CWRU PAT Coffee Agenda

Tuesdays 10:30 - 11:30 | Fridays 11:30 - 12:30

+1 Can the Baryon Asymmetry Arise From Initial Conditions?.

sxk1031 +1

+1 Diboson Excess from a New Strong Force.

kxp265 +1

+1 Dark Energy and Doubly Coupled Bigravity.

kxp265 +1

+1 Tracing dark energy with quasars.

jtd55 +1

+1 Doubly coupled matter fields in massive bigravity.

kxp265 +1

Showing votes from 2016-06-17 12:30 to 2016-06-21 11:30 | Next meeting is Tuesday Aug 5th, 10:30 am.

users

  • No papers in this section today!

astro-ph.CO

  • Generic instabilities of non-singular cosmologies in Horndeski theory: a no-go theorem.- [PDF] - [Article]

    Tsutomu Kobayashi
     

    The null energy condition can be violated stably in generalized Galileon theories, which gives rise to the possibilities of healthy non-singular cosmologies. However, it has been reported that in many cases cosmological solutions are plagued with instabilities or have some pathologies somewhere in the whole history of the universe. Recently, this was shown to be generically true in a certain subclass of the Horndeski theory. In this short paper, we extend this no-go argument to the full Horndeski theory, and show that non-singular models (with flat spatial sections) in general suffer either from gradient instabilities or some kind of pathology in the tensor sector. This implies that one must go beyond the Horndeski theory to implement healthy non-singular cosmologies.

  • Doubly coupled matter fields in massive bigravity.- [PDF] - [Article]

    Xian Gao, Lavinia Heisenberg
     

    In the context of massive (bi-)gravity non-minimal matter couplings have been proposed. These couplings are special in the sense that they are free of the Boulware-Deser ghost below the strong coupling scale and can be used consistently as an effective field theory. Furthermore, they enrich the phenomenology of massive gravity. We consider these couplings in the framework of bimetric gravity and study the cosmological implications for background and linear tensor, vector, and scalar perturbations. Previous works have investigated special branch of solutions. Here we perform a complete perturbation analysis for the general background equations of motion completing previous analysis.

astro-ph.HE

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astro-ph.GA

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astro-ph.IM

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gr-qc

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hep-ph

  • Diboson Excess from a New Strong Force.- [PDF] - [Article]

    Howard Georgi, Yuichiro Nakai
     

    We explore a "partial unification" model that could explain the diphoton event excess around $750 \, \rm GeV$ recently reported by the LHC experiments. A new strong gauge group is combined with the ordinary color and hypercharge gauge groups. The VEV responsible for the combination is of the order of the $SU(2)\times U(1)$ breaking scale, but the coupling of the new physics to standard model particles is suppressed by the strong interaction of the new gauge group. This simple extension of the standard model has a rich phenomenology, including composite particles of the new confining gauge interaction, a coloron and a $Z'$ which are rather weakly coupled to standard model particles, and massive vector bosons charged under both the ordinary color and hypercharge gauge groups and the new strong gauge group. The new scalar glueball could have mass of around $750 \, \rm GeV$, be produced by gluon fusion and decay into two photons, both through loops of the new massive vector bosons. The simplest version of the model has some issues: the massive vector bosons are stable and the coloron and the $Z'$ are strongly constrained by search data. An extension of the model to include additional fermions with the new gauge coupling, though not as simple and elegant, can address both issues and more. It allows the massive vector boson to decay into a colorless, neutral state that could be a candidate of the dark matter. And the coloron and $Z'$ can decay dominantly into the new fermions, completely changing the search bounds. In addition, $SU(N)$ fermions below the symmetry breaking scale make it more plausible that the lightest glueball is at $750$~GeV. Whatever becomes of the $750$~GeV diphoton excess, the model is an unusual example of how new physics at small scales could be hidden by strong interactions.

hep-th

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hep-ex

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quant-ph

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other

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