
80 | 1.8954 | 2.1100 | 2.3378 | 2.5789 |
85 | 2.4341 | 2.7199 | 3.0232 | 3.3443 |
90 | 2.6809 | 3.0137 | 3.3668 | 3.7405 |
95 | 7.3313 | 8.0241 | 8.7620 | 9.5467 |
100 | 12.5828 | 13.6637 | 14.8154 | 16.0409 |
105 | 17.8296 | 19.2957 | 20.8582 | 22.5214 |
110 | 23.0736 | 24.9227 | 26.8935 | 28.9916 |
115 | 28.3184 | 30.5486 | 32.9256 | 35.4567 |
120 | 33.5677 | 36.1775 | 38.9595 | 41.9220 |
S | ˉσ1=(0.1,0.15,0.2) | ˉσ2=(0.2,0.25,0.3) | ˉσ3=(0.3,0.35,0.4) | ˉσ4=(0.4,0.45,0.5) |
75 | 0.9617 | 2.8239 | 3.7386 | 11.8228 |
80 | 1.6937 | 5.4347 | 10.5512 | 21.4360 |
85 | 2.1655 | 8.1616 | 19.1924 | 31.2478 |
90 | 2.3682 | 15.3213 | 27.9598 | 41.2370 |
95 | 6.6820 | 22.5143 | 36.8354 | 51.3861 |
100 | 11.5698 | 29.7287 | 45.8048 | 61.6805 |
105 | 16.4553 | 36.9562 | 54.8566 | 72.1077 |
110 | 21.3405 | 44.1912 | 63.9814 | 82.6571 |
115 | 26.2281 | 51.4299 | 73.1715 | 93.3198 |
120 | 31.1214 | 58.6699 | 82.4206 | 104.0877 |
S | α=0.9 | α=0.8 | α=0.7 | α=0.6 |
75 | 1.0735 | 1.1924 | 1.3187 | 1.4523 |
80 | 1.8954 | 2.1100 | 2.3378 | 2.5789 |
85 | 2.4341 | 2.7199 | 3.0232 | 3.3443 |
90 | 2.6809 | 3.0137 | 3.3668 | 3.7405 |
95 | 7.3313 | 8.0241 | 8.7620 | 9.5467 |
100 | 12.5828 | 13.6637 | 14.8154 | 16.0409 |
105 | 17.8296 | 19.2957 | 20.8582 | 22.5214 |
110 | 23.0736 | 24.9227 | 26.8935 | 28.9916 |
115 | 28.3184 | 30.5486 | 32.9256 | 35.4567 |
120 | 33.5677 | 36.1775 | 38.9595 | 41.9220 |