Dual identities in fractional difference calculus within Riemann. Thabet Abdeljawad a b

Size: px
Start display at page:

Download "Dual identities in fractional difference calculus within Riemann. Thabet Abdeljawad a b"

Transcription

1 Dual identities in fractional difference calculus within Riemann Thabet Abdeljawad a b a Department of Mathematics, Çankaya University, 06530, Ankara, Turkey b Department of Mathematics and Physical Sciences arxiv:2.5795v2 [math.ds] 8 Jan 203 Prince Sultan University, P. O. Box 66833, Riyadh 586, Saudi Arabia Abstract. We Investigate two types of dual identities for Riemann fractional sums and differences. The first type relates nabla and delta type fractional sums and differences. The second type represented by the Q-operator relates left and right fractional sums and differences. These dual identities insist that in the definition of right fractional differences we have to use both the nabla and delta operators. The solution representation for higher order Riemann fractional difference equation is obtained as well. Keywords: right (left) delta and nabla fractional sums, right (left) delta and nabla Riemann. Q-operator, dual identity. Introduction During the last two decades, due to its widespread applications in different fields of science and engineering, fractional calculus has attracted the attention of many researchers [9, 0,, 23, 24, 25]. Starting from the idea of discretizing the Cauchy integral formula, Miller and Ross [8] and Gray and Zhang [8] obtained discrete versions of left type fractional integrals and derivatives, called fractional sums and differences. Fifteen years later, several authors started to deal with discrete fractional calculus [, 3, 4, 5, 6, 4, 2, 20, 2, 22], benefiting from the theory of time scales originated by Hilger in 988 (see [5]). In this article, we summarize some of the results mentioned in the above references and add more in right type fractional differences and the higher order. Throughout the article we almost agree with the previously presented definitions except for the definition of right fractional difference. We shall figure out that these definitions seem to be more convenient than the previously presented ones by proving some dual identities. These identities fall into two kinds. The first relates nabla type fractional differences and sums to delta ones. The second kind represented by the Q-operator relates left and right fractional sums and differences. This setting enables us to get identities resembling better the ordinary fractional case. Along with the previously mentioned points we are able to fit a reasonable nabla integration by parts formula which remains in accordance with the one obtained in [2] but different from those obtained in [6] and [4]. The obtained dual identities are also used to obtain a delta integration by parts formula from the nabla one. The solution representation for the higher order Riemann fractional difference equation is obtained as well and thus the result in [27] is generalized. We shall see that the higher order Riemann fractional difference initial value problem of non-integer order needs only one initial condition which is not the case for the higher order difference equation (i.e of positive integer order). The article is organized as follows: The remaining part of this section contains summary to some of the basic notations and definitions in delta and nabla calculus. Section 2 contains the definitions in the frame of delta and nabla fractional sums and differences in the Riemann sense. Moreover, some essential lemmas about the commutativity of the different fractional sum operators with the usual difference operators are established. These lemmas are vital to proceed in the next sections. The third section contains some dual identities relating nabla and delta fractional sums and differences in the left and right cases. Using these dual identities, power formulae for nabla left and right fractional sums and a commutative law for nabla left and right sums are obtained. In Section 4 the integration by parts formula for nabla fractional sums and differences obtained in [27] is used by the help of the dual identities to obtain delta integration by parts formulas. Section 5 is devoted to higher order initial fractional difference value problems into Riemann. Finally, in Section 6 the Q-operator is used

2 to relate left and right fractional sums in the nabla and delta case and hence relates delta and nabla Riemann fractional differences. The Q-dual identities obtained in this section expose the validity of the definition of delta and nabla right fractional differences where the delta and nabla operators are used in each of the definitions of delta and nabla right fractional differences. For a natural number n, the fractional polynomial is defined by, n t (n) = (t j) = Γ(t+) Γ(t+ n), () j=0 where Γ denotes the special gamma function and the product is zero when t+ j = 0 for some j. More generally, for arbitrary α, define t (α) = Γ(t+) Γ(t+ α), (2) where the convention that division at pole yields zero. Given that the forward and backward difference operators are defined by f(t) = f(t+) f(t), f(t) = f(t) f(t ) (3) respectively, we define iteratively the operators m = ( m ) and m = ( m ), where m is a natural number. Here are some properties of the factorial function. Lemma.. ([3]) Assume the following factorial functions are well defined. (i) t (α) = αt (α ). (ii) (t µ)t (µ) = t (µ+), where µ R. (iii) µ (µ) = Γ(µ+). (iv) If t r, then t (α) r (α) for any α > r. (v) If 0 < α <, then t (αν) (t (ν) ) α. (vi) t (α+β) = (t β) (α) t (β). Also, for our purposes we list down the following two properties, the proofs of which are straightforward. s(s t) (α ) = (α )(ρ(s) t) (α 2). (4) t(ρ(s) t) (α ) = (α )(ρ(s) t) (α 2). (5) For the sake of the nabla fractional calculus we have the following definition Definition.. ([5, 6, 7, 9]) (i) For a natural number m, the m rising (ascending) factorial of t is defined by (ii) For any real number the α rising function is defined by m t m = (t+k), t 0 =. (6) t α = Γ(t+α), t R {..., 2,,0}, 0 α = 0 (7) Γ(t) Regarding the rising factorial function we observe the following: (i) (t α ) = αt α (8) (ii) (t α ) = (t+α ) (α). (9) (iii) t(s ρ(t)) α = α(s ρ(t)) α (0) Notation: (i) For a real α > 0, we set n = [α]+, where [α] is the greatest integer less than α. (ii) For real numbers a and b, we denote N a = {a,a+,...} and b N = {b,b,...}. (iii) For n N and real a, we denote (iv) For n N and real b, we denote n f(t) ( ) n n f(t). n f(t) ( ) n n f(t). 2

3 2 Definitions and essential lemmas Definition 2.. Let σ(t) = t+ and ρ(t) = t be the forward and backward jumping operators, respectively. Then (i) The (delta) left fractional sum of order α > 0 (starting from a) is defined by: α a f(t) = t α (t σ(s)) (α ) f(s), t N a+α. () s=a (ii) The (delta) right fractional sum of order α > 0 (ending at b) is defined by: b α f(t) = b (s σ(t)) (α ) f(s) = b (ρ(s) t) (α ) f(s), t b α N. (2) +α +α (iii) The (nabla) left fractional sum of order α > 0 (starting from a) is defined by: a f(t) = t s=a+ (t ρ(s)) α f(s), t N a+. (3) (iv)the (nabla) right fractional sum of order α > 0 (ending at b) is defined by: b f(t) = b (s ρ(t)) α f(s) = Regarding the delta left fractional sum we observe the following: (i) α a maps functions defined on N a to functions defined on N a+α. (ii) u(t) = n a f(t), n N, satisfies the initial value problem b (σ(s) t) α f(s), t b N. (4) n u(t) = f(t), t N a, u(a+j ) = 0, j =,2,...,n. (5) (iii) The Cauchy function (t σ(s))(n ) (n )! vanishes at s = t (n ),...,t. Regarding the delta right fractional sum we observe the following: (i) b α maps functions defined on b N to functions defined on b α N. (ii) u(t) = b n f(t), n N, satisfies the initial value problem n u(t) = f(t), t bn, u(b j +) = 0, j =,2,...,n. (6) (iii) the Cauchy function (ρ(s) t)(n ) (n )! vanishes at s = t+,t+2,...,t+(n ). Regarding the nabla left fractional sum we observe the following: (i) a maps functions defined on N a to functions defined on N a. (ii) n a f(t) satisfies the n-th order discrete initial value problem n y(t) = f(t), i y(a) = 0, i = 0,,...,n (7) (iii) The Cauchy function (t ρ(s))n Γ(n) satisfies n y(t) = 0. Regarding the nabla right fractional sum we observe the following: (i) b maps functions defined on b N to functions defined on b N. (ii) b n f(t) satisfies the n-th order discrete initial value problem n y(t) = f(t), i y(b) = 0, i = 0,,...,n. (8) The proof can be done inductively. Namely, assuming it is true for n, we have By the help of (0), it follows that n+ b (n+) f(t) = n [ b (n+) f(t)]. (9) n+ b (n+) f(t) = n b n f(t) = f(t). (20) The other part is clear by using the convention that s k=s+ = 0. (iii) The Cauchy function (s ρ(t))n Γ(n) satisfies n y(t) = 0. 3

4 Definition 2.2. (i)[8] The (delta) left fractional difference of order α > 0 (starting from a ) is defined by: α a f(t) = n (n α) n t (n α) a f(t) = (t σ(s)) (n α ) f(s), t N a+(n α) (2) s=a (ii) [2] The (delta) right fractional difference of order α > 0 (ending at b ) is defined by: b α f(t) = n b (n α) f(t) = ( )n n b (s σ(t)) (n α ) f(s), t b (n α) N (22) +(n α) (iii) The (nabla) left fractional difference of order α > 0 (starting from a ) is defined by: α af(t) = n (n α) n t a f(t) = (t ρ(s)) n α f(s), t N a+ (23) s=a+ (iv) The (nabla) right fractional difference of order α > 0 (ending at b ) is defined by: b α f(t) = n b (n α) f(t) = ( )n n b (s ρ(t)) n α f(s), t b N (24) Regarding the domains of the fractional type differences we observe: (i) The delta left fractional difference α a maps functions defined on Na to functions defined on N a+(n α). (ii) The delta right fractional difference b α maps functions defined on b N to functions defined on b (n α) N. (iii) The nabla left fractional difference α a maps functions defined on N a to functions defined on N a+n. (iv) The nabla right fractional difference b α maps functions defined on b N to functions defined on b n N. Lemma 2.. [3] For any α > 0, the following equality holds: α a f(t) = α a f(t) (t a)α f(a). Lemma 2.2. [2] For any α > 0, the following equality holds: b α f(t) = b α f(t) (b t)α f(b). Lemma 2.3. [7] For any α > 0, the following equality holds: (t a+)α a+ f(t) = α a f(t) f(a) (25) The result of Lemma 2.3 was obtained in [7] by applying the nabla left fractional sum starting from a not from a+. Next will provide the version of Lemma 2.3 by applying the definition in this article. Actually, the nabla fractional sums defined in this article and those in [7] are related. For more details we refer to [27]. Lemma 2.4. For any α > 0, the following equality holds: Proof. By the help of the following by parts identity a f(t) = a f(t) (t a)α f(a). (26) we have s[(t s) α f(s)] = s(t s) α f(s)+(t ρ(s)) α sf(s) (27) = (α )(t ρ(s)) α 2 f(s)+(t ρ(s)) α sf(s) a f(t) = t s=a+ (t ρ(s)) α sf(s) = 4

5 On the other hand [(t s)α f(s) t a (t a)α f(a)+ t s=a+ +(α ) Γ(α ) t (t ρ(s)) α 2 f(s)] = (28) s=a+ t (t ρ(s)) α 2 f(s) (29) s=a+ a f(t) = t(t ρ(s)) α f(s) = Γ(α ) t s=a+ (t ρ(s)) α 2 f(s) (30) Remark 2.. Let α > 0 and n = [α]+. Then, by the help of Lemma 2.4 we have or Then, using the identity α a f(t) = n ( (n α) a f(t)) = n ( (n α) a f(t)). (3) α a f(t) = n [ (n α) a n(t a)n α we infer that (26) is valid for any real α. f(t)+ (t a)n α f(a)] (32) = (t a) α Γ( α) By the help of Lemma 2.4, Remark 2. and the identity (t a) α = (α )(t a) α 2, we arrive inductively at the following generalization. Theorem 2.5. For any real number α and any positive integer p, the following equality holds: a (33) p p f(t) = p a f(t) (t a) α p+k Γ(α+k p+) k f(a). (34) where f is defined on N a and some points before a. Lemma 2.6. For any α > 0, the following equality holds: b f(t) = b f(t) Proof. By the help of the following discrete by parts formula: we have s[(ρ(s) ρ(t)) α f(s)] = (b t)α f(b) (35) (α )(s ρ(t)) α 2 f(s)+(s ρ(t)) α f(s) (36) b a f(t) = b (s ρ(t)) α f(s) = b [ b s((ρ(s) ρ(t)) α f(s))+(α ) (s ρ(t)) α 2 f(s)] = (37) b (s ρ(t)) α 2 f(s) (b t)α f(b). (38) Γ(α ) On the other hand, b f(t) = b where the identity t(s ρ(t)) α f(s) = and the convention that (0) α = 0 are used. t(s ρ(t)) α = (α )(s ρ(t)) α 2 b (s ρ(t)) α 2 f(s) (39) Γ(α ) 5

6 Remark 2.2. Let α > 0 and n = [α]+. Then, by the help of Lemma 2.6 we can have or a b α f(t) = a n ( b (n α) f(t)) = n ( b (n α) f(t)) (40) b α f(t) = n [ b (n α) f(t)+ (b t)n α f(b)] (4) Then, using the identity we infer that (35) is valid for any real α. n(b t)n α = (b t) α Γ(n α) Γ( α) By the help of Lemma 2.6, Remark 2.2 and the identity (b t) α = (α )(b t) α 2, if we follow inductively we arrive at the following generalization Theorem 2.7. For any real number α and any positive integer p, the following equality holds: p b p f(t) = p b (b t) α p+k f(t) Γ(α+k p+) k f(b) (43) where f is defined on b N and some points after b. The following theorem modifies Theorem 2.5 when f is only defined at N a. Theorem 2.8. For any real number α and any positive integer p, the following equality holds: p a+p p f(t) = p a+p f(t) (t (a+p )) α p+k k f(a+p ). (44) Γ(α+k p+) where f is defined on only N a. The proof follows by applying Remark 2. inductively. Similarly, in the right case we have Theorem 2.9. For any real number α and any positive integer p, the following equality holds: (42) p b p+ p f(t) = p b p+ f(t) where f is defined on b N only. (b p+ t) α p+k Γ(α +k p+) k f(b p+) (45) 3 Dual identities for right fractional sums and differences The dual relations for left fractional sums and differences were investigated in [5]. Indeed, the following two lemmas are dual relations between the delta left fractional sums (differences) and the nabla left fractional sums (differences). Lemma 3.. [5] Let 0 n < α n and let y(t) be defined on N a. Then the following statements are valid. (i)( α a )y(t α) = α a y(t) for t N n+a. (ii) ( α a )y(t +α) = a y(t) for t N a. Lemma 3.2. [5] Let 0 n < α n and let y(t) be defined on N α n. Then the following statements are valid. (i) α α n y(t) = ( α α n y)(t +α) for t N n. (ii) (n α) α n y(t) = ( (n α) α n y)(t n+α) for t N 0. 6

7 We remind that the above two dual lemmas for left fractional sums and differences were obtained when the nabla left fractional sum was defined by a f(t) = t (t ρ(s)) α f(s), t N a (46) s=a Now, in analogous to Lemma 3. and Lemma 3.2, for the right fractional summations and differences we obtain Lemma 3.3. Let y(t) be defined on b+ N. Then the following statements are valid. (i)( b α )y(t+α) = b+ α y(t) for t b n N. (ii) ( b α )y(t α) = b+ y(t) for t b N. Proof. We prove only (i). The proof of (ii) is similar and easier. ( b α )y(t+α) = ( ) n n b (n α) y(t+α) = ( ) n n b (s t α) (n α ) y(s) = ( )n n b (s t +n α) (n α ) y(s) (47) +n Using the identity t α = (t+α ) (α), we arrive at ( b α )y(t+α) = ( )n n b (s ρ(t)) n α y(s) = ( ) n n b+ (n α) y(t) = b+ α y(t). (48) Lemma 3.4. Let 0 n < α n and let y(t) be defined on n α N. Then the following statements are valid. (i) n α α y(t) = n α+ α y(t α), t nn (ii) n α (n α) y(t) = n α+ (n α) y(t+n α), t 0 N Proof. We prove (i), the proof of (ii) is similar. By the definition of right nabla difference we have a n n α+ α y(t α) = a n n α α By using (9) it follows that (s ρ(t α)) n α y(s) = n b n α+ α y(t α) = n b n α +n α n α α (s ρ(t α)) n α y(s) = n α +n α (s ρ(t+n α)) n α y(s) (49) (s σ(t)) (n α ) y(s) = n α α y(t) (50) Note that the above two dual lemmas for right fractional differences can not be obtained if we apply the definition of the delta right fractional difference introduced in [4] and [6]. Lemma 3.5. [2] Let α > 0, µ > 0. Then, b µ α (b t) (µ) = Γ(µ+) Γ(µ+α+) (b t)(µ+α) (5) The following commutative property for delta right fractional sums is Theorem 9 in [2]. 7

8 Theorem 3.6. Let α > 0, µ > 0. Then, for all t such that t b (µ+α) (mod ), we have b α [ b µ f(t)] = b (µ+α) f(t) = b µ [ b α f(t)] (52) where f is defined on b N. Proposition 3.7. Let f be a real valued function defined on b N, and let α,β > 0. Then b [ b β f(t)] = b (α+β) f(t) = b β [ b f(t)] (53) Proof. The proof follows by applying Lemma 3.3(ii) and Theorem 3.6 above. Indeed, b [ b β f(t)] = b b β f(t β) = b α b β f(t (α+β)) = b (α+β) f(t (α +µ)) = b (α+β) y(t) (54) The following power rule for nabla right fractional differences plays an important rule. Proposition 3.8. Let α > 0, µ >. Then, for t b N, we have Proof. By the dual formula (ii) of Lemma 3.3, we have b (b t) µ = Γ(µ+) Γ(α+µ+) (b t)α+µ (55) b (b t) µ = b α (b r) µ r=t α = b (s t+α ) (α ) (b s) µ. (56) Then by the identity t α = (t+α ) (α ) and using the change of variable r = s µ+, it follows that b (b t) µ = b µ r=t µ+ Which by Lemma 3.5 leads to (r σ(t α µ+)) (α ) (b r) µ = ( b µ α (b u) µ ) u= α µ++t. (57) b (b t) µ = Γ(µ+) Γ(α+µ+) (b t+α+µ )(α+µ) = Γ(µ+) Γ(α +µ+) (b t)α+µ (58) Similarly, for the nabla left fractional sum we can have the following power formula and exponent law. Proposition 3.9. Let α > 0, µ >. Then, for t N a, we have a (t a)µ = Γ(µ+) Γ(α +µ+) (t a)α+µ (59) Proposition 3.0. Let f be a real valued function defined on N a, and let α,β > 0. Then a [ β a f(t)] = (α+β) a f(t) = β a [ a f(t)] (60) Proof. The proof can be achieved as in Theorem 2. [5], by expressing the left hand side of (60), interchanging the order of summation and using the power formula (59). Alternatively, the proof can be done by following as in the proof of Proposition 3.7 with the help of the dual formula for left fractional sum in Lemma 3. after its arrangement according to our definitions. 8

9 4 Integration by parts for fractional sums and differences In this section we state the integration by parts formulas for nabla fractional sums and differences obtained in [27], then use the dual identities to obtain delta integration by part formulas. Proposition 4.. [27] For α > 0, a,b R, f defined on N a and g defined on b N, we have b s=a+ g(s) a f(s) = b s=a+ Proof. By the definition of the nabla left fractional sum we have b s=a+ g(s) a f(s) = b s=a+ g(s) If we interchange the order of summation we reach at ( 6). f(s) b g(s). (6) s r=a+ (s ρ(r)) α f(r). (62) By the help of Theorem 2.5, Proposition 3.0, (7) and that (n α) a f(a) = 0, the authors in [27] obtained the following left important tools which lead to a nabla integration by parts formula for fractional differences. Proposition 4.2. [27] For α > 0, and f defined in a suitable domain N a, we have α a α a f(t) = f(t), (63) and a α af(t) = f(t), when α / N, (64) n a α a f(t) = f(t) (t a) k k f(a),,when α = n N. (65) k! By the help of Theorem 2.7, Proposition 3.7, (8) and that b (n α) f(b) = 0, the authors also in [27] also obtained the following right important tool: Proposition 4.3. [27] For α > 0, and f defined in a suitable domain b N, we have b α b f(t) = f(t), (66) and b b α f(t) = f(t), when α / N, (67) n b b α f(t) = f(t) (b t) k k! k f(b),when α = n N. (68) Proposition 4.4. [27] Let α > 0 be non-integer and a,b R such that a < b and b a (mod ).If f is defined on b N and g is defined on N a, then b s=a+ f(s) α ag(s) = b s=a+ g(s) b α f(s). (69) The proof was achieved by making use of Proposition 4. and the tools Proposition 4.2 and Proposition 4.3. Now by the above nabla integration by parts formulas and the dual identities in Lemma 3. adjusted to our definitions and Lemma 3.3 we can obtain delta integration by parts formulas. Proposition 4.5. Let α > 0, a,b R such that a < b and b a (mod ). If f is defined on N a and g is defined on b N, then we have b s=a+ b g(s)( α a+ f)(s+α) = s=a+ f(s) b α g(s α). (70) 9

10 Proposition 4.6. Let α > 0 be non-integer and assume that b a (mod ). If f is defined on b N and g is defined on N a, then b s=a+ f(s) α a+g(s α) = b s=a+ g(s) b α f(s+α). (7) 5 Higher order fractional difference initial value problem within Riemann Let α > 0 be a non-integer, n = [α]+ and a(α) = a+n. Consider the fractional initial difference equation α a(α) y(t) = f(t,y(t)), t = a(α) +,a(α)+2,... (72) (n α) a(α) y(t) t=a(α) = y(a(α)) = c. Apply the sum operator to both sides of (72) to get a(α) a(α) { α a(α) Applying (64), we reach at y(t)+ a(α) y(t) + n(t a(α)+)n α +)n α n(t a(α) y(a(α))} = f(t,y(t)). (73) a(α) y(a(α)) = f(t,y(t)). (74) a(α) Now, set g α(t) = (t a(α)+)n α y(a(α)), then by Theorem 2.8 with p = n and f(t) = g α(t) we have n a(α) n g α(t) = n a(α) gα(t) (t a(α)) α n+k Γ(α +k n+) k g α(a(α)) (75) Noting that k g α(a(α)) = y(a(α)) for k = 0,,...,n, by the power formula (59) we conclude that a(α) n g α(t) = 0 n(t a(α)+)α y(a(α)) n Then the substitution in (74) will lead to the following solution representation y(t) = n(t a(α)+)α y(a(α)) As a particular case, if 0 < α < then a(α) = a and hence which is the result obtained in [27]. y(t) = (t a+)α (t a(α)) α n+k y(a(α)). (76) Γ(α+k n+) n (t a(α)) α n+k + Γ(α+k n+) c+ α f(t,y(t)). (77) a(α) y(a)+ a f(t,y(t)), (78) If < α < 2, then n = 2 and a(α) = a+ and the initial value problem (72) becomes From (77), the solution is y(t) = (t a)α 3 c Γ(α 2) Combining the first two terms then α ay(t) = f(t,y(t)), t = a+2,a+3,... (79) (2 α) a y(t) t=a+ = y(a+) = c. + (t a )α 2 c Γ(α ) + (t a )α c + a+f(t,y(t)). (80) 0

11 y(t) = (t a)α 2 c + (t a )α c + a+f(t,y(t)). (8) Γ(α ) Again combining we reach at y(t) = (t a)α c If we proceed inductively we can state + a+f(t,y(t)). (82) Theorem 5.. Let α > 0 be a non-integer, n = [α]+ and a(α) = a+n. Then the solution of the fractional initial difference equation α a(α) y(t) = f(t,y(t)), t = a(α) +,a(α)+2,... (83) (n α) a(α) y(t) t=a(α) = y(a(α)) = c, is given by y(t) = (t a(α) +)α c + f(t,y(t)). (84) a(α) The surprise in Theorem 5. is that the higher order Riemann fractional difference initial value problem of non-integer order needs only one initial condition which is not the case for the higher order difference equation (i.e of positive integer order). Also the solution is consisting of two terms which is not the case for fractional Cauchy problems into Riemann. 6 The Q-operator and fractional difference equations If f(s) is defined on N a b N and a b (mod ) then (Qf)(s) = f(a + b s). The Q-operator generates a dual identity by which the left type and the right type fractional sums and differences are related. Using the change of variable u = a+b s, in [] it was shown that and hence The proof of (86) follows by the definition, (85) and by noting that Similarly, in the nabla case we have and hence α a Qf(t) = Q b α f(t), (85) α a Qf(t) = (Q b α f)(t). (86) Q f(t) = Qf(t). The proof of (88) follows by the definition, (87) and that a Qf(t) = Q b f(t), (87) α a Qf(t) = (Q b α f)(t). (88) Q f(t) = Qf(t). It is remarkable to mention that the Q-dual identity (86) can not be obtained if the definition of the delta right fractional difference introduced by Nuno R.O. Bastos et al. in [4] or by Atıcı F. et al. in [6] is used. Thus, the definition introduced in [] and [2] is more convenience. Analogously, the Q-dual identity (88) indicates that the nabla right Riemann fractional differences presented in this article are also more convenient. It is clear from the above argument that, the Q-operator agrees with its continuous counterpart when applied to left and right fractional Riemann Integrals Riemann derivatives. More generally, this discrete version of the Q-operator can be used to transform the discrete delay-type fractional functional difference dynamic equations to advanced ones. For details in the continuous counterparts see [2].

12 References [] T. Abdeljawad, On Riemann and Caputo fractional differences, Computers and Mathematics with Applications, Volume 62, Issue 3, August 20, Pages [2] T. Abdeljawad (Maraaba), Baleanu D. and Jarad F., Existence and uniqueness theorem for a class of delay differential equations with left and right Caputo fractional derivatives, Journal of Mathematical Physics, 49 (2008), [3] F.M. Atıcı and Eloe P. W., A Transform method in discrete fractional calculus, International Journal of Difference Equations, vol 2, no 2, (2007), [4] F.M. Atıcı and Eloe P. W., Initial value problems in discrete fractional calculus, Proceedings of the American Mathematical Society, 37, (2009), [5] F. M. Atıcı and Paul W.Eloe, Discrete fractional calculus with the nabla operator, Electronic Journal of Qualitative Theory of Differential equations, Spec. Ed. I, 2009 No.3, 2. [6] F.M. Atıcı, Şengül S., Modelling with fractional difference equations,journal of Mathematical Analysis and Applications, 369 (200) -9. [7] F. M. Atıcı, Paul W. Eloe, Gronwall s inequality on discrete fractional calculus, Copmuterand Mathematics with pplications, In Press, doi:0.06/camwa [8] K. S. Miller, Ross B.,Fractional difference calculus, Proceedings of the International Symposium on Univalent Functions, Fractional Calculus and Their Applications, Nihon University, Koriyama, Japan, (989), [9] I. Podlubny, Fractional Differential Equations, Academic Press: San Diego CA, (999). [0] Samko G. Kilbas A. A., Marichev, Fractional Integrals and Derivatives: Theory and Applications, Gordon and Breach, Yverdon, 993. [] Kilbas A., Srivastava M. H.,and Trujillo J. J., Theory and Application of Fractional Differential Equations, North Holland Mathematics Studies 204, [2] T. Abdeljawad, D. Baleanu, Fractional Differences and integration by parts, Journal of Computational Analysis and Applications vol 3 no. 3, (20). [3] Silva M. F., J. A. T. Machado, A. M. Lopes, Modelling and simulation of artificial locomotion systems, Robotica 23 (2005), [4] Nuno R. O. Bastos, Rui A. C. Ferreira, Delfim F. M. Torres, Discrete-time fractional variational problems, Signal Processing, 9(3): (20). [5] Bohner M. and A. Peterson, Advances in Dynamic Equations on Time Scales, Birkhäuser, Boston, [6] G. Boros and V. Moll, Iresistible Integrals; Symbols,Analysis and Expreiments in the Evaluation of Integrals, Cambridge University PressCambridge [7] R. L. Graham, D. E. Knuth and O. Patashnik, Concrete Mathematics, A Foundation for Copmuter Science, 2nd ed., Adison-Wesley,Reading, MA, 994. [8] H. L. Gray and N. F.Zhang, On a new definition ofthe fractional difference, Mathematicsof Computaion 50, (82), (988.) [9] J. Spanier and K. B. Oldham, The Pochhammer Polynomials (x) n, An Atlas of Functions, pp ,Hemisphere, Washington, DC, 987. [20] G. A. Anastassiou,Principles of delta fractional calculus on time scales and inequalities, Mathematical and Computer Modelling, 52 (200) [2] G. A. Anastassiou, Nabla discrete calcilus and nabla inequalities, Mathematical and Computer Modelling, 5 (200) [22] G. A. Anastassiou,Foundations of nabla fractional calculus on time scales and inequalities,computer and Mathematics with Applications, 59 (200) [23] O. P. Agrawal, D. Baleanu, A Hamiltonian Formulation and a direct numerical scheme for fractional optimal control problems. J. Vib. Contr. 3(9-0) (2007) [24] E. Scalas, Mixtures of compound Poisson processes as models of tick-by-tick financial data. Chaos Solit. Fract. 34() (2007) [25] D. Baleanu, J. J. Trujillo, On exact solutions of a class o f fractional Euler-Lagrange equations, Nonlin.Dyn. 52(4) (2008). [26] T. Maraaba(Abdeljawad), F. Jarad, D. Baleanu, On the existence and the uniqueness theorem for fractional differential equations with bounded delay within Caputo derivatives, Science in China Series A: Mathematics, 5 (0), (2008). [27] T. Abdeljawad, F. Atıcı, On the Definitions of Nabla Fractional Operators, submitted. 2

13 On delta and nabla Caputo fractional differences and dual identities Thabet Abdeljawad a b a Department of Mathematics, Çankaya University, 06530, Ankara, Turkey b Department of Mathematics and Physical Sciences arxiv:2.5795v2 [math.ds] 8 Jan 203 Prince Sultan University, P. O. Box 66833, Riyadh 586, Saudi Arabia Abstract. We Investigate two types of dual identities for Caputo fractional differences. The first type relates nabla and delta type fractional sums and differences. The second type represented by the Q-operator relates left and right fractional sums and differences. Two types of Caputo fractional differences are introduced, one of them (dual one) is defined so that it obeys the investigated dual identities. The relation between Rieamnn and Caputo fractional differences is investigated and the delta and nabla discrete Mittag-Leffler functions are confirmed by solving Caputo type linear fractional difference equations. A nabla integration by parts formula is obtained for Caputo fractional differences as well. Keywords: right (left) delta and nabla fractional sums, right (left) delta and nabla Riemann and Caputo fractional differences. Q-operator, dual identity. Introduction During the last two decades, due to its widespread applications in different fields of science and engineering, fractional calculus has attracted the attention of many researchers [9, 0,, 23, 24, 25]. Starting from the idea of discretizing the Cauchy integral formula, Miller and Ross [8] and Gray and Zhang [8] obtained discrete versions of left type fractional integrals and derivatives, called fractional sums and differences. After then, several authors started to deal with discrete fractional calculus [, 3, 4, 5, 6, 4, 2, 20, 2, 22, 27, 28], benefiting from time scales calculus originated in 988 (see [5]). In [], the concept of Caputo fractional difference was introduced and investigated. In this article we proceed deeply to investigate Caputo fractional differences under two kinds of dual identities. The first kind relates nabla and delta type Caputo fractional differences and the second one, represented by the Q-operator, relates left and right ones. Arbitrary order Riemann and Caputo fractional differences are related as well. By the help of the previously obtained results in [27] and [28] an integration by parts formula for Caputo fractional differences is originated. The article is organized as follows: The remaining part of this section contains summary to some of the basic notations and definitions in delta and nabla calculus. Section 2 contains the definitions in the frame of delta and nabla fractional sums and differences in the Riemann sense. The third section contains some dual identities relating nabla and delta type fractional sums and differences in Riemann sense as previously investigated in [28]. In Section 4 Caputo fractional differences are given and related to the Riemann ones. In section 5, slightly different modified (dual) Caputo fracctional differences are introduced and investigated under some dual identities. Section 6 is devoted to the integration by parts for delta and nabla Caputo fractional differences. Finally, Section 7 contains Caputo type fractional dynamical equations where a nonhomogeneous nabla Caputo fractional difference equation is solved to obtain nabla discrete versions for Mittag- Leffler functions. For the case α = we obtain the discrete nabla exponential function [5]. In addition to this, the Q-operator is used to relate left and right Caputo fractional differences in the nabla and delta case. The Q-dual identities obtained in this section expose the validity of the definition of delta and nabla right Caputo fractional differences. For a natural number n, the fractional polynomial is defined by, n t (n) = (t j) = Γ(t+) Γ(t+ n), () j=0

14 where Γ denotes the special gamma function and the product is zero when t+ j = 0 for some j. More generally, for arbitrary α, define t (α) = Γ(t+) Γ(t+ α), (2) where the convention that division at pole yields zero. Given that the forward and backward difference operators are defined by f(t) = f(t+) f(t), f(t) = f(t) f(t ) (3) respectively, we define iteratively the operators m = ( m ) and m = ( m ), where m is a natural number. Here are some properties of the factorial function. Lemma.. ([3]) Assume the following factorial functions are well defined. (i) t (α) = αt (α ). (ii) (t µ)t (µ) = t (µ+), where µ R. (iii) µ (µ) = Γ(µ+). (iv) If t r, then t (α) r (α) for any α > r. (v) If 0 < α <, then t (αν) (t (ν) ) α. (vi) t (α+β) = (t β) (α) t (β). Also, for our purposes we list down the following two properties, the proofs of which are straightforward. s(s t) (α ) = (α )(ρ(s) t) (α 2). (4) t(ρ(s) t) (α ) = (α )(ρ(s) t) (α 2). (5) For the sake of the nabla fractional calculus we have the following definition Definition.. ([5, 6, 7, 9]) (i) For a natural number m, the m rising (ascending) factorial of t is defined by (ii) For any real number the α rising function is defined by m t m = (t+k), t 0 =. (6) t α = Γ(t+α), t R {..., 2,,0}, 0 α = 0 (7) Γ(t) Regarding the rising factorial function we observe the following: (i) (t α ) = αt α (8) (ii) (iii) Notation: (t α ) = (t+α ) (α). (9) t(s ρ(t)) α = α(s ρ(t)) α (0) (i) For a real α > 0, we set n = [α]+, where [α] is the greatest integer less than α. (ii) For real numbers a and b, we denote N a = {a,a+,...} and b N = {b,b,...}. (iii) For n N and real a, we denote (iv) For n N and real b, we denote n f(t) ( ) n n f(t). n f(t) ( ) n n f(t). 2

15 2 Definitions and essential lemmas Definition 2.. Let σ(t) = t+ and ρ(t) = t be the forward and backward jumping operators, respectively. Then (i) The (delta) left fractional sum of order α > 0 (starting from a) is defined by: α a f(t) = t α (t σ(s)) (α ) f(s), t N a+α. () s=a (ii) The (delta) right fractional sum of order α > 0 (ending at b) is defined by: b α f(t) = b (s σ(t)) (α ) f(s) = b (ρ(s) t) (α ) f(s), t b α N. (2) +α +α (iii) The (nabla) left fractional sum of order α > 0 (starting from a) is defined by: a f(t) = t s=a+ (t ρ(s)) α f(s), t N a+. (3) (iv)the (nabla) right fractional sum of order α > 0 (ending at b) is defined by: b f(t) = b (s ρ(t)) α f(s) = Regarding the delta left fractional sum we observe the following: (i) α a maps functions defined on N a to functions defined on N a+α. (ii) u(t) = n a f(t), n N, satisfies the initial value problem b (σ(s) t) α f(s), t b N. (4) n u(t) = f(t), t N a, u(a+j ) = 0, j =,2,...,n. (5) (iii) The Cauchy function (t σ(s))(n ) (n )! vanishes at s = t (n ),...,t. Regarding the delta right fractional sum we observe the following: (i) b α maps functions defined on b N to functions defined on b α N. (ii) u(t) = b n f(t), n N, satisfies the initial value problem n u(t) = f(t), t bn, u(b j +) = 0, j =,2,...,n. (6) (iii) the Cauchy function (ρ(s) t)(n ) (n )! vanishes at s = t+,t+2,...,t+(n ). Regarding the nabla left fractional sum we observe the following: (i) a maps functions defined on N a to functions defined on N a. (ii) n a f(t) satisfies the n-th order discrete initial value problem n y(t) = f(t), i y(a) = 0, i = 0,,...,n (7) (iii) The Cauchy function (t ρ(s))n Γ(n) satisfies n y(t) = 0. Regarding the nabla right fractional sum we observe the following: (i) b maps functions defined on b N to functions defined on b N. (ii) b n f(t) satisfies the n-th order discrete initial value problem n y(t) = f(t), i y(b) = 0, i = 0,,...,n. (8) The proof can be done inductively. Namely, assuming it is true for n, we have By the help of (0), it follows that n+ b (n+) f(t) = n [ b (n+) f(t)]. (9) n+ b (n+) f(t) = n b n f(t) = f(t). (20) The other part is clear by using the convention that s k=s+ = 0. (iii) The Cauchy function (s ρ(t))n Γ(n) satisfies n y(t) = 0. 3

16 Definition 2.2. (i)[8] The (delta) left fractional difference of order α > 0 (starting from a ) is defined by: α a f(t) = n (n α) n t (n α) a f(t) = (t σ(s)) (n α ) f(s), t N a+(n α) (2) s=a (ii) [2] The (delta) right fractional difference of order α > 0 (ending at b ) is defined by: b α f(t) = n b (n α) f(t) = ( )n n b (s σ(t)) (n α ) f(s), t b (n α) N (22) +(n α) (iii) The (nabla) left fractional difference of order α > 0 (starting from a ) is defined by: α af(t) = n (n α) n t a f(t) = (t ρ(s)) n α f(s), t N a+ (23) s=a+ (iv) The (nabla) right fractional difference of order α > 0 (ending at b ) is defined by: b α f(t) = n b (n α) f(t) = ( )n n b (s ρ(t)) n α f(s), t b N (24) Regarding the domains of the fractional type differences we observe: (i) The delta left fractional difference α a maps functions defined on Na to functions defined on N a+(n α). (ii) The delta right fractional difference b α maps functions defined on b N to functions defined on b (n α) N. (iii) The nabla left fractional difference α a maps functions defined on N a to functions defined on N a+n (on N a if we think f defined at some points before a). (iv) The nabla right fractional difference b α maps functions defined on b N to functions defined on b n N (on b N if we think f defined at some points after b). Lemma 2.. [3] For any α > 0, the following equality holds: α a (t a)α f(t) = α a f(t) f(a). Lemma 2.2. [2] For any α > 0, the following equality holds: b α f(t) = b α f(t) (b t)α f(b). Lemma 2.3. [7] For any α > 0, the following equality holds: a+ f(t) = α a f(t) (t a+)α f(a) (25) The result of Lemma 2.3 was obtained in [7] by applying the nabla left fractional sum starting from a not from a+. Next will provide the version of Lemma 2.3 by applying the definition in this article. Actually, the nabla fractional sums defined in this article and those in [7] are related. For more details we refer to [27]. Lemma 2.4. (see [27] and [28]) For any α > 0, the following equality holds: a (t a)α f(t) = α a f(t) f(a). (26) Remark 2.. (see [27] and [28]) Let α > 0 and n = [α]+. Then, by the help of Lemma 2.4 we have α af(t) = n ( (n α) a f(t)) = n ( (n α) a f(t)). (27) or α a f(t) = n [ (n α) a f(t)+ (t a)n α f(a)] (28) Then, using the identity n(t a)n α we infer that (26) is valid for any real α. = (t a) α Γ( α) (29) 4

17 By the help of Lemma 2.4, Remark 2. and the identity (t a) α = (α )(t a) α 2, we arrive inductively at the following generalization. Theorem 2.5. (see [27] and [28]) For any real number α and any positive integer p, the following equality holds: p a p f(t) = p a f(t) (t a) α p+k Γ(α+k p+) k f(a). (30) where f is defined on N a and some points before a. Lemma 2.6. (see [27] and [28]) For any α > 0, the following equality holds: b f(t) = b f(t) (b t)α f(b). (3) Remark 2.2. (see [27] and [28]) Let α > 0 and n = [α]+. Then, by the help of Lemma 2.6 we can have or b α f(t) = n ( b (n α) f(t)) = n ( b (n α) f(t)) (32) b α f(t) = n [ b (n α) f(t)+ (b t)n α f(b)] (33) Then, using the identity n(b t)n α = (b t) α Γ(n α) Γ( α) we infer that (3) is valid for any real α. By the help of Lemma 2.6, Remark 2.2 and the identity (b t) α = (α )(b t) α 2, if we follow inductively we arrive at the following generalization. Theorem 2.7. (see [27] and [28]) For any real number α and any positive integer p, the following equality holds: p b p f(t) = p b (b t) α p+k f(t) Γ(α+k p+) k f(b) (35) where f is defined on b N and some points after b. 3 Dual identities for fractional sums and Riemann fractional differences The dual relations for left fractional sums and differences were investigated in [5]. Indeed, the following two lemmas are dual relations between the delta left fractional sums (differences) and the nabla left fractional sums (differences). Lemma 3.. [5] Let 0 n < α n and let y(t) be defined on N a. Then the following statements are valid. (i)( α a )y(t α) = α a y(t) for t N n+a. (ii) ( α a )y(t +α) = a y(t) for t N a. Lemma 3.2. [5] Let 0 n < α n and let y(t) be defined on N α n. Then the following statements are valid. (i) α α n y(t) = ( α α n y)(t +α) for t N n. (ii) (n α) α n y(t) = ( (n α) α n y)(t n+α) for t N 0. We remind that the above two dual lemmas for left fractional sums and differences were obtained when the nabla left fractional sum was defined by a f(t) = t (t ρ(s)) α f(s), t N a (36) s=a Now, in analogous to Lemma 3. and Lemma 3.2, for the right fractional summations and differences the author in [28] obtained: (34) 5

18 Lemma 3.3. Let y(t) be defined on b+ N. Then the following statements are valid. (i)( b α )y(t+α) = b+ α y(t) for t b n N. (ii) ( b α )y(t α) = b+ y(t) for t b N. Lemma 3.4. [28] Let 0 n < α n and let y(t) be defined on n α N. Then the following statements are valid. (i) n α α y(t) = n α+ α y(t α), t nn (ii) n α (n α) y(t) = n α+ (n α) y(t+n α), t 0 N Proof. We prove (i), the proof of (ii) is similar. By the definition of right nabla difference we have a n n α+ α y(t α) = a n n α α By using (9) it follows that (s ρ(t α)) n α y(s) = n b n α+ α y(t α) = n b n α +n α n α α (s ρ(t α)) n α y(s) = n α +n α (s ρ(t+n α)) n α y(s) (37) (s σ(t)) (n α ) y(s) = n α α y(t) (38) Note that the above two dual lemmas for right fractional differences can not be obtained if we apply the definition of the delta right fractional difference introduced in [4] and [6]. Lemma 3.5. [2] Let α > 0, µ > 0. Then, b µ α (b t) (µ) = Γ(µ+) Γ(µ+α+) (b t)(µ+α) (39) The following commutative property for delta right fractional sums is Theorem 9 in [2]. Theorem 3.6. Let α > 0, µ > 0. Then, for all t such that t b (µ+α) (mod ), we have where f is defined on b N. b α [ b µ f(t)] = b (µ+α) f(t) = b µ [ b α f(t)] (40) Proposition 3.7. [28] Let f be a real valued function defined on b N, and let α,β > 0. Then b [ b β f(t)] = b (α+β) f(t) = b β [ b f(t)] (4) Proof. The proof follows by applying Lemma 3.3(ii) and Theorem 3.6 above. Indeed, b [ b β f(t)] = b b β f(t β) = b α b β f(t (α+β)) = b (α+β) f(t (α +µ)) = b (α+β) y(t) (42) The following power rule for nabla right fractional differences plays an important rule. Proposition 3.8. ([27], [28]) Let α > 0, µ >. Then, for t b N, we have b (b t) µ = Γ(µ+) Γ(α+µ+) (b t)α+µ (43) 6

19 Proof. By the dual formula (ii) of Lemma 3.3, we have b (b t) µ = b α (b r) µ r=t α = b (s t+α ) (α ) (b s) µ. (44) Then by the identity t α = (t+α ) (α ) and using the change of variable r = s µ+, it follows that b (b t) µ = b µ r=t µ+ Which by Lemma 3.5 leads to (r σ(t α µ+)) (α ) (b r) µ = ( b µ α (b u) µ ) u= α µ++t. (45) b (b t) µ = Γ(µ+) Γ(α+µ+) (b t+α+µ )(α+µ) = Γ(µ+) Γ(α +µ+) (b t)α+µ (46) Similarly, for the nabla left fractional sum we can have the following power formula and exponent law Proposition 3.9. (see [27] and [28]) Let α > 0, µ >. Then, for t N a, we have a (t a)µ = Γ(µ+) Γ(α +µ+) (t a)α+µ (47) Proposition 3.0. (see [27] and [28]) Let f be a real valued function defined on N a, and let α,β > 0. Then a [ β a f(t)] = (α+β) a f(t) = β a [ a f(t)] (48) Proof. The proof can be achieved as in Theorem 2. [5], by expressing the left hand side of (48), interchanging the order of summation and using the power formula (47). Alternatively, the proof can be done by following as in the proof of Proposition 3.7 with the help of the dual formula for left fractional sum in Lemma 3. after its arrangement according to our definitions. 4 Caputo fractional differences In analogous to the usual fractional calculus we can formulate the following definition Definition 4.. Let α > 0, α / N. Then, (i)[] the delta α order Caputo left fractional difference of a function f defined on N a is defined by t (n α) C α af(t) (n α) a n f(t) = (t σ(s)) (n α ) n sf(s) (49) s=a (ii) [] the delta α order Caputo right fractional difference of a function f defined on b N is defined by C b α f(t) b (n α) n f(t) = where n = [α]+. If α = n N, then b +(n α) C α af(t) n f(t) and C b α f(t) n b f(t) (s σ(t)) (n α ) n f(s) (50) 7

20 (iii) the nabla α order Caputo left fractional difference of a function f defined on N a and some points before a, is defined by t (n α) C α af(t) (n α) a n f(t) = (t ρ(s)) n α n f(s) (5) s=a+ (iv) the nabla α order Caputo right fractional difference of a function f defined on b N and some points after b, is defined by b C b α f(t) b (n α) a n f(t) = (s ρ(t)) n α n f(s) (52) If α = n N, then C α a f(t) n f(t) and C b α f(t) a n f(t) It is clear that C α a maps functions defined on Na to functions defined on N a+(n α), and that C b α maps functions defined on b N to functions defined on b (n α) N. Also, it is clear that the nabla left fractional difference α a maps functions defined on N a to functions defined on N a+ n and the nabla right fractional difference b α maps functions defined on b N to functions defined on b +n N. Riemann and Caputo delta fractional differences are related by the following theorem Theorem 4.. [] For any α > 0, we have n C α af(t) = α (t a) (k α) af(t) Γ(k α+) k f(a) (53) and n C b α f(t) = b α (b t) (k α) f(t) Γ(k α+) k f(b). (54) In particular, when 0 < α <, we have C af(t) = α af(t) (t a)( α) f(a). (55) Γ( α) C b f(t) = b α f(t) (b t)( α) f(b) (56) Γ( α) One can note that the Riemann and Caputo fractional differences, for 0 < α <, coincide when f vanishes at the end points. The following identity is useful to transform delta type Caputo fractional difference equations into fractional summations. Proposition 4.2. [] Assume α > 0 and f is defined on suitable domains N a and b N. Then n α C α a+(n α) a f(t) = f(t) (t a) (k) k f(a) (57) k! and n b (n α) α C (b t) (k) b α f(t) = f(t) k f(b) (58) k! In particular, if 0 < α then α C α a+(n α) a f(t) = f(t) f(a) and b (n α) α C b α f(t) = f(t) f(b). (59) Similar to what we have above, for the nabla fractional differences we obtain Theorem 4.3. For any α > 0, we have and n C α a f(t) = α a f(t) (t a) k α Γ(k α+) k f(a) (60) n C b α f(t) = b α (b t) k α f(t) Γ(k α+) k f(b). (6) 8

21 In particular, when 0 < α <, we have and C α af(t) = α af(t) (t a) α f(a) (62) Γ( α) C b α f(t) = b α f(t) (b t) α f(b) (63) Γ( α) Proof. The proof follows by replacing α by n α and p by n in Theorem 5 and Theorem 2.7, respectively. One can see that the nabla Riemann and Caputo fractional differences, for 0 < α <, coincide when f vanishes at the end points. Proposition 4.4. Assume α > 0 and f is defined on suitable domains N a and b N. Then and a In particular, if 0 < α then a n C α a f(t) = f(t) (t a) k k f(a) (64) k! n b b C α f(t) = f(t) (b t) k k! k f(b). (65) C α a f(t) = f(t) f(a) and b C b α f(t) = f(t) f(b) (66) Proof. The proof of (64) follows by the definition and applying Proposition 3.0 and (89) of Proposition 6.2. The proof of (65) follows by the definition and applying Proposition 3.7 and (92) of Proposition 6.3. Using the definition and Proposition 3.9 and Proposition 3.8, we can find the nabla type Caputo fractional differences for certain power functions. For example, for β > 0 and α 0 we have and However, whereas C α a (t a)β = Γ(β) Γ(β α) (t a)β α (67) C b α (b t) β = Γ(β) Γ(β α) (b t)β α. (68) C α a = C b α = 0 (69) α a = (t a)( α) Γ( α), b α = (b t)( α) Γ( α). (70) In the above formulae (67) and (68), we apply the convention that dividing over a pole leads to zero. Therefore the fractional difference when β = α j, j =,2,...,n is zero. Remark 4.. The results obtained in Theorem 4.and afterward agree with those in the usual continuous case (See [] pages 9,96). 5 A dual nabla Caputo fractional difference In the previous section the nabla Caputo fractional difference is defined under the assumption that f is known before a in the left case and under the assumption that f is known after b in the right case. In this section we define other nabla Caputo fractional differences for which not necessary to request any information about f before a or after b. Since we shall show that these Caputo fractional differences are the dual ones for the delta Caputo fractional differences, we call them dual nabla Caputo fractional differences. 9

22 Definition 5.. Let α > 0, n = [α] +, a(α) = a + n and b(α) = b n +. Then the dual nabla left and right Caputo fractional differences are defined by and respectively. C α a(α) f(t) = (n α) n f(t), t N a(α) a+n (7) b(α) C α f(t) = b(α) (n α) n f(t), t b n N, (72) Notice that the Caputo and the dual Caputo differences coincide when 0 < α and differ for higher order. That is for 0 < α C α a(α) f(t) = C α a f(t) and C b(α) α f(t) = C b α f(t). The following proposition states a dual relation between left delta Caputo fractional differences and left nabla (dual) Caputo fractional differences. Proposition 5.. For α > 0, n = [α]+, a(α) = a+n, we have Proof. For t N a+n, we have ( C α a f)(t α) = ( C α a(α) f)(t), t N a+n. (73) t n ( C α a f)(t α) = (t α σ(s)) (n α ) n f(s) s=a = = = t n (t α σ(s)) (n α ) n f(s+n) s=a t (t ρ(r)+n α 2) (n α ) n f(r) (74) r=a+n t (t ρ(r)) n α n f(r) r=a+n = ( C α a(α) f)(t). Analogously, the following proposition relates right delta Caputo fractional differences and right nabla (dual) Caputo fractional differences. Proposition 5.2. For α > 0, n = [α]+, b(α) = b n+, we have ( C b α f)(t+α) = ( C b(α) α f)(t), t b n N. (75) The following theorem modifies Theorem when f is only defined at N a. Theorem 5.3. For any real number α and any positive integer p, the following equality holds: p a+p p f(t) = p a+p f(t) (t (a+p )) α p+k k f(a+p ). (76) Γ(α+k p+) where f is defined on only N a. The proof follows by applying Remark 2. inductively. Similarly, in the right case we have Theorem 5.4. For any real number α and any positive integer p, the following equality holds: p b p+ p f(t) = p b p+ f(t) where f is defined on b N only. (b p+ t) α p+k Γ(α +k p+) k f(b p+) (77) 0

23 Now by using the modified Theorem 5.3 and Theorem 5.4 we have Theorem 5.5. For any α > 0, we have and n C α a(α) f(t) = α a(α) f(t) n C b(α) α f(t) = b(α) α f(t) (t a(α)) k α Γ(k α+) k f(a(α)) (78) (b(α) t) k α Γ(k α+) k f(b(α)). (79) In particular, when 0 < α <, then a(α) = a and b(α) = b and hence we have and C α a f(t) = α a C b α f(t) = b α f(t) (t a) α f(t) f(a) (80) Γ( α) (b t) α f(b) (8) Γ( α) Also, by using the modified Theorem 5.3 and Theorem 5.4 we have Proposition 5.6. Assume α > 0 and f is defined on suitable domains N a and b N. Then n C α a(α) a(α) f(t) = f(t) (t a(α)) k k f(a(α)) (82) k! and n b(α) C (b(α) t) k b(α) α f(t) = f(t) k f(b(α)). (83) k! In particular, if 0 < α then a(α) = a and b(α) = b and hence a C α a f(t) = f(t) f(a) and b b C α f(t) = f(t) f(b) (84) 6 Integration by parts for Caputo fractional differences In this section we state the integration by parts formulas for nabla fractional sums and differences obtained in [27], then use the dual identities to obtain delta integration by part formulas. Proposition 6.. [27] For α > 0, a,b R, f defined on N a and g defined on b N, we have b s=a+ g(s) a f(s) = b s=a+ f(s) b g(s). (85) Proof. By the definition of the nabla left fractional sum we have b g(s) a f(s) = b s g(s) (s ρ(r)) α f(r). (86) s=a+ s=a+ r=a+ If we interchange the order of summation we reach at ( 85). By the help of Theorem 5, Proposition 3.0, (7) and that (n α) a f(a) = 0, the authors in [27] obtained the following left important tools which lead to a nabla integration by parts formula for fractional differences. Proposition 6.2. [27] For α > 0, and f defined in a suitable domain N a, we have α a a f(t) = f(t), (87) and a α af(t) = f(t), when α / N, (88) n a α a f(t) = f(t) (t a) k k f(a),,when α = n N. (89) k!

Multi-Term Linear Fractional Nabla Difference Equations with Constant Coefficients

Multi-Term Linear Fractional Nabla Difference Equations with Constant Coefficients International Journal of Difference Equations ISSN 0973-6069, Volume 0, Number, pp. 9 06 205 http://campus.mst.edu/ijde Multi-Term Linear Fractional Nabla Difference Equations with Constant Coefficients

More information

ANALYSIS OF NONLINEAR FRACTIONAL NABLA DIFFERENCE EQUATIONS

ANALYSIS OF NONLINEAR FRACTIONAL NABLA DIFFERENCE EQUATIONS International Journal of Analysis and Applications ISSN 229-8639 Volume 7, Number (205), 79-95 http://www.etamaths.com ANALYSIS OF NONLINEAR FRACTIONAL NABLA DIFFERENCE EQUATIONS JAGAN MOHAN JONNALAGADDA

More information

Positive solutions for discrete fractional intiail value problem

Positive solutions for discrete fractional intiail value problem Computational Methods for Differential Equations http://cmde.tabrizu.ac.ir Vol. 4, No. 4, 2016, pp. 285-297 Positive solutions for discrete fractional intiail value problem Tahereh Haghi Sahand University

More information

On Two-Point Riemann Liouville Type Nabla Fractional Boundary Value Problems

On Two-Point Riemann Liouville Type Nabla Fractional Boundary Value Problems Advances in Dynamical Systems and Applications ISSN 0973-5321, Volume 13, Number 2, pp. 141 166 (2018) http://campus.mst.edu/adsa On Two-Point Riemann Liouville Type Nabla Fractional Boundary Value Problems

More information

On boundary value problems for fractional integro-differential equations in Banach spaces

On boundary value problems for fractional integro-differential equations in Banach spaces Malaya J. Mat. 3425 54 553 On boundary value problems for fractional integro-differential equations in Banach spaces Sabri T. M. Thabet a, and Machindra B. Dhakne b a,b Department of Mathematics, Dr. Babasaheb

More information

On a new class of fractional difference-sum operators based on discrete Atangana Baleanu sums

On a new class of fractional difference-sum operators based on discrete Atangana Baleanu sums On a new class of fractional difference-sum operators ased on discrete Atangana Baleanu sums Thaet Adeljawad 1 and Arran Fernandez 2,3 arxiv:1901.08268v1 [math.ca] 24 Jan 2019 1 Department of Mathematics

More information

A generalized Gronwall inequality and its application to fractional differential equations with Hadamard derivatives

A generalized Gronwall inequality and its application to fractional differential equations with Hadamard derivatives A generalized Gronwall inequality and its application to fractional differential equations with Hadamard derivatives Deliang Qian Ziqing Gong Changpin Li Department of Mathematics, Shanghai University,

More information

Existence and Uniqueness Results for Nonlinear Implicit Fractional Differential Equations with Boundary Conditions

Existence and Uniqueness Results for Nonlinear Implicit Fractional Differential Equations with Boundary Conditions Existence and Uniqueness Results for Nonlinear Implicit Fractional Differential Equations with Boundary Conditions Mouffak Benchohra a,b 1 and Jamal E. Lazreg a, a Laboratory of Mathematics, University

More information

arxiv: v2 [math.ca] 8 Nov 2014

arxiv: v2 [math.ca] 8 Nov 2014 JOURNAL OF THE AMERICAN MATHEMATICAL SOCIETY Volume 00, Number 0, Pages 000 000 S 0894-0347(XX)0000-0 A NEW FRACTIONAL DERIVATIVE WITH CLASSICAL PROPERTIES arxiv:1410.6535v2 [math.ca] 8 Nov 2014 UDITA

More information

On Local Asymptotic Stability of q-fractional Nonlinear Dynamical Systems

On Local Asymptotic Stability of q-fractional Nonlinear Dynamical Systems Available at http://pvamuedu/aam Appl Appl Math ISSN: 1932-9466 Vol 11, Issue 1 (June 2016), pp 174-183 Applications and Applied Mathematics: An International Journal (AAM) On Local Asymptotic Stability

More information

Existence of Minimizers for Fractional Variational Problems Containing Caputo Derivatives

Existence of Minimizers for Fractional Variational Problems Containing Caputo Derivatives Advances in Dynamical Systems and Applications ISSN 0973-5321, Volume 8, Number 1, pp. 3 12 (2013) http://campus.mst.edu/adsa Existence of Minimizers for Fractional Variational Problems Containing Caputo

More information

A study on nabla discrete fractional operator in mass - spring - damper system

A study on nabla discrete fractional operator in mass - spring - damper system NTMSCI 4, No. 4, 137-144 (2016) 137 New Trends in Mathematical Sciences http://dx.doi.org/10.20852/ntmsci.2016422559 A study on nabla discrete fractional operator in mass - spring - damper system Okkes

More information

Positive solutions for a class of fractional boundary value problems

Positive solutions for a class of fractional boundary value problems Nonlinear Analysis: Modelling and Control, Vol. 21, No. 1, 1 17 ISSN 1392-5113 http://dx.doi.org/1.15388/na.216.1.1 Positive solutions for a class of fractional boundary value problems Jiafa Xu a, Zhongli

More information

DETERMINATION OF AN UNKNOWN SOURCE TERM IN A SPACE-TIME FRACTIONAL DIFFUSION EQUATION

DETERMINATION OF AN UNKNOWN SOURCE TERM IN A SPACE-TIME FRACTIONAL DIFFUSION EQUATION Journal of Fractional Calculus and Applications, Vol. 6(1) Jan. 2015, pp. 83-90. ISSN: 2090-5858. http://fcag-egypt.com/journals/jfca/ DETERMINATION OF AN UNKNOWN SOURCE TERM IN A SPACE-TIME FRACTIONAL

More information

1 Introduction ON NABLA DISCRETE FRACTIONAL CALCULUS OPERATOR FOR A MODIFIED BESSEL EQUATION. Resat YILMAZER a,, and Okkes OZTURK b

1 Introduction ON NABLA DISCRETE FRACTIONAL CALCULUS OPERATOR FOR A MODIFIED BESSEL EQUATION. Resat YILMAZER a,, and Okkes OZTURK b ON NABLA DISCRETE FRACTIONAL CALCULUS OPERATOR FOR A MODIFIED BESSEL EQUATION by Resat YILMAZER a,, and Okkes OZTURK b a Department of Mathematics, Firat University, 23119, Elazig, Turkey b Department

More information

LAGRANGIAN FORMULATION OF MAXWELL S FIELD IN FRACTIONAL D DIMENSIONAL SPACE-TIME

LAGRANGIAN FORMULATION OF MAXWELL S FIELD IN FRACTIONAL D DIMENSIONAL SPACE-TIME THEORETICAL PHYSICS LAGRANGIAN FORMULATION OF MAXWELL S FIELD IN FRACTIONAL D DIMENSIONAL SPACE-TIME SAMI I. MUSLIH 1,, MADHAT SADDALLAH 2, DUMITRU BALEANU 3,, EQAB RABEI 4 1 Department of Mechanical Engineering,

More information

Picard s Iterative Method for Caputo Fractional Differential Equations with Numerical Results

Picard s Iterative Method for Caputo Fractional Differential Equations with Numerical Results mathematics Article Picard s Iterative Method for Caputo Fractional Differential Equations with Numerical Results Rainey Lyons *, Aghalaya S. Vatsala * and Ross A. Chiquet Department of Mathematics, University

More information

Oscillatory Solutions of Nonlinear Fractional Difference Equations

Oscillatory Solutions of Nonlinear Fractional Difference Equations International Journal of Difference Equations ISSN 0973-6069, Volume 3, Number, pp. 9 3 208 http://campus.mst.edu/ijde Oscillaty Solutions of Nonlinear Fractional Difference Equations G. E. Chatzarakis

More information

arxiv: v1 [math.ca] 12 Feb 2010

arxiv: v1 [math.ca] 12 Feb 2010 YOUNG S INTEGRAL INEQUALITY WITH UPPER AND LOWER BOUNDS DOUGLAS R. ANDERSON, STEVEN NOREN, AND BRENT PERREAULT arxiv:12.2463v1 [math.ca] 12 Feb 21 Abstract. Young s integral inequality is reformulated

More information

A collocation method for solving the fractional calculus of variation problems

A collocation method for solving the fractional calculus of variation problems Bol. Soc. Paran. Mat. (3s.) v. 35 1 (2017): 163 172. c SPM ISSN-2175-1188 on line ISSN-00378712 in press SPM: www.spm.uem.br/bspm doi:10.5269/bspm.v35i1.26333 A collocation method for solving the fractional

More information

Applied Mathematics Letters

Applied Mathematics Letters Applied Mathematics Letters 24 (211) 219 223 Contents lists available at ScienceDirect Applied Mathematics Letters journal homepage: www.elsevier.com/locate/aml Laplace transform and fractional differential

More information

EXISTENCE AND UNIQUENESS OF POSITIVE SOLUTIONS TO HIGHER-ORDER NONLINEAR FRACTIONAL DIFFERENTIAL EQUATION WITH INTEGRAL BOUNDARY CONDITIONS

EXISTENCE AND UNIQUENESS OF POSITIVE SOLUTIONS TO HIGHER-ORDER NONLINEAR FRACTIONAL DIFFERENTIAL EQUATION WITH INTEGRAL BOUNDARY CONDITIONS Electronic Journal of Differential Equations, Vol. 212 (212), No. 234, pp. 1 11. ISSN: 172-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu EXISTENCE AND UNIQUENESS

More information

A NEW CLASS OF FOUR-POINT FRACTIONAL SUM BOUNDARY VALUE PROBLEMS FOR NONLINEAR SEQUENTIAL FRACTIONAL DIFFERENCE EQUATIONS INVOLVING SHIFT OPERATORS

A NEW CLASS OF FOUR-POINT FRACTIONAL SUM BOUNDARY VALUE PROBLEMS FOR NONLINEAR SEQUENTIAL FRACTIONAL DIFFERENCE EQUATIONS INVOLVING SHIFT OPERATORS Kragujevac Journal of Mathematics Volume 23) 208), Pages 37 387. A NEW CLASS OF FOUR-POINT FRACTIONAL SUM BOUNDARY VALUE PROBLEMS FOR NONLINEAR SEQUENTIAL FRACTIONAL DIFFERENCE EQUATIONS INVOLVING SHIFT

More information

Transformation formulas for the generalized hypergeometric function with integral parameter differences

Transformation formulas for the generalized hypergeometric function with integral parameter differences Transformation formulas for the generalized hypergeometric function with integral parameter differences A. R. Miller Formerly Professor of Mathematics at George Washington University, 66 8th Street NW,

More information

IMPROVEMENTS OF COMPOSITION RULE FOR THE CANAVATI FRACTIONAL DERIVATIVES AND APPLICATIONS TO OPIAL-TYPE INEQUALITIES

IMPROVEMENTS OF COMPOSITION RULE FOR THE CANAVATI FRACTIONAL DERIVATIVES AND APPLICATIONS TO OPIAL-TYPE INEQUALITIES Dynamic Systems and Applications ( 383-394 IMPROVEMENTS OF COMPOSITION RULE FOR THE CANAVATI FRACTIONAL DERIVATIVES AND APPLICATIONS TO OPIAL-TYPE INEQUALITIES M ANDRIĆ, J PEČARIĆ, AND I PERIĆ Faculty

More information

A Comparison Result for the Fractional Difference Operator

A Comparison Result for the Fractional Difference Operator International Journal of Difference Equations ISSN 0973-6069, Volume 6, Number 1, pp. 17 37 (2011) http://campus.mst.edu/ijde A Comparison Result for the Fractional Difference Operator Christopher S. Goodrich

More information

Oscillation results for certain forced fractional difference equations with damping term

Oscillation results for certain forced fractional difference equations with damping term Li Advances in Difference Equations 06) 06:70 DOI 0.86/s66-06-0798- R E S E A R C H Open Access Oscillation results for certain forced fractional difference equations with damping term Wei Nian Li * *

More information

EXISTENCE AND UNIQUENESS OF SOLUTIONS TO FUNCTIONAL INTEGRO-DIFFERENTIAL FRACTIONAL EQUATIONS

EXISTENCE AND UNIQUENESS OF SOLUTIONS TO FUNCTIONAL INTEGRO-DIFFERENTIAL FRACTIONAL EQUATIONS Electronic Journal of Differential Equations, Vol. 212 212, No. 13, pp. 1 9. ISSN: 172-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu EXISTENCE AND UNIQUENESS

More information

A Numerical Scheme for Generalized Fractional Optimal Control Problems

A Numerical Scheme for Generalized Fractional Optimal Control Problems Available at http://pvamuedu/aam Appl Appl Math ISSN: 1932-9466 Vol 11, Issue 2 (December 216), pp 798 814 Applications and Applied Mathematics: An International Journal (AAM) A Numerical Scheme for Generalized

More information

Numerical solution for complex systems of fractional order

Numerical solution for complex systems of fractional order Shiraz University of Technology From the SelectedWorks of Habibolla Latifizadeh 213 Numerical solution for complex systems of fractional order Habibolla Latifizadeh, Shiraz University of Technology Available

More information

REFLECTION SYMMETRIC FORMULATION OF GENERALIZED FRACTIONAL VARIATIONAL CALCULUS

REFLECTION SYMMETRIC FORMULATION OF GENERALIZED FRACTIONAL VARIATIONAL CALCULUS RESEARCH PAPER REFLECTION SYMMETRIC FORMULATION OF GENERALIZED FRACTIONAL VARIATIONAL CALCULUS Ma lgorzata Klimek 1, Maria Lupa 2 Abstract We define generalized fractional derivatives GFDs symmetric and

More information

On The Uniqueness and Solution of Certain Fractional Differential Equations

On The Uniqueness and Solution of Certain Fractional Differential Equations On The Uniqueness and Solution of Certain Fractional Differential Equations Prof. Saad N.Al-Azawi, Assit.Prof. Radhi I.M. Ali, and Muna Ismail Ilyas Abstract We consider the fractional differential equations

More information

FRACTIONAL INTEGRAL INEQUALITIES FOR DIFFERENTIABLE CONVEX MAPPINGS AND APPLICATIONS TO SPECIAL MEANS AND A MIDPOINT FORMULA

FRACTIONAL INTEGRAL INEQUALITIES FOR DIFFERENTIABLE CONVEX MAPPINGS AND APPLICATIONS TO SPECIAL MEANS AND A MIDPOINT FORMULA Journal of Applied Mathematics, Statistics and Informatics (JAMSI), 8 (), No. FRACTIONAL INTEGRAL INEQUALITIES FOR DIFFERENTIABLE CONVEX MAPPINGS AND APPLICATIONS TO SPECIAL MEANS AND A MIDPOINT FORMULA

More information

Submitted Version to CAMWA, September 30, 2009 THE LAPLACE TRANSFORM ON ISOLATED TIME SCALES

Submitted Version to CAMWA, September 30, 2009 THE LAPLACE TRANSFORM ON ISOLATED TIME SCALES Submitted Version to CAMWA, September 30, 2009 THE LAPLACE TRANSFORM ON ISOLATED TIME SCALES MARTIN BOHNER AND GUSEIN SH. GUSEINOV Missouri University of Science and Technology, Department of Mathematics

More information

HOMOTOPY PERTURBATION METHOD TO FRACTIONAL BIOLOGICAL POPULATION EQUATION. 1. Introduction

HOMOTOPY PERTURBATION METHOD TO FRACTIONAL BIOLOGICAL POPULATION EQUATION. 1. Introduction Fractional Differential Calculus Volume 1, Number 1 (211), 117 124 HOMOTOPY PERTURBATION METHOD TO FRACTIONAL BIOLOGICAL POPULATION EQUATION YANQIN LIU, ZHAOLI LI AND YUEYUN ZHANG Abstract In this paper,

More information

Iterative scheme to a coupled system of highly nonlinear fractional order differential equations

Iterative scheme to a coupled system of highly nonlinear fractional order differential equations Computational Methods for Differential Equations http://cmde.tabrizu.ac.ir Vol. 3, No. 3, 215, pp. 163-176 Iterative scheme to a coupled system of highly nonlinear fractional order differential equations

More information

Elena Gogovcheva, Lyubomir Boyadjiev 1 Dedicated to Professor H.M. Srivastava, on the occasion of his 65th Birth Anniversary Abstract

Elena Gogovcheva, Lyubomir Boyadjiev 1 Dedicated to Professor H.M. Srivastava, on the occasion of his 65th Birth Anniversary Abstract FRACTIONAL EXTENSIONS OF JACOBI POLYNOMIALS AND GAUSS HYPERGEOMETRIC FUNCTION Elena Gogovcheva, Lyubomir Boyadjiev 1 Dedicated to Professor H.M. Srivastava, on the occasion of his 65th Birth Anniversary

More information

arxiv: v1 [math.oc] 28 Mar 2011

arxiv: v1 [math.oc] 28 Mar 2011 Fractional variational calculus for nondifferentiable functions arxiv:3.546v [math.oc] 28 Mar 2 Ricardo Almeida ricardo.almeida@ua.pt Delfim F. M. Torres delfim@ua.pt Department of Mathematics, University

More information

BOUNDARY VALUE PROBLEMS FOR DISCRETE FRACTIONAL EQUATIONS

BOUNDARY VALUE PROBLEMS FOR DISCRETE FRACTIONAL EQUATIONS University of Nebraska - Lincoln DigitalCommons@University of Nebraska - Lincoln Dissertations, Theses, and Student Research Papers in Mathematics Mathematics, Department of 5-28-2013 BOUNDARY VALUE PROBLEMS

More information

DIfferential equations of fractional order have been the

DIfferential equations of fractional order have been the Multistage Telescoping Decomposition Method for Solving Fractional Differential Equations Abdelkader Bouhassoun Abstract The application of telescoping decomposition method, developed for ordinary differential

More information

Yi Wang Department of Applied Mathematics, Dalian University of Technology, Dalian , China (Submitted June 2002)

Yi Wang Department of Applied Mathematics, Dalian University of Technology, Dalian , China (Submitted June 2002) SELF-INVERSE SEQUENCES RELATED TO A BINOMIAL INVERSE PAIR Yi Wang Department of Applied Mathematics, Dalian University of Technology, Dalian 116024, China (Submitted June 2002) 1 INTRODUCTION Pairs of

More information

Computers and Mathematics with Applications. Fractional variational calculus for nondifferentiable functions

Computers and Mathematics with Applications. Fractional variational calculus for nondifferentiable functions Computers and Mathematics with Applications 6 (2) 397 34 Contents lists available at ScienceDirect Computers and Mathematics with Applications journal homepage: www.elsevier.com/locate/camwa Fractional

More information

Research Article Solvability for a Coupled System of Fractional Integrodifferential Equations with m-point Boundary Conditions on the Half-Line

Research Article Solvability for a Coupled System of Fractional Integrodifferential Equations with m-point Boundary Conditions on the Half-Line Abstract and Applied Analysis Volume 24, Article ID 29734, 7 pages http://dx.doi.org/.55/24/29734 Research Article Solvability for a Coupled System of Fractional Integrodifferential Equations with m-point

More information

On The Leibniz Rule And Fractional Derivative For Differentiable And Non-Differentiable Functions

On The Leibniz Rule And Fractional Derivative For Differentiable And Non-Differentiable Functions On The Leibniz Rule And Fractional Derivative For Differentiable And Non-Differentiable Functions Xiong Wang Center of Chaos and Complex Network, Department of Electronic Engineering, City University of

More information

ON THE C-LAGUERRE FUNCTIONS

ON THE C-LAGUERRE FUNCTIONS ON THE C-LAGUERRE FUNCTIONS M. Ishteva, L. Boyadjiev 2 (Submitted by... on... ) MATHEMATIQUES Fonctions Specialles This announcement refers to a fractional extension of the classical Laguerre polynomials.

More information

CLASSICAL AND FRACTIONAL ASPECTS OF TWO COUPLED PENDULUMS

CLASSICAL AND FRACTIONAL ASPECTS OF TWO COUPLED PENDULUMS (c) 018 Rom. Rep. Phys. (for accepted papers only) CLASSICAL AND FRACTIONAL ASPECTS OF TWO COUPLED PENDULUMS D. BALEANU 1,, A. JAJARMI 3,, J.H. ASAD 4 1 Department of Mathematics, Faculty of Arts and Sciences,

More information

EXISTENCE AND UNIQUENESS OF SOLUTIONS FOR A SYSTEM OF FRACTIONAL DIFFERENTIAL EQUATIONS 1. Yong Zhou. Abstract

EXISTENCE AND UNIQUENESS OF SOLUTIONS FOR A SYSTEM OF FRACTIONAL DIFFERENTIAL EQUATIONS 1. Yong Zhou. Abstract EXISTENCE AND UNIQUENESS OF SOLUTIONS FOR A SYSTEM OF FRACTIONAL DIFFERENTIAL EQUATIONS 1 Yong Zhou Abstract In this paper, the initial value problem is discussed for a system of fractional differential

More information

A novel difference schemes for analyzing the fractional Navier- Stokes equations

A novel difference schemes for analyzing the fractional Navier- Stokes equations DOI: 0.55/auom-207-005 An. Şt. Univ. Ovidius Constanţa Vol. 25(),207, 95 206 A novel difference schemes for analyzing the fractional Navier- Stokes equations Khosro Sayevand, Dumitru Baleanu, Fatemeh Sahsavand

More information

Existence of Solutions for Nonlocal Boundary Value Problems of Nonlinear Fractional Differential Equations

Existence of Solutions for Nonlocal Boundary Value Problems of Nonlinear Fractional Differential Equations Advances in Dynamical Systems and Applications ISSN 973-5321, Volume 7, Number 1, pp. 31 4 (212) http://campus.mst.edu/adsa Existence of Solutions for Nonlocal Boundary Value Problems of Nonlinear Fractional

More information

POSITIVE SOLUTIONS FOR BOUNDARY VALUE PROBLEM OF SINGULAR FRACTIONAL FUNCTIONAL DIFFERENTIAL EQUATION

POSITIVE SOLUTIONS FOR BOUNDARY VALUE PROBLEM OF SINGULAR FRACTIONAL FUNCTIONAL DIFFERENTIAL EQUATION International Journal of Pure and Applied Mathematics Volume 92 No. 2 24, 69-79 ISSN: 3-88 (printed version); ISSN: 34-3395 (on-line version) url: http://www.ijpam.eu doi: http://dx.doi.org/.2732/ijpam.v92i2.3

More information

On Bessel Functions in the framework of the Fractional Calculus

On Bessel Functions in the framework of the Fractional Calculus On Bessel Functions in the framework of the Fractional Calculus Luis Rodríguez-Germá 1, Juan J. Trujillo 1, Luis Vázquez 2, M. Pilar Velasco 2. 1 Universidad de La Laguna. Departamento de Análisis Matemático.

More information

TAYLOR POLYNOMIALS FOR NABLA DYNAMIC EQUATIONS ON TIME SCALES

TAYLOR POLYNOMIALS FOR NABLA DYNAMIC EQUATIONS ON TIME SCALES TAYLOR POLYNOMIALS FOR NABLA DYNAMIC EQUATIONS ON TIME SCALES DOUGLAS R. ANDERSON Abtract. We are concerned with the repreentation of polynomial for nabla dynamic equation on time cale. Once etablihed,

More information

Existence of solutions for multi-point boundary value problem of fractional q-difference equation

Existence of solutions for multi-point boundary value problem of fractional q-difference equation Electronic Journal of Qualitative Theory of Differential Euations 211, No. 92, 1-1; http://www.math.u-szeged.hu/ejtde/ Existence of solutions for multi-point boundary value problem of fractional -difference

More information

A Mean Value Theorem for the Conformable Fractional Calculus on Arbitrary Time Scales

A Mean Value Theorem for the Conformable Fractional Calculus on Arbitrary Time Scales Progr. Fract. Differ. Appl. 2, No. 4, 287-291 (2016) 287 Progress in Fractional Differentiation and Applications An International Journal http://dx.doi.org/10.18576/pfda/020406 A Mean Value Theorem for

More information

The Generating Functions for Pochhammer

The Generating Functions for Pochhammer The Generating Functions for Pochhammer Symbol { }, n N Aleksandar Petoević University of Novi Sad Teacher Training Faculty, Department of Mathematics Podgorička 4, 25000 Sombor SERBIA and MONTENEGRO Email

More information

Exact Solution of Some Linear Fractional Differential Equations by Laplace Transform. 1 Introduction. 2 Preliminaries and notations

Exact Solution of Some Linear Fractional Differential Equations by Laplace Transform. 1 Introduction. 2 Preliminaries and notations ISSN 1749-3889 (print), 1749-3897 (online) International Journal of Nonlinear Science Vol.16(213) No.1,pp.3-11 Exact Solution of Some Linear Fractional Differential Equations by Laplace Transform Saeed

More information

Q-INTEGRAL EQUATIONS OF FRACTIONAL ORDERS. 1. Introduction In this paper, we are concerned with the following functional equation

Q-INTEGRAL EQUATIONS OF FRACTIONAL ORDERS. 1. Introduction In this paper, we are concerned with the following functional equation Electronic Journal of Differential Equations, Vol. 216 216, No. 17, pp. 1 14. ISSN: 172-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu Q-INTEGRAL EQUATIONS

More information

Mahmoud M. El-Borai a, Abou-Zaid H. El-Banna b, Walid H. Ahmed c a Department of Mathematics, faculty of science, Alexandria university, Alexandria.

Mahmoud M. El-Borai a, Abou-Zaid H. El-Banna b, Walid H. Ahmed c a Department of Mathematics, faculty of science, Alexandria university, Alexandria. International Journal of Basic & Applied Sciences IJBAS-IJENS Vol:13 No:01 52 On Some Fractional-Integro Partial Differential Equations Mahmoud M. El-Borai a, Abou-Zaid H. El-Banna b, Walid H. Ahmed c

More information

Abstract We paid attention to the methodology of two integral

Abstract We paid attention to the methodology of two integral Comparison of Homotopy Perturbation Sumudu Transform method and Homotopy Decomposition method for solving nonlinear Fractional Partial Differential Equations 1 Rodrigue Batogna Gnitchogna 2 Abdon Atangana

More information

Green s Function for an n-point Right Focal Boundary Value Problem

Green s Function for an n-point Right Focal Boundary Value Problem Green s Function for an n-point Right Focal Boundary Value Problem Doug Anderson Department of Mathematics and Computer Science, Concordia College Moorhead, MN 56562, USA Abstract We determine sufficient

More information

India

India italian journal of pure and applied mathematics n. 36 216 (819 826) 819 ANALYTIC SOLUTION FOR RLC CIRCUIT OF NON-INTGR ORDR Jignesh P. Chauhan Department of Applied Mathematics & Humanities S.V. National

More information

A Note about the Pochhammer Symbol

A Note about the Pochhammer Symbol Mathematica Moravica Vol. 12-1 (2008), 37 42 A Note about the Pochhammer Symbol Aleksandar Petoević Abstract. In this paper we give elementary proofs of the generating functions for the Pochhammer symbol

More information

The geometric and physical interpretation of fractional order derivatives of polynomial functions

The geometric and physical interpretation of fractional order derivatives of polynomial functions The geometric and physical interpretation of fractional order derivatives of polynomial functions M.H. Tavassoli, A. Tavassoli, M.R. Ostad Rahimi Abstract. In this paper, after a brief mention of the definitions

More information

RIEMANN-LIOUVILLE FRACTIONAL COSINE FUNCTIONS. = Au(t), t > 0 u(0) = x,

RIEMANN-LIOUVILLE FRACTIONAL COSINE FUNCTIONS. = Au(t), t > 0 u(0) = x, Electronic Journal of Differential Equations, Vol. 216 (216, No. 249, pp. 1 14. ISSN: 172-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu RIEMANN-LIOUVILLE FRACTIONAL COSINE FUNCTIONS

More information

Peter Bala, Nov

Peter Bala, Nov Fractional iteration of a series inversion operator Peter Bala, Nov 16 2015 We consider an operator on formal power series, closely related to the series reversion operator, and show how to dene comple

More information

POSITIVE SOLUTIONS OF FRACTIONAL DIFFERENTIAL EQUATIONS WITH DERIVATIVE TERMS

POSITIVE SOLUTIONS OF FRACTIONAL DIFFERENTIAL EQUATIONS WITH DERIVATIVE TERMS Electronic Journal of Differential Equations, Vol. 212 (212), No. 215, pp. 1 27. ISSN: 172-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu POSITIVE SOLUTIONS

More information

A computationally effective predictor-corrector method for simulating fractional order dynamical control system

A computationally effective predictor-corrector method for simulating fractional order dynamical control system ANZIAM J. 47 (EMA25) pp.168 184, 26 168 A computationally effective predictor-corrector method for simulating fractional order dynamical control system. Yang F. Liu (Received 14 October 25; revised 24

More information

Boundary Value Problems of Nabla Fractional Difference Equations

Boundary Value Problems of Nabla Fractional Difference Equations University of Nebraska - Lincoln DigitalCommons@University of Nebraska - Lincoln Dissertations, Theses, and Student Research Papers in Mathematics Mathematics, Department of Summer 8-204 Boundary Value

More information

On the Finite Caputo and Finite Riesz Derivatives

On the Finite Caputo and Finite Riesz Derivatives EJTP 3, No. 1 (006) 81 95 Electronic Journal of Theoretical Physics On the Finite Caputo and Finite Riesz Derivatives A. M. A. El-Sayed 1 and M. Gaber 1 Faculty of Science University of Alexandria, Egypt

More information

EXISTENCE THEOREM FOR A FRACTIONAL MULTI-POINT BOUNDARY VALUE PROBLEM

EXISTENCE THEOREM FOR A FRACTIONAL MULTI-POINT BOUNDARY VALUE PROBLEM Fixed Point Theory, 5(, No., 3-58 http://www.math.ubbcluj.ro/ nodeacj/sfptcj.html EXISTENCE THEOREM FOR A FRACTIONAL MULTI-POINT BOUNDARY VALUE PROBLEM FULAI CHEN AND YONG ZHOU Department of Mathematics,

More information

The solutions of time and space conformable fractional heat equations with conformable Fourier transform

The solutions of time and space conformable fractional heat equations with conformable Fourier transform Acta Univ. Sapientiae, Mathematica, 7, 2 (25) 3 4 DOI:.55/ausm-25-9 The solutions of time and space conformable fractional heat equations with conformable Fourier transform Yücel Çenesiz Department of

More information

Polyexponentials. Khristo N. Boyadzhiev Ohio Northern University Departnment of Mathematics Ada, OH

Polyexponentials. Khristo N. Boyadzhiev Ohio Northern University Departnment of Mathematics Ada, OH Polyexponentials Khristo N. Boyadzhiev Ohio Northern University Departnment of Mathematics Ada, OH 45810 k-boyadzhiev@onu.edu 1. Introduction. The polylogarithmic function [15] (1.1) and the more general

More information

Dynamic Systems and Applications 13 (2004) PARTIAL DIFFERENTIATION ON TIME SCALES

Dynamic Systems and Applications 13 (2004) PARTIAL DIFFERENTIATION ON TIME SCALES Dynamic Systems and Applications 13 (2004) 351-379 PARTIAL DIFFERENTIATION ON TIME SCALES MARTIN BOHNER AND GUSEIN SH GUSEINOV University of Missouri Rolla, Department of Mathematics and Statistics, Rolla,

More information

Economic Interpretation of Fractional Derivatives

Economic Interpretation of Fractional Derivatives Progr. Fract. Differ. Appl. 3, No. 1, 1-6 (217) 1 Progress in Fractional Differentiation and Applications An International Journal http://dx.doi.org/1.18576/pfda/311 Economic Interpretation of Fractional

More information

EXACT TRAVELING WAVE SOLUTIONS FOR NONLINEAR FRACTIONAL PARTIAL DIFFERENTIAL EQUATIONS USING THE IMPROVED (G /G) EXPANSION METHOD

EXACT TRAVELING WAVE SOLUTIONS FOR NONLINEAR FRACTIONAL PARTIAL DIFFERENTIAL EQUATIONS USING THE IMPROVED (G /G) EXPANSION METHOD Jan 4. Vol. 4 No. 7-4 EAAS & ARF. All rights reserved ISSN5-869 EXACT TRAVELIN WAVE SOLUTIONS FOR NONLINEAR FRACTIONAL PARTIAL DIFFERENTIAL EQUATIONS USIN THE IMPROVED ( /) EXPANSION METHOD Elsayed M.

More information

FRACTIONAL FOURIER TRANSFORM AND FRACTIONAL DIFFUSION-WAVE EQUATIONS

FRACTIONAL FOURIER TRANSFORM AND FRACTIONAL DIFFUSION-WAVE EQUATIONS FRACTIONAL FOURIER TRANSFORM AND FRACTIONAL DIFFUSION-WAVE EQUATIONS L. Boyadjiev*, B. Al-Saqabi** Department of Mathematics, Faculty of Science, Kuwait University *E-mail: boyadjievl@yahoo.com **E-mail:

More information

Nontrivial solutions for fractional q-difference boundary value problems

Nontrivial solutions for fractional q-difference boundary value problems Electronic Journal of Qualitative Theory of Differential Equations 21, No. 7, 1-1; http://www.math.u-szeged.hu/ejqtde/ Nontrivial solutions for fractional q-difference boundary value problems Rui A. C.

More information

Homotopy Analysis Method for Nonlinear Differential Equations with Fractional Orders

Homotopy Analysis Method for Nonlinear Differential Equations with Fractional Orders Homotopy Analysis Method for Nonlinear Differential Equations with Fractional Orders Yin-Ping Liu and Zhi-Bin Li Department of Computer Science, East China Normal University, Shanghai, 200062, China Reprint

More information

Research Article On Local Fractional Continuous Wavelet Transform

Research Article On Local Fractional Continuous Wavelet Transform Hindawi Publishing Corporation Abstract and Applied Analysis Volume 203, Article ID 72546, 5 pages http://dx.doi.org/0.55/203/72546 Research Article On Local Fractional Continuous Wavelet Transform Xiao-Jun

More information

Dynamic Response and Oscillating Behaviour of Fractionally Damped Beam

Dynamic Response and Oscillating Behaviour of Fractionally Damped Beam Copyright 2015 Tech Science Press CMES, vol.104, no.3, pp.211-225, 2015 Dynamic Response and Oscillating Behaviour of Fractionally Damped Beam Diptiranjan Behera 1 and S. Chakraverty 2 Abstract: This paper

More information

Periodic Solutions in Shifts δ ± for a Dynamic Equation on Time Scales

Periodic Solutions in Shifts δ ± for a Dynamic Equation on Time Scales Advances in Dynamical Systems and Applications ISSN 0973-5321, Volume 9, Number 1, pp. 97 108 (2014) http://campus.mst.edu/adsa Periodic Solutions in Shifts δ ± for a Dynamic Equation on Time Scales Erbil

More information

Existence of triple positive solutions for boundary value problem of nonlinear fractional differential equations

Existence of triple positive solutions for boundary value problem of nonlinear fractional differential equations Computational Methods for Differential Equations http://cmde.tabrizu.ac.ir Vol. 5, No. 2, 217, pp. 158-169 Existence of triple positive solutions for boundary value problem of nonlinear fractional differential

More information

Even Number of Positive Solutions for 3n th Order Three-Point Boundary Value Problems on Time Scales K. R. Prasad 1 and N.

Even Number of Positive Solutions for 3n th Order Three-Point Boundary Value Problems on Time Scales K. R. Prasad 1 and N. Electronic Journal of Qualitative Theory of Differential Equations 011, No. 98, 1-16; http://www.math.u-szeged.hu/ejqtde/ Even Number of Positive Solutions for 3n th Order Three-Point Boundary Value Problems

More information

Fractional Calculus for Solving Abel s Integral Equations Using Chebyshev Polynomials

Fractional Calculus for Solving Abel s Integral Equations Using Chebyshev Polynomials Applied Mathematical Sciences, Vol. 5, 211, no. 45, 227-2216 Fractional Calculus for Solving Abel s Integral Equations Using Chebyshev Polynomials Z. Avazzadeh, B. Shafiee and G. B. Loghmani Department

More information

On four-point nonlocal boundary value problems of nonlinear impulsive equations of fractional order

On four-point nonlocal boundary value problems of nonlinear impulsive equations of fractional order On four-point nonlocal boundary value problems of nonlinear impulsive equations of fractional order Dehong Ji Tianjin University of Technology Department of Applied Mathematics Hongqi Nanlu Extension,

More information

Research Article The Extended Fractional Subequation Method for Nonlinear Fractional Differential Equations

Research Article The Extended Fractional Subequation Method for Nonlinear Fractional Differential Equations Hindawi Publishing Corporation Mathematical Problems in Engineering Volume 2012, Article ID 924956, 11 pages doi:10.1155/2012/924956 Research Article The Extended Fractional Subequation Method for Nonlinear

More information

NUMERICAL SOLUTION OF FRACTIONAL ORDER DIFFERENTIAL EQUATIONS USING HAAR WAVELET OPERATIONAL MATRIX

NUMERICAL SOLUTION OF FRACTIONAL ORDER DIFFERENTIAL EQUATIONS USING HAAR WAVELET OPERATIONAL MATRIX Palestine Journal of Mathematics Vol. 6(2) (217), 515 523 Palestine Polytechnic University-PPU 217 NUMERICAL SOLUTION OF FRACTIONAL ORDER DIFFERENTIAL EQUATIONS USING HAAR WAVELET OPERATIONAL MATRIX Raghvendra

More information

ANALYTIC SOLUTIONS AND NUMERICAL SIMULATIONS OF MASS-SPRING AND DAMPER-SPRING SYSTEMS DESCRIBED BY FRACTIONAL DIFFERENTIAL EQUATIONS

ANALYTIC SOLUTIONS AND NUMERICAL SIMULATIONS OF MASS-SPRING AND DAMPER-SPRING SYSTEMS DESCRIBED BY FRACTIONAL DIFFERENTIAL EQUATIONS ANALYTIC SOLUTIONS AND NUMERICAL SIMULATIONS OF MASS-SPRING AND DAMPER-SPRING SYSTEMS DESCRIBED BY FRACTIONAL DIFFERENTIAL EQUATIONS J.F. GÓMEZ-AGUILAR Departamento de Materiales Solares, Instituto de

More information

This work has been submitted to ChesterRep the University of Chester s online research repository.

This work has been submitted to ChesterRep the University of Chester s online research repository. This work has been submitted to ChesterRep the University of Chester s online research repository http://chesterrep.openrepository.com Author(s): Kai Diethelm; Neville J Ford Title: Volterra integral equations

More information

UNIQUENESS OF SOLUTIONS TO MATRIX EQUATIONS ON TIME SCALES

UNIQUENESS OF SOLUTIONS TO MATRIX EQUATIONS ON TIME SCALES Electronic Journal of Differential Equations, Vol. 2013 (2013), No. 50, pp. 1 13. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu UNIQUENESS OF

More information

Optimal Controllers with Complex Order Derivatives

Optimal Controllers with Complex Order Derivatives Optimal Controllers with Complex Order Derivatives J.A. Tenreiro Machado Abstract This paper studies the optimization of complex-order algorithms for the discrete-time control of linear and nonlinear systems.

More information

SMOOTHNESS PROPERTIES OF SOLUTIONS OF CAPUTO- TYPE FRACTIONAL DIFFERENTIAL EQUATIONS. Kai Diethelm. Abstract

SMOOTHNESS PROPERTIES OF SOLUTIONS OF CAPUTO- TYPE FRACTIONAL DIFFERENTIAL EQUATIONS. Kai Diethelm. Abstract SMOOTHNESS PROPERTIES OF SOLUTIONS OF CAPUTO- TYPE FRACTIONAL DIFFERENTIAL EQUATIONS Kai Diethelm Abstract Dedicated to Prof. Michele Caputo on the occasion of his 8th birthday We consider ordinary fractional

More information

Some New Results on the New Conformable Fractional Calculus with Application Using D Alambert Approach

Some New Results on the New Conformable Fractional Calculus with Application Using D Alambert Approach Progr. Fract. Differ. Appl. 2, No. 2, 115-122 (2016) 115 Progress in Fractional Differentiation and Applications An International Journal http://dx.doi.org/10.18576/pfda/020204 Some New Results on the

More information

Research Article Applying GG-Convex Function to Hermite-Hadamard Inequalities Involving Hadamard Fractional Integrals

Research Article Applying GG-Convex Function to Hermite-Hadamard Inequalities Involving Hadamard Fractional Integrals International Journal of Mathematics and Mathematical Sciences Volume 4, Article ID 3635, pages http://dx.doi.org/.55/4/3635 Research Article Applying GG-Convex Function to Hermite-Hadamard Inequalities

More information

SOLUTION OF SPACE-TIME FRACTIONAL SCHRÖDINGER EQUATION OCCURRING IN QUANTUM MECHANICS. Abstract

SOLUTION OF SPACE-TIME FRACTIONAL SCHRÖDINGER EQUATION OCCURRING IN QUANTUM MECHANICS. Abstract SOLUTION OF SPACE-TIME FRACTIONAL SCHRÖDINGER EQUATION OCCURRING IN QUANTUM MECHANICS R.K. Saxena a, Ravi Saxena b and S.L. Kalla c Abstract Dedicated to Professor A.M. Mathai on the occasion of his 75

More information

Numerical solution of the Bagley Torvik equation. Kai Diethelm & Neville J. Ford

Numerical solution of the Bagley Torvik equation. Kai Diethelm & Neville J. Ford ISSN 1360-1725 UMIST Numerical solution of the Bagley Torvik equation Kai Diethelm & Neville J. Ford Numerical Analysis Report No. 378 A report in association with Chester College Manchester Centre for

More information

Analytic solution of fractional integro-differential equations

Analytic solution of fractional integro-differential equations Annals of the University of Craiova, Mathematics and Computer Science Series Volume 38(1), 211, Pages 1 1 ISSN: 1223-6934 Analytic solution of fractional integro-differential equations Fadi Awawdeh, E.A.

More information

Hopf bifurcation for a class of fractional differential equations with delay

Hopf bifurcation for a class of fractional differential equations with delay Nonlinear Dyn (01 69:71 79 DOI 10.1007/s11071-011-099-5 ORIGINAL PAPER Hopf bifurcation for a class of fractional differential equations with delay Azizollah Babakhani Dumitru Baleanu Reza Khanbabaie Received:

More information

arxiv: v1 [math.na] 8 Jan 2019

arxiv: v1 [math.na] 8 Jan 2019 arxiv:190102503v1 [mathna] 8 Jan 2019 A Numerical Approach for Solving of Fractional Emden-Fowler Type Equations Josef Rebenda Zdeněk Šmarda c 2018 AIP Publishing This article may be downloaded for personal

More information

Application of new iterative transform method and modified fractional homotopy analysis transform method for fractional Fornberg-Whitham equation

Application of new iterative transform method and modified fractional homotopy analysis transform method for fractional Fornberg-Whitham equation Available online at www.tjnsa.com J. Nonlinear Sci. Appl. 9 (2016), 2419 2433 Research Article Application of new iterative transform method and modified fractional homotopy analysis transform method for

More information