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A Study of Dark Matter Models at $\sqrt{s}$ = 13 TeV pp Collisions for Mono-Lepton Searches
A significance study considering new physical findings in proton proton collisions with leptons and missing transverse energy (E6T ) in the final state is performed for a center of mass energy of 13 TeV. The discovery of Dark Matter (DM) is one of the main tasks of the LHC analysis for 13 TeV and 14 Te...
Autor principal: | |
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Lenguaje: | eng |
Publicado: |
2017
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Materias: | |
Acceso en línea: | http://cds.cern.ch/record/2285518 |
Sumario: | A significance study considering new physical findings in proton proton collisions with leptons
and missing transverse energy (E6T ) in the final state is performed for a center of mass energy
of 13 TeV.
The discovery of Dark Matter (DM) is one of the main tasks of the LHC analysis for 13 TeV
and 14 TeV data. As well as other discoveries like large extra dimensions and quantum black
holes DM has a signature which shows a large imbalance in transverse energy. An analysis of the
DM production in CMS at generator level is performed. This analysis uses a simplified model
where the DM particle is assumed to be a weakly interacting massive particle (WIMP) and is
directly produced by a mediator particle (med). This DM particle is assumed to be a Dirac
fermion.
The process is studied in different ways, in terms of cross sections (xsecs) and shape, concerning
different coupling structures and strengths for the mediator particle coupling to Standard Model
matter (in the following called matter) and DM. We will study three different mediator models.
These models distinguish in the structure, how the mediator particle couples. These models are
the axialvector (AV), scalar (S) and pseudoscalar (PS) model. Whithin these models, we will
vary the coupling strenght.
Former analyses assumed that the coupling strengths DM↔med and matter↔med are equal
in the DM generation process.
Such an analysis concerning different coupling structures and different coupling strengths
for DM↔med and matter↔med has never been done before. It shall extend the assumptions
about the coupling structure and strength in former papers, to ’fully map out the MSDM1
landscape’ [1]. Different mediator and DM masses are discussed in the background of this
simplified model as well.
To connect the generator level processes with the experiment, full simulations with respect to
the CMS system are done. Then the expected limits can be set into the parameter space of the
simplified model.
This paper shows that the different couplings scale the cross section in dependence of the
coupling strength but provide new analysis methods when concerning the difference in the shape
of the signals for different coupling structures. It shows, that the difference in cross section and
shape concerning different coupling structures are huge. We show that the AV model is the best
model to study processes with a heavy mediator particle and the PS is the best model to study
processes with relatively light mediators. |
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