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Mitigating geographical basis risk of weather derivatives using spatial-temporal regime-switching temperature model

  • In this paper, geographical basis risk in weather derivative design and pricing is mitigated by using spatial-temporal pricing models. A two-state regime-switching temperature model is constructed and extended to multi-dimensional locations that are highly correlated in temperature. The "normal" and "shifted" regime of this model are characterized by a heteroscedastic Ornstein-Uhlenbeck process and a Brownian motion with mean different from zero respectively. The correlation between the driving noise in each regime is assumed to be a function of the space between the locations and increases with decreasing space. A weight is assigned to each location in the temperature basket. However, a location with a higher risk is assigned a larger weight and vice versa. The weightings in the temperature basket gave considerable importance to farming locations having greater exposure to temperature risk. The further the farming location from the weather station, the larger the weight. With this spatial-temporal weather derivatives pricing model, the holder of a weather derivative contract will have the opportunity to select the most appropriate composite of weather stations with their desired weight that can reduce geographical basis risks.

    Citation: Samuel Asante Gyamerah, Philip Ngare, Dennis Ikpe. Mitigating geographical basis risk of weather derivatives using spatial-temporal regime-switching temperature model[J]. AIMS Mathematics, 2019, 4(4): 1274-1290. doi: 10.3934/math.2019.4.1274

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  • In this paper, geographical basis risk in weather derivative design and pricing is mitigated by using spatial-temporal pricing models. A two-state regime-switching temperature model is constructed and extended to multi-dimensional locations that are highly correlated in temperature. The "normal" and "shifted" regime of this model are characterized by a heteroscedastic Ornstein-Uhlenbeck process and a Brownian motion with mean different from zero respectively. The correlation between the driving noise in each regime is assumed to be a function of the space between the locations and increases with decreasing space. A weight is assigned to each location in the temperature basket. However, a location with a higher risk is assigned a larger weight and vice versa. The weightings in the temperature basket gave considerable importance to farming locations having greater exposure to temperature risk. The further the farming location from the weather station, the larger the weight. With this spatial-temporal weather derivatives pricing model, the holder of a weather derivative contract will have the opportunity to select the most appropriate composite of weather stations with their desired weight that can reduce geographical basis risks.


    Agriculture is the main source of livelihood in Africa [1]. However, extreme changes in weather patterns, unpredictable temperature changes, frequent heat wave, and increasing temperature as a result of climate change make agriculture look like a costly gamble in Africa. The report of the Intergovernmental Panel on Climate Change (IPCC) 2007 [2] gives a comprehensive evaluation of the impacts of climate change on agriculture in Africa. As stated by the IPCC report, the estimated prediction of agriculture losses by 2100 is between 2% to 7% of gross domestic product (GDP) in parts of the Sahara. The report revealed that Northern and Southern Africa are anticipated to record GDP losses of between 0.4-1.3%, and between 2-4% for the Western and Central Africa. According to [3], Africa is extremely affected by climate change from two causes: a limited social, economic, and human abilities needed to adjust to the impact of climate change, and its geographical features of having a predominantly vast land lying across the warming tropics. From planting to harvest, extreme changes in weather can severely affect the quality and the complete production levels of crop yields.

    The effects of weather do differ considerably in the agricultural supply and demand chain. Most farmers in Africa have used traditional ways to improve the negative effect of extreme weather conditions on their farmlands. However, most of these farmlands are in the same geographical locations and as a result crop losses are correlated across farmers due to the covariant nature of weather risks. This implies that farmers in the same geographical locations are vulnerable by the same weather event and are probably going to endure extensive losses concurrently. Covariant risk controls the success of traditional risk management techniques of smallholder farmers. Consequently, there is the need for a suitable and efficient risk management tool for farmers to control weather extremes and uncertainties. An emerging shift has been the success of a weather risk management tool-weather derivative, which is use to reduce the financial effects of weather extremes and uncertainties. The uptake of this tool has been lower than expected in the agricultural sector [4] due to basis risks. As defined by [5], "Basis risk arises when the production pattern of the individual operation is not perfectly correlated with the agammaegated pattern of the area for which the derivative has been designed". Product-design and geographical basis risk are forms of basis risks. Product-design basis risks can easily be mitigated if the appropriate weather variable is used as the underlying index for designing the weather derivative. Geographical basis risk is difficult to mitigate especially in most developing countries due to the unavailability of weather stations at most farming locations under interest. For this reason, the need to develop spatial-temporal mathematical model that considers different farming locations and assigning weights to weather stations relative to the distance from the reference farming locations. This model is also beneficial to farmers with farmlands in the same geographical locations.

    Unlike traditional agricultural insurance that is used to hedge against risks from idiosyncratic occurrences, weather derivatives allow agricultural stakeholders (farmers, input suppliers and other stakeholders at the farm level) to hedge against covariant risks. Weather derivative is seen as an efficient tool for mitigating risk that affects most farmers, input suppliers and other stakeholders at the farm level. In a survey report conducted in 2008-2009 and prepared for the weather risk management association, the agricultural sector contributed about 11%* of the total weather derivatives purchase in the weather market. Unlike traditional insurance, the payoff of a weather derivative depends on an index (specially designed measure) that is linked to the risk being hedged against.

    *the second largest percentage after the energy sector

    The price of a weather derivative is usually dependent on different weather indices (heating degree days (HDD), cooling degree days (CDD), Pacific Rim (PRIM), cumulative average temperature (CAT), growing degree days (GDD)) that help in pricing weather derivatives. Different authors [6,7,8] have used HDD and CDD indices as the major indices for pricing weather derivatives in the energy industry. Similar to the CDD and HDD indices in the energy sector, the GDD and CAT indices are powerful indices that can be use to price weather derivatives for the agricultural sector in Africa. For this reason, CAT and GDD are used as the major indices for the temperature based weather derivative pricing. GDD measures the growth and development of crops, weeds, and insects during a growing season.

    The contributions made in this study are: (1) Motivated by [9], we develop a temperature dynamics model for spatial-temporal locations in Ghana. This model captures the stylized facts of temperature at different locations. (2) We develop an analytical weather derivative pricing model for basket futures written on CAT and GDD indices. With the proposed basket futures pricing model, it will be cost efficient and pragmatic for farmers to buy weather derivatives contracts for different but correlated farming locations than a single farming location. Geographical basis risk will also be reduced when using this spatial-temporal pricing model.

    To the best our knowledge, the proposed analytical weather derivatives basket futures pricing formulas using multi-dimensional regime-switching model is the first of its kind in literature.

    Assume DB represent the random payoff at expiry for the owner of a futures contract. At time tt1<t2 for a measurement period [t1,t2], the holder of the contract enters into the contract. Let F(t,t1,t2) represent the price against receiving the random payment DB at time t2. For a constant continuously compounded interest rate r>0 and a risk-neutral probability measure Q, the arbitrage-free future price for a measurement period [t1,t2] on the CAT and GDD can be define as Ft-adapted stochastic process satisfying

    0=er(t2t)EQ[DBF(t,t1,t2)|Ft] (2.1)

    Assume that the futures price F(t,t1,t2) is Ft adapted, then the futures price is define as

    F(t,t1,t2)=EQ[DB|Ft] (2.2)

    where t,t1,t2 are the current, starting and maturity time of the futures contract respectively and Ft is σ-algebra up to a specified time t. From equation 2.2, it is important to calculate the risk-neutral measure Q (also referred to as equivalent martingale measure) in order to determine futures prices.

    To derive an explicit formula for the future price, we specify Q to help in calculating the expectation. Following the analysis of [11], we use the Girsanov theorem to find a sub-family of probability measures for the normal and shifted regimes. By using the option pricing technique under independent regime-switching model of [12], the CAT and GDD futures are priced by splitting the futures price into a normal and shifted price component. The two pricing component are joined up using the idea of weighted mixture of probability in each regime from t1 to t2.

    Suppose that for a contract period [t1,t2], the temperature dynamics follow the temperature model in Lemma 3.1. Then, there is a price dynamic of futures written on a CAT index with tt1<t2. From equation 2.1, the futures price of CAT is

    0=er(t2t)EQ[t2t1TxdxFCAT(t,t1,t2)Ft]. (2.3)

    Since the futures price F(t,t1,t2) is Ft adapted under the measure Q, FCAT is Ft-adapted. We can therefore define the CAT futures price FCAT(t,t1,t2) for a weather derivative contract as

    FCAT(t,t1,t2)=EQ[t2t1TxdxFt] (2.4)

    Similar to the definition of the CAT futures price, the GDD futures price is given as

    0=er(t2t)EQ[t2t1max(TxK,0)dxFGDD(t,t1,t2)|Ft] (2.5)

    Using the same idea in deriving the CAT futures price, the price of the GDD futures can be derived as

    FGDD(t,t1,t2)=EQ[t2t1max(TxK,0)dx|Ft]. (2.6)

    Where K is the optimal normal temperature at which a crop will develop. The rate of development of most plants depends on the daily air temperature [13].

    Because the market price of temperature risk remains unchanged for all derivatives that depends on temperature, we use the same risk-neutral measure Q used in pricing the CAT futures to price the GDD futures.

    To find a mathematical expression for the futures price of the chosen indices, an arbitrage-free and explicit dynamics for future price of the indices are constructed. The real-world measure P is changed to a risk-neutral measure Q, in a way that the discounted price process of the underlying is a martingale under Q. To transform the P to Q, the Girsanov theorem is employed. The Girsanov theorem provides techniques for transforming P to Q under the setting of a Brownian motion, where Q is a second probability measure.

    Theorem 2.1 (Girsanov Theorem). Let Wt be a Brownian motion on a probability space (Ω,F,P) and λ={λt:0tT} is an adaptive process satisfying the Novikov condition

    E[exp(12t0λ2udu)]<. (2.7)
    LetZ(t)=exp(t0λudWu12t0λ2udu), (2.8)

    then QP can be determined by the Radon-Nikodym derivative

    dQdPFt=Z(t), (2.9)

    Then we can define the random process

    andVt=Wtt0λsds. (2.10)

    Equivalently,

    dVt=dWtλtdt (2.11)

    The process Vt is a Brownian motion under the measure Qλ

    Proof. See [14] for the proof of this theorem.

    Let B(t)=(B1(t),B2(t),B3(t),,BN(t)) be an N-dimensional Brownian motion on a probability space (Ω,F,P) and λ=(λ1(t),λ2(t),λ3(t),,λN(t)) be an N-dimensional adapted process on [0,T].

    Define

    Zλ(t):=exp(t0λ(s)dB(s)12t0∣∣λ(s)2ds), (2.12)

    where λ(s)2=Ni=1λi(s)2.

    Let

    ˜B(t)=B(t)+t0λ(s)ds (2.13)

    and suppose that

    Et0∣∣λ(s)2Z(s)2ds<,

    then ˜B(t) is a N-dimensional standard Brownian motion under the measure Q defined as

    dQdP|Ft=Z(T) (2.14)

    Observe that for each j,

    ˜Bj(t)=Bj(t)+t0λj(s)ds (2.15)

    The component process of ˜B(t) are independent under the measure Q.

    Remark 1.The Novikov condition in the Girsanov theorem makes sure Z is positive martingale and whenever E(Z)=1. This is referred to as the Radon-Nikodym derivative.

    Remark 2. λ is referred to as the market price of temperature risk (MPR). Since there is no real weather derivative market in Africa from which the prices can be obtained, λ is assumed to be a constant. For a constant λ, equation 2.11 can be redefined as

    dVt=dWtλdt (2.16)

    Different temperature models have been proposed to capture the dynamics of temperature [6,8,9,10,15].. The usual assumptions in these models are: volatility of temperature is lower in summer than in winter, temperature is autoregressive, temperature follows a predicted pattern and it goes around a seasonal mean. Early models used autoregressive moving average (ARMA) processes, autoregressive process of order one (AR(1)) processes, mean reverting stochastic differential equations (SDE) [9,15,16]. All these models assumed no changes in the state of the dynamics of temperature. That is, they used single-regime model to describe the dynamics of temperature. However, temperature can go through different latent states in a particular period of time and a single SDE can not accurately capture all this states. More complex models have been proposed in recent literatures, an example is the model of [7,17,18], which uses a two-state Markov regime-switching model. [17] extended the model of [7] by replacing the constant volatility in the base regime with heteroscedastic volatility. This was necessary because volatility of temperature changes at different states. [18] further extended this model by replacing the Brownian process in the shifted regime with a Lévy process. However, none of these authors proposed a spatial-temporal pricing model for weather derivatives. Motivated by [7,17,18], a regime-switching temperature dynamics model is proposed and later extended to a multi-dimensional model. The switching dynamics between the regimes are assumed to be controlled by an unobservable latent variable Rt. The model is governed by a two-state regime-switching model Rt={1,2} in which a two-state Markov chain controls the characterization of the probability law of switching between Rt=1 and Rt=2 with transition probabilities

    pik=Pr(Rt=kRt1=i)i,k=1,2
    0pik1and2k=1pik=1

    The daily average temperature on day t, Tt is modelled as the sum of a deseasonalized temperature ˜Tt and a deterministic seasonal component St,

    Tt=˜Tt+St

    The deterministic seasonality component at time t, St is given by

    St=a1sin(2π365(tφ))+a2t+a3

    where a1,a2,a3 and φ are constants.

    The proposed model is distinctly appropriate to capture the dynamics of temperature through time. The proposed daily temperature model is given as

    Tt={Tt,1:dTt,1=dSt,1+β(Tt,1St,1)dt+σ1Tt,1dWt,if Tt is in the normal regime,Tt,2:dTt,2=μdt+σ2dWt, if Tt is in the shifted regime, (3.1)

    where σ1Tt,1 is the daily local volatility of the normal regime through time, σ2 is the volatility of the shifted regime, and β is the mean-reversion rate of the daily temperature in the normal regime which reverses to the long term equilibrium level after the daily temperature has drifted from its equilibrium. The probabilities for the process to be in the normal and shifted regimes are p1 and p2 respectively and p1+p2=1. WtN(0,t) is the standard Brownian motion. Tt(T(t)) is the daily temperature at time t. The regimes are assumed to be independent to each other and the futures contract is calculated for each regime model. The final futures price is calculated using the weighted sum of the individual regimes.

    Lemma 3.1. If the daily average temperature Tt,1 follows the proposed model 3.1, then the explicit solution is given by

    T(t)={Tt,1:Tt,1=St,1+(T0,1S0,1)eβt+t0σTueβ(ts)dWsTt,2:Tt,2=T0,2+μt+t0σ2dWs (3.2)

    Proof. For the normal regime,

    dTt=dSt+β(TtSt)dt+σTtdBt
    d˜Tt=β˜Tt+σTtdBt, (3.3)

    where ˜Tt,1=Tt,1St,1. Using the transformation below, d˜Tt,1 will be evaluated,

    F[˜Tt,1,t]=˜Tt,1eβt
    F˜Tt,1=eβt;2F˜T2t,1=0;Ft=β˜Tteβt

    By Itô's Lemma and from equation (3.3),

    dFt,1=σTt,1eβtdWt (3.4)

    Integrating equation (3.4) over the interval [0,t],

    Ft,1=F0,1+t0σTs,1eβsdWs˜Tteβt=˜T0,1+t0σTs,1eβsdWs˜Tt=˜T0,1eβt+t0σTueβ(ts)dWsTt=St,1+(T0,1S0,1)eβt+t0σTs,1eβ(ts)dWs

    For the shifted regime

    dTt,2=μdt+σ2dWtt0dTt,2=t0μds+t0σ2dWsTt,2=T0,2+μt+t0σ2dWs

    Let N be the spatial locations in the basket, (ωi)Ni=1 be the collection of weights for spatial locations (yi)Ni=1. At time t, the basket of the deseasonalized average temperature at the N spatial locations is given as

    D(t):=Ni=1ωiTit (3.5)

    Where Ni=1ωi=1.

    Assume temperature is spatially correlated across the random noise term. To allow analytical pricing of the basket temperature derivatives contract, assume the risk-neutral distribution of temperature for each location is normally distributed in the temperature model. That is, the basket been a weighted sum of normally distributed temperature is also normally distributed. Consequently, we are able to outwit the principal difficulty associated with pricing basket options of assets when determining the distribution of the sum or average of the underlying assets. From these settings, a spatial-temporal temperature model at each spatial location yi is proposed,

    Tit={Tit,1:dTit,1=dSit,1+βi(Tit,1Sit,1)dt+σi1Tit,1dWit,Tit,2:dTit,2=μidt+σi2dWit (3.6)

    Model 3.6 can be expressed for locations i=1,2,,N as an N-dimensional system,

    Tt={Tt,1:dTt,1=dSt,1+β(Tt,1St,1)dt+σ1Tt,1dWt,Tt,2:dTt,2=μdt+σ2dWt (3.7)

    where WtN(0,Ωt). From the property of linear transformation of multivariate normal distribution,

    YN(μ,Σ)XYN(Xμ,XΣXT)

    Suppose ZN(0,It) and Y=XZ, then it follows that YN(0,XXTt). By applying Cholesky factorization to Σ, a lower triangular form for X is derived. Using this theory, Wt can be expressed as an N-dimensional Brownian motion Bt,

    Wt=LBt, (3.8)

    LLT=Ω, L is a lower triangular matrix with non-negative diagonal entries, LT is an upper traingular matrix, and Bt=(B1t,B2t,B3t,,BNt)T with dBitdBjt=δijdt. From equation 3.8, equation 3.7 can be reformulated as

    Tt={Tt,1:dTt,1=dSt,1+β(Tt,1St,1)dt+σ1Tt,1LdBt,Tt,2:dTt,2=μdt+σ2LdBt (3.9)

    Equation 2.8 can be transformed for the normal and shifted regime,

    Zλt={exp(t0(σ1Ts,1L)1λsdBs12t0∣∣σ1Ts,1L2∣∣λs2ds)exp(t0(σ2L)1λ(s)dBs12t0∣∣σ2L2∣∣λ(s)2ds) (3.10)

    From equation 3.10, and assuming λ is a constant for each reference measurement station, it can be inferred that;

    Vλt={Btt0(σ1Ts,1L)1λdsBtt0(σ2L)1λds (3.11)

    Equivalently

    dVλt={dBt(σ1Tt,1L)1λdtdBt(σ2L)1λdt (3.12)

    Where Vλt is a Brownian motion under the measure Qλ

    Consequently, the TML model under the equivalent martingale measure Qλ is

    {dTt,1=dSt,1+(λ+β(Tt,1St,1))dt+σ1Tt,1LdVλ(t),dTt,2=(μ+λ)dt+σ2LdVλ(t), (3.13)

    Lemma 3.2. For a spatial location i, if the dynamics of the daily average temperature follows equation 3.13, then the explicit solution for the ith location yi is given as

    {Tit,1=Sit,1+(Ti0,1Si0,1)eβit+(λβ)i(eβit1)+t0σi1Tis,1eβi(ts)ij=1LijdVjλ(s),Tit,2=Ti0,2+(μ+λ)it+t0σi2ij=1LijdVjλ(s) (3.14)

    Proof. From the normal regime of model 3.13,

    dTt,1=dSt,1+(λ+β(Tt,1St,1))dt+σ1Tt,1LdVλ(t),
    d˜Tt,1=β˜Tt,1+λdt+σ1Tt,1LdVλ(t), (3.15)

    where ˜Tt,1=Tt,1St,1. d˜Tt,1 will be evaluated using the transformation in equation 3.16,

    F[˜Tt,1,t]=˜Tt,1eβt (3.16)

    By Itô's Lemma and from equation (3.15),

    dF=λeβtdt+σ1Tt,1eβtLdVt (3.17)

    Integrating equation (3.17) over the interval [0,t] gives

    Tt,1=St,1+(T0,1S0,1)eβt+λβ(eβt1)+t0σ1Ts,1eβ(ts)LdVs

    At location yi,

    Tit,1=Sit,1+(Ti0,1Si0,1)eβit+(λβ)i(eβit1)+t0σi1Tis,1eβi(ts)ij=1LijdVjλ(s)

    From the shifted regime of model 3.13,

    dTt,2=μdt+λdt+σ2LdBλ(t)Tt,2=T0,2+(μ+λ)t+t0σ2LdVλ(s)

    At location yi,

    Tt,2=Ti0,2+(μ+λ)it+t0σi2ij=1LijdVjλ(s),

    hence the lemma.

    The CAT and GDD futures will be priced by splitting the futures price into normal and shifted price components and added up with probabilities in each regime for the contract period.

    F(t,t1,t2)=Pr(R[t1,t2]=N)FN(t,t1,t2)+Pr(R[t1,t2]=S)FS(t,t1,t2) (4.1)

    Where FN(t,t1,t2) and FS(t,t1,t2) are the futures price of the normal and shifted regimes respectively. Pr(R[t1,t2]=N) and Pr(R[t1,t2]=S) are the probability of the observed daily average temperature data under the normal and shifted regimes throughout the contract period [t1,t2]. The splitting is possible since it is assumed that the futures price under the normal regime is independent of the futures price under the shifted regime.

    By the same reasoning as in deriving the futures price of a single CAT, the futures price of a basket CAT is given by

    FCAT(t,t1,t2;D)=EQ[Ni=1ωi(t2t1Tixdx)Ft] (4.2)

    Definition 4.1. At a spatial location yi and a specificied contract period, tt1<t2, the GDD futures price is define as

    GDD(t1,t2):=t2t1max{D(t)K,0}dt=t2t1max{Ni=1ωiTitK,0}dt (4.3)

    Analogously, the futures price of a basket GDD is defined as

    FGDD(t,t1,t2;D)=EQ(t2t1max{Ni=1ωiTixK,0}dx|Ft)=t2t1EQ(max{Ni=1ωiTixK,0}|Ft)dx (4.4)

    Proposition 4.2. At a spatial location yi, the futures contract price on basket of CAT index following the normal regime in equation 3.6 is calculated as

    FNCAT(t,t1,t2;D)=Ni=1ωi[t2t1Six,1dx+t2t1(Tit,1Sit,1)eβi(xt)dx+t2t1(λβ)i(eβi(xt)1)dx]

    Proof. For xt in Lemma 3.2,

    Tix,1=Six,1+(Tit,1Sit,1)eβi(xt)+(λβ)i(eβi(xt)1)+xtσi1Tis,1eβi(xs)ij=1LijdVjλ(s) (4.5)
    EQ[t2t1Tix,1dxFt]=EQ[t2t1(Six,1+(Tit,1Sit,1)eβi(xt)+(λβ)i(eβi(xt)1)+xtσi1Tis,1eβi(xs)ij=1LijdVjλ(s))dx|Ft]=t2t1Six,1dx+t2t1(Tit,1Sit,1)eβi(xt)dx+t2t1(λβ)i(eβi(xt)1)dx
    FNCAT(t,t1,t2;D)=Ni=1ωiEQ[t2t1Tix,1dxFt]=Ni=1ωi[t2t1Six,1dx+t2t1(Tit,1Sit,1)eβi(xt)dx+t2t1(λβ)i(eβi(xt)1)dx]

    Proposition 4.3. For a specificied contract period, tt1<t2 at spatial location yi, the futures contract price on basket of CAT index following the shifted regime in equation 3.6 is

    FSCAT(t,t1,t2;D)=Ni=1ωi[Tit,2(t2t1)+12(μ+λ)i((t2t)2(t1t)2)] (4.6)

    Proof. We first integrate the shifted regime in lemma 3.2 at a spatial location yi over the time interval [t1,t2].

    t2t1Tit,2dx=t2t1Ti0,2dx+t2t1(μ+λ)itdx+t2t1t0σi2ij=1LijdVjλ(s)dx=Ti0,2(t2t1)+12(μ+λ)i(t22t21)+t2t1t0σi2ij=1LijdVjλ(s)dx (4.7)

    For xt and a spatial location yi

    t2t1Tix,2dx=Tit,2(t2t1)+12(μ+λ)i((t2t)2(t1t)2)+t2t1xtσi2ij=1LijdVjλ(s)dx
    FSCAT(t,t1,t2;D)=Ni=1ωiEQ[t2t1Tix,2dxFt]=Ni=1ωiEQ[(Tit,2(t2t1)+12(μ+λ)i((t2t)2(t1t)2)+t2t1xtσi2ij=1LijdVjλ(s)dx)|Ft]=Ni=1ωi(Tit,2(t2t1)+12(μ+λ)i((t2t)2(t1t)2))

    Generally, if we assume that the daily average temperature follows model 3.6, then the CAT futures price on temperature basket is computed using Equation 4.1, Proposition 4.2 and 4.3.

    Proposition 4.4. For a specificied contract period, tt1<t2 at spatial location yi, the futures contract price on basket GDD index following the normal regime in equation 3.6 is given by

    FNGDD(t,t1,t2;D)=t2t1(ξ(t,x)+2Δ(t,x)) 12(ϕ(Λ(t,x))+Λ(t,x)Φ(Λ(t,x)))dx, (4.8)

    where Φ is the cumulative standard normal distribution function, ϕ is the standard normal density function,

    Λ(t,x)=Ψ(t,x)K(ξ(t,x)+2Δ(t,x)) 12,
    Ψ(t,x)=Ni=1ωi(Sit,1+(Ti0,1Si0,1)eβit+(λβ)i(eβit1)),
    ξ(t,x)=Ni=1ω2i2(t,x)=Ni=1ω2iij=1xtσ2iT2(t,1),iL2ije2βi(xs)ds,
    Δ(t,x)=Ni=1Nj=i+1ωiωj(iq=1LiqLjq)Υij(t,x)=Ni=1Nj=i+1ωiωj(iq=1LiqLjq)xtσi1σj1Tiu,1Tju,1e(βi+βj)(xs)ds

    Proof. Let

    D(x)=Ni=1ωiTix (4.9)

    For xt in Lemma 3.2,

    Tix,1=Six,1+(Tit,1Sit,1)eβi(xt)+(λβ)i(eβi(xt)1)+xtσi1Tis,1eβi(xs)ij=1LijdVjλ(s) (4.10)

    For convenience, we shall denote the deterministic and random component of equation 4.10 as Gi(t,x) and Hi(t,x) respectively. That is,

    Gi(t,x)=Six,1+(Tit,1Sit,1)eβi(xt)+(λβ)i(eβi(xt)1)Hi(t,x)=xtσi1Tis,1eβi(xs)ij=1LijdVjλ(s)=ij=1xtσi1Tis,1eβi(xs)LijdVjλ(s)

    Hence

    D(x)=Ni=1ωi(Gi(t,x)+Hi(t,x)) (4.11)

    At time t, the distribution of the basket D(x) can be computed. However, Gi(t,x) is deterministic. Hence, at time t and by Itô isometry,

    xtσi1Tis,1eβi(xs)LijdVjλ(s)N(0,xtσ2iT2(s,1),iL2ije2βi(xs)ds)

    But Vjλ(s) are independent for each j. So the variances can be summed to obtain the variance of Hi(t,x),

    Hi(t,x)N(0,ij=1xtσ2iT2iL2ije2βi(xu)du)=N(0,2(t,x))

    Since Ni=1ωiHi(t,x) is a sum of normally distributed random variables, it implies that it is normally distributed with the following respective mean and variance:

    E(Ni=1ωiHi(t,x))=Ni=1ωiE(Hi(t,x))=0

    and

    Var(Ni=1ωiHi(t,x))=Ni=1Var(ωiHi(t,x))+2i<jCov(ωiHi,ωjHj)=Ni=1ω2iVar(Hi(t,x))+2i<jωiωjCov(Hi,Hj)=Ni=1ω2i2(t,x)+2i<jωiωjCov(Hi,Hj)

    Now, take into account Cov(Hi,Hj) for j>1. Both H1 and Hj are in the same integral form with respect to the standard Brownian motion V1λ(u). By the independence property of V1λ(u) and Vjλ(u), the covariance only exist between these two integrals. Therefore,

    Cov(Hi,Hj)=xtσi1σj1Tis,1Tjs,1e(βi+βj)(xs)(iq=1LiqLjq)ds,j>1=(iq=1LiqLjq)xtσi1σj1Tis,1Tjs,1e(βi+βj)(xs)ds,j>1

    Define Υij(t,x):=xtσi1σj1Tis,1Tjs,1e(βi+βj)(xs)ds.

    Var(Ni=1ωiHi(t,x))=Ni=1ω2i2(t,x)+2i<jωiωj(iq=1LiqLjq)Υij(t,x)=Ni=1ω2i2(t,x)+2Ni=1Nj=i+1ωiωj(iq=1LiqLjq)Υij(t,x)

    From 4.11,

    D(x)N(Ni=1ωiGi(t,x),Ni=1ω2i2(t,x)+2Ni=1Nj=i+1ωiωj(iq=1LiqLjq)Υij(t,x))

    Let

    Ψ(t,x)=Ni=1ωiGi(t,x);ξ(t,x)=Ni=1ω2i2(t,x)
    Δ(t,x)=Ni=1Nj=i+1ωiωj(iq=1LiqLjq)Υij(t,x)

    D(x) can be written in the form of a standard normal random variable ZN(0,1) as

    F(x)=Ψ(t,x)+(ξ(t,x)+2Δ(t,x))12Z (4.12)

    From equation 4.4, consider

    Ni=1ωiTitK>0 (4.13)

    This requires

    (ξ(t,x)+2Δ(t,x))12Z>KΨ(t,x)
    Z>KΨ(t,x)(ξ(t,x)+2Δ(t,x))12:=Λ(t,x) (4.14)

    From Equation 4.14,

    K=Ψ(t,x)+Λ(t,x)(ξ(t,x)+2Δ(t,x))12 (4.15)

    From equations 4.4 and 4.14,

    EQ(max{Ni=1ωiTitC,0}dx|Ft)=+Λ(t,x)(D(x)K)e12z22πdz (4.16)

    Substituting 4.12 and 4.15,

    EQ(max{Ni=1ωiTitK,0}dx|Ft)=+Λ(t,x)(Ψ(t,x)+(ξ(t,x)+2Δ(t,x))12zΨ(t,x)Λ(t,x)(ξ(t,x)+2Δ(t,x))12)e12z22πdz
    =+Λ1(t,x)((ξ(t,x)+2Δ(t,x))12zΛ(t,x)(ξ(t,x)+2Δ(t,x))12)e12z22πdz=(ξ(t,x)+2Δ(t,x))12(+Λ(t,x)ze12z22πdz+Λ1(t,x)Φ(Λ(t,x))=(ξ(t,x)+2Δ(t,x))12(e12Λ(t,x)22π+Λ(t,x)Φ(Λ(t,x))=(ξ(t,x)+2Δ(t,x)) 12(ϕ(Λ(t,x))+Λ(t,x)Φ(Λ(t,x)))

    Therefore

    FNGDD(t,t1,t2;D)=t2t1(ξ(t,x)+2Δ(t,x)) 12(ϕ(Λ(t,x))+Λ(t,x)Φ(Λ(t,x)))dx

    where

    Λ(t,x)=Λ(t,x)=Ψ(t,x)K(ξ(t,x)+2Δ(t,x))12

    Proposition 4.5. The price of a futures contract on basket GDD index following the shifted regime in equation 3.6 at time tt1<t2 is given by

    FEGDD(t,t1,t2;D)=t2t1(S(t,x)+2Y(t,x)) 12(ϕ(g(t,x))+g(t,x)Φ(g(t,x)))dx

    where ϕ and Φ as their usual meaning as in Proposition 4.4.

    g(t,x)=U(t,x)K(S(t,x)+2Y(t,x)) 12,U(t,x)=Ni=1ωi(Tit,2+(μ+λ)i)
    S(t,x)=Ni=1ω2iΣ2(t,x)=Ni=1ω2iij=1xtσ22,iL2ijdu
    Y(t,x)=Ni=1Nj=i+1ωiωjiq=1LiqLjqxtσi2σj2du

    Proof. The proof of Proposition 4.5 follows in the same way as the proof of Proposition 4.4

    In summary, if the daily average temperature follows the regime-switching model in equation 3.6, equation 4.1, Proposition 4.4, and Proposition 4.5 are used to calculate the GDD futures price on the temperature basket.

    In this paper, a regime-switching temperature dynamics model for spatial-temporal farming location was developed. To allow analytical tractability of the pricing models, the driving noise of the regimes were captured by a Brownian motion. Based on this model, pricing models for basket futures written on cumulative average temperature (CAT) and growing degree-days (GDD) indices were proposed. Pricing futures on temperature basket provides significant benefit as it mitigates geographical basis risks and changing of contracts relative to risk exposures of hedgers. With the proposed spatial-temporal regime-switching pricing model, investors in the weather derivative market have the opportunity to select the most appropriate composite of weather stations with their desired weight to optimize basis risk.

    An extension of this research would be to use the multi-dimensional regime-switching temperature model to price basket options on futures at different locations, also called rainbow options.

    The first author wishes to thank African Union and Pan African University, Institute for Basic Sciences, Technology and Innovation, Kenya, for their financial support for this research. Authors will like to thank the anonymous reviewers for their insightful comments.

    The authors declare that there is no conflict of interest.



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