33 research outputs found
Higgs Boson Decays to Dark Photons through the Vectorized Lepton Portal
Vector-like fermions charged under both the Standard Model and a new dark
gauge group arise in many theories of new physics. If these fermions include an
electroweak doublet and singlet with equal dark charges, they can potentially
connect to the Higgs field through a Yukawa coupling in analogy to the standard
neutrino portal. With such a coupling, fermion loops generate exotic decays of
the Higgs boson to one or more dark vector bosons. In this work we study a
minimal realization of this scenario with an Abelian dark group. We investigate
the potential new Higgs decays modes, we compute their rates, and we study the
prospects for observing them at the Large Hadron Collider and beyond given the
other experimental constraints on the theory. We also discuss extensions of the
theory to non-Abelian dark groups.Comment: 32 pages, 5 figures, updated to match JHEP versio
Interpreting the Electron EDM Constraint
The ACME collaboration has recently announced a new constraint on the
electron EDM, , from measurements
of the ThO molecule. This is a powerful constraint on CP-violating new physics:
even new physics generating the EDM at two loops is constrained at the
multi-TeV scale. We interpret the bound in the context of different scenarios
for new physics: a general order-of-magnitude analysis for both the electron
EDM and the CP-odd electron-nucleon coupling; 1-loop SUSY, probing sleptons
above 10 TeV; 2-loop SUSY, probing multi-TeV charginos or stops; and finally,
new physics that generates the EDM via the charm quark or top quark Yukawa
couplings. In the last scenario, new physics generates a "QULE operator" , which in turn generates the EDM through RG evolution. If the QULE
operator is generated at tree level, this corresponds to a previously studied
leptoquark model. For the first time, we also classify scenarios in which the
QULE operator is generated at one loop through a box diagram, which include
SUSY and leptoquark models. The electron EDM bound is the leading constraint on
a wide variety of theories of CP-violating new physics interacting with the
Higgs boson or the top quark. We argue that any future nonzero measurement of
an electron EDM will provide a strong motivation for constructing new colliders
at the highest feasible energies.Comment: 23 pages plus appendices, 16 figure
Savior Curvatons and Large non-Gaussianity
Curvatons are light (compared to the Hubble scale during inflation) spectator
fields during inflation that potentially contribute to adiabatic curvature
perturbations post-inflation. They can alter CMB observables such as the
spectral index , the tensor-to-scalar ratio , and the local
non-Gaussianity . We systematically explore the
observable space of a curvaton with a quadratic potential. We find that when
the underlying inflation model does not satisfy the and observational
constraints but can be made viable with a significant contribution from what we
call a savior curvaton, a large is inevitable. On
the other hand, when the underlying inflation model already satisfies the
and observational constraints, so significant curvaton contribution is
forbidden, a large is possible in the exceptional
case when the isocurvature fluctuation in the curvaton fluid is much greater
than the global curvature fluctuation.Comment: 20 pages + appendices, 8 figure
The Quality/Cosmology Tension for a Post-Inflation QCD Axion
It is difficult to construct a post-inflation QCD axion model that solves the
axion quality problem (and hence the Strong CP problem) without introducing a
cosmological disaster. In a post-inflation axion model, the axion field value
is randomized during the Peccei-Quinn phase transition, and axion domain walls
form at the QCD phase transition. We emphasize that the gauge equivalence of
all minima of the axion potential (i.e., domain wall number one) is
insufficient to solve the cosmological domain wall problem. The axion string on
which a domain wall ends must exist as an individual object (as opposed to a
multi-string state), and it must be produced in the early universe. These
conditions are often not satisfied in concrete models. Post-inflation axion
models also face a potential problem from fractionally charged relics; solving
this problem often leads to low-energy Landau poles for Standard Model gauge
couplings, reintroducing the quality problem. We study several examples,
finding that models that solve the quality problem face cosmological problems,
and vice versa. This is not a no-go theorem; nonetheless, we argue that it is
much more difficult than generally appreciated to find a viable post-inflation
QCD axion model. Successful examples may have a nonstandard cosmological
history (e.g., multiple types of cosmic axion strings of different tensions),
undermining the widespread expectation that the post-inflation QCD axion
scenario predicts a unique mass for axion dark matter.Comment: 32 pages, 3 figure
Towards a muon collider
A muon collider would enable the big jump ahead in energy reach that is needed for a fruitful exploration of fundamental interactions. The challenges of producing muon collisions at high luminosity and 10 TeV centre of mass energy are being investigated by the recently-formed International Muon Collider Collaboration. This Review summarises the status and the recent advances on muon colliders design, physics and detector studies. The aim is to provide a global perspective of the field and to outline directions for future work
Towards a Muon Collider
A muon collider would enable the big jump ahead in energy reach that is
needed for a fruitful exploration of fundamental interactions. The challenges
of producing muon collisions at high luminosity and 10 TeV centre of mass
energy are being investigated by the recently-formed International Muon
Collider Collaboration. This Review summarises the status and the recent
advances on muon colliders design, physics and detector studies. The aim is to
provide a global perspective of the field and to outline directions for future
work.Comment: 118 pages, 103 figure
Erratum: Towards a muon collider
The original online version of this article was revised: The additional reference [139] has been added. Tao Han’s ORICD ID has been incorrectly assigned to Chengcheng Han and Chengcheng Han’s ORCID ID to Tao Han. Yang Ma’s ORCID ID has been incorrectly assigned to Lianliang Ma, and Lianliang Ma’s ORCID ID to Yang Ma. The original article has been corrected