Pricing correlation options: from the P. Carr and D. Madan approach to the new method based on the Fourier transform
1Arkadiusz Orzechowski
2Abstract : Pricing of options plays an important role in the financial industry. Investors knowing how to price derivative contracts quickly and accurately can beat the market.
On the other hand market participants constructing their investment strategies with the use of options based on techniques that do not assure the highest computational speed and efficiency are doomed to failure. The aim of the article is to extend the ex- isting methodology of pricing correlation options based on the Fourier transform. The article starts with a presentation of Carr and Madan’s concept (Carr & Madan, 1999).
Then other methods of pricing options with the use of the Fourier transform are sum- marized. Finally, a new approach to pricing derivative contracts is derived and then applied to the correlation options.
Keywords : Fourier transform, pricing of options, correlation options.
JEL Codes : G13, C02.
Introduction
The rapid development of option markets worldwide in recent years is accompa- nied by a rise in trading activities of investors and a development of new, highly sophisticated, financial products. One direct consequence of such a trend is the possibility for buyers and sellers of the derivatives to more efficiently speculate on the movements of interest and exchange rates, commodity and equity prices, as well as credit ratings of the issuers of bonds. As the capacity for speculation using derivatives is growing, increased demand for new instruments allowing to hedge against different aspects of risks appears. Options, along with forwards and futures, seem to be the best tools that can be used to protect market par- ticipants against potential capital losses. One of the most interesting type of options used for managing risks are exotic options where pay-offs depend on
1 Article received 15 February 2017, accepted 22 January 2018.
2 Warsaw School of Economics, Collegium of Socio-Economics, Department of Banking, ul. Wiśniowa 41, 02-520 Warszawa, aorzec@sgh.waw.pl.
17
A. Orzechowski, Pricing correlation options: from the P. Carr and D. Madan…
the correlation between asset prices, e.g. exchange options, quotient options, correlation options. Some of the contracts, e.g. spread options, are traded on exchanges (NYMEX, NYCE, CBOT), others, like quotient and product options, can be bought or sold in the OTC market (Zhu, 2000).
The aim of the article is to extend the analysis of the Carr and Madan method (Carr & Madan, 1999) for pricing correlation options in the Black and Scholes framework (Black & Scholes, 1973). The article consists of several sections. At the beginning the martingale method is applied to the valuation of analyzed derivatives. Next, the method is modified to the form proposed by Carr and Madan (1999). Finally, alternative methods of pricing correlation options, which are based on the Fourier transform, are presented and a new model for pricing of this type of derivatives is developed.
1. Pricing correlation options using the martingale method
One of the most popular methods of pricing correlation options is based on the risk-neural concept (method referred to as BS-M) (Black & Scholes, 1973).
The method is based on the assumption that the price of the underlying instru- ment follows geometric Brownian motion. In consequence the natural loga- rithm of market value of the underlying instrument has normal distribution.
The joint probability density function of the two-dimensional variable that has to be analyzed for the correlation options can be described with the use of an elegant formula as follows:
− + − − + − − + − − + −
2 2
2 2 2 2
1 1 1 1 1 1 2 2 2 2 2 2
2 2
1 1 2 2
2
1 2 2
1 2
1 1 1 1
2 2 2 2
2 2
1
( , ) 1
2 1
T t T t T t T t
T T
S S r σ τ ρ S S r σ τ S S r σ τ S S r σ τ
σ τ τσ σ σ τ
ρ
q S S
πτσ σ ρ
e
− +
− −
= ×
−
×
, (1) where: S
1T, S
2Tare the prices of the underlying assets 1 and 2 at time T, σ
1, σ
2are the standard deviations of rates of return on the assets 1 and 2, r is the risk-free rate of return, ρ is the coefficient of correlation and τ = T – t.
One dimensional analogue of the equation (1) for the single asset plain va- nilla European option can be expressed as:
− + −
2
2 2
1 1 2
( ) 2 2
T t
T T
lnS lnS r σ τ
q S exp
S σ πτ σ τ
= −
, (2)
for 0 ≤ t ≤ T and τ = T – t.
In equation (2) the natural logarithm of the market price of the underlying security is replaced by market price of the security itself.
If the price of the instrument being the basis for the analyzed contracts is equal to 60, the risk-free rate of return amounts to 5%, standard deviation of the rates of return is 20% and relative time to expiration, i.e. t/T changes from 0,5 to 0,9 the distribution of the underlying asset is presented on Figure 1.
As the BS-M method is based on the assumption that the theoretical value of the European option equals the value of future payments discounted with the risk-free rate with respect to the martingale measure q, the following for- mulas for the prices of the European calls and puts respectively become valid:
C S t e E S K ( , )
t=
−rτ q( ( T− ,0) Ω
+ t) , (3)
( )
( , )
t rτ q(
T T,0)
tP S t e E K =
− − S
+Ω , (4) where: q(.|Ω
t) is the probability density function dependent on filtration Ω
t, K is the strike price of the European option.
Alternatively one can write that:
( , )
t(
T)
T t TC S t e
rτS K q S ( ) dS
K
∞
=
−∫ − Ω , (5)
( )
0
( , )
t rτK(
T)
T t TP S t e =
−∫ K S q S − Ω dS . (6) Figure 1. Distribution of underlying asset prices in the martingale method
30 40 50 60 70 80 90 100
0.00 0.01 0.02 0.03 0.04 0.05 0.06
Price of underlying asset (S)
Density of probability LN BS
LN BS t/T = 0,5
t/T = 0,7 t/T = 0,9 LN BS
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A. Orzechowski, Pricing correlation options: from the P. Carr and D. Madan…
Substituting the analytical expression of probability density function for q(S
T|Ω
t) allows the formulation of the following statements:
2
σ τ2
2
1 lnS lnS r 2
t T σ τ T
C S t e S K e dS
− + −
2 2
( , ) ( ) 1
2
T t
rτ
K
S
Tπσ τ
∞ −
=
−∫ − , (7)
− + −
2
t T T
P S t e K S e dS
2 2
1 2 2 0 2
( , ) ( ) 1
2
T t
lnS lnS r σ τ
rtK σ τ
S
Tπσ τ
− −
= ∫ − . (8)
Equations (7) and (8) can be easily extended to the two-dimensional case.
In the pay-off functions of the correlation call and put options are defined re- spectively as (Dempster & Hong, 2000):
1 2 1 1 2 2
( , , )
t t(
T,0) (
T,0
tC S S t e E S =
−rτ q( − K + S − K ) Ω
+ ) , (9)
1 2 1 1 2 2
)
( , , )
t t(
T,0) (
T,0 )
tP S S t e E K S =
−rτ q( − + K S −
+ Ω , (10) the equations allowing for the valuation of the contracts can be formulated with the use of equation (1), i.e.:
1 2
1 2 1 1 2 2 1 2 2 1
( , , )
t t rτ(
T)(
T) (
T,
TΩ
t)
T TK K
C S S t e =
− ∞ ∞∫ ∫ S − K S − K q S S dS dS , (11)
1 2
1 2 1 1 2 2 1 2 2 1
( , , )
t t rτ(
T)(
T) ( ,
T TΩ
t)
T TK K
P S S t e =
− ∞ ∞∫ ∫ K S − K S q S S − dS dS , (12) where: q(.,.|Ω
t) is the joint probability density function dependent on filtra- tion Ω
t.
Unfortunately applying this procedure to the two-dimensional variable in order to conclude about the final shape of the pay-off function is highly ineffi- cient. That is why application of an alternative approach seems to be necessary.
2. Method of P. Carr and D. Madan
Unlike the BS-M concept the method developed by Carr and Madan (1999) is based on the Fourier transform (the method is referred to as BS-FTCM). The approach applied to the valuation of correlation options consists of several steps.
At the beginning variables representing spot prices of the underlying assets
and strike prices of the option (see equations (11) and (12)) are transformed
according to the following scheme: s
1T= lnS
1T, s
2T= lnS
2T, k
1= lnK
1, k
2= lnK
2. Finally, equations (13) and (14) are written as:
1 1 2 2
1 2
1 2 1 2 2 1
( , , )
t t rτ(
sT k)(
sT k) ( ,
T TΩ
t)
T Tk k
C s s t e =
− ∞ ∞∫∫ e − e e − e q s s ds ds , (13)
1 1 2 2
1 2
1 2 1 2 2 1
( , , )
t t rτ(
k sT)(
k sT) ( ,
T TΩ )
t T Tk k
P s s t e =
− ∞ ∞∫∫ e − e e − e q s s ds ds . (14) Limiting the analysis only to call options the equation (13) can be modified by parameters α
1and α
2in the following way:
1 1 2 2
1
,
2, (
1,
2)
( )
α k α k,
mod t t t t
C s s t e =
+C s s t , (15) where: α
1and α
2are the positive constants.
Calculation of the Fourier transform of the modified function C
mod(s
1t, s
2t, t) allows the conclusion that:
1 1 2 2
1 1 1 2 2 2
2
( ) (
1 2 mod 1 2 2 1
1 1
1 2 1 2
1 1 2 2 1 1 2 2
)
( , ) , ,
( , )
( )( )(1 )(
( )
1 )
Ω
T T.
iξ k iξ k
t t
rτ s
T T t
ψ ξ ξ e C s s t dk dk
e q s s e d
α iξ α iξ α iξ α iξ
∞ ∞ +
−∞−∞
+ + + + +
−
= =
= ∫∫ + + + + + +
∫ ∫
α iξ s α iξ
ξ dξ
(16)
Proof:
1 (+ +1 1)+2 (+ +2 2) 1 (+ +1 1)+2 (+ +2 2)
2 1
1
)(
2 2) ds ds
T Tξ α iξ
=
+ +
+ + + +
1 1 1 2 2 2
1 2 2 1
1 1 2 2 1 1 2
( ( )
2
(1 .
) )
e q s s s ds
α iξ α iξ + + + + α iξ + + α iξ
1 1 1 2 2 2 1 1 1 2 2 2
1 1 2 2 1 1 2 2
( ) ( ) ( ) ( )
( α iξ α iξ )( ) ( α iξ )(1 α iξ )
+ + + + + + + + + +
− +
)
1 2 1 1 1 2 2 2
) 2
1 2 1
( T T
e
+e
+ + +dk dk ds ds
+ =
1 +2 1( 1+ 1)+ 2(2+ 2) 2 +1 1(1+ 1)+2( 2+ 2)
− − +
+ + + +
1 2
Ω
( , )
rτ T T t
e
− ∞ ∞q s s e e
−∞−∞ −∞−∞
= ∫ ∫ ∫ ∫ +
= e e C s s ( , , )
1t 2t 2 1=
1 1 2 2
1 1 2 2 1 1 2 2
1 1 2 2 1 1 2 2 1 1 2 2
1 2
1 2 1 2 2 1
1 2 2 1
( , ) , ,
( )( )
( , )
( )
Ω
T T
iξ k iξ k mod
t t
iξ k iξ k α k α k
iξ k iξ k α k α k rτ s k s k
k k
T T t T T
ψ ξ ξ e C s s t dk dk
e e e e e e e
q s s ds ds
∞ ∞ +
−∞−∞
∞ ∞ + +
−∞−∞
∞ ∞ ∞ ∞
+ + −
−∞−∞
= =
= − −
∫ ∫
∫ ∫
∫ ∫ ∫∫
(
1 2
1 2 1( 1 1) 2(2 2)
(
2 1
)
T T
T T
s s
s s k α iξ k α iξ
s k k α iξ k α iξ s k k α iξ k α iξ
k k k α iξ k α iξ
dk dk
e e e e
e
=
=
1 2 1 1 1 11 1 1 1
1 1 2 2 1
( , )
(1 )( )
Ω
(1
T T T T
T T T T
rτ s
T T t
s α iξ s α iξ s α iξ s α iξ
e e
q s s
e e
α iξ α iξ α
− ∞ ∞
−∞−∞
+ + + + +
− +
+ + + +
∫ ∫
2
1 1
)
( , )
( )( )(1
Ω
sT α iξ sT α iξrτ T T t
i
e
+=
−∫∫
τ dk dk
α iξ s α iξ s α iξ s α iξ
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A. Orzechowski, Pricing correlation options: from the P. Carr and D. Madan…
1 (+ +1 1)+2 (+ +2 2) 1 (+ +1 1)+2 (+ +2 2)
2 1
1
)(
2 2) ds ds
T Tξ α iξ
=
+ +
+ + + +
1 1 1 2 2 2
1 2 2 1
1 1 2 2 1 1 2
( ( )
2
(1 .
) )
e q s s s ds
α iξ α iξ + + + + α iξ + + α iξ
1 1 1 2 2 2 1 1 1 2 2 2
1 1 2 2 1 1 2 2
( ) ( ) ( ) ( )
( α iξ α iξ )( ) ( α iξ )(1 α iξ )
+ + + + + + + + + +
− +
)
1 2 1 1 1 2 2 2
) 2
1 2 1
( T T
e
+e
+ + +dk dk ds ds
+ =
1 +2 1( 1+ 1)+ 2(2+ 2) 2 +1 1(1+ 1)+2( 2+ 2)
− − +
+ + + +
1 2
Ω
( , )
rτ T T t
e
− ∞ ∞q s s e e
−∞−∞ −∞−∞
= ∫ ∫ ∫ ∫ +
= e e C s s ( , , )
1t 2t 2 1=
1 1 2 2
1 1 2 2 1 1 2 2
1 1 2 2 1 1 2 2 1 1 2 2
1 2
1 2 1 2 2 1
1 2 2 1
( , ) , ,
( )( )
( , )
( )
Ω
T T
iξ k iξ k mod
t t
iξ k iξ k α k α k
iξ k iξ k α k α k rτ s k s k
k k
T T t T T
ψ ξ ξ e C s s t dk dk
e e e e e e e
q s s ds ds
∞ ∞ +
−∞−∞
∞ ∞ + +
−∞−∞
∞ ∞ ∞ ∞
+ + −
−∞−∞
= =
= − −
∫ ∫
∫ ∫
∫ ∫ ∫∫
(
1 2
1 2 1( 1 1) 2(2 2)
(
2 1
)
T T
T T
s s
s s k α iξ k α iξ
s k k α iξ k α iξ s k k α iξ k α iξ
k k k α iξ k α iξ
dk dk
e e e e
e
=
=
1 2 1 1 1 11 1 1 1
1 1 2 2 1
( , )
(1 )( )
Ω
(1
T T T T
T T T T
rτ s
T T t
s α iξ s α iξ s α iξ s α iξ
e e
q s s
e e
α iξ α iξ α
∞ ∞
−
−∞−∞
+ + + + +
− +
+ + + +
∫ ∫
2
1 1
)
( , )
( )( )(1
Ω
sT α iξ sT α iξrτ T T t
i
e
+=
−∫∫
τ dk dk
α iξ s α iξ s α iξ s α iξ
(17)
It is worth noting that:
1 1 2 2
1 1 1 2 2 1
Φ( , ξ ξ )
∞ ∞e
iξ s iξ s+q s s (
T,
TΩ
t) ds ds
−∞−∞
= ∫ ∫ (18)
is the two-dimensional characteristic function for the variables s
1tand s
2t. It means that the equation (17) can be expressed as:
( )
(
1 1)(
2 2)
1 2 2 2 2 2
1 1 1 1 1 2 2 2 2 2
Φ ( 1) , ( 1)
( , )
(2 1) (2 1)
e
rτψ ξ ξ
α α ξ i α ξ α α ξ i α ξ
−
− + − +
= + − + + + − + +
ξ α i ξ α i
. (19)
Calculation of the inverse Fourier transform allows the determination of the price of the correlation call option, i.e.:
− + − + )
1 1 2 2
Φ ( ( 1) , ( 1)
(
12 1e
12rτ(2
11)
1)(
22 2 22(2
21)
2)
2 1. dξ dξ α α ξ i α ξ α α ξ i α ξ
−
+ − + + + − + +
1 1 2 2
iξ k iξ k
e
∞ ∞ − −
−∞−∞
× ∫ ∫ ξ α i ξ α i
1 1 2 2
1 1 2 2
1 1 2 2
1 2 1 2 2 1
( , , ) ( , )
2 2
α k α k
iξ k iξ k
t t
α k α k
C s s t e e
π
e π
− − ∞ ∞
− −
−∞−∞
− −
= ∫ ∫ ψ ξ ξ dξ dξ == ×
(20)
If the prices of the instruments being the basis for the analyzed contracts are equal to 60 and 62, risk-free rate of return amounts to 5%, standard devia- tions of the rates of return are 10% and 5%, relative time to expiration is equal to 0,1, coefficient of correlation ρ = 0 and α
1= α
2= 1 the payoff function of the correlation call option is presented on Figure 2.
Although the BS-FTCM method can be applied to pricing correlation op-
tions it is far from being perfect. The biggest problem that appears when using
the method is associated with the tendency of the subintegral function from
equation (20) to rapid oscillation when out-of-the-money (OTM) near-to-ex- piration contracts are considered. That is why other concepts for pricing op- tions should be explored.
3. Alternative methods of pricing options utilizing Fourier transform
There are many alternative concepts based on the Fourier transform which can be used to value derivatives (Orzechowski, 2016). To the best knowledge of the author only two of them were applied to pricing correlation options.
Nevertheless almost all of them can be good alternatives to the BS-M and BS- FTCM methods. Only the four most important approaches are presented below.
The first method of pricing options using Fourier transform was devel- oped by Bakshi and Madan (the method is referred to as BS-FTBM) (Bakshi
& Madan, 2000). In this approach the price of the underlying assets and the exercise price of the option in equation (5) are converted to logarithmic values.
Then the right hand side of a new equation is split into two parts. For each of them Fourier transforms are determined and reversed. Finally the theoretical value of the option may be obtained with the use of equation (21):
1 1 ( ) ξ Ke 1 ( ) dξ
= − + −
0 0
( , ) ( )
2 ( 1)
iξk iξk
rτ rτ
t t t
e
C S t S Ke S d
∞ − ∞ −
−
−
− −
∫ R ϕ ξ i ∫ R e ϕ ξ
π iξϕ π iξ , (21) where: R is the real part of the subintegral function and i is the imaginary part of the complex number.
Figure 2. Pay-off function of the correlation call option in the BS-FTCM method
Price of underlying asset (S2)Price of underlying asset (S1) Payoff
100 50
50 50
40
40 60
60
70
70
80
80 0
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A. Orzechowski, Pricing correlation options: from the P. Carr and D. Madan…
The second method of pricing options with the use of the Fourier transform was derived by Attari (the method is referred to as BS-FTA) (Attari, 2004). This approach begins with the generalization of the process responsible for the stock price movements. Next equation (5) is transformed into the following formula:
∫ ( , ) ( , )
τ∫ ( ( , ) ) ( , )
1 rτ 2t t
S e
x t T( , )q ( x t T dx t T e K ) −
−rq x t T dx t T S = −
−l l
π e Kπ
∞ ∞
, (22)
where: l = K/S
te
rτand x(t, T) is the unpredictable shock in prices of the security.
Noting that 0
x t T( , )( ( , ) ) ( , ) 1
l
e q x t T dx t T
∞
≤ ∫ ≤ allows to treat both π
1and π
2as probability density functions. Determining their Fourier and inverse Fourier transforms leads directly to the price of the option, i.e.:
∞
∫
( )
( ) .
= + +
0
( )
0
( , ) 1 ( )
1 1 2
l iξl
t t
r T t iξl
e e
C S t S
π i ξ i
e K ϕ ξ e dξ
π iξ
−
∞ −
− −
+
− +
∫ R
R
ϕ ξ dξ
(23)
The third method of pricing option using Fourier transform was proposed by Bates (the method is referred to as BS-FTB) (Bates, 2006). This approach is based on the modification of the previous concept. As before equation (5) is transformed but in this case to the following form:
C S t S e K ( , )
t= −
0 rτ K∫
T ( Ω ) S
T tdS e
T−
rτ∫ K S q (
TΩ )
td S
TK
S q K
− − ∞
−∞
. (24)
Next, it is modified and Fourier transformed. Finally, the price of the option is determined in the following way:
0
( , ) 1 1 ( )
2 (1 )
e
iξkπ iξ iξ
∞ −
= −
0 rτ + ∫ R −
C S t S e K
t −ϕ ξ dξ . (25)
The fourth method of pricing options using Fourier transform was devel-
oped by Lewis (the method is referred to as BS-FTL) (Lewis, 2001). This con-
cept is based on a multiple transformation of the equation (5), conversion of
the dependent variables to logarithmic values and calculation of the Fourier
and inverse Fourier transforms. Finally, the price of the option can be deter-
mined with the use of the following formula:
2
1
2 4
i e
iuku
= − ℜ − +
2 0
( , )
rτ
t t t
C S t S S Ke
π
− ∞
∫ ϕ u du. (26)
Although all the methods presented above can be easily applied to the valu- ation of correlation options (Fan & Wang, 2017), the remaining part of the arti- cle is devoted only to the new method of pricing options based on the Fourier transform and its application to the valuation of correlation options.
4. New method of pricing correlation options using Fourier transform
The new method of pricing options using Fourier transform (the method is referred to as BS-FTAu) consists of several steps. At the beginning dependent variables in equation (5) are converted to logarithmic values. Next, the right hand side of the equation obtained is split into two parts, i.e.:
t
( Ω )
T t Te e s
T t) ds
T( , )
rτ sT rτ k( Ω
k k
C S t e =
− ∞∫ e q s d s −
− ∞∫ q . (27) The first part of equation (27) is Fourier transformed as in BS-FTBM model, i.e.:
e s ds
∞
e s ds
∞T
ξ = e e e s
T tds dk
T
1
( Ω )
( ) ( Ω )
( )
Ψ
Ω
T
T T
s T t T
iξk rτ k s
s T t T
q
q q
∞
−
∞
−∞ −∞
−∞
∫ ∫ ∫
∫
. (28)
It can easily be seen that
∞e
sTq ( Ω ) s
T tds
T−∞
∫ may be treated both as the char- acteristic function of s
Tassuming ξ = –i, i.e. ϕ(–i), and expected value of S
T. It allows the transformation of the equation (28) to the following form:
1
( )
0( )
Ψ
T( )
S ξ i ξ iξϕ
ϕ i
= −
− . (29)
25
A. Orzechowski, Pricing correlation options: from the P. Carr and D. Madan…
Proof:
s ds
sT
T t T
−∞
=
− −
)
0 0
( ).
( )
T t T( )
S s ds S
ϕ i i ξ iξ ϕ i
−
= = (30)
ϕ ξ i
(
0
1
( Ω )
( ( )
)
T
T
iξk s
s iξ
S e
ϕ i iξ
e q
q
∞ +
−∞
∞ +
−∞
= −
∫
∫
−∞ −∞
e e s ds dk s e
∫ ∫
sT T t T∫
T t ∫ e dk ds
sT
T= = =
T t T T t T
e s ds e s ds
ξ e e S e dk S e dk
= = =
1 0 0
0 0
( Ω ) ( Ω )
( )
( Ω ) ( Ω )
Ψ ( ) ( )
( ) ( )
T T
T
s s
iξk rT k rT iξk k
T
s
iξk iξk
k
ϕ i ϕ i
S S
q q
q q
∞ ∞
∞ ∞
−
∞ ∞ ∞
−∞ −∞ −∞
− −
− −
∫ ∫
∫ ∫
ϕ i ϕ i
Ω
The second part of equation (27) is also Fourier transformed, i.e.:
( ) (
T2
ξ e e s
T tds d
TΨ = Ω ) = ( )
1
iξk k k
ϕ ξ i
q k
iξ
∞ ∞
−∞
−
∫ ∫ + . (31)
Proof:
T
ξ K e e s
T tds dk
T
= =
sT
rT i
T t T
Ke s e dk ds
−∞ −∞
= =
∫ ∫
sT
iξk
T t
e
TKe s ds
iξ
−∞
= =
2
( ) ( Ω )
( Ω )
( Ω )
( Ψ
Ω )
T( ) .
iξk rT k
ξk
rT
rT iξs rT
T t
e
Tϕ ξ
Ke s d
q
s q
q
q Ke
iξ iξ
∞ ∞
−
−∞
− ∞
− ∞
−∞
− ∞ −
−∞
= =
∫ ∫
∫
∫
(32)
Inverting both Fourier transforms allows obtention of the final price of the option, i.e.:
C S t S e e d
ξ
= −
0
1 1 ( )
2 ( 1)
rτ iξk
ϕ ξ i
π iξ iξ
− ∞ −
−
∫ R +
( , )
t t. (33)
Before applying equation (33) to the valuation of correlation options it pays
to transform equation (13) to the form:
1 1 2 2 1 2
1 2 2 1 1 2 1
( , , )
t t rτ(
sT k)(
sT k) (
T T) ( )
T T Tk k
C s s t e =
− ∞ ∞∫∫ e − e e − e q s s q s ds ds , (34) where: q s s (
2T 1T) is the conditional probability density function of s
2Tgiven s
1Tand q s ( )
1Tis the probability density function of s
1T(Carmona & Durrleman, 2003).
It is worthy of note that s
1Tand s
2Tare normally distributed variables with known analytical probability distribution functions.
As the application of the formula (33) to equation (34) is evident the closed- form formula for the final price of the correlation option is presented without derivation (Feunou & Tafolong, 2015).
2 2 2 2 2
2 2
0
( )
( )
1 1 .
2
rτ iξ k1
φ ξ i
S e e d
π iξ iξ
∞ −
−
+
∫ R
1 1 1
1 2 1 1 1
1 1
0
( )
( )
1 1 1
2 2
iξ k1
rτ rτ
t t t
φ ξ i
C s s t e S e K e d
π iξ iξ
∞ −
− −
= − − ∫ R + ( , , )
t
ξ
ξ
−
−(35)
It should be noted that equation (35) is correct but only under the previ- ously introduced assumption that ρ = 0.
Given the same data as previously the pay-off function of the correlation option in the BS-FTAu method can be easily determined (see Figure 3).
Applying the BS-FTAu method for the calculation of the correlation op- tion has one advantage over other concepts based on the Fourier transform.
The speed of calculating the final price of the option is greater than in other approaches.
Figure 3. Pay-off function of the correlation call option in the BS-FTAu method
Price of underlying asset (S2)Price of underlying asset (S1) Payoff
100 50
50 50
40
40 60
60
70
70
80
80 0
27
A. Orzechowski, Pricing correlation options: from the P. Carr and D. Madan…