11 research outputs found
Search for R-parity Violating Decays of Supersymmetric Particles in e+e- Collisions at LEP
A search, in e^+e^- collisions, for chargino, neutralino, scalar lepton and
scalar quark pair-production is performed, without assuming R-parity
conservation in decays, in the case that only one of the coupling constants
lambda_ijk or lambda''_ijk is non-negligible. No signal is found in data up to
a centre-of-mass energy of 208GeV. Limits on the production cross sections and
on the masses of supersymmetric particles are derived
How to find a Higgs boson with a mass between 155-180 GeV at the*LHC
Also numbered ETHZ-IPP PR-96-02; LHC - Large Hadron ColliderSIGLEAvailable from British Library Document Supply Centre-DSC:8053.4153(RAL--96-049) / BLDSC - British Library Document Supply CentreGBUnited Kingdo
How to find a Higgs boson with a mass between 155-180 GeV at the*LHC
Also numbered as ETHZ-IPP PR-96-02Available from British Library Document Supply Centre-DSC:8715.1804(CLRC-RAL-TR--96-049) / BLDSC - British Library Document Supply CentreSIGLEGBUnited Kingdo
How to find a Higgs boson with a mass between 155-GeV - 180-GeV at the LHC
We reconsider the signature of events with two charged leptons and missing
energy as a signal for the detection of the Standard Model Higgs boson in the
mass region M(Higgs)=155--180 GeV. It is shown that a few simple experimental
criteria allow to distinguish events originating from the Higgs boson decaying
to H --> W+W- from the non resonant production of W+W- X at the LHC. With this
set of cuts, signal to background ratios of about one to one are obtained,
allowing a 5--10 sigma detection with about 5~fb-1 of luminosity. This
corresponds to less than one year of running at the initial lower luminosity L=
10**33/ cm**2/sec. This is significantly better than for the hitherto
considered Higgs detection mode H --> Z Z* --> l+ l+ l- l-, where in this mass
range about 100~fb-1 of integrated luminosity are required for a 5 sigma
signal.Comment: latex, 12 pages 4 figure
From the LHC to future colliders
Discoveries at the LHC will soon set the physics agenda for future colliders. This report of a CERN Theory Institute includes the summaries of Working Groups that reviewed the physics goals and prospects of LHC running with 10 to 300 fb-1 of integrated luminosity, of the proposed sLHC luminosity upgrade, of the ILC, of CLIC, of the LHeC and of a muon collider. The four Working Groups considered possible scenarios for the first 10 fb-1 of data at the LHC in which (i) a state with properties that are compatible with a Higgs boson is discovered, (ii) no such state is discovered either because the Higgs properties are such that it is difficult to detect or because no Higgs boson exists, (iii) a missing-energy signal beyond the Standard Model is discovered as in some supersymmetric models, and (iv) some other exotic signature of new physics is discovered. In the contexts of these scenarios, the Working Groups reviewed the capabilities of the future colliders to study in more detail whatever new physics may be discovered by the LHC. Their reports provide the particle physics community with some tools for reviewing the scientific priorities for future colliders after the LHC produces its first harvest of new physics from multi-TeV collisions. © Springer-Verlag / Società Italiana di Fisica 2010
From the LHC to future colliders
Discoveries at the LHC will soon set the physics agenda for future colliders. This report of a CERN Theory Institute includes the summaries of Working Groups that reviewed the physics goals and prospects of LHC running with 10 to 300 fb(-1) of integrated luminosity, of the proposed sLHC luminosity upgrade, of the ILC, of CLIC, of the LHeC and of a muon collider. The four Working Groups considered possible scenarios for the first 10 fb(-1) of data at the LHC in which (i) a state with properties that are compatible with a Higgs boson is discovered, (ii) no such state is discovered either because the Higgs properties are such that it is difficult to detect or because no Higgs boson exists, (iii) a missing-energy signal beyond the Standard Model is discovered as in some supersymmetric models, and (iv) some other exotic signature of new physics is discovered. In the contexts of these scenarios, the Working Groups reviewed the capabilities of the future colliders to study in more detail whatever new physics may be discovered by the LHC. Their reports provide the particle physics community with some tools for reviewing the scientific priorities for future colliders after the LHC produces its first harvest of new physics from multi-TeV collisions
From the LHC to Future Colliders
Discoveries at the LHC will soon set the physics agenda for future colliders.
This report of a CERN Theory Institute includes the summaries of Working Groups
that reviewed the physics goals and prospects of LHC running with 10 to 300/fb
of integrated luminosity, of the proposed sLHC luminosity upgrade, of the ILC,
of CLIC, of the LHeC and of a muon collider. The four Working Groups considered
possible scenarios for the first 10/fb of data at the LHC in which (i) a state
with properties that are compatible with a Higgs boson is discovered, (ii) no
such state is discovered either because the Higgs properties are such that it
is difficult to detect or because no Higgs boson exists, (iii) a missing-energy
signal beyond the Standard Model is discovered as in some supersymmetric
models, and (iv) some other exotic signature of new physics is discovered. In
the contexts of these scenarios, the Working Groups reviewed the capabilities
of the future colliders to study in more detail whatever new physics may be
discovered by the LHC. Their reports provide the particle physics community
with some tools for reviewing the scientific priorities for future colliders
after the LHC produces its first harvest of new physics from multi-TeV
collisions.Comment: 98 pages, CERN Theory Institute Summary Repor
A search for pair production of new light bosons decaying into muons
A search for the pair production of new light bosons, each decaying into a pair of muons, is performed with the CMS experiment at the LHC, using a dataset corresponding to an integrated luminosity of 20.7 fb-1 collected in proton-proton collisions at center-of-mass energy of √s=8 TeV. No excess is observed in the data relative to standard model background expectation and a model independent upper limit on the product of the cross section, branching fraction, and acceptance is derived. The results are compared with two benchmark models, the first one in the context of the next-to-minimal supersymmetric standard model, and the second one in scenarios containing a hidden sector, including those predicting a nonnegligible light boson lifetime. © 2015 CERN for the benefit of the CMS Collaboration