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TeV Scale Leptogenesis, theta_13 And Doubly Charged Particles At LHC
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BA-05-05
TeV Scale Leptogenesis, θ13 And Doubly Charged Particles At
LHC
Shahida Dar, Qaisar Shafi, and Arunansu Sil
Bartol Research Institute, Department of Physics and Astronomy,
University of Delaware, Newark, DE 19716, USA
Abstract
We explore a realistic supersymmetric SU(2)L×SU(2)R×U(1)B?L model spontaneously broken
at around 1012 GeV. The presence of D and F -flat directions gives rise to TeV mass doubly charged
particles which can be found at the LHC. We implement TeV scale leptogenesis and employing
both type I and II seesaw, the three light neutrinos are partially degenerate with masses in the
0.02? 0.1 eV range. The effective mass parameter for neutrinoless double beta decay is 0.03? 0.05
eV. We also find the interesting relation tan 2θ13 ? sin 2θ12tan 2θ23
(
?m2
⊙
?m2atm
)
. 0.02.
1
It has been recognized for some time that spontaneously broken supersymmetric models
with D and F -flat directions can lead to interesting phenomenological and cosmological
consequences [1, 2, 3, 4, 5, 6, 7]. An intermediate symmetry breaking scale of order 108?1016
GeV is a characteristic feature of these models. Another important aspect is the appearance
of thermal inflation typically involving about 10 or so e-foldings [2, 4, 6, 7]. The entropy
generation associated with thermal inflation has been exploited to try to resolve the gravitino
[2] and moduli problem [8], and to suppress the primordial monopole number density to
acceptable levels [5]. The entropy production does have an important drawback though. It
will dilute , and in some cases completely wash away, any pre- existing baryon asymmetry.
This very depends on the magnitude of the intermediate scale MI [6].
In [9], with an intermediate scale of order 108 GeV, the observed baryon asymmetry
was explained via resonant leptogenesis [10]. The relatively low intermediate scale causes
a moderate amount of dilution of an initially large lepton asymmetry, such
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