Table 1 Numerical values of \(\int ^{ \grave{ \iota}}_{\grave{a}} \mathcal{G}_{1} (\grave{\iota}, \xi ) \,{\mathrm {d}}\xi \), \(\breve{M}_{2}\), γ, \(\int _{\grave{a}}^{\grave{\iota}} \mathcal{G}_{2}(\grave{\iota}, \xi ) \,{\mathrm {d}}\xi \), \(\int _{\grave{a}}^{\grave{\iota}} \mathcal{H}(\grave{a}, \xi ) \hslash (\xi ) \,{\mathrm {d}}\xi \), and \(\Delta =\upphi _{\bar{p}} ( \int _{\grave{a}}^{\grave{\iota}} \mathcal{H}(\grave{a}, \xi ) \hslash (\xi ) \,{\mathrm {d}}\xi )\) in Example 6.1 for \(\tau \in J\)

From: Existence of positive solutions for p-Laplacian boundary value problems of fractional differential equations