Bumned SoodchomshomI. Ming TangRassmidara HoonsawatCommission on Higher EducationMahidol University2018-09-242018-09-242010-04-01Physica C: Superconductivity and its Applications. Vol.470, No.7-8 (2010), 415-420092145342-s2.0-77950355538https://repository.li.mahidol.ac.th/handle/20.500.14594/29056Coexistence 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 P ∼ 2 Eex / fenced(ℏ vF sqrt(1 - (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 P ∼ 2 Eex / ℏ vF. 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 m → EFS, 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. © 2010.Mahidol UniversityEnergyEngineeringMaterials SciencePhysics and AstronomyArticleSCOPUS10.1016/j.physc.2010.03.001