1. Introduction
Fractional differential equations are an essential means of modeling complex processes in different fields of science [
3,
10,
35,
50,
51,
53]. The Riemann-Liouville fractional integral of order
is defined as
When
n is a positive integer and
, the Caputo and Riemann-Liouville fractional derivatives of order
are defined as
The Caputo and Riemann-Liouville fractional derivatives are related as
Without loss of generality the lower limit of the integral in the definition of fractional derivative is zero. When
the Caputo derivative is defined as
Fractional derivatives and integrals are nonlocal and have a singularity at the endpoint. The properties of the fractional derivatives make them an important tool for describing memory processes. The exponential, sine and cosine functions have Caputo derivatives,
where
is the Mittag-Lefler function
Finite difference schemes for numerical solution of fractional differential equations use discretizations of the fractional derivative. Two important discretizations of the Caputo fractional derivative are the Grünwald difference approximation and L1 approximation [
8,
26,
30,
49]. Grünwald difference approximation has a first order accuracy and a generating function
. Central difference approximations of integer order derivatives have a second order accuracy. Grünwald difference approximation is a second order shifted approximation of the fractional derivative with a shift parameter
, and it is a generalization of finite difference approximations [
37,
58]. L1 approximation has an order
and a generating function
. In Apostolov [
7] and Dimitrov [
16] we use the L1 approximation and approximations of the second derivative for construction of a second order approximations of the fractional derivative. Alikhanov [
4] and Gao et al. [
22] construct approximations of the fractional derivative of order
, which are called
and
formulas. Finite difference schemes using L2 formula approximations of the fractional derivative of order
, and their convergence are studied by Alikhanov [
5], Lv and Xu [
33], Wong and Ren [
55]. High order approximations of the fractional derivative and finite difference schemes for fractional differential equations are constructed in [
8,
9,
12,
14,
29,
32,
44,
48,
57]. Navot [
38] uses Taylor polynomials to deal with the singularity of the fractional integral
. He derives the asymptotic formula for Riemann sums on a uniform net, called extended Euler-Maclaurin summation formula. The formula is extended in Navot [
39] to functions with a logarithmic singularity. In [
18] we derive the asymptotic formula of the Riemann sum of the fractional integral using the series expansion of the generating function
. Other types of numerical methods for fractional differential equations include fractional multistep methods and methods using spline interpolation and wavelets [
1,
20,
31,
34,
46,
47].
Let
n be a positive integer,
and
for
. In [
17] we derive an approximation of Caputo fractional derivative and its asymptotic formula
Approximation (
1) has a generating function
, the polylogarithmic function of order
. By substituting the derivative in the right-hand side of (1) using first order backward difference
we find an approximation of the fractional derivative
Approximations (
1) and (
2) have an order
when the function
f satisfies the condition
. In paper [
17] we extend approximation (
2) to all functions in the class
by assigning values of the last two weights.
where
. In this paper we investigate the properties of approximations (
2) and (
3) and applications of the approximations for numerical solution of ordinary and partial fractional differential equations. The outline of the paper is as follows. In section 2 we study the properties of the weights of approximation (
3) and we derive the inequality
In section 3 we derive estimates for the errors of approximations (
2) and (
3). In sections 4 and 5 we construct numerical solutions of the two-term ordinary fractional differential equation and the time-fractional Black-Scholes equation for option pricing and we prove the convergence and order of the methods.
2. Properties of the Weights
L1 approximation and approximation (
2) have an order
and similar performance and properties of the weights [
17]
The weights of
and
of approximation (
2) are chosen such that the values of
and
are equal to the fractional derivatives.
In this section we prove inequality (
7) and we derive an estimate for the weight
of approximation (
2). The proof uses the inequalities in Claim 1 and Claim 2.
Claim 1.
Let and . Then
Proof. From the binomial formula
The numbers
are negative for
. Then
□
Proof. The Riemann zeta function has a series expansion [
36]
where
is Euler’s constant and
are Stieltjes constants
The value of
. From Taylor’s Theorem
Inequality (
9) holds when
The function
has a first derivative
and a minimum value
. Therefore
is positive on
. □
The asymptotic formula of
is obtained from the asymptotic formula of the fractional integral [
18,
38]
Let
. From the properties of gamma function
From (
13) we find the asymptotic formula of
of order
Proof.
Sum of the
-th powers of the first
integers has an asymptotic formula [
21]
where
are the Bernoulli numbers. Formula (
15) is derived using Euler-Maclaurin formula and the actual value of
lies between two consecutive partial sums [
21]. Then
and
From Claim 2 it follows that
□
Now we derive an estimate for the weight
of approximation (
3). Denote
3. Estimate for the Error
In this section we use the method from [
38] to derive estimates for the errors of approximations (
2) and (
3). Let
and
The function
satisfies
. From Taylor’s Theorem
where
for
. Let
Then
Denote
. The function
satisfies
and its second derivative of is not defined at the point
x.
Lemma 6.
Let . Then
Proof.
The function
satisfies
The fractional derivative of the function
satisfies
From (
17) and (
18) it follows that
□
The trapezoidal rule of a function
has a second order accuracy when
. The error of the trapezoidal rule
satisfies [
56]
The second derivative of the function
is undefined at the point
x, which leads to a lower order of accuracy of the trapezoidal rule in the interval
. Now we estimate the error of the trapezoidal rule of the function
. Let
and
be the error of trapezoidal rule of
in the interval
.
Proof. The error
of trapezoidal rule (
19) satisfies
□
Let
be the error of the trapezoidal rule of
in the interval
.
Proof.
The error
satisfies
□
Let be the error of the trapezoidal rule of in the interval .
Let
be the error of approximation (
1).
Theorem 10.
Let . Then
Proof. The trapezoidal rule of the function
on the interval
satisfies
and the function
has a value at zero
From the definition (
16) of the function
From Taylor’s Theorem
where
for
. Therefore
The terms on the right hand side of (
21) satisfy the estimates
□
Let
be the error of approximation (
2).
Approximation (
2) is constructed from approximation (
1) by substituting
with first order backward difference approximation
.
Claim 11.
Let and . Then
Proof. From Taylor’s Theorem
where
. The error
of approximation (
2) satisfies
□
Let
be the error of approximation (
3).
The weights of approximation (3) are defined with (4), (5) and (6). Denote
The function
satisfies
and the second and third derivatives of
f and
are equal. Therefore
Lemma 12.
Let . Then
4. Numerical Solution of Two-Term Equation
The two-term equation is an ordinary fractional differential equation in the form
Numerical and analytical solutions of ordinary fractional differential equations are studied in [
6,
24,
25,
41,
43,
45]. In this section we construct the numerical solution of the two-term equation (
22) which uses approximation (
3) of the fractional derivative and prove its convergence and order. Let
and
for
. By approximating the fractional derivative at the point
we find
where
.
The numerical solution
of equation (
22) is computed as
The value of the numerical solution
on the first step is computed with the following approximation [
17]
From the estimate for the error of L1 approximation [
8]
where
. Numerical solution (
23) has initial conditions [
17]
When the solution of two-term equation (
22) satisfies the condition
both approximations (
2) and (
3) can be used for computation of numerical solution (
23).
Example 1: Consider the following two-term equation
Two-term equation (
26) has a solution
which satisfies
. Experimental results for the error and order of numerical solution (
23) of equation (
26) which uses approximation (
2) of the fractional derivative are given in
Table 1 and
Table 2.
Example 2:Equation (
27) has a solution
. Experimental results for the error and order of numerical solution (
23) of equation (
27) are given in
Table 3 and
Table 4. The experimental results in
Table 1,
Table 2,
Table 3 and
Table 4 suggest that numerical solution (
23) of two-term equation (
22) converges and has an order
for all positive values of the parameter
D and negative values with small and large modulus.
Denote by
the error of numerical solution (
23) at the point
, where
. The errors
satisfy
In Theorem 13 and Theorem 14 we prove the convergence of numerical solution (
23) of two-term equation (
22) and derive estimates for the error, depending on the value of the parameter
D. The proofs use induction on
n, where
.
Theorem 13.
Let and . Then
where .
Proof. The value of the error
on the first step satisfies
When
the denominator
and
Now we estimate the error
when the parameter
.
From (
10)
Hence
In this case the denominator of (
30) is again greater than one,
and the error
satisfies
Suppose that inequality (
29) holds for all
. The values of
and
are negative. In both cases
and
the following estimate holds
□
Theorem 14.
Let and . Then
where .
Proof. The error
on the first step satisfies the bound
Assume that (
31) holds for all
. Then
□
From Theorem 13 and Theorem 14 the errors
of numerical solution (
23) of the two-term equation in the interval
, satisfy the estimate
for all
. Now we generalize the results of Theorem 13 and Theorem 14 to an arbitrary interval
. Consider the two-term equation
Substitute
and
The function
satisfies a two-term equation
Let
be an
N-dimensional vector with the errors of numerical solution (
23) of equation (
33). The
(maximum) norm of a vector is the maximum of the absolute values of its elements. From Theorem 13 and Theorem 14 we get conditions for the convergence of numerical solution (
23) of two-term equations (
33) and (
34).
Corollary 15.
The maximum error of numerical solution (23) of two-term equation (33), satisfies
when the solution and ,
□
5. Time Fractional Black–Scholes Equation
The time fractional Black–Scholes equation is a fractional partial differential equation which is used for modeling the prices of the options [
1,
11,
13,
28,
42,
54,
59].
where
C is the option price,
T is the expiry time,
r is the risk-free rate,
is the volatility and
S is the underlying stock price. Fractional Black-Scholes equation (
35) has terminal and boundary conditions
and the fractional derivative is
The terminal condition is transformed to an initial condition with the substitution [
59]
By applying the substitution to (
36) we find [
59]
The function
satisfies the partial fractional differential equation
The substitution
transforms (
37) into a linear partial fractional differential equation [
59]
Finite difference schemes for the time fractional Black-Scholes equation are constructed in [
19,
23,
52,
59]. Now we construct an implicit finite difference scheme which uses approximation (
3) of the fractional derivative and central difference approximations of the partial derivatives for the following time fractional Black-Scholes equation
where
. Equation (
39) has initial and boundary conditions
Let
M and
N be positive integers and
be a rectangular grid on
which has a step size
in space and
in time,
Denote
. The central difference approximations of the partial derivatives of equation (
39) have second order accuracy
where
and
. The numbers
and
are bounds for the third and fourth order partial derivatives
The numerical solution
of equation (
39) on layer
m of the grid
satisfies
for
and has has initial conditions
Denote
and
The numerical solution of time-fractional Black-Scholes equation (
39) is a solution of the system of linear equations
Denote by
the error of finite difference scheme (
40) at the point
and by
and
be the the truncation errors of the approximations of the left-hand and right-hand sides of (
39). The errors
on row
of the grid
satisfy
The errors are equal to zero,
at the boundary points of
. Let
be the
-dimensional tridiagonal matrix with entries
on the main diagonal and
and
bellow and above the main diagonal. The error vector
of row
m is a solution of the matrix equation
where
The numerical solution on the first row of
is computed with approximation (
24)
Denote
. Then
where
and
The errors of the numerical solution of the fractional Black-Scholes equation (
39) on the first row of
are the solutions of the system of linear equations
Let
be the
-dimensional tridiagonal matrix with elements
and
. The error vector for the first row satisfies
where
Let
for all
and
. The
norm of a matrix is the maximum of the absolute row sums.
Theorem 16.
Let and . Then
for all .
Proof. When
, the gamma function satisfies [
15]
When
we have that
The matrices
and
are
M-matrices. From the Ahlberg-Nilson-Varah bound [
27,
40]
The
norm of the error vector of the first row of
satisfies the bound
Suppose that inequality (
42) holds for all
. From (
41)
□
Corollary 17.
for all .
Example 3: Consider the following time fractional Black-Scholes equation
Equation (
43) has a solution
. Experimental results of the numerical solution of equation (
43) with parameters
are given in
Table 5 and
Table 6. The orders of convergence of the finite difference scheme are
in time and
in space.
Example 4: Consider the time fractional Black-Scholes equation (
37) for pricing European call options, with a source term
and initial and boudary conditions
The European call option premium curves for different values of
are given in
Figure 1, for values of the parameters
,
,
,
,
(year) and strike price
. Regarding near-the-money options, lower values of
prices them lower, and evaluates higher out-of-the-money and in-the-money options, compared to the classical Black-Scholes dynamics.
The graphs of call option and put option premiums for
and all
t are given in
Figure 2 and
Figure 3.
6. Conclusions
In this paper we study the convergence and order of numerical solutions of ordinary and partial fractional differential equations which use approximation (
3) of the fractional derivative. The results of the numerical experiments given in the paper illustrate the theoretical results. In future work we will use the method from [
7] for construction of secon-order and high-order approximations of the fractional derivative and we will study the convergence of the finite difference schemes for numerical solution of fractional differential equations.
Author Contributions
Conceptualization, Y.D and V.T.; Methodology, Y.D. and S.A.; Software, S.G.; Validation, V.T.; Formal analysis, Y.D.; Writing–original draft preparation, Y.D. and S.G.; writing–review and editing, Y.D. and V.T.; Visualization, S.G.; Project administration, Y.D. and V.T.; Funding acquisition, S.G. All authors have read and agreed to the published version of the manuscript.
Funding
This study is supported by the Bulgarian National Science Fund under Project KP-06-M62/1 “Numerical deterministic, stochastic, machine and deep learning methods with applications in computational, quantitative, algorithmic finance, biomathematics, ecology and algebra” from 2022 and by the National Program “Young Scientists and Postdoctoral Researchers - 2” – Bulgarian Academy of Sciences.
Conflicts of Interest
The authors declare no conflict of interest.
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