Abstract
We establish the existence, uniqueness, and positivity for the fractional Navier boundary value problem:
$$\begin{aligned} \textstyle\begin{cases} D^{\alpha }(D^{\beta }\omega )(t)=h(t,\omega (t),D^{\beta }\omega (t)), & 0< t< 1, \\ \omega (0)=\omega (1)=D^{\beta }\omega (0)=D^{\beta }\omega (1)=0, \end{cases}\displaystyle \end{aligned}$$
{
D
α
(
D
β
ω
)
(
t
)
=
h
(
t
,
ω
(
t
)
,
D
β
ω
(
t
)
)
,
0
<
t
<
1
,
ω
(
0
)
=
ω
(
1
)
=
D
β
ω
(
0
)
=
D
β
ω
(
1
)
=
0
,
where $\alpha,\beta \in (1,2]$
α
,
β
∈
(
1
,
2
]
, $D^{\alpha }$
D
α
and $D^{\beta }$
D
β
are the Riemann–Liouville fractional derivatives. The nonlinear real function h is supposed to be continuous on $[0,1]\times \mathbb{R\times R}$
[
0
,
1
]
×
R
×
R
and satisfy appropriate conditions. Our approach consists in reducing the problem to an operator equation and then applying known results. We provide an approximation of the solution. Our results extend those obtained in (Dang et al. in Numer. Algorithms 76(2):427–439, 2017) to the fractional setting.
Existence and Uniqueness Results for Perturbed Neumann Boundary Value Problems