Abstract
Recently, Jarad et al. in (Adv. Differ. Equ. 2017:247, 2017) defined a new class of nonlocal generalized fractional derivatives, called conformable fractional derivatives (CFDs), based on conformable derivatives. In this paper, sufficient conditions are established for the oscillation of solutions of generalized fractional differential equations of the form \t\t\t{Dα,ρax(t)+f1(t,x)=r(t)+f2(t,x),t>a,limt→a+aIj−α,ρx(t)=bj(j=1,2,…,m),\\documentclass[12pt]{minimal}\t\t\t\t\\usepackage{amsmath}\t\t\t\t\\usepackage{wasysym}\t\t\t\t\\usepackage{amsfonts}\t\t\t\t\\usepackage{amssymb}\t\t\t\t\\usepackage{amsbsy}\t\t\t\t\\usepackage{mathrsfs}\t\t\t\t\\usepackage{upgreek}\t\t\t\t\\setlength{\\oddsidemargin}{-69pt}\t\t\t\t\\begin{document}$$ \\textstyle\\begin{cases} {}_{a}\\mathfrak{D}^{\\alpha,\\rho}x(t)+f_{1}(t,x)=r(t)+f_{2}(t,x),\\quad t>a, \\\\ \\lim_{t \\to a^{+}}{ {}_{a}\\mathfrak{I}^{j-\\alpha,\\rho}x(t)}=b_{j} \\quad (j=1,2,\\ldots,m), \\end{cases} $$\\end{document} where m=lceilalpharceil, {}_{a}mathfrak{D}^{alpha,rho} is the left-fractional conformable derivative of order alphainmathbb{C}, operatorname{Re}(alpha)geq0 in the Riemann–Liouville setting and {}_{a}mathfrak {I}^{alpha,rho} is the left-fractional conformable integral operator. The results are also obtained for CFDs in the Caputo setting. Examples are provided to demonstrate the effectiveness of the main result.
Highlights
Fractional calculus is still being developed continuously and its operators are used to model complex systems where the kernel of the fractional operators reflects the nonlocality [2, 3]
The theory of fractional calculus with operators having nonsingular kernels depends on a limiting approach via dirac delta functions
The fractional derivative with the nonsingular kernel is first defined so that in the limiting case α → 0 we get the function itself and when α → 1 we get the usual derivative of the function
Summary
Fractional calculus is still being developed continuously and its operators are used to model complex systems where the kernel of the fractional operators reflects the nonlocality [2, 3]. The singularity of the kernel of the fractional operators has recently motivated researchers to present new types of fractional operators with nonsingular kernels and their discrete versions [4,5,6,7,8,9,10,11,12]. This new trend added another approach in defining fractional derivatives and integrals. The theory of fractional calculus with operators having nonsingular kernels depends on a limiting approach via dirac delta functions. The corresponding integral operators are evaluated by the help of Laplace transforms for functions whose convolu-
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