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On the solutions for generalised multiorder fractional partial differential equations arising in physics

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dc.contributor.author Purohit, Sunil Dutt
dc.contributor.author Baleanu, Dumitru
dc.contributor.author Jangid, Kamlesh
dc.date.accessioned 2022-11-30T08:40:11Z
dc.date.available 2022-11-30T08:40:11Z
dc.date.issued 2021
dc.identifier.citation Purohit, Sunil Dutt; Baleanu, Dumitru; Jangid, Kamlesh (2021). "On the solutions for generalised multiorder fractional partial differential equations arising in physics", Mathematical Methods in the Applied Sciences. tr_TR
dc.identifier.issn 0170-4214
dc.identifier.uri http://hdl.handle.net/20.500.12416/5884
dc.description.abstract In this article, we have studied solutions of a generalised multiorder fractional partial differential equations involving the Caputo time-fractional derivative and the Riemann–Liouville space fractional derivatives using Laplace–Fourier transform technique. Proposed generalised multiorder fractional partial differential equation is reducible to Schrödinger equation, wave equation and diffusion equation in a more general sense, and hence, solutions of these equations are specifically noted. Not only this, solutions of equation proposed in the stochastic resetting theory in the context of Brownian motion can also be found in a general regime. tr_TR
dc.language.iso eng tr_TR
dc.relation.isversionof 10.1002/mma.7431 tr_TR
dc.rights info:eu-repo/semantics/closedAccess tr_TR
dc.subject Brownian Motion tr_TR
dc.subject Diffusion Equation in Nonstatic Stochastic Resetting tr_TR
dc.subject Fractional Calculus tr_TR
dc.subject Fractional Diffusion Equation tr_TR
dc.subject Fractional Schrödinger Wave Equation tr_TR
dc.title On the solutions for generalised multiorder fractional partial differential equations arising in physics tr_TR
dc.type article tr_TR
dc.relation.journal Mathematical Methods in the Applied Sciences tr_TR
dc.contributor.authorID 56389 tr_TR
dc.contributor.department Çankaya Üniversitesi, Fen - Edebiyat Fakültesi, Matematik Bölümü tr_TR


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