2005
DOI: 10.1140/epjc/s2005-02356-0
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Vector bosons in the expanding universe

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Cited by 28 publications
(26 citation statements)
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“…Various additional couplings, impossible to be explored in conventional Klein-Gordon and Proca equations, gave rise to a large area of physical applications such as describing the scattering of mesons by nuclei [5][6][7], the dynamics of bosons in curved space-time [8] and noninertial effect of rotating frames [9], thermodynamic properties of bosons in noncommutative plane [10], all works involving spin 0 systems. Vector bosons in the expanding universe [11] and in an Aharonov-Bohm potential [12] are examples of applications to spin 1 systems. The Bose-Einstein condensate [13,14], very special relativity [15], among others works, are applications for both spin systems.…”
Section: Introductionmentioning
confidence: 99%
“…Various additional couplings, impossible to be explored in conventional Klein-Gordon and Proca equations, gave rise to a large area of physical applications such as describing the scattering of mesons by nuclei [5][6][7], the dynamics of bosons in curved space-time [8] and noninertial effect of rotating frames [9], thermodynamic properties of bosons in noncommutative plane [10], all works involving spin 0 systems. Vector bosons in the expanding universe [11] and in an Aharonov-Bohm potential [12] are examples of applications to spin 1 systems. The Bose-Einstein condensate [13,14], very special relativity [15], among others works, are applications for both spin systems.…”
Section: Introductionmentioning
confidence: 99%
“…respectively [57,58]. To calculate the quantum gravity effect on the tunnelling probability of the massive vector boson from the black hole, we use the following ansatz for the modified wave function [41,57,58],…”
Section: Tunneling Of Massive Dirac Particle From Spinning Dilaton Blmentioning
confidence: 99%
“…We now concentrate on finding an upper limit on the photon (spin-1 particle) rest mass. To do so, we use the covariant form of the massive spin-1 particle equation in a curved spacetime which is given by (Sucu and Unal 2005):…”
Section: Introductionmentioning
confidence: 99%
“…where β µ (x) = [γ µ (x) ⊗ I + I ⊗ γ µ (x)]/2 represents the Kemmer matrices and Ψ γδ (x) is the 16 × 1 symmetric spinor (Sucu and Unal 2005). Also M = m 0 c/ is the inverse Compton wavelength of the spin-1 particle where its mass is m 0 and c is the speed of light in vacuum.…”
Section: Introductionmentioning
confidence: 99%