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Hyers-Ulam stability of Davison functional equation on restricted domains

  • Choonkil Park , Mohammad Amin Tareeghee , Abbas Najati EMAIL logo and Batool Noori
Published/Copyright: September 26, 2024
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Abstract

In this article, we study the Hyers-Ulam stability of Davison functional equation

f ( x y ) + f ( x + y ) = f ( x y + x ) + f ( y )

on some unbounded restricted domains. Using the obtained results, we study an interesting asymptotic behavior of Davison functions. We also investigate the Hyers-Ulam stability of Davison functional equation and its generalized form given by

f ( x y ) + g ( x + y ) = h ( x y + x ) + k ( y ) ,

for x , y R 0 = { t R : t 0 } .

MSC 2010: 39B82; 39B62

1 Introduction and preliminaries

During the 17th International Symposium on functional equations, the following functional equation

(1) f ( x y ) + f ( x + y ) = f ( x y + x ) + f ( y ) ,

was introduced by Davison [1]. He specifically asked about the general solution of (1) when the domain and range of f are assumed to be (commutative) fields. Benz [2] proved that if f : R R is a continuous solution of (1), then f is of the form f ( x ) = a x + b , where a and b are arbitrary constants. The general solution (without any regularity assumptions on f : R R ) of the Davison functional equation (1) was obtained by Girgensohn and Lajkó [3]. They proved that if f : R R is a solution (1), then f has the form f ( x ) = A ( x ) + b , where A : R R is an additive function and b R is an arbitrary constant. Moreover, they obtained the general solution of the generalized version of (1) as follows.

Theorem 1.1

[3] The functions f , g , h , k : R R satisfy

(2) f ( x y ) + g ( x + y ) = h ( x y + x ) + k ( y ) , x , y R ,

if and only if they have the form

f ( x ) = A ( x ) + b 1 , g ( x ) = A ( x ) + b 2 , h ( x ) = A ( x ) + b 3 , k ( x ) = A ( x ) + b 4 ,

where A : R R is additive and b 1 , b 2 , b 3 , b 4 are real constants with b 1 + b 2 = b 3 + b 4 .

It should be noted that the aforementioned results can be extended to functions f : K G , where K is a commutative field of characteristic different from 2 and 3, and G is an abelian group.

Girgensohn and Lajkó [3] also presented the general solution of (1) and (2) for x , y ( 0 , + ) .

Davison [4] solved the functional equation (1) in two cases for functions with values in an abelian group G . First f : N G , and second f : Z G , where N and Z are, respectively, the set of natural numbers and the set of integer numbers. Indeed, he proved that every solution of (1) is a linear combination (in the codomain) of four functions.

In 1940, Ulam [5] posed the following problem concerning the stability of group homomorphisms: Let ( G 1 , * ) be a group, ( G 2 , ) a metric group with a metric d ( . , . ) and ε > 0 . Find a δ > 0 such that if f : G 1 G 2 fulfills d ( f ( x * y ) , f ( x ) f ( y ) ) δ for all x , y G 1 , then there exists a homomorphism h : G 1 G 2 such that d ( f ( x ) , h ( x ) ) ε for all x G 1 . This problem was first solved by Hyers [6] for the case where G 1 and G 2 are Banach spaces. The Hyers-Ulam stability problem for various functional equations have been investigated by numerous mathematicians. For more information on this area we refer the reader to [79].

The Hyers-Ulam stability of the Davison functional equation was first treated by Jung and Sahoo [10]. They investigated the Hyers-Ulam stability of Davison functional equation (1) by following an idea of Girgensohn and Lajkó [3] (see also [11]).

Theorem 1.2

[10] If the function f : R R satisfies the inequality

f ( x y ) + f ( x + y ) f ( x y + x ) f ( y ) ε , x , y R ,

for some ε 0 , then there exists an additive function A : R R such that

f ( x ) A ( x ) f ( 0 ) 12 ε , x R .

It was shown in [12,13] that the estimate 12 ε in Theorem 1.2 can be improved to 9 ε .

Kim [14] studied the Hyers-Ulam stability of two generalized Davison functional equations, namely,

(3) f ( x y ) + f ( x + y ) = g ( x y + x ) + g ( y )

and

f ( x y ) + g ( x + y ) = f ( x y + x ) + g ( y )

for all x , y X and f , g : X Y , where X is a normed algebra with a unit element and Y is a Banach space. The Hyers-Ulam stability of (3) has been investigated in [12].

It will also be interesting to study the Hyers-Ulam stability of Davison functional equations (1) and (2) on restricted domains. In this article, we prove the Hyers-Ulam stability of the Davison functional equation on unbounded restricted domains by following ideas of [3] and [12]. We apply the obtained results to the study of an interesting asymptotic behavior of Davison functions.

2 Hyers-Ulam stability

Throughout this article, we denote by A a normed algebra with the unit element 1 and by a Banach space.

Theorem 2.1

Let f : A be a function which for ε 0 and d > 0 satisfies

(4) f ( x y ) + f ( x + y ) f ( x y + x ) f ( y ) ε , x d , y A .

Then there is a unique additive function φ : A , such that

φ ( x ) f ( x ) + f ( 0 ) 28 ε , x 1 ; φ ( 1 ) f ( 1 ) + f ( 0 ) 19 ε .

Proof

Replace y by y + 1 in (4) to obtain

(5) f ( x y + x ) + f ( x + y + 1 ) f ( x y + 2 x ) f ( y + 1 ) ε ,

for all x , y A with x d . Thus, it follows from (4) and (5) that

(6) f ( x y ) + f ( x + y ) + f ( x + y + 1 ) f ( y ) f ( x y + 2 x ) f ( y + 1 ) f ( x y ) + f ( x + y ) f ( x y + x ) f ( y ) + f ( x y + x ) + f ( x + y + 1 ) f ( x y + 2 x ) f ( y + 1 ) 2 ε ,

for all x , y A with x d . Replacing y by 4 y in (6), we obtain

f ( 4 x y ) + f ( x + 4 y ) + f ( x + 4 y + 1 ) f ( 4 y ) f ( 4 x y + 2 x ) f ( 4 y + 1 ) 2 ε ,

for all x , y A with x d . From (4) and the last inequality, we obtain

f ( x + 4 y ) + f ( x + 4 y + 1 ) f ( 2 x + 2 y ) f ( 4 y ) f ( 4 y + 1 ) + f ( 2 y ) f ( 4 x y ) + f ( x + 4 y ) + f ( x + 4 y + 1 ) f ( 4 y ) f ( 4 x y + 2 x ) f ( 4 y + 1 ) + f ( 4 x y ) + f ( 2 x + 2 y ) f ( 4 x y + 2 x ) f ( 2 y ) 3 ε ,

for all x , y A with x d . If we replace x by x y in the above inequality and then substitute 3 x for x in the resultant inequality, we obtain

(7) f ( 3 x + 3 y ) + f ( 3 x + 3 y + 1 ) f ( 6 x ) f ( 4 y ) f ( 4 y + 1 ) + f ( 2 y ) 3 ε ,

for all x , y A with 3 x y d . Letting y = 0 and y = x separately in (7), we obtain

(8) f ( 3 x ) + f ( 3 x + 1 ) f ( 6 x ) f ( 1 ) 3 ε ,

(9) f ( 0 ) + f ( 1 ) f ( 6 x ) f ( 4 x ) f ( 4 x + 1 ) + f ( 2 x ) 3 ε ,

for all x A with x d . If we replace x , y by 2 x , x , respectively in (7), we have

(10) f ( 3 x ) f ( 3 x + 1 ) + f ( 12 x ) + f ( 4 x ) + f ( 4 x + 1 ) f ( 2 x ) 3 ε ,

for all x A with x d . Adding (8), (9), and (10), we infer that

f ( 12 x ) 2 f ( 6 x ) + f ( 0 ) 9 ε , x d .

Let g ( x ) f ( 6 x ) f ( 0 ) . Then the last inequality means

g ( 2 x ) 2 g ( x ) 9 ε , x d .

It is easy to see that

(11) g ( 2 n + 1 x ) 2 n + 1 g ( 2 m x ) 2 m k = m n 9 ε 2 k + 1 , x d .

This implies that g ( 2 n x ) 2 n n is a Cauchy sequence for x d . It is easy to show that g ( 2 n x ) 2 n n is a Cauchy sequence for each x A and thus converges. Therefore, we can define

T : A , T ( x ) = lim n g ( 2 n x ) 2 n .

Obviously,

(12) T ( 0 ) = 0 , T ( 2 x ) = 2 T ( x ) , T ( x ) = lim n f ( 2 n 6 x ) 2 n , x A .

By (8), we obtain

(13) T ( x ) = lim n f ( 2 n 6 x + 1 ) 2 n , x A .

Using (7), (12), and (13), we obtain

T ( 3 x + 3 y ) = T ( 3 x ) + 3 T ( y ) , x , y A , y 3 x .

Letting x = 0 in the last equation and using T ( 0 ) = 0 , we obtain T ( 3 y ) = 3 T ( y ) for all y A . So, T is additive. Setting m = 0 and taking the limit on both sides of (11) as n , we obtain

T ( x ) f ( 6 x ) + f ( 0 ) 9 ε , x d .

Since T is additive, this inequality implies

(14) φ ( x ) f ( x ) + f ( 0 ) 9 ε , x 6 d ,

where φ ( x ) = 1 6 T ( x ) . Obviously, (14) holds for x = 0 . Let y A and y 1 . We can choose x A such that min { x , x y , x + y , x y + x } 6 d . By (14), we have

φ ( x y ) f ( x y ) + f ( 0 ) 9 ε , φ ( x + y ) f ( x + y ) + f ( 0 ) 9 ε , f ( x y + x ) φ ( x y + x ) f ( 0 ) 9 ε .

Adding these inequalities and (4), we obtain

φ ( x y ) + φ ( x + y ) φ ( x y + x ) f ( y ) + f ( 0 ) 28 ε .

Since φ is additive, the last inequality yields

φ ( y ) f ( y ) + f ( 0 ) 28 ε .

In the case y = 1 , we choose x A such that x 6 d + 1 . By (4) and (14), we have

f ( x ) + f ( x 1 ) f ( 0 ) f ( 1 ) ε , φ ( x 1 ) f ( x 1 ) + f ( 0 ) 9 ε , φ ( x ) f ( x ) + f ( 0 ) 9 ε .

Adding these inequalities and using the additivity of φ , we obtain

φ ( 1 ) f ( 1 ) + f ( 0 ) 19 ε .

The uniqueness of φ is obvious. Hence, the proof is complete.□

With a proof similar to the one presented in Theorem 2.1, we obtain the following result.

Corollary 2.2

Let Y be a linear space and f : A Y a function satisfying

f ( x y ) + f ( x + y ) = f ( x y + x ) + f ( y ) , x d .

Then f is affine, that is, f f ( 0 ) is additive on A .

Remark 2.3

Since

{ ( x , y ) A × A : x 2 d } { ( x , y ) A × A : x + y 2 d } { ( x , y ) A × A : max { x , y } d } ,

the above results are valid if the condition x d is replaced by x + y d or max { x , y } d .

Corollary 2.4

Let Y be a normed linear space. A function f : A Y is affine on A if and only if one of the following conditions hold:

  1. lim x sup y A f ( x y ) + f ( x + y ) f ( x y + x ) f ( y ) = 0 ;

  2. lim x + y [ f ( x y ) + f ( x + y ) f ( x y + x ) f ( y ) ] = 0 ;

  3. lim max { x , y } [ f ( x y ) + f ( x + y ) f ( x y + x ) f ( y ) ] = 0 .

Proof

It is clear that an affine function f : A Y fulfills ( i ) , ( i i ) , ( i i i ) . Obviously, ( i i ) ( i ) and ( i i i ) ( i ) . Let f satisfy ( i ) and ε > 0 be arbitrary. Then there exists d > 0 such that

f ( x y ) + f ( x + y ) f ( x y + x ) f ( y ) ε , x d , y A .

Let Y ˜ be the completion of Y . By Theorem 2.1, there exists an additive function φ : A Y ˜ satisfying

f ( x ) f ( 0 ) φ ( x ) 28 ε , x A .

Let g ( x ) = f ( x ) f ( 0 ) . Then

g ( x + y ) g ( x ) g ( y ) g ( x + y ) φ ( x + y ) + g ( x ) φ ( x ) + g ( y ) φ ( y ) 84 ε , x , y A .

Since ε > 0 is arbitrary, we obtain g is additive. This means f is affine.□

Corollary 2.5

Let f : R R be a function given by

f ( x ) 1 1 + x 2 , x R .

It is clear that

lim y [ f ( x y ) + f ( x + y ) f ( x y + x ) f ( y ) ] = 0 ,

but f is not affine.

Note that, as a consequence of Corollary 2.4, we obtain the result that every function f : R R is either affine or satisfies the condition

sup x , y R f ( x y ) + f ( x + y ) f ( x y + x ) f ( y ) x p = ,

for all p > 0 .

3 Stability on R 0

The aim of this section is to present the Hyers-Ulam stability of Davison functional equation and its generalized form (2) for x , y R 0 = { t R : t 0 } .

Theorem 3.1

Let ε 0 and f : [ 0 , + ) be a function satisfying

(15) f ( x y ) + f ( x + y ) f ( x y + x ) f ( y ) ε , x , y 0 .

Then there is an affine function ψ : R such that

ψ ( x ) f ( x ) 55 ε , x > 0 .

Proof

Replacing y by y + 1 in (15), we obtain

f ( x y + x ) + f ( x + y + 1 ) f ( x y + 2 x ) f ( y + 1 ) ε , x , y 0 .

Adding this inequality and (15), we obtain

f ( x y ) + f ( x + y ) + f ( x + y + 1 ) f ( y ) f ( x y + 2 x ) f ( y + 1 ) 2 ε , x , y 0 .

Now, replacing x by x 2 and y by 2 y , we obtain

f ( x y ) + f x 2 + 2 y + f x 2 + 2 y + 1 f ( 2 y ) f ( x y + x ) f ( 2 y + 1 ) 2 ε , x , y 0 .

By this inequality and (15), one obtains

(16) f x 2 + 2 y + f x 2 + 2 y + 1 f ( x + y ) f ( 2 y ) f ( 2 y + 1 ) + f ( y ) 3 ε ,

for all x , y 0 . Replacing x by x y 3 and y by y 3 in (16), we obtain

f x + y 2 + f x + y 2 + 1 f 2 3 y f 2 3 y + 1 + f 1 3 y f ( x ) 3 ε ,

for all x y 3 0 . The last inequality can be written as follows:

(17) G ( x + y ) f ( x ) H ( y ) 3 ε , x y 3 0 ,

where

G ( t ) f t 2 + f t 2 + 1 , H ( t ) f 2 3 t + f 2 3 t + 1 f 1 3 t .

Letting y = x and y = 0 separately in (17), we obtain

(18) f ( x + 1 ) H ( x ) 3 ε , x 0 ,

(19) G ( x ) f ( x ) f ( 1 ) 3 ε , x 0 .

By (19), we obtain

(20) G ( x + y ) f ( x + y ) f ( 1 ) 3 ε , x , y 0 .

It follows from (17), (18), and (20) that

(21) f ( x + y ) f ( x ) f ( y + 1 ) + f ( 1 ) 9 ε , x y 3 0 .

Putting y = 1 in (21), we obtain

(22) f ( x + 1 ) f ( x ) f ( 2 ) + f ( 1 ) 9 ε , x 1 3 .

It follows from (21) and (22) that

(23) f ( x + y ) f ( x ) f ( y ) f ( 2 ) + 2 f ( 1 ) 18 ε , x y 3 , y 1 3 .

Letting y = x in (23), we obtain

f ( 2 x ) 2 f ( x ) + c 18 ε , x 1 3 ,

where c = 2 f ( 1 ) f ( 2 ) . Then

(24) f ( 2 n + 1 x ) 2 n + 1 f ( 2 m x ) 2 m + k = m n c 2 k + 1 k = m n 9 ε 2 k , x 1 3 .

Then { f ( 2 n x ) 2 n } n is a Cauchy sequence for all x 0 . Define

A : [ 0 , + ) , A ( x ) lim n f ( 2 n x ) 2 n .

It follows from (19) and the definition of G that

A ( x ) lim n G ( 2 n x ) 2 n = lim n f ( 2 n x + 1 ) 2 n , x 0 .

Hence, (18) yields

A ( x ) lim n H ( 2 n x ) 2 n , x 0 .

Therefore, (17) implies

A ( x + y ) = A ( x ) + A ( y ) , ( x , y ) D ( x , y ) R 2 : x > y 3 > 0 .

Since D is an open connected set in R 2 , by the extension theorem of Rimán [15] there is an additive function φ : R and a constant a R such that A ( x ) = φ ( x ) + a for all x > 0 . Putting m = 0 and letting n in (24), it follows

(25) φ ( x ) f ( x ) + a + 2 f ( 1 ) f ( 2 ) 18 ε , x 1 3 .

Let y > 0 and choose x > 0 such that min { x y , x + y , x y + x } > 1 3 . By (25), we have

φ ( x y ) f ( x y ) + a + 2 f ( 1 ) f ( 2 ) 18 ε , φ ( x + y ) f ( x + y ) + a + 2 f ( 1 ) f ( 2 ) 18 ε , f ( x y + x ) φ ( x y + x ) a 2 f ( 1 ) + f ( 2 ) 18 ε .

Adding these inequalities and (15), we obtain

φ ( x y ) + φ ( x + y ) φ ( x y + x ) f ( y ) + a + 2 f ( 1 ) f ( 2 ) 55 ε .

Since φ is additive, we infer

φ ( y ) f ( y ) + a + 2 f ( 1 ) f ( 2 ) 55 ε .

This completes the proof.□

Theorem 3.2

Let ε 0 and f , g , h , k : [ 0 , + ) be functions satisfying

(26) f ( x y ) + g ( x + y ) h ( x y + x ) k ( y ) ε , x , y 0 .

Then there is an affine function φ : R such that

(27) φ ( x ) g ( x ) 330 ε , x > 0 ;

(28) φ ( x ) h ( x ) + f ( 0 ) k ( 0 ) 331 ε , x > 0 ;

(29) φ ( x ) k ( x ) + f ( 0 ) h ( 0 ) 331 ε , x > 0 ;

(30) φ ( x ) f ( x ) + 2 f ( 0 ) h ( 0 ) k ( 0 ) 333 ε , x > 0 .

Proof

Letting x = 0 and y = 0 separately in (26), we obtain

(31) f ( 0 ) + g ( x ) h ( x ) k ( 0 ) ε , x 0 ,

(32) f ( 0 ) + g ( y ) h ( 0 ) k ( y ) ε , y 0 .

It follows from (31) that

(33) f ( 0 ) + g ( x y + x ) h ( x y + x ) k ( 0 ) ε , x , y 0 .

By (26), (32), and (33), one obtains

(34) f ( x y ) + g ( x + y ) g ( x y + x ) g ( y ) 2 f ( 0 ) + h ( 0 ) + k ( 0 ) 3 ε , x , y 0 .

Setting x = 1 in (34), we have

(35) f ( y ) g ( y ) 2 f ( 0 ) + h ( 0 ) + k ( 0 ) 3 ε , y 0 .

Then

(36) g ( x y ) f ( x y ) + 2 f ( 0 ) h ( 0 ) k ( 0 ) 3 ε , x , y 0 .

Adding (34) and (36), we obtain

g ( x y ) + g ( x + y ) g ( x y + x ) g ( y ) 6 ε , x , y 0 .

By Theorem 3.1, there is an affine function φ : R such that

φ ( x ) g ( x ) 330 ε , x > 0 .

This inequality with (31), (32), and (35) yield (28), (29), and (30).□

Corollary 3.3

Let ε 0 and f , g , h , k : [ 0 , + ) be functions satisfying

f ( x y ) + g ( x + y ) h ( x y + x ) k ( y ) = 0 , x , y 0 .

Then f , g , h , k are affine functions on ( 0 , + ) . Moreover,

h ( x ) = g ( x ) + f ( 0 ) k ( 0 ) , k ( x ) = g ( x ) + f ( 0 ) h ( 0 ) , f ( x ) = g ( x ) + f ( 0 ) g ( 0 ) , x > 0 .

4 Conclusions

The functional equation f ( x y ) + f ( x + y ) = f ( x y + x ) + f ( y ) is known as the Davison functional equation. We treated the Hyers-Ulam stability of the Davison functional equation in two cases. The first is for functions defined on a normed unitary algebra with values in a Banach space and the functional inequality associated with Davison equation is valid only on a restricted unbounded domain. The second one is for the case of functions defined on interval [ 0 , + ) with values in a Banach space. In the second case, we considered also a generalization form of Davison functional equation. Finally, as an application of the obtained results, the asymptotic behavior of Davison functions has been investigated. Investigation and solving Davison’s functional equation and its generalization in other certain restricted domains can be future research prospects.

Acknowledgments

The authors would like to thank the reviewers for their valuable suggestions and comments.

  1. Funding information: The authors state no funding involved.

  2. Author contributions: All authors have accepted responsibility for the entire content of this manuscript and approved its submission.

  3. Conflict of interest: The authors declare that they have no competing interests.

  4. Data availability statement: Not applicable.

References

[1] T. M. K. Davison, 191. Probem, Aequationes Math. 20 (1980), 306. 10.1007/BF02190522Search in Google Scholar

[2] W. Benz, 191R1. Remark, Aequationes Math. 20 (1980), 307. 10.1007/BF02190187Search in Google Scholar

[3] R. Girgensohn and K. Lajkó, A functional equation of Davison and its generalization, Aequationes Math. 60 (2000), no. 3, 219–224, DOI: https://doi.org/10.1007/s000100050148. 10.1007/s000100050148Search in Google Scholar

[4] T. M. K. Davison, A Hosszú-like functional equation, Publ. Math. Debrecen 58 (2001), 505–513, DOI: https://doi.org/10.5486/PMD.2001.2326. 10.5486/PMD.2001.2326Search in Google Scholar

[5] S. M. Ulam, Problems in Modern Mathematics (Science Editions), John Wiley & Sons, New York, 1964. Search in Google Scholar

[6] D. H. Hyers, On the stability of the linear functional equation, Proc. Natl. Acad. Sci. USA 27 (1941), 222–224, DOI: https://doi.org/10.1073/pnas.27.4.222. 10.1073/pnas.27.4.222Search in Google Scholar PubMed PubMed Central

[7] D. H. Hyers, G. Isac, and Th. M. Rassias, Stability of Functional Equations in Several Variables, Birkhäuser, Basel, 1998. 10.1007/978-1-4612-1790-9Search in Google Scholar

[8] S.-M. Jung, Hyers–Ulam–Rassias Stability of Functional Equations in Nonlinear Analysis, Springer, New York, Dordrecht, Heidelberg, London, 2011. 10.1007/978-1-4419-9637-4Search in Google Scholar

[9] Pl. Kannappan, Functional Equations and Inequalities with Applications, Springer, New York, 2009. 10.1007/978-0-387-89492-8Search in Google Scholar

[10] S.-M. Jung and P. K. Sahoo, Hyers-Ulam-Rassias stability of an equation of Davison, J. Math. Anal. Appl. 238 (1999), no. 1, 297–304, DOI: https://doi.org/10.1006/jmaa.1999.6545. 10.1006/jmaa.1999.6545Search in Google Scholar

[11] S.-M. Jung and P. K. Sahoo, On the Hyers-Ulam stability of a functional equation of Davison, Kyungpook Math. J. 40 (2000), no. 1, 87–92. Search in Google Scholar

[12] K.-W. Jun, S.-M. Jung, and Y.-H. Lee, A generalization of the Hyers-Ulam-Rassias stability of a functional equation of Davison, J. Korean Math. Soc. 41 (2004), no. 3, 501–511, DOI: https://doi.org/10.4134/JKMS.2004.41.3.501. 10.4134/JKMS.2004.41.3.501Search in Google Scholar

[13] S.-M. Jung and P. K. Sahoo, Hyers-Ulam-Rassias stability of a functional equation of Davison in rings, Nonlinear Funct. Anal. Appl. 11 (2006), no. 5, 891–896. Search in Google Scholar

[14] Y.-H. Kim, On the Hyers-Ulam-Rassias stability of an equation of Davison, Indian J. Pure Appl. Math. 33 (2002), 713–726. Search in Google Scholar

[15] J. Rimán, On an extension of Pexider’s equation, Zb. Rad. (Beogr.) 1 (1976), no. 9, 65–72. Search in Google Scholar

Received: 2022-08-05
Revised: 2023-10-28
Accepted: 2024-06-07
Published Online: 2024-09-26

© 2024 the author(s), published by De Gruyter

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  54. Embeddings of anisotropic Sobolev spaces into spaces of anisotropic Hölder-continuous functions
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  63. A note on 1-semi-greedy bases in p-Banach spaces with 0 < p ≤ 1
  64. Fixed point results for generalized convex orbital Lipschitz operators
  65. Asymptotic model for the propagation of surface waves on a rotating magnetoelastic half-space
  66. Multiplicity of k-convex solutions for a singular k-Hessian system
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  75. Quantitative estimates for perturbed sampling Kantorovich operators in Orlicz spaces
  76. Review Articles
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  78. Differential sandwich theorems for p-valent analytic functions associated with a generalization of the integral operator
  79. Special Issue on Development of Fuzzy Sets and Their Extensions - Part II
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  99. On the generalized Mellin integral operators
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  101. Approximation process of a positive linear operator of hypergeometric type
  102. On Kantorovich variant of Brass-Stancu operators
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  104. Special Issue on Some Integral Inequalities, Integral Equations, and Applications - Part I
  105. On parameterized inequalities for fractional multiplicative integrals
  106. On inverse source term for heat equation with memory term
  107. On Fejér-type inequalities for generalized trigonometrically and hyperbolic k-convex functions
  108. New extensions related to Fejér-type inequalities for GA-convex functions
  109. Derivation of Hermite-Hadamard-Jensen-Mercer conticrete inequalities for Atangana-Baleanu fractional integrals by means of majorization
  110. Some Hardy's inequalities on conformable fractional calculus
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  115. Generalized Yosida inclusion problem involving multi-valued operator with XOR operation
  116. Periodic and fixed points for mappings in extended b-gauge spaces equipped with a graph
  117. Convergence of Peaceman-Rachford splitting method with Bregman distance for three-block nonconvex nonseparable optimization
  118. Topological structure of the solution sets to neutral evolution inclusions driven by measures
  119. (α, F)-Geraghty-type generalized F-contractions on non-Archimedean fuzzy metric-unlike spaces
  120. Solvability of infinite system of integral equations of Hammerstein type in three variables in tempering sequence spaces c 0 β and 1 β
  121. Special Issue on Nonlinear Evolution Equations and Their Applications - Part I
  122. Fuzzy fractional delay integro-differential equation with the generalized Atangana-Baleanu fractional derivative
  123. Klein-Gordon potential in characteristic coordinates
  124. Asymptotic analysis of Leray solution for the incompressible NSE with damping
  125. Special Issue on Blow-up Phenomena in Nonlinear Equations of Mathematical Physics - Part I
  126. Long time decay of incompressible convective Brinkman-Forchheimer in L2(ℝ3)
  127. Numerical solution of general order Emden-Fowler-type Pantograph delay differential equations
  128. Global smooth solution to the n-dimensional liquid crystal equations with fractional dissipation
  129. Spectral properties for a system of Dirac equations with nonlinear dependence on the spectral parameter
  130. A memory-type thermoelastic laminated beam with structural damping and microtemperature effects: Well-posedness and general decay
  131. The asymptotic behavior for the Navier-Stokes-Voigt-Brinkman-Forchheimer equations with memory and Tresca friction in a thin domain
  132. Absence of global solutions to wave equations with structural damping and nonlinear memory
  133. Special Issue on Differential Equations and Numerical Analysis - Part I
  134. Vanishing viscosity limit for a one-dimensional viscous conservation law in the presence of two noninteracting shocks
  135. Limiting dynamics for stochastic complex Ginzburg-Landau systems with time-varying delays on unbounded thin domains
  136. A comparison of two nonconforming finite element methods for linear three-field poroelasticity
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