184 research outputs found
A general method for determining the masses of semi-invisibly decaying particles at hadron colliders
We present a general solution to the long standing problem of determining the
masses of pair-produced, semi-invisibly decaying particles at hadron colliders.
We define two new transverse kinematic variables, and
, which are suitable one-dimensional projections of the
contransverse mass . We derive analytical formulas for the boundaries
of the kinematically allowed regions in the
and parameter planes, and introduce suitable variables
and to measure the distance to those boundaries on
an event per event basis. We show that the masses can be reliably extracted
from the endpoint measurements of and (or
). We illustrate our method with dilepton
events at the LHC.Comment: thoroughly revised; all new figures; new results on pages 3 and 4;
new illustrative example; includes detector simulation. 4 pages, 6 figures,
uses revtex and axodra
Supersymmetric Higgs-portal and X-ray lines
We consider a Dirac singlet fermion as thermal dark matter for explaining the
X-ray line in the context of a supersymmetric Higgs-portal model or a
generalized Dirac NMSSM. The Dirac singlet fermion gets a mass splitting due to
their Yukawa couplings to two Higgs doublets and their superpartners,
Higgsinos, after electroweak symmetry breaking. We show that a correct relic
density can be obtained from thermal freeze-out, due to the co-annihilation
with Higgsinos for the same Yukawa couplings. We discuss the phenomenology of
the Higgsinos in this model such as displaced vertices at the LHC.Comment: 15 pages, 4 figures, references adde
The Hierarchy Solution to the LHC Inverse Problem
Supersymmetric (SUSY) models, even those described by relatively few
parameters, generically allow many possible SUSY particle (sparticle) mass
hierarchies. As the sparticle mass hierarchy determines, to a great extent, the
collider phenomenology of a model, the enumeration of these hierarchies is of
the utmost importance. We therefore provide a readily generalizable procedure
for determining the number of sparticle mass hierarchies in a given SUSY model.
As an application, we analyze the gravity-mediated SUSY breaking scenario with
various combinations of GUT-scale boundary conditions involving different
levels of universality among the gaugino and scalar masses. For each of the
eight considered models, we provide the complete list of forbidden hierarchies
in a compact form. Our main result is that the complete (typically rather
large) set of forbidden hierarchies among the eight sparticles considered in
this analysis can be fully specified by just a few forbidden relations
involving much smaller subsets of sparticles.Comment: 44 pages, 2 figures. Python code providing lists of allowed and
forbidden hierarchy is included in ancillary file
Gravity-mediated (or composite) dark matter
Dark matter could have an electroweak origin, yet it could communicate with the visible sector exclusively through gravitational interactions. In a setup addressing the hierarchy problem, we propose a new dark-matter scenario where gravitational mediators, arising from the compactification of extra dimensions, are responsible for dark-matter interactions and its relic abundance in the Universe. We write an explicit example of this mechanism in warped extra dimensions and work out its constraints. We also develop a dual picture of the model, based on a four-dimensional scenario with partial compositeness. We show that gravity-mediated dark matter is equivalent to a mechanism of generating viable dark matter scenarios in a strongly coupled, near-conformal theory, such as in composite Higgs models
Re-interpreting the Oxbridge stransverse mass variable MT2 in general cases
We extend the range of possible applications of MT2 type analyses to decay
chains with multiple invisible particles, as well as to asymmetric event
topologies with different parent and/or different children particles. We
advocate two possible approaches. In the first, we introduce suitably defined
3+1-dimensional analogues of the MT2 variable, which take into account all
relevant on-shell kinematic constraints in a given event topology. The second
approach utilizes the conventional MT2 variable, but its kinematic endpoint is
suitably reinterpreted on a case by case basis, depending on the specific event
topology at hand. We provide the general prescription for this
reinterpretation, including the formulas relating the measured MT2 endpoint (as
a function of the test masses of all the invisible particles) to the underlying
physical mass spectrum. We also provide analytical formulas for the shape of
the differential distribution of the doubly projected MT2(perp) variable for
the ten possible event topologies with one visible particle and up to two
invisible particles per decay chain. We illustrate our results with the example
of leptonic chargino decays, (chargino to lepton, neutrino and LSP) in
supersymmetry.Comment: 36 pages, 9 figures, Preprint typeset in JHEP styl
Beyond the Dark matter effective field theory and a simplified model approach at colliders
Direct detection of and LHC search for the singlet fermion dark matter (SFDM)
model with Higgs portal interaction are considered in a renormalizable model
where the full Standard Model (SM) gauge symmetry is imposed by introducing a
singlet scalar messenger. In this model, direct detection is described by an
effective operator m_q \bar{q} q \bar{\chi} \chi as usual, but the full
amplitude for monojet + \not E_T involves two intermediate scalar propagators,
which cannot be seen within the effective field theory (EFT) or in the
simplified model without the full SM gauge symmetry. We derive the collider
bounds from the ATLAS monojet + \not E_T as well as the CMS t\bar{t} + \not E_T
data, finding out that the bounds and the interpretation of the results are
completely different from those obtained within the EFT or simplified models.
It is pointed out that it is important to respect unitarity, renormalizability
and local gauge invariance of the SM.Comment: 7 pages, 3 figures, version published in Phys. Lett.
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