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Theory and Modern Applications

Figure 4 | Advances in Difference Equations

Figure 4

From: Identifying the space source term problem for a generalization of the fractional diffusion equation with hyper-Bessel operator

Figure 4

The source functions \(\mathcal{F}_{1}^{\upepsilon}(\textrm{x},t) =\mathscr{F}_{\mathtt{m},\uptheta}^{1,\upepsilon}(\textrm{x}) \mathcal{Q}(t)\) and \(\mathcal{F}_{2}^{\upepsilon}(\textrm{x},t) =\mathscr {F}_{\mathtt{n},\uptheta}^{2,\upepsilon}(\textrm{x}) \mathcal{Q}(t)\) for \((\textrm{x}, t) \in(0,\pi) \times(0,1)\), \(\upepsilon= 0.001\), \(\upalpha=\upbeta =0.9\)

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