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Research article

Pricing equity warrants under the sub-mixed fractional Brownian motion regime with stochastic interest rate

  • Received: 25 March 2022 Revised: 01 July 2022 Accepted: 04 July 2022 Published: 11 July 2022
  • MSC : 58J35, 60H10, 91B26

  • This paper proposes a pricing model for equity warrants under the sub-mixed fractional Brownian motion regime with the interest rate following the Merton short rate model. By using the delta hedging strategy, the corresponding partial differential equations for equity warrants are obtained. Moreover, the explicit pricing formula for equity warrants and some numerical results are given.

    Citation: Xinyi Wang, Jingshen Wang, Zhidong Guo. Pricing equity warrants under the sub-mixed fractional Brownian motion regime with stochastic interest rate[J]. AIMS Mathematics, 2022, 7(9): 16612-16631. doi: 10.3934/math.2022910

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  • This paper proposes a pricing model for equity warrants under the sub-mixed fractional Brownian motion regime with the interest rate following the Merton short rate model. By using the delta hedging strategy, the corresponding partial differential equations for equity warrants are obtained. Moreover, the explicit pricing formula for equity warrants and some numerical results are given.



    An equity warrant allows warrant holders to buy stocks of listed companies at a certain price on a promissory day. It has many similarities with call options; therefore, many researchers [1,2] used the same model of option pricing to model the price of equity warrants. The classical option pricing model is the Black-Scholes model, which was proposed by Fischer Black and Myron Scholes in 1973 [3]. In the Black-Scholes model, the random driving source of the underlying asset is Brownian motion. However, Brownian motion cannot capture some characteristics of underlying assets, such as long-range correlations and heavy-tailed. Some researchers suggested using fractional Brownian motion to replace Brownian motion as the random driving source and have obtained some research results [4,5,6,7,8].

    However, as fractional Brownian motion is not a semi-martingale, researchers have found that arbitrage opportunities exist when choosing fractional Brownian motion as the random driving source [9,10]. Bojdecki et al. [11] proposed a new stochastic process called sub-fractional Brownian motion (sfBm). The sfBm not only captures the long-range correlations of changes in the underlying assets, but also has non-stationary increments that are more weakly correlated in non-overlapping intervals, and the covariance decays faster. Therefore, the sfBm is more reasonable for using in the option pricing model [12,13]. To make the market completely free of arbitrage, EI-Nouty and Zili [14] presented sub-mixed fractional Brownian motion (smfBm), which is a linear combination of Brownian motion and sub-fractional Brownian motion. Tudor [15,16] proposed that when parameter H(34,1), smfBm is "equivalent in law" to a standard Brownian motion, which means that it is a semi-martingale in that domain. Consequently, the class of regular portfolios is arbitrage-free (i.e., suitable for option pricing). As shown in [17], neither is there arbitrage for any value of H(0,1) if a suitable portfolio is adopted. Moreover, there are some studies on pricing models based on the smfBm. For example, Xu and Zhou [18] studied the pricing problem of perpetual American put options in sub-mixed fractional Brownian motion. They obtained the pricing formula by using partial differential equations. Araneda and Bertschinger [19] established the constant elasticity of variance model driven by sub-mixed fractional Brownian motion. They obtained the relevant Fokker-Planck equations and the prices of the European call options according to the M-Whittaker function and non-central chi square distribution function. Specifically, many scholars have incorporated the stochastic volatility model into the problems of option pricing for research and numerical analysis [20,21,22,23,24,25].

    However, all the above studies assumed that the short interest rate is constant. This is not consistent with reality. Therefore, many scholars incorporated stochastic interest rates into the option pricing models. Merton [26] proposed a stochastic interest rate model based on the BS model. Guo [27] established the subdiffusive Merton short rate model and obtained the pricing formula and the call-put parity relationship for European options. Liu and Li [28] studied the Merton credit risk pricing model by using sub-fractional as a random driving source, which can describe the characteristic of correlations and modify the classical credit risk structure model. The numerical calculation results show that the stochastic interest rate for the probability of default, values of bonds and equity and credit spreads has a certain influence. Based on these, in this paper, we incorporate sub-mixed fractional Brownian motion and the stochastic short rate into the equity warrants pricing model. We will establish an equity warrant pricing model under the sub-mixed fractional Brownian motion regime with the interest rate following the Merton short rate model.

    The rest of the paper proceeds as follows. In Section 2, we briefly introduce the background of sub-mixed fractional Brownian motion. In Section 3, we give the formula for the pricing of a zero-coupon bond. In Section 4, the pricing formula for equity warrants is derived. In Section 5 and Section 6, we provide the numerical results and present an empirical analysis of this model.

    Many models depict changes in the short rate, and the Merton short rate model is one of the most classical stochastic short rate models. An accurate grasp of changes in the short rate can effectively avoid financial risks. An increasing number of people bring long-range correlations into pricing models, and the sub-mixed fractional Brownian motion not only satisfies this property but is also more suitable for the research of financial market modelling. First, we introduce the background of the smfBm, which involves [14,19].

    Definition 2.1. {MHt(β,γ),t0}=βB(t)+γξH(t),β0,γ0 is a sub-mixed fractional Brownian motion, where B(t) is a Brownian motion, and ξH(t) is a sub-fractional Brownian motion. Then we have

    E(MHt(β,γ)MHs(β,γ))=β2min(s,t)+γ2{s2H+t2H12[(s+t)2H+|ts|2H]},

    while β=0 and γ=1 , MHt(β,γ) is a sfBm; and while β=1 and γ=0 or while β=0 , γ=1 and H=12 , MHt(β,γ) is a Bm.

    Now, we list some properties of the smfBm MHt in the following remarks.

    Remark 2.1. For h>0 , MHht(β,γ)MHt(βh12,γhH)}, 

    where means "to have the same law".

    Remark 2.2. For 12<H<1 , MHt(β,γ) has the property of long-range correlations.

    Remark 2.3. msfBm has non-stationary increments for any 0s<t

    E[(MHt(β,γ)MHs(β,γ))2]=β2(ts)+γ2[22H1(t2H+s2H)+(s+t)2H+(ts)2H],

    then

    β2(ts) + γ2a(ts)2HE[(MHt(β,γ)MHs(β,γ))2]β2(ts) + γ2b(ts)2H,

    where

    a={1,0<H12,222H1,12<H<1.
    b={222H1,0<H<12,1,12H<1.

    Remark 2.4. For 0u<vs<t , the covariance over non-overlapping increments is given by

    E[(MHv(β,γ)MHu(β,γ))(MHt(β,γ)MHs(β,γ))]=γ22[(t+u)2H+(tu)2H+(s+v)2H+(sv)2H(t+v)2H(tv)2H(s+u)2H(su)2H],

    where

    {E[(MHv(β,γ)MHu(β,γ))(MHt(β,γ)MHs(β,γ))]>0,12<H<1,E[(MHv(β,γ)MHu(β,γ))(MHt(β,γ)MHs(β,γ))]<0,0<H<12.

    In this section, we incorporate the long-range correlations of the short rate into our pricing model under the condition of β=γ=1 and calculate the price of a zero-coupon bond when the stochastic interest rate follows the sub-mixed fractional Merton process.

    The Merton process is a widely used stochastic interest rate model combined with sub-mixed fractional Brownian motion. In the following sections, we will state some basic assumptions that will be used in this paper.

    Assumption 3.1. Based on the risk neutral probability measure, we provide some ideal conditions for the market of corporate value and equity warrants:

    (i) There are no transaction costs, margins or taxes;

    (ii) Dividends are not paid during the time of the outstanding equity warrants;

    (iii) The value Vt of the firm consists of N shares of stock at price St and M warrants outstanding at price ct ; thus, we have

    Vt=NSt+Mct.

    (iv) We assume that the short rate rt is given by

    drt=μrdt+σr1dBr1(t)+σr2dξHr2(t), (3.1)

    and the value of firm Vt , in which Vt follows

    dVt=μVVtdt+σV1VtdBV1(t)+σV2VtdξHV2(t), (3.2)

    where μr, σr1, σr2, μV, σV1 and σV2 are constants, Br1(t), ξHr2(t), BV1(t) and ξHV2(t) are independent Brownian motions.

    In this section, P(r,t;T) is the price of a zero-coupon bond with maturity T at time t[0,T]. Then, we obtain the pricing formula for a zero-coupon bond by the following theorem.

    Theorem 3.1. In the sub-mixed fractional Merton model, the price of a zero-coupon bond with maturity T at time t[0,T] is given by

    P(r,t;T)=erA2(τ)+A1(τ).

    where

    {A1(τ)=12σ2r1τ0s2ds+H(222H1)σ2r2τ0(Ts)2H1s2dsμrτ0sds, A2(τ)=τ.

    Proof. Here, P(r,T;T)=1, that is, the zero-coupon bond P(r,t;T) will pay for 1 dollar at expiration date T. Using Lemma 2.1 and Theorem 2.1 in [19], we can obtain

    {Pt + μrPr+12σ2r12Pr2+Ht2H1(222H1)σ2r22Pr2rP=0,P(r,T;T)=1. (3.3)

    Denoting τ = Tt, P(r,t;T)=eA1(τ)rA2(τ), it is easy to calculate

    {Pt=P(A1(τ)τ+rA2(τ)τ),Pr=PA2(τ),2Pr2=P(A2(τ))2. (3.4)

    Substituting Eq (3.4) into Eq (3.3), we obtain

    {A1(τ)τ=μrA2(τ)+12σ2r1(A2(τ))2+Ht2H1(222H1)σ2r2(A2(τ))2,A2(τ)τ=1. (3.5)

    From Eq (3.5), we can obtain

    {A1(τ)=12σ2r1τ0s2ds+H(222H1)σ2r2τ0(Ts)2H1s2dsμrτ0sds,A2(τ)=τ. (3.6)

    Then, the pricing formula for the zero-coupon bond can be given by

    P(r,t;T)=erτ+A1(τ). (3.7)

    In this section, let K be the exercise price, T be the expiration date of the equity warrants and c=c(V,r,t) be the price of equity warrants.

    Theorem 4.1. When rt satisfies Eq (3.1) and Vt satisfies Eq (3.2), c(V,r,t) satisfies the following BS equation and the boundary condition

    {ct+˜σ2V(t)V22cV2+˜σ2r(t)2cr2+rVcV+μrcrrc=0,cT=1N+Mk(kVTNX)+, (4.1)

    where

    {˜σ2V(t)=12σ2V1+Ht2H1(222H1)σ2V2,˜σ2r(t)=12σ2r1+Ht2H1(222H1)σ2r2.

    Proof. Considering a portfolio consisting of c(V,r,t), Δ1t units of stock and Δ2tunits of zero-coupon bond, we obtain the price of the portfolio at time t.

    Πt=ctΔ1tVtΔ2tPt,
    dΠt=dctΔ1tdVtΔ2tdPt=(ct+12σ2V1V22cV2+Ht2H1(222H1)σ2V2V22cV2)dt+(12σ2r12cr2+Ht2H1(222H1)σ2r22cr2)dt+(cVΔ1t)dV+(crΔ2tPr)drΔ2t(Pt+12σ2r12Pr2+Ht2H1(222H1)σ2r22Pr2)dt. (4.2)

    Assuming

    Δ1t=cV,Δ2t=c/rP/r,

    as

    E(dΠt)=r(t)Πdt=r(dctΔ1tdVtΔ2tdPt),

    from Eq (4.2), we have

    ct+12σ2V1V22cV2+Ht2H1(222H1)σ2V2V22cV2+12σ2r12cr2+Ht2H1(222H1)σ2r22cr2+rVcV+μrcrrc=0. (4.3)

    Denoting

    {˜σ2V(t)=12σ2V1+Ht2H1(222H1)σ2V2,˜σ2r(t)=12σ2r1+Ht2H1(222H1)σ2r2.

    Then

    ct+˜σ2V(t)V22cV2+˜σ2r(t)2cr2+rVcV+μrcrrc=0,

    with the boundary condition

    cT=1N+Mk(kVTNX)+.

    Proof is completed.

    Solving the partial differential Eq (4.1), we obtain:

    Theorem 4.2. When rt satisfies Eq (3.1) and Vt satisfies Eq (3.2), we have the pricing formula for equity warrants c(V,r,t) with expiration date T , strike price X , shares of stock N , exercise ratio k and shares of warrants outstanding M , which are

    ct(Vt,T,t;X,σ,r,k,N,M,H)=1N+Mk[kVtΦ(d1)NXP(r,t;T)Φ(d2))], (4.4)

    where

    d1=lnkVtNXlnP(r,t;T)+(12σ2V1(Tt)+(222H1)2σ2V2(T2Ht2H))+Tt(12σ2r1+Hs2H1(222H1)σ2r2)(Ts)2ds(σ2V1(Tt)+(222H1)σ2V2(T2Ht2H))+Tt(σ2r1+2Hs2H1(222H1)σ2r2)(Ts)2ds,d2=d1(σ2V1(Tt)+(222H1)σ2V2(T2Ht2H))+Tt(σ2r1+2Hs2H1(222H1)σ2r2)(Ts)2ds,

    and Φ() denotes the cumulative probability function for a standard normal distribution.

    Proof. Let us make the following change of variables

    {y=VP(r,t;T),ˆc(y,t)=c(V,r,t)P(r,t;T). (4.5)

    By calculating, we can obtain

    {ct=ˆcPt+PˆctyˆcyPt,cr=ˆcPryˆcyPr,cS=ˆcy,2cr2=ˆc2Pr2yˆcy2Pr2+y22ˆcy21P(Pr)2,2cS2=1P2ˆcy2. (4.6)

    Substituting Eq (4.6) into Eq (4.1), we have

    ˆct+2ˆcy2(˜σ2V(t)V21P2+˜σ2r(t)y21P2(Pr)2)1Pyˆcy(Pt+˜σ2r(t)2Pr2+μrPrrVy)+1Pˆc(Pt+˜σ2r(t)2Pr2+μrPrrP)=0. (4.7)

    By the price of zero-coupon bond P(r,t;T) satisfying Eq (3.3), we have ˆc(y,t) that satisfies

    ˆct+(˜σ2V(t)+˜σ2r(t)τ2)y22ˆcy2=0. (4.8)

    Letting x=lny, Eq (3.5) can be converted to

    ˆct+˜σ2V(t)2ˆcx2˜σ2V(t)ˆcx+˜σ2r(t)τ22ˆcx2˜σ2r(t)τ2ˆcx=0. (4.9)

    Letting

    ˆc(y,t)=u(η,λ), η=x+α(t), λ=β(t), α(T)=β(T)=0,

    then, we obtain

    {ˆct=uηα(t)+uλβ(t),ˆcx=uη,2ˆcx2=2uη2. (4.10)

    Substituting Eq (4.10) into Eq (4.9), we have

    uλβ(t)+uη[α(t)˜σ2V(t)˜σ2r(t)τ2]+2uη2[˜σ2V(t)+˜σ2r(t)τ2]=0, (4.11)

    where

    {β(t)=˜σ2V(t)˜σ2r(t)τ2,α(t)=˜σ2V(t)+˜σ2r(t)τ2.

    By calculating, we obtain

    {β(t)=Tt(˜σ2V(t)+˜σ2r(t)(Ts)2)ds,α(t)=Tt(˜σ2V(t)+˜σ2r(t)(Ts)2)ds.

    Finally, Eq (4.11) can be written as

    2uη2 = uλ, (4.12)

    with final condition

    u(η,0)=1N+Mk(keηNX)+.

    By Poisson's formula, the solution of the Cauchy problem of the heat equation is expressed as

    u(η,λ)=12πλ+1N+Mk(keθNX)+e(ηθ)24λdθ.

    Thus,

    ˆc=u(η,λ)=12πλ+lnNXk1N+Mk(keθNX)+e(ηθ)24λdθ=k2πλ+lnNXkeθe(ηθ)24λN+MkdθNX2πλ+lnNXke(ηθ)24λN+Mkdθ=I1I2.

    I2 is relatively easy to compute. We can let z2=ηθ2λ,2λdz2=dθ; then,

    I2=NX2πλ+lnNXke(ηθ)24λN+Mkdθ=NX2πλ1N+MkηlnNXk2λez222(2λ)dz2=NX2π1N+MkηlnNXk2λez222dz2=NXN+MkΦ(d2),

    where

    d2=lnkVtNXlnP(r,t;T)+β(t)2α(t)=lnkVtNXlnP(r,t;T)(12σ2V1(Tt)+(222H1)2σ2V2(T2Ht2H))Tt(12σ2r1+Hs2H1(222H1)σ2r2)(Ts)2ds(σ2V1(Tt)+(222H1)σ2V2(T2Ht2H))+Tt(σ2r1+2Hs2H1(222H1)σ2r2)(Ts)2ds.

    We calculate I1. Letting z1=ηθ+2λ2λ, 2λdz1=dθ, in the same way, we have

    I1=12πλ+lnNXkkeθN+Mke(ηθ)24λdθ=keη+λ2πλ1N+MklnNXk+η+2λ2λez122(2λ)dz1=keη+λ2πλ1N+MklnNXk+η+2λ2λez1222λdz1=kVtN+Mk1P(r,t;T)Φ(d1),

    where

    d1=lnkVtNXlnP(r,t;T)+α(t)2α(t)=lnkVtNXlnP(r,t;T)+(12σ2V1(Tt)+(222H1)2σ2V2(T2Ht2H))+Tt(12σ2r1+Hs2H1(222H1)σ2r2)(Ts)2ds(σ2V1(Tt)+(222H1)σ2V2(T2Ht2H))+Tt(σ2r1+2Hs2H1(222H1)σ2r2)(Ts)2ds.

    And our model satisfies the following nonlinear equations [29]:

    {NSt=VtMN+Mk[kVtΦ(d1)NXP(r,t;T)Φ(d2))],σS1=VtσV1StN+MkMkΦ(d1)N(N+Mk),σS2=VtσV2StN+MkMkΦ(d1)N(N+Mk).

    Proof is completed.

    In this section, we present some numerical results of our model.

    Corollary 5.1 When t=0 , the price of equity warrants is given by

    c(V0,T;X,σ,r0,k,N,M,H)=1N+Mk[kV0Φ(d1)NXP0Φ(d2)],

    where

    P0=exp(r0T+222H1(2H+1)(2H+2)σ2r2T2H+2+16σ2r1T312μrT2),
    d1=lnkV0NXlnP0+12σ2V1T+12(222H1)σ2V2T2H+16σ2r1T3+222H1(2H+1)(2H+2)σ2r2T2H+2σ2V1T+(222H1)σ2V2T2H+13σ2r1T3+2222H1(2H+1)(2H+2)σ2r2T2H+2,
    d2=d1σ2V1T+(222H1)σ2V2T2H+13σ2r1T3+2222H1(2H+1)(2H+2)σ2r2T2H+2.

    Corollary 5.2 In particular, when the interest rate is constant and t=0 , the price of equity warrants is given by

    c(V0,T;X,σ,r0,k,N,M,H)=1N+Mk[kV0Φ(d1)NXer0TΦ(d2)],

    where

    d1=lnkV0NX+r0T+12σ2V1T+12(222H1)σ2V2T2Hσ2V1T+(222H1)σ2V2T2H,
    d2=lnkV0NX+r0T12σ2V1T12(222H1)σ2V2T2Hσ2V1T+(222H1)σ2V2T2H,

    this is consistent with the result in [15].

    We give relevant numerical calculations by setting different parameter values. From Figure 1 to Figure 5, we can see that the prices of equity warrants decrease when the strike price X is larger. From Figure 2, when the strike price is fixed, the value of equity warrants decreases with the increase in the Hurst index. From Figure 3, we find that when the value of S0 is smaller, the declining trend of equity warrant prices is gentler; when the value of S0 is larger, the declining speed of the equity warrant prices is faster. From Figure 4, when the expected return rate is smaller, the prices of equity warrant also gradually decrease. From Figure 5, when the risk-free interest rate takes different values, the decline range of equity warrant prices is relatively consistent. They show that the Hurst parameter, initial prices of underlying assets, expected return rate and risk-free interest rate have different effects on the prices of equity warrants.

    Figure 1.  The equity warrant price c1 under the sub-mixed fractional Merton short rate model, according to the exercise date T and strike price X. Here, S0=30, k=1, H=0.6, M=100000000, N=200000000, μr=0.4, r0=0.06, σr1=0.35, σr2=0.36, σS1=0.37, σS2=0.38, and X[35,50].
    Figure 2.  The equity warrant price under the sub-mixed fractional Merton short rate model, according to the Hurst index H and strike price X. Here, S0=30, k=1, M=100000000, N=200000000, μr=0.4, r0=0.06, σr1=0.35, σr2=0.36, σS1=0.37, and σS2=0.38.
    Figure 3.  The equity warrant price under the sub-mixed fractional Merton short rate model, according to the stock price S0 and strike price X. Here, k=1, M=100000000, N=200000000, μr=0.4, r0=0.06, σr1=0.35, σr2=0.36, σS1=0.37, and σS2=0.38.
    Figure 4.  The equity warrant price under the sub-mixed fractional Merton short rate model, according to the expected return rate μr and strike price X. Here, S0=30, k=1, M=100000000, N=200000000, r0=0.06, σr1=0.35, σr2=0.36, σS1=0.37, and σS2=0.38.
    Figure 5.  The equity warrant price under the sub-mixed fractional Merton short rate model, according to the risk-free short rate r0 and strike price X. Here, S0=30, k=1, M=100000000, N=200000000, μr=0.4, σr1=0.35, σr2=0.36, σS1=0.37, and σS2=0.38.

    In this section, we verify the equity warrant prices under the sub-mixed fractional Merton short rate model. We derive the prices of equity warrants in the classical Merton stochastic interest rate model, the sub-fractional Merton short rate model, the BS model and the Ukhov model. Then, we compare prices of equity warrants between these models and our model.

    The Ukhov model [29] is a pricing model for equity warrants based on a new algorithm developed. It is given by

    (ⅰ) Solve (numerically) the following system of nonlinear equations for (V,σ),

    {NS=VMN+Mk(kVΦ(d1)NXer(Tt)Φ(d2)),σS=VσSN+kMkMΦ(d1)N(N+kM).

    where

    d1=ln(kVNX)+(r+12σ2)(Tt)σTt,
    d2=d1σTt.

    (ⅱ) The warrant price is obtained as

    c=VNSM.

    The pricing formula is based on observable variables and is used to calculate the value of equity warrants.

    From Table 1, when T1, the difference in price between the BS model, the Ukhov model and our model is smaller. We find that the difference in price between the Merton model, the sub-fractional Merton model and our model is relatively small. When the expiration date is smaller, the difference in value between the BS model and our model is larger.

    Table 1.  Equity warrant prices with respect to different values of S0=25, k=1, M=100000000, N=200000000, μr=0.4, σr1=0.35, σr2=0.36, σS1=0.37, σS2=0.38, and X=20.
    T 0.6 0.7 0.8 0.9 1
    Our price 5.2492 5.6374 6.0306 6.4265 6.8231
    cOPcBS -1.0813 -0.9166 -0.7392 -0.5518 -0.3571
    cOPcMerton 0.3059 0.3170 0.3160 0.3035 0.2804
    cOPcsfBmMerton 0.3989 0.4023 0.3900 0.3638 0.3252
    cOPcUkhov -0.7896 -0.5581 -0.3490 -0.1337 0.0859

     | Show Table
    DownLoad: CSV
    Table 2.  Basic information of three types of equity warrants.
    Names of equity warrants Stock prices Issued stocks Issued warrants Exercise price Exercise ratio Duration (year)
    Yunhua 22.62 536400000 540000000 18.23 1 2
    Shouchuang 4.75 2200000000 60000000 4.55 1 1
    Magang 3.48 6455300000 1265000000 3.40 1 2

     | Show Table
    DownLoad: CSV

    We take three types of equity warrants as research objects for an empirical study. As of May 22, 2008, the selected data are from the GTA Research Service Centre of China.

    We set the value of the one-year risk-free rate r1=0.02 and the two-year risk-free rate r2=0.04. To obtain the historical volatility of equity warrants, we calculate it from the closing price of each day. The logarithmic return rate μi is computed by using data of the closing price of day Si and yesterday's closing price Si1, s is a standard deviation of the logarithmic return rate, and σ is given by

    σ=sn,

    where

    s=1n1ni=1(μiˉμ)2,
    μi=lnSiSi1,i=1,2,,n,
    ˉμ=ni=1μi.

    Then, we use the R/S method to estimate the value of the Hurst parameter. The logarithmic return series is equally divided into A subsets, with the length n=N/A of each subset. The mean of each subset is equal to ea(a=1,2,,A), and Xk,a is the cumulative deviation of the first K points relative to the mean value ea of this subset. According to the fluctuation range Ra and standard deviation Sa of the logarithmic return series in each subset A, we have the rescaled range (RS)n. Thus, the formula of parameter H is given

    lg(RS)n=Hlgn+lgC,

    where

    (RS)n=1AAa=1RaSa,
    Ra=max(Xk,a)min(Xk,a),1kn,
    Xk,a=ki=1(Ni,aea),k=1,2,,n.

    Finally, we obtain the values of volatility of underlying assets of three equity warrants as 0.44, 0.31 and 0.36, respectively, and the values of the Hurst index as 0.64, 0.66 and 0.61, respectively.

    From Table 3, we can see that the MSE (mean square error) of the BS model is the largest, indicating that the simulated value is quite different from the real price. This is because the long-range correlations of underlying assets, the stochastic interest rate and other factors are not considered in the BS model. Although the price of the Merton model is closer to the market price than that of the Ukhov model, it is still not fully considered. The result of the sub-fractional Merton model is the best among the four models compared (i.e., the lowest MSE), and the price of this model is the closest to that of our model. This indicates that the long-range correlations of underlying assets have a certain impact on the option price, which is relatively consistent with the characteristic of the actual financial market. Moreover, it is also found by comparing the sfBm-Merton price and Merton price. Therefore, through comprehensive comparison, we find that the price of our model is closest to the market price.

    Table 3.  Our model is compared with the BS model, Merton model, sfBm-Merton model and Ukhov model.
    Market price Our price BS price Merton price sfBm-Merton price Ukhov price
    9.3430 9.1082 11.9713 8.0543 9.2732 7.2779
    1.0130 1.3280 1.2566 1.2651 1.2703 1.2232
    1.1330 1.3306 0.8490 1.1717 1.5881 0.7099
    MSE 0.0645 2.3493 0.5753 0.0927 1.4959

     | Show Table
    DownLoad: CSV

    Option pricing models typically choose geometric Brownian motion or fractional Brownian motion as random driving sources. In this paper, sub-mixed fractional Brownian motion is selected as the random driving source, and the Merton random interest rate is incorporated into the pricing problem of equity warrants. We derive the explicit pricing formula for equity warrants. In the numerical calculation, we discuss the influence of multiple factors on the model results and compare our model with other classical models. The disadvantage is that the Merton model may result in a negative interest rate. In subsequent studies, the CIR model, Hull-White model and other more complex stochastic interest rate models can be considered, or stochastic volatility can be added to expand to a more general process.

    This work was supported by the Natural Science Foundation of Anhui Province (No.1908085QA29).

    The authors declare that they have no conflicts of interest to this work.



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