Loading [MathJax]/jax/output/SVG/jax.js
Research article

New fixed point results in controlled metric type spaces based on new contractive conditions

  • Received: 06 December 2022 Revised: 23 January 2023 Accepted: 01 February 2023 Published: 15 February 2023
  • MSC : 37C25, 47H10, 54H25

  • In the present work, we will establish and prove some fixed point theorems for mappings that satisfy a set of conditions in controlled metric type spaces introduced by Mlaiki et al. [N. Mlaiki, H. Aydi, N. Souayah, T. Abdeljawad, Controlled metric type spaces and the related contraction principle. Mathematics 2018, 6,194]. Our technique in constructing our new contraction conditions is to insert the control function θ(u,l) that appears on the right hand side of the triangular inequality of the definition of the controlled metric spaces in the right hand side of our proposed contraction conditions. Our results enrich the field of fixed point theory with novel findings that generalize many findings found in the literature. We provide an example to show the usefulness of our results. Also, we present an application to our results to show their significance.

    Citation: Wasfi Shatanawi, Taqi A. M. Shatnawi. New fixed point results in controlled metric type spaces based on new contractive conditions[J]. AIMS Mathematics, 2023, 8(4): 9314-9330. doi: 10.3934/math.2023468

    Related Papers:

    [1] Takao Komatsu, Ram Krishna Pandey . On hypergeometric Cauchy numbers of higher grade. AIMS Mathematics, 2021, 6(7): 6630-6646. doi: 10.3934/math.2021390
    [2] Takao Komatsu, Huilin Zhu . Hypergeometric Euler numbers. AIMS Mathematics, 2020, 5(2): 1284-1303. doi: 10.3934/math.2020088
    [3] Nadia N. Li, Wenchang Chu . Explicit formulae for Bernoulli numbers. AIMS Mathematics, 2024, 9(10): 28170-28194. doi: 10.3934/math.20241366
    [4] Taekyun Kim, Hye Kyung Kim, Dae San Kim . Some identities on degenerate hyperbolic functions arising from p-adic integrals on Zp. AIMS Mathematics, 2023, 8(11): 25443-25453. doi: 10.3934/math.20231298
    [5] Jizhen Yang, Yunpeng Wang . Congruences involving generalized Catalan numbers and Bernoulli numbers. AIMS Mathematics, 2023, 8(10): 24331-24344. doi: 10.3934/math.20231240
    [6] Taekyun Kim, Dae San Kim, Jin-Woo Park . Degenerate r-truncated Stirling numbers. AIMS Mathematics, 2023, 8(11): 25957-25965. doi: 10.3934/math.20231322
    [7] Dojin Kim, Patcharee Wongsason, Jongkyum Kwon . Type 2 degenerate modified poly-Bernoulli polynomials arising from the degenerate poly-exponential functions. AIMS Mathematics, 2022, 7(6): 9716-9730. doi: 10.3934/math.2022541
    [8] Aimin Xu . Some identities connecting Stirling numbers, central factorial numbers and higher-order Bernoulli polynomials. AIMS Mathematics, 2025, 10(2): 3197-3206. doi: 10.3934/math.2025148
    [9] Waseem A. Khan, Abdulghani Muhyi, Rifaqat Ali, Khaled Ahmad Hassan Alzobydi, Manoj Singh, Praveen Agarwal . A new family of degenerate poly-Bernoulli polynomials of the second kind with its certain related properties. AIMS Mathematics, 2021, 6(11): 12680-12697. doi: 10.3934/math.2021731
    [10] Xhevat Z. Krasniqi . Approximation of functions in a certain Banach space by some generalized singular integrals. AIMS Mathematics, 2024, 9(2): 3386-3398. doi: 10.3934/math.2024166
  • In the present work, we will establish and prove some fixed point theorems for mappings that satisfy a set of conditions in controlled metric type spaces introduced by Mlaiki et al. [N. Mlaiki, H. Aydi, N. Souayah, T. Abdeljawad, Controlled metric type spaces and the related contraction principle. Mathematics 2018, 6,194]. Our technique in constructing our new contraction conditions is to insert the control function θ(u,l) that appears on the right hand side of the triangular inequality of the definition of the controlled metric spaces in the right hand side of our proposed contraction conditions. Our results enrich the field of fixed point theory with novel findings that generalize many findings found in the literature. We provide an example to show the usefulness of our results. Also, we present an application to our results to show their significance.



    L. Carlitz ([1]) introduced analogues of Bernoulli numbers for the rational function (finite) field K=Fr(T), which are called Bernoulli-Carlitz numbers now. Bernoulli-Carlitz numbers have been studied since then (e.g., see [2,3,4,5,6]). According to the notations by Goss [7], Bernoulli-Carlitz numbers BCn are defined by

    xeC(x)=n=0BCnΠ(n)xn. (1.1)

    Here, eC(x) is the Carlitz exponential defined by

    eC(x)=i=0xriDi, (1.2)

    where Di=[i][i1]r[1]ri1 (i1) with D0=1, and [i]=TriT. The Carlitz factorial Π(i) is defined by

    Π(i)=mj=0Dcjj (1.3)

    for a non-negative integer i with r-ary expansion:

    i=mj=0cjrj(0cj<r). (1.4)

    As analogues of the classical Cauchy numbers cn, Cauchy-Carlitz numbers CCn ([8]) are introduced as

    xlogC(x)=n=0CCnΠ(n)xn. (1.5)

    Here, logC(x) is the Carlitz logarithm defined by

    logC(x)=i=0(1)ixriLi, (1.6)

    where Li=[i][i1][1] (i1) with L0=1.

    In [8], Bernoulli-Carlitz numbers and Cauchy-Carlitz numbers are expressed explicitly by using the Stirling-Carlitz numbers of the second kind and of the first kind, respectively. These properties are the extensions that Bernoulli numbers and Cauchy numbers are expressed explicitly by using the Stirling numbers of the second kind and of the first kind, respectively.

    On the other hand, for N1, hypergeometric Bernoulli numbers BN,n ([9,10,11,12]) are defined by the generating function

    11F1(1;N+1;x)=xN/N!exN1n=0xn/n!=n=0BN,nxnn!, (1.7)

    where

    1F1(a;b;z)=n=0(a)(n)(b)(n)znn!

    is the confluent hypergeometric function with (x)(n)=x(x+1)(x+n1) (n1) and (x)(0)=1. When N=1, Bn=B1,n are classical Bernoulli numbers defined by

    xex1=n=0Bnxnn!.

    In addition, hypergeometric Cauchy numbers cN,n (see [13]) are defined by

    12F1(1,N;N+1;x)=(1)N1xN/Nlog(1+t)N1n=1(1)n1xn/n=n=0cN,nxnn!, (1.8)

    where

    2F1(a,b;c;z)=n=0(a)(n)(b)(n)(c)(n)znn!

    is the Gauss hypergeometric function. When N=1, cn=c1,n are classical Cauchy numbers defined by

    xlog(1+x)=n=0cnxnn!.

    In [14], for N0, the truncated Bernoulli-Carlitz numbers BCN,n and the truncated Cauchy-Carlitz numbers CCN,n are defined by

    xrN/DNeC(x)N1i=0xri/Di=n=0BCN,nΠ(n)xn (1.9)

    and

    (1)NxrN/LNlogC(x)N1i=0(1)ixri/Li=n=0CCN,nΠ(n)xn, (1.10)

    respectively. When N=0, BCn=BC0,n and CCn=CC0,n are the original Bernoulli-Carlitz numbers and Cauchy-Carlitz numbers, respectively. These numbers BCN,n and CCN,n in (1.9) and (1.10) in function fields are analogues of hypergeometric Bernoulli numbers in (1.7) and hypergeometric Cauchy numbers in (1.8) in complex numbers, respectively. In [15], the truncated Euler polynomials are introduced and studied in complex numbers.

    It is known that any real number α can be expressed uniquely as the simple continued fraction expansion:

    α=a0+1a1+1a2+1a3+, (1.11)

    where a0 is an integer and a1,a2, are positive integers. Though the expression is not unique, there exist general continued fraction expansions for real or complex numbers, and in general, analytic functions f(x):

    f(x)=a0(x)+b1(x)a1(x)+b2(x)a2(x)+b3(x)a3(x)+, (1.12)

    where a0(x),a1(x), and b1(x),b2(x), are polynomials in x. In [16,17] several continued fraction expansions for non-exponential Bernoulli numbers are given. For example,

    n=1B2n(4x)n=x1+12+x12+13+x13+14+x. (1.13)

    More general continued fractions expansions for analytic functions are recorded, for example, in [18]. In this paper, we shall give expressions for truncated Bernoulli-Carlitz numbers and truncated Cauchy-Carlitz numbers.

    In [19], the hypergeometric Bernoulli numbers BN,n (N1, n1) can be expressed as

    BN,n=(1)nn!|N!(N+1)!10N!(N+2)!N!(N+1)!10N!(N+n1)!N!(N+n2)!N!(N+1)!1N!(N+n)!N!(N+n1)!N!(N+2)!N!(N+1)!|.

    When N=1, we have a determinant expression of Bernoulli numbers ([20,p.53]). In addition, relations between BN,n and BN1,n are shown in [19].

    In [21,22], the hypergeometric Cauchy numbers cN,n (N1, n1) can be expressed as

    cN,n=n!|NN+110NN+2NN+110NN+n1NN+n2NN+11NN+nNN+n1NN+2NN+1|.

    When N=1, we have a determinant expression of Cauchy numbers ([20,p.50]).

    Recently, in ([23]) the truncated Euler-Carlitz numbers ECN,n (N0), introduced as

    xq2N/D2NCoshC(x)N1i=0xq2i/D2i=n=0ECN,nΠ(n)xn,

    are shown to have some determinant expressions. When N=0, ECn=EC0,n are the Euler-Carlitz numbers, denoted by

    xCoshC(x)=n=0ECnΠ(n)xn,

    where

    CoshC(x)=i=0xq2iD2i

    is the Carlitz hyperbolic cosine. This reminds us that the hypergeometric Euler numbers EN,n ([24]), defined by

    t2N/(2N)!coshtN1n=0t2n/(2n)!=n=0EN,nxnn!,

    have a determinant expression [25,Theorem 2.3] for N0 and n1,

    EN,2n=(1)n(2n)!|(2N)!(2N+2)!10(2N)!(2N+4)!01(2N)!(2N+2n)!(2N)!(2N+4)!(2N)!(2N+2)!|.

    When N=0, we have a determinant expression of Euler numbers (cf. [20,p.52]). More general cases are studied in [26].

    In this paper, we also give similar determinant expressions of truncated Bernoulli-Carlitz numbers and truncated Cauchy-Carlitz numbers as natural extensions of those of hypergeometric numbers.

    Let the n-th convergent of the continued fraction expansion of (1.12) be

    Pn(x)Qn(x)=a0(x)+b1(x)a1(x)+b2(x)a2(x)++bn(x)an(x). (2.1)

    There exist the fundamental recurrence formulas:

    Pn(x)=an(x)Pn1(x)+bn(x)Pn2(x)(n1),Qn(x)=an(x)Qn1(x)+bn(x)Qn2(x)(n1), (2.2)

    with P1(x)=1, Q1(x)=0, P0(x)=a0(x) and Q0(x)=1.

    From the definition in (1.9), truncated Bernoulli-Carlitz numbers satisfy the relation

    (DNi=0xrN+irNDN+i)(n=0BCN,nΠ(n)xn)=1.

    Thus,

    Pm(x)=DN+mDN,Qm(x)=DN+mmi=0xrN+irNDN+i

    yield that

    Qm(x)n=0BCN,nΠ(n)xnPm(x)(m).

    Notice that the n-th convergent pn/qn of the simple continued fraction (1.11) of a real number α yields the approximation property

    |qnαpn|<1qn+1.

    Now,

    P0(x)Q0(x)=1=11,P1(x)Q1(x)=1xrN+1rNDN+1/DN+xrN+1rN

    and Pn(x) and Qn(x) (n2) satisfy the recurrence relations

    Pn(x)=(DN+nDN+n1+xrN+nrN+n1)Pn1(x)DN+n1DN+n2xrN+nrN+n1Pn2(x)Qn(x)=(DN+nDN+n1+xrN+nrN+n1)Qn1(x)DN+n1DN+n2xrN+nrN+n1Qn2(x)

    (They are proved by induction). Since by (2.2) for n2

    an(x)=DN+nDN+n1+xrN+nrN+n1andbn(x)=DN+n1DN+n2xrN+nrN+n1,

    we have the following continued fraction expansion.

    Theorem 1.

    n=0BCN,nΠ(n)xn=1xrN+1rNDN+1DN+xrN+1rNDN+1DNxrN+2rN+1DN+2DN+1+xrN+2rN+1DN+2DN+1xrN+3rN+2DN+3DN+2+xrN+3rN+2.

    Put N=0 in Theorem 1 to illustrate a simpler case. Then, we have a continued fraction expansion concerning the original Bernoulli-Carlitz numbers.

    Corollary 1.

    n=0BCnΠ(n)xn=1xr1D1+xr1D1xr2rD2D1+xr2rD2D1xr3r2D3D2+xr3r2.

    From the definition in (1.10), truncated Cauchy-Carlitz numbers satisfy the relation

    (LNi=0(1)ixrN+irNLN+i)(n=0CCN,nΠ(n)xn)=1.

    Thus,

    Pm(x)=LN+mLN,Qm(x)=LN+mmi=0(1)ixrN+irNLN+i

    yield that

    Qm(x)n=0CCN,nΠ(n)xnPm(x)(m).

    Now,

    P0(x)Q0(x)=1=11,P1(x)Q1(x)=1+xrN+1rNLN+1/LNxrN+1rN

    and Pn(x) and Qn(x) (n2) satisfy the recurrence relations

    Pn(x)=(LN+nLN+n1xrN+nrN+n1)Pn1(x)+LN+n1LN+n2xrN+nrN+n1Pn2(x)Qn(x)=(LN+nLN+n1xrN+nrN+n1)Qn1(x)+LN+n1LN+n2xrN+nrN+n1Qn2(x).

    Since by (2.2) for n2

    an(x)=LN+nLN+n1xrN+n+rN+n1andbn(x)=LN+n1LN+n2xrN+nrN+n1,

    we have the following continued fraction expansion.

    Theorem 2.

    n=0CCN,nΠ(n)xn=1+xrN+1rNLN+1LNxrN+1rN+LN+1LNxrN+2rN+1LN+2LN+1xrN+2rN+1+LN+2LN+1xrN+3rN+2LN+3LN+2xrN+3rN+2+.

    In [14], some expressions of truncated Cauchy-Carlitz numbers have been shown. One of them is for integers N0 and n1,

    CCN,n=Π(n)nk=1(LN)ki1,,ik1rN+i1++rN+ik=n+krN(1)i1++ikLN+i1LN+ik (3.1)

    [14,Theorem 2].

    Now, we give a determinant expression of truncated Cauchy-Carlitz numbers.

    Theorem 3. For integers N0 and n1,

    CCN,n=Π(n)|a110a2a10a11(1)nana2a1|,

    where

    al=(1)iLNδlLN+i(l1)

    with

    δl={1if l=rN+irN(i=0,1,);0otherwise. (3.2)

    We need the following Lemma in [27] in order to prove Theorem 3.

    Lemma 1. Let {αn}n0 be a sequence with α0=1, and R(j) be a function independent of n. Then

    αn=|R(1)10R(2)R(1)10R(n1)R(n2)R(1)1R(n)R(n1)R(2)R(1)|. (3.3)

    if and only if

    αn=nj=1(1)j1R(j)αnj(n1) (3.4)

    with α0=1.

    Proof of Theorem 3. By the definition (1.10) with (1.6), we have

    1=(i=0(1)iLNLN+i)xrN+irN(m=0CCmΠ(m)xm)=(l=0alxl)(m=0CCmΠ(m)xm)=n=0l=0alCCnlΠ(nl)xn.

    Thus, for n1, we get

    l=0alCCnlΠ(nl)=0.

    By Lemma 1, we have

    CCnΠ(n)=nl=1alCCnlΠ(nl)=nl=1(1)l1(1)lalCCnlΠ(nl)=|a110a2a10a11(1)nana2a1|.

    Examples. When n=rN+1rN,

    CCrN+1rNΠ(rN+1rN)=|0101(1)rN+1rNarN+1rN00|=(1)rN+1rN+1(1)rN+1rN(1)2N+1LNLN+1=LNLN+1.

    Let n=rN+2rN. For simplicity, put

    ˉa=(1)rN+1rN(1)2N+1LNLN+1,ˆa=(1)rN+2rN(1)2N+2LNLN+2.

    Then by expanding at the first column, we have

    CCrN+1rNΠ(rN+1rN)=|0100ˉa00ˆa00rN+2rN+1ˉa0100rN+1rN1|=(1)rN+1rN+1ˉa|11ˉarN+1rN101ˉa210rN+1rN1|+(1)rN+2rN+1ˆa|10ˉa0ˉa1|.

    The second term is equal to

    (1)rN+2rN+1(1)rN+2rNLNLN+2=LNLN+2.

    The first term is

    (1)rN+1rN+1ˉa|01ˉarN+22rN+1+rNˉa10rN+1rN1|=(1)2(rN+1rN+1)ˉa2|11ˉarN+1rN101ˉa210rN+1rN1|=(1)r(rN+1rN+1)ˉar|0101ˉa00|rN+1rN=(1)(r+1)(rN+1rN+1)ˉar+1=(1)(r+1)(rN+1rN+1)(1)(rN+1rN)(r+1)(1)r+1Lr+1NLr+1N+1=Lr+1NLr+1N+1.

    Therefore,

    CCrN+1rNΠ(rN+1rN)=Lr+1NLr+1N+1LNLN+2.

    From this procedure, it is also clear that CCN,n=0 if rN+1rNn, since all the elements of one column (or row) become zero.

    In [14], some expressions of truncated Bernoulli-Carlitz numbers have been shown. One of them is for integers N0 and n1,

    BCN,n=Π(n)nk=1(DN)ki1,,ik1rN+i1++rN+ik=n+krN1DN+i1DN+ik (4.1)

    [14,Theorem 1].

    Now, we give a determinant expression of truncated Bernoulli-Carlitz numbers.

    Theorem 4. For integers N0 and n1,

    BCN,n=Π(n)|d110d2d10d11(1)ndnd2d1|,

    where

    dl=DNδlDN+i(l1)

    with δl as in (3.2).

    Proof. The proof is similar to that of Theorem 3, using (1.9) and (1.2).

    Example. Let n=2(rN+1rN). For convenience, put

    ˉd=DNDN+1.

    Then, we have

    BCN,2(rN+1rN)Π(2(rN+1rN))=|010ˉdˉdrN+1rN+1100rN+1rN1|=(1)rN+1rN+1|11ˉdrN+1rN10ˉd110rN+1rN1|=(1)rN+1rN+1ˉd|011ˉd0|rN+1rN=(1)2(rN+1rN+1)ˉd2|11|=D2ND2N+1.

    It is also clear that BCN,n=0 if rN+1rNn.

    We shall use Trudi's formula to obtain different explicit expressions and inversion relations for the numbers CCN,n and BCN,n.

    Lemma 2. For a positive integer n, we have

    |a1a00a2a10an1a1a0anan1a2a1|=t1+2t2++ntn=n(t1++tnt1,,tn)(a0)nt1tnat11at22atnn,

    where (t1++tnt1,,tn)=(t1++tn)!t1!tn! are the multinomial coefficients.

    This relation is known as Trudi's formula [28,Vol.3,p.214], [29] and the case a0=1 of this formula is known as Brioschi's formula [30], [28,Vol.3,pp.208–209].

    In addition, there exists the following inversion formula (see, e.g. [27]), which is based upon the relation

    nk=0(1)nkαkD(nk)=0(n1).

    Lemma 3. If {αn}n0 is a sequence defined by α0=1 and

    αn=|D(1)10D(2)01D(n)D(2)D(1)|, then D(n)=|α110α201αnα2α1|.

    From Trudi's formula, it is possible to give the combinatorial expression

    αn=t1+2t2++ntn=n(t1++tnt1,,tn)(1)nt1tnD(1)t1D(2)t2D(n)tn.

    By applying these lemmata to Theorem 3 and Theorem 4, we obtain an explicit expression for the truncated Cauchy-Carlitz numbers and the truncated Bernoulli-Carlitz numbers.

    Theorem 5. For integers N0 and n1, we have

    CCN,n=Π(n)t1+2t2++ntn=n(t1++tnt1,,tn)(1)nt2t4t2n/2at11atnn,

    where an are given in Theorem 3.

    Theorem 6. For integers N0 and n1, we have

    BCN,n=Π(n)t1+2t2++ntn=n(t1++tnt1,,tn)(1)nt2t4t2n/2dt11dtnn,

    where dn are given in Theorem 4.

    By applying the inversion relation in Lemma 3 to Theorem 3 and Theorem 4, we have the following.

    Theorem 7. For integers N0 and n1, we have

    an=(1)n|CCN,1Π(1)10CCN,2Π(2)CCN,1Π(1)10CCN,n1Π(n1)CCN,n2Π(n2)CCN,1Π(1)1CCN,nΠ(n)CCN,n1Π(n1)CCN,2Π(2)CCN,1Π(1)|,

    where an is given in Theorem 3.

    Theorem 8. For integers N0 and n1, we have

    dn=(1)n|BCN,1Π(1)10BCN,2Π(2)BCN,1Π(1)10BCN,n1Π(n1)BCN,n2Π(n2)BCN,1Π(1)1BCN,nΠ(n)BCN,n1Π(n1)BCN,2Π(2)BCN,1Π(1)|,

    where dn is given in Theorem 4.

    We would like to thank the referees for their valuable comments.

    The authors declare no conflict of interest.



    [1] S. Banach, Sur les operations dans les ensembles abstraits et leur application aux equation int egrals, Fundam. Math., 3 (1922), 133–181. https://doi.org/10.4064/fm-3-1-133-181 doi: 10.4064/fm-3-1-133-181
    [2] I. A. Bakhtin, The contraction mapping principle in almost metric spaces, Funct. Anal., 30 (1989), 26–37.
    [3] S. Czerwik, Contraction mappings in b-metric spaces, Acta Math. Inform. Univ. Ostra., 1 (1993), 5–11.
    [4] H. Huang, G. Deng, S. Radevovic, Fixed point theorems in b-metric spaces with applications to differential equations, J. Fix. Point Theory A., 20 (2018), 1–24. https://doi.org/10.1007/s11784-018-0491-z doi: 10.1007/s11784-018-0491-z
    [5] J. R. Roshan, V. Parvaneh, S. Sedghi, N. Shobkolaei, W. Shatanawi, Common fixed points of almost generalized (ψ,φ)s-contractive mappings in ordered b-metric spaces, Fixed Point Theory A., 2013 (2013), 159. http://dx.doi.org/10.1186/1687-1812-2013-159 doi: 10.1186/1687-1812-2013-159
    [6] A. Mukheimer, N. Mlaiki, K. Abodayeh, W. Shatanawi, New theorems on extended b-metric spaces under new contractions, Nonlinear Anal.-Model., 24 (2019), 870–883. http://doi.org/10.15388/NA.2019.6.2 doi: 10.15388/NA.2019.6.2
    [7] W. Shatanawi, A. Pitea, R. Lazovic, Contraction conditions using comparison functions on b-metric spaces, Fixed Point Theory A., 2014 (2014), 135. https://doi.org/10.1186/1687-1812-2014-135 doi: 10.1186/1687-1812-2014-135
    [8] M. Younis, D. Singh, L. Shi, Revisiting graphical rectangular b-metric spaces, Asian-Eur. J. Math., 15 (2022), 2250072. https://doi.org/10.1142/S1793557122500723 doi: 10.1142/S1793557122500723
    [9] T. Abdeljawad, K. Abodayeh, N. Mlaiki, On fixed point generalizations to partial b-metric spaces, J. Comput. Anal. Appl., 19 (2015), 883–891.
    [10] W. Shatanawi, Z. Mustafa, N. Tahat, Some coincidence point theorems for nonlinear contraction in ordered metric spaces, Fixed Point Theory A., 2011 (2011), 68. https://doi.org/10.1186/1687-1812-2011-68 doi: 10.1186/1687-1812-2011-68
    [11] T. Rasham, S. Shabbir, P. Agarwal, S. Momani, On a pair of fuzzy dominated mappings on closed ball in the multiplicative metric space with applications, Fuzzy Set. Syst., 437 (2022), 81–96. https://doi.org/10.1016/j.fss.2021.09.002 doi: 10.1016/j.fss.2021.09.002
    [12] V. Gupta, A. Gondhi, Fixed points of weakly compatible maps on modified intuitionistic fuzzy soft metric spaces, Int. J. Syst. Assur. Eng. Mang., 13 (2022), 1232–1238. https://doi.org/10.1007/s13198-021-01423-1 doi: 10.1007/s13198-021-01423-1
    [13] V. Gupta, N. Mani, R. Sharma, A. K. Tripathi, Some fixed point results and their applications on integral type contractive condition in fuzzy metric spaces, Bol. Soc. Paran. Mat., 40 (2022), 1–9. https://doi.org/10.5269/bspm.51777 doi: 10.5269/bspm.51777
    [14] S. Chauhan, V. Gupta, Banach contraction theorem on fuzzy cone b-metric space, J. Appl. Res. Technol., 18 (2020), 154–160. https://doi.org/10.22201/icat.24486736e.2020.18.4.1188 doi: 10.22201/icat.24486736e.2020.18.4.1188
    [15] M. Gamal, T. Rasham, W. Cholamjiak, F. Shi, C. Park, New iterative scheme for fixed point results of weakly compatible maps in multiplicative GM-metric space via various contractions with application, AIMS Math., 7 (2022), 13681–13703. https://doi.org/10.3934/math.2022754 doi: 10.3934/math.2022754
    [16] T. Rasham, M. Nazam, H. Aydi, A. Shoaib, C. Park, J. R. Lee, Hybrid pair of multivalued mappings in modular-like metric spaces and applications, AIMS Math., 7 (2022), 10582–10595. https://doi.org/10.3934/math.2022590 doi: 10.3934/math.2022590
    [17] M. Younis, D. Singh, L. Chen, M. Metwal, A study on the solutions of notable engineering models, Math. Model. Anal., 27 (2022), 492–509. https://doi.org/10.3846/mma.2022.15276 doi: 10.3846/mma.2022.15276
    [18] T. Kamran, M. Samreen, Q. U. L. Ain, A generalization of b-metric space and some fixed point theorems, Mathematics, 5 (2017), 1–7. https://doi.org/10.3390/math5020019 doi: 10.3390/math5020019
    [19] N. Mlaiki, H. Aydi, N. Souayah, T. Abdeljawad, Controlled metric type spaces and the related contraction principle, Mathematics, 6 (2018), 1–7. https://doi.org/10.3390/math6100194 doi: 10.3390/math6100194
    [20] S. S. Aiadi, W. A. M. Othman, K. Wang, N. Mlaiki, Fixed point theorems in controlled J-metric spaces, AIMS Math., 8 (2023), 4753–4763. https://doi.org/10.3934/math.2023235 doi: 10.3934/math.2023235
    [21] H. Ahmad, M. Younis, M. E. Köksal, Double controlled partial metric type spaces and convergence results, J. Math., 2021 (2021), 1–11. https://doi.org/10.1155/2021/7008737 doi: 10.1155/2021/7008737
    [22] T. Rasham, A. Shoaib, S. Alshoraify, C. Park, J. R. Lee, Study of multivalued fixed point problems for generalized contractions in double controlled dislocated quasi metric type spaces, AIMS Math., 7 (2022), 1058–1073. https://doi.org/10.3934/math.2022063 doi: 10.3934/math.2022063
    [23] A. Z. Rezazgui, A. Tallafha, W. Shatanawi, Common fixed point results via Aθ-α-contractions with a pair and two pairs of self-mappings in the frame of an extended quasi b-metric space, AIMS Math., 8 (2023), 7225–7241. https://doi.org/10.3934/math.2023363 doi: 10.3934/math.2023363
  • Reader Comments
  • © 2023 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Metrics

Article views(1701) PDF downloads(122) Cited by(26)

Other Articles By Authors

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog