Bumned SoodchomshomTang, I.-M.Rassmidara HoonsawatMahidol University. International College.2015-08-202018-04-052015-08-202018-04-0520152010Physica C: Superconductivity and its Applications. Vol. 470, No. 7-8 (2010), 415-420https://repository.li.mahidol.ac.th/handle/20.500.14594/10494Coexistence of superconductivity and ferromagnetism in a gapped graphene-based system (FS) is theoretically investigated. The center-of-mass momentum, P, of a Cooper pair in FS is found to be Psimilarity2Eex/similarityvF1-(m/EFS)2, where m, Eex, EFS are the rest mass energy of the Dirac electron, exchange energy and the Fermi energy in the superconductor FS, respectively. It is unlike the nature in a conventional FFLO state where Psimilarity2Eex/similarityvF. This work studies the magneto effect on the transport property of a F/(FS) junction where F is a ferromagnetic gapless graphene. In this work, FS is achieved by depositing a conventional ferromagnetic s-wave superconductor on the top of gapped graphene sheet. The Zeeman splitting in FS induces spin-dependent Andreev resonance. The conductances effected by both spin-dependent specular Andreev reflections and spin-dependent Andreev resonances are investigated. The interplay between the spin-dependent specular Andreev reflection in the F region and the spin-dependent Andreev resonance in the FS region causes a very large tunneling magnetoresistance |TMR|?3000% for mEFS, possibly valuable in the graphene-based spintronic devices. This is because of the coexistence of the superconductivity and ferromagnetism in FS and the relativistic nature of electrons in graphene. Theory of large tunneling magnetoresistance in a gapped.... Available from: https://www.researchgate.net/publication/243242956_Theory_of_large_tunneling_magnetoresistance_in_a_gapped_graphene-based_ferromagnetic_superconductor_FFS_junction [accessed Apr 02 2018]..engMahidol UniversityFerromagnetic superconductorGapped grapheneMassive dirac electronSpintronicsSwitching effectTunneling magnetoresistanceArticleScienceDirect