2013
DOI: 10.1142/s0217732313501216
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Elko Spinor Model With Torsion and Cosmology

Abstract: We study cosmological consequences of the dark spinor model when torsion is included. Only some components of the torsion are allowed to be non-vanishing in homogeneous and isotropic cosmology, but there exist freedoms in the choice of these components which is consistent with the evolution equations. We exploit this and discuss several cases which can result in interesting cosmological consequences. Especially, we show that there exist exact cosmological solutions in which the Universe began its acceleration … Show more

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Cited by 17 publications
(23 citation statements)
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“…In order to use the Elko field as the matter content in the universe, we will work with its classical formulation, or in terms of average values of its quantum field in a classical background. Also, in a curved homogeneous and isotropic space-time we assume that the Elko field is filling all the space homogeneously [13][14][15][16][17][18][19][20][21][22][23][24][25][26][27][28][29][30][31][32], thus we can assume that it can be split into a time dependent part and a flat space-time dependent part, which carries all the spinor structure, namely, λ(x µ ) = φ(t)ξ(x), such that ξ stands here, for simplicity, for one of the four kinds of Elko discussed above, normalized as ¬ ξ ξ = ±1. A convenient choice for the bare spinor ξ and its dual ¬ ξ is:…”
Section: Elko Dynamics In Frwmentioning
confidence: 99%
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“…In order to use the Elko field as the matter content in the universe, we will work with its classical formulation, or in terms of average values of its quantum field in a classical background. Also, in a curved homogeneous and isotropic space-time we assume that the Elko field is filling all the space homogeneously [13][14][15][16][17][18][19][20][21][22][23][24][25][26][27][28][29][30][31][32], thus we can assume that it can be split into a time dependent part and a flat space-time dependent part, which carries all the spinor structure, namely, λ(x µ ) = φ(t)ξ(x), such that ξ stands here, for simplicity, for one of the four kinds of Elko discussed above, normalized as ¬ ξ ξ = ±1. A convenient choice for the bare spinor ξ and its dual ¬ ξ is:…”
Section: Elko Dynamics In Frwmentioning
confidence: 99%
“…Appendix A contain a brief derivation of the main equations. The action for the Elko field coupled to gravity in a homogeneous and isotropic metric has been already presented in the literature [16,17,20,[27][28][29][30][31][32], for both torsion free and torsion coupled equations. The Friedmann equations are given by:…”
Section: Elko Dynamics In Frwmentioning
confidence: 99%
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“…Such kind of potential follows naturally from the theory of mass dimension one fermions [7]. In a flat Friedmann-Robertson-Walker (FRW) metric ds 2 = dt 2 − a(t) 2 [dx 2 + dy 2 + dz 2 ], the two Friedmann equations and the dynamic field equation for the time component φ(t) of the Elko field 3 plus a ordinary 3 We will refer to φ(t) as Elko field from now on, but the com-matter i can be obtained [18,22]:…”
Section: Dynamic Equations For Elko Fieldmentioning
confidence: 99%
“…For the MDO fermionic field we have used just one of the four different fields represented by Λ, satisfying Λ = φ(t)λ, where λ represents the fermionic field in a Minkowski space-time which is normalized as ¬ λ λ = 1, and φ(t) carries its time evolution in a Friedmann-Lemaître-Robertson-Walker (FLRW) background [11][12][13][14][16][17][18][19][20][21][22][23].…”
Section: Dynamic Equations For the Mdo Fermionic Fieldmentioning
confidence: 99%