LAUSR

AbstractRecently, 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 {Dα,ρax(t)+f1(t,x)=r(t)+f2(t,x),t>a,limt→a+aIj−α,ρx(t)=bj(j=1,2,…,m),$$ \textstyle\begin{cases} {}_{a}\mathfrak{D}^{\alpha,\rho}x(t)+f_{1}(t,x)=r(t)+f_{2}(t,x),\quad t>a, \\ \lim_{t \to a^{+}}{ {}_{a}\mathfrak{I}^{j-\alpha,\rho}x(t)}=b_{j} \quad (j=1,2,\ldots,m), \end{cases} $$ where m=⌈α⌉$m=\lceil\alpha\rceil$, Dα,ρa${}_{a}\mathfrak{D}^{\alpha,\rho}$ is the left-fractional conformable derivative of order α∈C$\alpha\in\mathbb{C}$, Re(α)≥0$\operatorname{Re}(\alpha)\geq0$ in the Riemann–Liouville setting and Iα,ρa${}_{a}\mathfrak {I}^{\alpha,\rho}$ 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.