Complex derivatives valuation: applying the LeastSquares Monte Carlo Simulation Method with several polynomial basis
 Ursula Silveira Monteiro de Lima^{1}Email author and
 Carlos Patricio Samanez^{1}
Received: 7 February 2015
Accepted: 21 December 2015
Published: 13 January 2016
Abstract
Background
This article investigates the LeastSquares Monte Carlo Method by using different polynomial basis in American Asian Options pricing. The standard approach in the option pricing literature is to choose the basis arbitrarily. By comparing four different polynomial basis we show that the choice of basis interferes in the option's price.
Methods
We assess LeastSquares Method performance in pricing four different American Asian Options by using four polynomial basis: Power, Laguerre, Legendre and Hermite A. To every American Asian Option priced, three sets of parameters are used in order to evaluate it properly.
Results
We show that the choice of the basis interferes in the option's price by showing that one of them converges to the option's value faster than any other by using fewer simulated paths. In the case of an Amerasian call option, for example, we find that the preferable polynomial basis is Hermite A. For an Amerasian put option, the Power polynomial basis is recommended. Such empirical outcome is theoretically unpredictable, since in principle all basis can be indistinctly used when pricing the derivative.
Conclusion
In this article The LeastSquares Monte Carlo Method performance is assessed in pricing four different types of American Asian Options by using four different polynomial basis through three different sets of parameters. Our results suggest that one polynomial basis is best suited to perform the method when pricing an American Asian option. Theoretically all basis can be indistinctly used when pricing the derivative. However, our results does not confirm these. We find that when pricing an American Asian put option, Power A is better than the other basis we have studied here whereas when pricing an American Asian call, Hermite A is better.
Keywords
Complex derivatives valuation LeastSquares Monte Carlo Method Amerasian options Polynomial basisBackground
Asian options are often used for cash flow hedges in companies whose purchase programming is set to mitigate the fluctuation of raw materials’ prices. Its versatility is confirmed by its presence in markets like commodities, electric power, interest rates and currency rates (McDonald 2006). Because they are complex (or exotic), the Asian options are usually traded over the counter. The characteristics of the contract (subject, premium, strike price, deadlines and maturity) are freely agreed between the parties, emphasizing their nonstandardization.
Traditional techniques such as the finitedifferences method and lattice become less attractive when dealing with pricing derivatives with multiple stochastic variables, problems with many dimensions, or even pathdependent American options, as it is the case of American Asian (Amerasian) options. The most flexible technique for pricing exotic options, such as American options, is the use of stochastic simulation with optimization algorithm. This technique includes different methods, such as the LeastSquares Monte Carlo method (LSM), first introduced by Longstaff and Schwartz (2001). Besides being faster and more precise to compute than other methodologies, the LSM methodology helps assess pathdependent American options with multiple dimensions and multiple state variables, being also applied to Markovian and nonMarkovian problems.
The LeastSquares Monte Carlo Method has been used to price American Asian options. Longstaff and Schwartz (2001) exemplified the use of their technique in pricing an American Asian Arithmetic Average Fixed Strike call option with a specific polynomial basis, i.e., power. Moreno and Navas (2003) access the performance of Least Squares Monte Carlo Method numerically, by using two different polynomial basis, i.e., Laguerre and Hermite B, to value the same American Asian option priced by Longstaff and Schwartz (2001). Moreno and Navas (2003) found that the choice of the polynomial basis and the degree of these polynomials influence the estimated prices. Chaudhary (2005) used quasirandom sequences to improve the performance of this technique by pricing an American Asian Arithmetic Average call option without varying the polynomial basis used. In their experiment, they used power polynomial basis. Also to access the performance of this techniques, Cerrato and Cheung (2007) priced an American Asian Arithmetic Average call option using three sets of simulated trajectories. They applied two different polynomial basis, i.e., exponential and Laguerre. Although not dedicated to the task of pricing an American Asian option, other authors, such as Glasserman (2004) states that “accuracy depends on the choice of basis functions, which may require experimentation or good information about the structure of the problem”.
In this paper, we apply the LeastSquares Monte Carlo method intensively to price four different American Asian (Amerasian) options with four different polynomial basis. We do this for both put and call option. To access the performance of this algorithm, we use three sets of parameters.
The LeastSquares Monte Carlo Method
Every minute prior to the expiration date of an American option, the option holder must choose the optimal outcome between exercising the option or keeping it for another term. The choice is based on the immediate exercise payoff and the future payoff expected. If the former is greater than the latter, then the option is exercised.
The idea of the LeastSquares Monte Carlo Method is to approximate the continuation value by using leastsquares regression at every moment in which it is possible to exercise the option. The regression is done based on the data obtained for the state variables via Monte Carlo simulation and by choosing the trajectories where the option is in the money.
where the polynomial basis, represented by Φ _{ j }, is a function of one of the state variables. Note that the coefficients of the basis, α _{ j }, are not previously known, but they can be estimated by linear regression. The properties of the estimator and the convergence of the method are addressed algebraically by Clement et al. (2002) and Stentoft (2004).
When considering the number of basis to be used, it is important to point out a problem mentioned by Moreno and Navas (2003). They analyze the use of a large number of basis and conclude that several degrees of the chosen polynomial basis and its respective crossed products can increase the accuracy of the estimation. In some cases, however, an excessive increase in the number of basis can reduce the precision of the method, making it computationally expensive.
Methods
The LeastSquares Monte Carlo Method is applied in four different cases of FixedStart Time Window^{3} American Asian options: Case 1 –Arithmetic Average Floating Strike American Asian option; Case 2 –Geometric Average Floating Strike American Asian Option; Case 3 –Arithmetic Average Fixed Strike American Asian Option; and Case 4 – Geometric Average Fixed Strike American Asian Option.
Following Moreno and Navas (2003), we use the BermudaAsian option as a discrete approximation of the Amerasian option, whereby the price of the assetobject is monthly noted. All the priced options have a term of one year, and can be exercised from the third month of their issuance. It is assumed that the price of the assetobject follows a riskneutral Geometric Brownian Motion.

t _{ j } ≡ j represents month in which early exercise is possible, j = 1,2,…,12.

S(t _{ j }) = S _{ j } ≡ underlying asset price observed at jth month

\( \overline{S}\left({t}_j\right)={\overline{S}}_j\equiv \mathrm{discretely}\kern0.5em \mathrm{sampled}\kern0.5em \mathrm{average}\kern0.5em \mathrm{of}\kern0.5em \mathrm{underlying}\kern0.5em \mathrm{asset}\kern0.5em \mathrm{price} \)

\( {\overline{S}}_j={A}_j\equiv \operatorname{}\frac{{\displaystyle \sum_{k=1}^j{S}_k}}{j}\Rightarrow \kern0.5em \mathrm{discretely}\kern0.5em \mathrm{sampled}\kern0.5em \mathrm{arithmetic}\kern0.5em \mathrm{average} \)

\( {\overline{S}}_j={G}_j\equiv {\left({\displaystyle \prod_{k=1}^j{S}_k}\right)}^{\raisebox{1ex}{$1$}\!\left/ \!\raisebox{1ex}{$j$}\right.}\Rightarrow \mathrm{discretely}\kern0.5em \mathrm{sampled}\kern0.5em \mathrm{geometric}\kern0.5em \mathrm{average} \)

K ≡ strike price

\( \eta =\left\{\begin{array}{c}\hfill 1\kern1em \mathrm{f}\mathrm{o}\mathrm{r}\kern0.5em \mathrm{call}\kern0.5em \mathrm{o}\mathrm{ption},\hfill \\ {}\hfill 1\kern1em \mathrm{f}\mathrm{o}\mathrm{r}\kern0.5em \mathrm{put}\kern0.5em \mathrm{o}\mathrm{ption}.\hfill \end{array}\right. \)

y ≡ dividend yield

r ≡ riskless rate

σ ≡ volatility
According to Longstaff and Schwartz (2001), the structure used in regressions, expressed below by equation (1), comprises a constant, the two first degrees of the chosen polynomial basis and their crossed product up to the third degree, totaling eight basis. The polynomials used are Power, Legendre, Laguerre and Hermite A.
The matrix of the underlying asset prices, S, is defined recursively. The i ^{th} row vector corresponds to the i ^{th} simulated path and its elements are defined by:
\( {s}_{i,j+1}={s}_{i,j}\ {e}^{\left(ry\raisebox{1ex}{${\sigma}^2$}\!\left/ \!\raisebox{1ex}{$2$}\right.\right)\varDelta t+\sigma\ \varepsilon \sqrt{\varDelta t}},\ \varepsilon \sim N\left(0,1\right) \) and Δt = t _{ j + 1} − t _{ j } , j = 1, 2, …, 12.
Note that each column vector of the matrix corresponds to a specific time step.
Once the matrix of the underlying asset prices is set, the matrix of averages, \( \overline{\mathbf{S}} \), is determined by using relations introduced latter, in which the form depends solely on what kind of average is considered, i.e., whether it is an arithmetic average or it is a geometric one.
Let,
Φ _{1}(S)≡B _{ m,j }; Φ _{2}(S)≡C _{ m,j }; \( {\varPhi}_1\left(\overline{\mathbf{S}}\right)\equiv {\mathbf{D}}_{m,j} \); \( {\varPhi}_2\left(\overline{\mathbf{S}}\right)\equiv {\mathbf{E}}_{m,j} \);
\( {\varPhi}_1\left(\mathbf{S}\right)\odot {\varPhi}_1\left(\overline{\mathbf{S}}\right)\equiv {\mathbf{Z}}_{m,j} \); \( {\varPhi}_2\left(\mathbf{S}\right)\odot {\varPhi}_1\left(\overline{\mathbf{S}}\right)\equiv {\mathbf{G}}_{m,j} \); \( {\varPhi}_1\left(\mathbf{S}\right)\odot {\varPhi}_2\left(\overline{\mathbf{S}}\right)\equiv {\mathbf{H}}_{m,j} \)
Polynomial basis used
As mentioned above, the polynomials used in this study are Power, Legendre, Laguerre and Hermite A. All of them can be alternatively expressed by Rodrigues’ formula, explicit form or by the recurrence law (Abramowitz and Stegun 1972).
Coefficients and functions of the basis functions using Rodrigues’ formula
f _{ n } (x)  a _{ n }  ρ(x)  g (x)  

Power  W _{ n } (x)  \( (2.n)!/n! \)  x ^{2.n }  1 
Legendre  P _{ n } (x)  (−1)^{ n } .2^{ n }.n!  1  1 – x ^{2} 
Laguerre  L _{ n } (x)  n!  e^{−x}  x 
Hermite A  H _{ n } (x)  (−1)^{ n }  \( {e}^{{x}^2} \)  1 
Explicit expressions of the basis functions
f _{ n } (x)  N  d _{ n }  c _{ m }  g _{ m } (x)  

Power  W _{ n } (x)  0  1  1  x ^{ n } 
Legendre  P _{ n } (x)  [n/2]  2^{−n }  \( {\left(1\right)}^m.\left(\underset{m}{\overset{n}{}}\right).\left(\underset{n}{\overset{2.n2.m}{}}\right) \)  x ^{ n−2.m } 
Laguerre  L _{ n } (x)  n  1  \( \frac{{\left(1\right)}^m}{m!}.\left(\underset{nm}{\overset{n}{}}\right) \)  x ^{ m } 
Hermite A  H _{ n } (x)  \( \left[\raisebox{1ex}{$n$}\!\left/ \!\raisebox{1ex}{$2$}\right.\right] \)  n!  \( {\left(1\right)}^m.\frac{1}{m!\left(n2.m\right)!} \)  (2.x)^{ n−2.m } 
Recurrence law for the basis functions reported
f _{ n } (x)  a _{ n + 1}  a _{ n }  b _{ n }  a _{ n − 1}  f _{0} (x)  f _{1} (x)  

Power  W _{ n } (x)  1  0  1  0  1  _{ X } 
Legendre  P _{ n } (x)  n+1  0  2.n+1  n  1  x 
Laguerre  L _{ n } (x)  n+1  2.n+1  −1  n  1  1−x 
Hermite A  H _{ n } (x)  1  0  2  2.n  1  2.x 
The format used to write a polynomial is chosen in such a way that the pricing procedure becomes operationally more practical. This method proved to be effective throughout the whole process, excluding the possibility that the rank of the coefficient matrix of the least square regression is insufficient. Thus, the explicit form of the Power and Laguerre polynomials is applied, the recurrence law is used to express the Hermite A polynomial, and Rodrigues’ formula is used to write the Legendre polynomial.
Results and discussion
Case 1: Estimated prices for different set of simulated paths
Case 1  Arithmetic floating strike  

PUT  Strike 105  100  500  1000  5000  10000  50000 
Power  5,5292 (0,38652)  5,1195 (0,12007)  5,0274 (0,0677)  4,9441 (0,0346)  4,9519 (0,03081)  4,9541 (0,01721) 
Legendre  5,5277 (0,37698)  5,0311 (0,11412)  5,0073 (0,10189)  4,9647 (0,05079)  4,9573 (0,03045)  4,9511 (0,01641) 
Laguerre  5,4596 (0,26394)  5,1052 (0,24922)  5,0131 (0,07685)  4,9642 (0,0636)  4,9631 (0,02601)  4,9566 (0,01498) 
Hermite A  5,2566 (0,30584)  5,0787 (0,14616)  5,0821 (0,10896)  4,9606 (0,04224)  4,9645 (0,04333)  4,9566 (0,01496) 
PUT  Strike 100  100  500  1000  5000  10000  50000 
Power  4,8737 (0,25913)  4,392 (0,14042)  4,4421 (0,08279)  4,3984 (0,03246)  4,3822 (0,03117)  4,3898 (0,01394) 
Legendre  4,8186 (0,24198)  4,5005 (0,1226)  4,5409 (0,0741)  4,4328 (0,04683)  4,395 (0,025)  4,3905 (0,01458) 
Laguerre  4,8157 (0,26914)  4,4182 (0,14124)  4,4109 (0,07254)  4,394 (0,03582)  4,3984 (0,01837)  4,3906 (0,01461) 
Hermite A  4,8801 (0,26384)  4,5168 (0,12988)  4,4292 (0,0761)  4,3965 (0,04536)  4,3969 (0,02133)  4,3905 (0,01195) 
PUT  Strike 95  100  500  1000  5000  10000  50000 
Power  4,887 (0,44331)  4,5837 (0,10469)  4,5932 (0,10125)  4,4892 (0,05058)  4,4924 (0,02487)  4,4837 (0,01323) 
Legendre  4,905 (0,30647)  4,6709 (0,10534)  4,5098 (0,08731)  4,5039 (0,04946)  4,4732 (0,02929)  4,4846 (0,01352) 
Laguerre  5,0175 (0,30984)  4,565 (0,11335)  4,5149 (0,09689)  4,49 (0,02836)  4,4904 (0,02779)  4,4846 (0,01338) 
Hermite A  5,011 (0,27431)  4,6248 (0,14327)  4,5676 (0,12363)  4,4965 (0,04904)  4,4732 (0,02929)  4,4846 (0,01352) 
CALL  Strike 105  100  500  1000  5000  10000  50000 
Power  3,1783 (0,24351)  3,2916 (0,11733)  3,3286 (0,07488)  3,2771 (0,03209)  3,2903 (0,01621)  3,2758 (0,01799) 
Legendre  3,1421 (0,26638)  3,2268 (0,11876)  3,2538 (0,04496)  3,265 (0,03664)  3,2888 (0,01995)  3,2818 (0,01131) 
Laguerre  3,2969 (0,2)  3,2741 (0,15825)  3,2853 (0,09247)  3,2713 (0,0395)  3,2859 (0,02331)  3,2764 (0,01669) 
Hermite A  3,3147 (0,30627)  3,2757 (0,10231)  3,2679 (0,06761)  3,2849 (0,02703)  3,2796 (0,03082)  3,2764 (0,01668) 
CALL  Strike 100  100  500  1000  5000  10000  50000 
Power  3,0867 (0,38686)  2,984 (0,1241)  3,0561 (0,07181)  3,0186 (0,03374)  2,9977 (0,03123)  3,0122 (0,01231) 
Legendre  3,0231 (0,35521)  3,0533 (0,12091)  3,0219 (0,08862)  3,0323 (0,03966)  3,0275 (0,02892)  3,0125 (0,01349) 
Laguerre  3,1118 (0,38252)  2,9581 (0,13003)  3,0992 (0,07227)  3,0287 (0,03935)  3,0127 (0,02573)  3,0126 (0,01371) 
Hermite A  2,9222 (0,3244)  3,0657 (0,12064)  3,0454 (0,08328)  3,0199 (0,05572)  3,0092 (0,03606)  3,0156 (0,015) 
CALL  Strike 95  100  500  1000  5000  10000  50000 
Power  3,085 (0,23395)  2,9682 (0,16596)  3,0049 (0,05549)  2,9916 (0,03029)  2,9789 (0,02461)  2,9641 (0,01496) 
Legendre  2,8932 (0,2631)  3,0064 (0,12606)  2,987 (0,10273)  2,9663 (0,05163)  2,9482 (0,01573)  2,9644 (0,01507) 
Laguerre  2,8498 (0,26982)  2,9404 (0,11433)  2,9354 (0,07099)  2,9595 (0,03359)  2,9694 (0,02955)  2,9644 (0,01508) 
Hermite A  2,8649 (0,25414)  2,9375 (0,15739)  2,9957 (0,08331)  2,9702 (0,04905)  2,9482 (0,01573)  2,9644 (0,01507) 
Case 2: Estimated prices for different set of simulated paths
Case 2  Geometric floating strike  

PUT  Strike 105  100  500  1000  5000  10000  50000 
Power  5,4008 (0,40284)  5,0057 (0,11024)  4,9288 (0,07604)  4,8491 (0,04653)  4,852 (0,03007)  4,8519 (0,01425) 
Legendre  5,3411 (0,33629)  4,9315 (0,12912)  4,8444 (0,09204)  4,8634 (0,05167)  4,8612 (0,05081)  4,8526 (0,0147) 
Laguerre  5,5355 (0,20011)  4,8723 (0,15434)  4,8561 (0,0866)  4,8863 (0,04501)  4,8703 (0,0353)  4,8529 (0,01454) 
Hermite A  5,3667 (0,41746)  4,9731 (0,13953)  4,9061 (0,08725)  4,8608 (0,04106)  4,858 (0,03583)  4,8524 (0,01237) 
PUT  Strike 100  100  500  1000  5000  10000  50000 
Power  4,8737 (0,2144)  4,392 (0,13649)  4,4421 (0,0691)  4,3984 (0,03888)  4,3822 (0,02424)  4,3898 (0,01473) 
Legendre  4,8186 (0,27618)  4,5005 (0,08995)  4,5409 (0,10719)  4,4328 (0,03967)  4,395 (0,02285)  4,3905 (0,01474) 
Laguerre  4,8157 (0,18517)  4,4182 (0,13916)  4,4109 (0,07725)  4,394 (0,04539)  4,3984 (0,02433)  4,3906 (0,01433) 
Hermite A  4,8801 (0,20338)  4,5168 (0,16687)  4,4292 (0,07855)  4,3965 (0,03733)  4,3969 (0,02125)  4,3905 (0,01342) 
PUT  Strike 95  100  500  1000  5000  10000  50000 
Power  4,8737 (0,2946)  4,392 (0,15808)  4,4421 (0,07126)  4,3984 (0,04749)  4,3822 (0,02766)  4,3898 (0,0129) 
Legendre  4,8186 (0,21728)  4,5005 (0,13473)  4,5409 (0,08409)  4,4328 (0,03236)  4,395 (0,03323)  4,3905 (0,01331) 
Laguerre  4,8157 (0,20457)  4,4182 (0,11763)  4,4109 (0,06621)  4,394 (0,03963)  4,3984 (0,02963)  4,3906 (0,01332) 
Hermite A  4,8801 (0,54061)  4,5168 (0,19166)  4,4292 (0,11576)  4,3965 (0,05203)  4,3969 (0,04185)  4,3905 (0,01331) 
CALL  Strike 105  100  500  1000  5000  10000  50000 
Power  3,2097 (0,22214)  3,3416 (0,12657)  3,3249 (0,09254)  3,336 (0,03828)  3,324 (0,03941)  3,3293 (0,01685) 
Legendre  3,214 (0,28978)  3,3615 (0,14556)  3,3733 (0,09039)  3,321 (0,04469)  3,3486 (0,0313)  3,3296 (0,01689) 
Laguerre  3,252 (0,28853)  3,3193 (0,13172)  3,354 (0,10208)  3,3189 (0,02632)  3,3495 (0,02309)  3,3297 (0,01692) 
Hermite A  3,3304 (0,21868)  3,4262 (0,14675)  3,2753 (0,07181)  3,3237 (0,05071)  3,3376 (0,02572)  3,3297 (0,01661) 
CALL  Strike 100  100  500  1000  5000  10000  50000 
Power  3,0867 (0,35108)  2,984 (0,13725)  3,0561 (0,09443)  3,0186 (0,03458)  2,9977 (0,02952)  3,0122 (0,01336) 
Legendre  3,0231 (0,27413)  3,0533 (0,09543)  3,0219 (0,08744)  3,0323 (0,04844)  3,0275 (0,03365)  3,0125 (0,01356) 
Laguerre  3,1118 (0,31237)  2,9581 (0,15785)  3,0992 (0,08248)  3,0287 (0,04877)  3,0127 (0,03003)  3,0126 (0,01666) 
Hermite A  2,9222 (0,35909)  3,0657 (0,1357)  3,0454 (0,05049)  3,0199 (0,03075)  3,0092 (0,02814)  3,0156 (0,01356) 
CALL  Strike 95  100  500  1000  5000  10000  50000 
Power  3,0867 (0,2807)  2,984 (0,07714)  3,0561 (0,069)  3,0186 (0,05047)  2,9977 (0,01636)  3,0122 (0,01525) 
Legendre  3,0231 (0,24697)  3,0533 (0,14612)  3,0219 (0,09397)  3,0323 (0,02256)  3,0275 (0,02232)  3,0125 (0,01527) 
Laguerre  3,1118 (0,22394)  2,9581 (0,09095)  3,0992 (0,09578)  3,0287 (0,02069)  3,0127 (0,02792)  3,0126 (0,01531) 
Hermite A  2,9222 (0,2811)  3,0657 (0,08468)  3,0454 (0,09731)  3,0199 (0,0453)  3,0092 (0,01941)  3,0156 (0,01422) 
Case 3: Estimated prices for different set of simulated paths
Case 3  Arithmetic fixed strike  

PUT  Strike 105  100  500  1000  5000  10000  50000 
Power  6,7237 (0,33767)  6,7068 (0,10996)  6,6948 (0,07619)  6,6841 (0,05154)  6,6669 (0,05266)  6,6692 (0,02473) 
Legendre  6,6299 (0,25683)  6,7175 (0,11842)  6,636 (0,0711)  6,6629 (0,04606)  6,6631 (0,0545)  6,6622 (0,02162) 
Laguerre  6,7273 (0,34734)  6,6902 (0,10582)  6,7413 (0,09639)  6,6739 (0,0597)  6,666 (0,05421)  6,6622 (0,02166) 
Hermite A  6,7695 (0,37345)  6,7103 (0,09924)  6,7262 (0,17196)  6,6625 (0,04541)  6,6481 (0,02537)  6,6622 (0,02167) 
PUT  Strike 100  100  500  1000  5000  10000  50000 
Power  4,8737 (0,20587)  4,392 (0,08289)  4,4421 (0,05145)  4,3984 (0,02722)  4,3822 (0,01973)  4,3898 (0,0101) 
Legendre  4,8186 (0,22622)  4,5005 (0,08516)  4,5409 (0,06124)  4,4328 (0,02677)  4,395 (0,02303)  4,3905 (0,01009) 
Laguerre  4,8157 (0,18574)  4,4182 (0,07473)  4,4109 (0,04725)  4,394 (0,03594)  4,3984 (0,01532)  4,3906 (0,01004) 
Hermite A  4,8801 (0,19166)  4,5168 (0,08783)  4,4292 (0,0467)  4,3965 (0,02859)  4,3969 (0,01286)  4,3905 (0,01001) 
PUT  Strike 95  100  500  1000  5000  10000  50000 
Power  1,5292 (0,23719)  1,6134 (0,15668)  1,6079 (0,10196)  1,5839 (0,02465)  1,5744 (0,01738)  1,5612 (0,01605) 
Legendre  1,6529 (0,24375)  1,5715 (0,09924)  1,5483 (0,06678)  1,5543 (0,03563)  1,5712 (0,02131)  1,5609 (0,0159) 
Laguerre  1,66 (0,30421)  1,5603 (0,09967)  1,6074 (0,11454)  1,5781 (0,02878)  1,5747 (0,01671)  1,5609 (0,0159) 
Hermite A  1,6873 (0,35452)  1,5603 (0,09967)  1,6074 (0,11454)  1,5781 (0,02882)  1,5747 (0,01667)  1,5609 (0,0159) 
CALL  Strike 105  100  500  1000  5000  10000  50000 
Power  0,6458 (0,07247)  0,6472 (0,0309)  0,655 (0,02674)  0,6554 (0,02315)  0,6488 (0,01533)  0,6547 (0,00766) 
Legendre  0,6166 (0,14273)  0,6607 (0,03518)  0,662 (0,03774)  0,6557 (0,01901)  0,6524 (0,01889)  0,6539 (0,00705) 
Laguerre  0,5946 (0,08017)  0,6477 (0,04393)  0,6554 (0,0448)  0,6585 (0,02542)  0,649 (0,01538)  0,6539 (0,00705) 
Hermite A  0,6286 (0,10374)  0,6688 (0,04487)  0,6663 (0,02847)  0,6532 (0,01512)  0,6508 (0,01129)  0,6539 (0,00705) 
CALL  Strike 100  100  500  1000  5000  10000  50000 
Power  3,0867 (0,37492)  2,984 (0,10728)  3,0561 (0,0726)  3,0186 (0,06132)  2,9977 (0,04801)  3,0122 (0,01715) 
Legendre  3,0231 (0,35095)  3,0533 (0,13885)  3,0219 (0,08161)  3,0323 (0,05333)  3,0275 (0,04622)  3,0125 (0,01748) 
Laguerre  3,1118 (0,31191)  2,9581 (0,1255)  3,0992 (0,09784)  3,0287 (0,066)  3,0127 (0,03268)  3,0126 (0,01796) 
Hermite A  2,9222 (0,35167)  3,0657 (0,16015)  3,0454 (0,0979)  3,0199 (0,05945)  3,0092 (0,03579)  3,0156 (0,01795) 
CALL  Strike 95  100  500  1000  5000  10000  50000 
Power  5,5638 (0,06386)  5,5919 (0,04907)  5,5676 (0,03613)  5,5884 (0,01042)  5,5865 (0,00963)  5,5795 (0,00573) 
Legendre  5,5388 (0,06966)  5,5773 (0,02321)  5,5956 (0,03641)  5,5818 (0,0193)  5,5825 (0,01016)  5,5795 (0,00576) 
Laguerre  5,617 (0,11439)  5,5729 (0,04111)  5,5777 (0,03414)  5,5875 (0,01177)  5,5865 (0,00956)  5,5795 (0,00576) 
Hermite A  5,6234 (0,10946)  5,5729 (0,04111)  5,5777 (0,03414)  5,5875 (0,01177)  5,5865 (0,00956)  5,5795 (0,00576) 
Case 4: Estimated prices for different set of simulated paths
Case 4  Geometric fixed strike  

PUT  Strike 105  100  500  1000  5000  10000  50000 
Power  6,8045 (0,23302)  6,8008 (0,13203)  6,7869 (0,07603)  6,7925 (0,05448)  6,7882 (0,03496)  6,801 (0,02277) 
Legendre  6,7919 (0,32414)  6,8177 (0,15514)  6,8438 (0,05622)  6,8042 (0,06049)  6,7796 (0,04728)  6,7942 (0,02165) 
Laguerre  6,9194 (0,20012)  6,838 (0,14021)  6,8201 (0,07885)  6,8014 (0,05276)  6,8106 (0,03512)  6,7942 (0,02156) 
Hermite A  6,8552 (0,26187)  6,8255 (0,09763)  6,8773 (0,11303)  6,809 (0,04093)  6,7957 (0,03321)  6,7967 (0,02055) 
PUT  Strike 100  100  500  1000  5000  10000  50000 
Power  4,8737 (0,19727)  4,392 (0,10796)  4,4421 (0,04911)  4,3984 (0,03353)  4,3822 (0,01958)  4,3898 (0,00954) 
Legendre  4,8186 (0,15306)  4,5005 (0,05025)  4,5409 (0,04643)  4,4328 (0,02551)  4,395 (0,01771)  4,3905 (0,0067) 
Laguerre  4,8157 (0,21805)  4,4182 (0,07679)  4,4109 (0,04758)  4,394 (0,0257)  4,3984 (0,02187)  4,3906 (0,00958) 
Hermite A  4,8801 (0,22004)  4,5168 (0,07318)  4,4292 (0,04935)  4,3965 (0,02862)  4,3969 (0,0216)  4,3905 (0,00917) 
PUT  Strike 95  100  500  1000  5000  10000  50000 
Power  1,7424 (0,32208)  1,6518 (0,10318)  1,6974 (0,12042)  1,6701 (0,03038)  1,6648 (0,01796)  1,6514 (0,01658) 
Legendre  1,6857 (0,42331)  1,7019 (0,17981)  1,6196 (0,08402)  1,6541 (0,03042)  1,6618 (0,02214)  1,6512 (0,01646) 
Laguerre  1,7466 (0,32841)  1,6519 (0,10429)  1,697 (0,11716)  1,6682 (0,02973)  1,6652 (0,01772)  1,6512 (0,01645) 
Hermite A  1,7466 (0,32841)  1,6519 (0,10429)  1,697 (0,11716)  1,6682 (0,02974)  1,6651 (0,01771)  1,6512 (0,01646) 
CALL  Strike 105  100  500  1000  5000  10000  50000 
Power  0,5694 (0,11528)  0,6052 (0,02571)  0,6195 (0,0231)  0,6091 (0,02097)  0,609 (0,00636)  0,6107 (0,00642) 
Legendre  0,5937 (0,12399)  0,6198 (0,05949)  0,6181 (0,04114)  0,6153 (0,01535)  0,6111 (0,01035)  0,6096 (0,00624) 
Laguerre  0,5683 (0,08619)  0,6195 (0,03649)  0,5991 (0,02705)  0,6056 (0,01875)  0,6075 (0,01303)  0,6096 (0,00624) 
Hermite A  0,639 (0,08424)  0,6061 (0,05311)  0,6229 (0,03654)  0,6164 (0,01723)  0,6094 (0,01446)  0,6097 (0,00549) 
CALL  Strike 100  100  500  1000  5000  10000  50000 
Power  3,0867 (0,28263)  2,984 (0,18382)  3,0561 (0,11169)  3,0186 (0,04615)  2,9977 (0,03817)  3,0122 (0,01919) 
Legendre  3,0231 (0,26407)  3,0533 (0,10516)  3,0219 (0,10515)  3,0323 (0,06786)  3,0275 (0,03656)  3,0125 (0,01501) 
Laguerre  3,1118 (0,39224)  2,9581 (0,14587)  3,0992 (0,09989)  3,0287 (0,05675)  3,0127 (0,03434)  3,0126 (0,02285) 
Hermite A  2,9222 (0,32296)  3,0657 (0,12974)  3,0454 (0,08487)  3,0199 (0,05707)  3,0092 (0,04068)  3,0156 (0,01976) 
CALL  Strike 95  100  500  1000  5000  10000  50000 
Power  5,5603 (0,10979)  5,5171 (0,04009)  5,5203 (0,03478)  5,5298 (0,01079)  5,5283 (0,00947)  5,5215 (0,00545) 
Legendre  5,4441 (0,08543)  5,5499 (0,06434)  5,5135 (0,02599)  5,5259 (0,01888)  5,5246 (0,01067)  5,5214 (0,00543) 
Laguerre  5,5604 (0,10972)  5,5173 (0,04024)  5,5202 (0,03487)  5,5299 (0,01076)  5,5282 (0,00947)  5,5214 (0,00543) 
Hermite A  5,5604 (0,10972)  5,5173 (0,04024)  5,5202 (0,03487)  5,5299 (0,01076)  5,5282 (0,00947)  5,5214 (0,00543) 
Such pattern is the same for both put options and for call options of all the American Asian options considered. This result suggests two basic conclusions. First, it ratifies one of the main features of the method: if all of the polynomial basis are orthogonal, then theoretically all of them could be indistinctly used in derivative pricing. Second, it shows that the gradual reduction of differences among the price estimates for each of the basis due to the incremental increase in the number of simulated paths is a direct result of the law of large numbers.
The polynomial basis whose standard deviation is the lowest at 50.000 simulated paths
PUT  
Strike  Case 1  Case 2  Case 3  Case 4 
95  Power  Power  Legendre  Laguerre 
100  Hermite A  Hermite A  Hermite A  Legendre 
105  Hermite A  Hermite A  Legendre  Hermite A 
CALL  
Strike  Case 1  Case 2  Case 3  Case 4 
95  Power  Hermite A  Power  Legendre 
100  Power  Power  Power  Legendre 
105  Legendre  Hermite A  Legendre  Hermite A 
When analyzing one of the cases in study throughout strike prices, we observe that a specific basis delivers the lowest standard deviation in most of experiments. For example, in case 1, if it is a put option, then Hermite A delivers a price whose standard deviation is the lowest in two of the three set of parameters used. Whereas, for example, in case 3 for a call option across all strike prices considered, the polynomial basis that delivers a price with the lowest standard deviation is power. By repeating this process of column analysis of Table 8, in most of strikes considered, when pricing an American Asian put option, Hermite A provides a better performance to the algorithm. On the other hand, when pricing an American Asian call option, Power provides a better performance through different strikes.
Considering a specific strike price throughout cases in Table 8, we figure out that the same feature happens, i.e., there is, in most cases, one polynomial basis whose price delivered has the lowest standard deviation. For example, for a put option whose strike price is 100 in three out of the four cases studied, Hermite A delivers the lowest standard deviation for the price estimates. Whereas, for a call option with the same strike price, the polynomial basis power provides a better performance, i.e., the lowest standard deviation in most cases. By proceeding this process of row analysis in Table 8, we got in most cases when pricing an American Asian put option that Hermite A had the best performance. Whereas when pricing an American Asian call option, Power delivers a better performance in most of cases.
These results suggest that pricing American Asian options using the LeastSquares Monte Carlo Method enables the selection of one polynomial basis, regardless of the kind of Amerasian. In fact, the main concern is whether we are pricing put or call option.
Conclusions
Our experiments using the four chosen polynomial basis ratified one of the method’s elements, i.e., that any orthogonal polynomial basis can be used for pricing American Asian options, since in all of the simulated paths the estimated prices of the options are virtually the same.
For all of the Amerasian options priced, and for each of the basis used, the convergence of the price estimate results from the decrease of the standard deviation while the number of simulated paths increases.
Considering 50,000 simulated trajectories, our study suggests that it is possible to empirically choose one specific polynomial basis for pricing an American Asian option. The results show that one polynomial basis is marginally more accurate than others, by providing a lower standard deviation it delivers a better performance to the algorithm when pricing a complex option as American Asian options. Such empirical outcome is theoretically unpredictable, since in principle all basis can be indistinctly used when pricing the derivative.
Therefore, for practical purposes, if a trader is looking for a faster and more accurate way to valuing an American Asian call option, the polynomial basis suggested to perform this procedure is Hermite A. On the other hand, if their concern is valuing an Amerasian put option, the Power polynomial basis is recommended. This speediness means being capable of measuring the worthiness of any derivative in order to screen accurately business opportunities not only for hedge purposes but also for arbitrage purposes.
Where Ω is the set of all possible paths; ℑ is the filter of events at a certain time; and Q is the riskneutral probability measure of the elements of ℑ
Hilbert space is a vector space with internal product and complete regarding the rule set for this internal product
The FixedStart Time Window Asian options are options whose number of elements’ average increases in time, having its beginning at some point of the timeline
Declarations
Open AccessThis article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.
Authors’ Affiliations
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