[PDF] Top 20 FELIX: the new detector interface for the ATLAS experiment
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FELIX: the new detector interface for the ATLAS experiment
... The new electromagnetic calorimeter electronics, the NSW muon detectors, BIS78, and L1 calorimeter trigger electronics will require a new infrastructure for reading out data and sending control information ... See full document
6
Measurements of and production in collisions at with the ATLAS detector
... The production of Z bosons has been used in many experiments to test the electroweak sector of the Standard Model (SM). Precision measurements made at LEP and at the SLAC Linear Collider established Z boson properties ... See full document
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Standard Model measurements with the ATLAS detector
... Precise measurements of the production of vector bosons in association with jets are important tests of QCD and provide constraints on background processes to Higgs boson studies and to searches for new physics. ... See full document
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Run Control Software For The Upgrade Of The Atlas Muon To Central Trigger Processor Interface (MUCTPI)
... Processor Interface (MUCTPI) of the ATLAS experiment at the Large Hadron Collider (LHC) at CERN is being upgraded for the next run of the LHC in order to use optical inputs and to provide ... See full document
5
Felix Based Readout of The Single-Phase Protodune Detector
... the ATLAS collaboration and is based on custom FPGA-based PCIe I/O cards in combination with commodity ...servers. FELIX will be used in the single-phase ProtoDUNE setup to read the data coming from 2560 ... See full document
8
Study of the Efficiency and Resolution of the New sMDT Chambers at the ATLAS Experiment
... The ATLAS experiment is composed of three detectors: the inner detector, the calorime- ters, and the muon ...inner detector sits close to the beam axis out to a radius of ...pixel ... See full document
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Jets and their substructure at the ATLAS detector : new tools for new physics
... It was established in §3.2.2 that observing a bare quark is somewhat tricky. In fact, this is only the beginning of a physicist’s problems, as shall be shown in §4.1. Even in the weakly-bound UV regime, ambiguities in ... See full document
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Performance of the ATLAS Detector in Run-2
... a new era for high energy ...the ATLAS experiment, while the existence of dark matter and unnatural fine tuning in the Standard Model also motivate potential new physics near the electroweak ... See full document
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Development of radiation hard planar silicon tracking detectors for the ATLAS Experiment at the HL-LHC
... One of the biggest issues in the SM is the inability to include gravity, since General Relativity and Quantum Mechanics are difficult to include in a common framework. In todays particle physics experiments, the energy ... See full document
258
Searches for new physics with tau leptons at the ATLAS detector
... Leptoquarks (LQ) are colour-triplet bosons that carry both lepton and baryon numbers and have a fractional elec- tric charge. They are predicted by many extensions of the Standard Model (SM) [9–15] and may provide uni- ... See full document
5
The ATLAS Hadronic Physics Program and High Energy Cosmic Rays
... the ATLAS Forward Proton (AFP) project [13] is to enhance the diffractive physics programme of the ATLAS experiment by installing new detectors that will be able to tag forward protons ... See full document
7
Searches for monojets and monophotons with the ATLAS detector
... Events with an energetic jet or photon, and large miss- ing momentum in the final state are a distinctive signa- ture in searches for new physics at colliders. In particular, monojet and monophoton events have ... See full document
6
Search for top squark pair production in compressed-mass-spectrum scenarios in proton-proton collisions at root s=8 TeV using the alpha(T) variable
... CMS detector provided by the following funding agencies: BMWFW and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MES (Bulgaria); CERN; CAST Innovation Foundation, MoST, and NSFC ... See full document
28
Search for heavy resonances with the ATLAS detector
... various new physics scenarios considers final states with two isolated leptons ...full ATLAS detector simulation based on GEANT4, multi-jet processes are derived by a data-driven matrix ... See full document
10
Measurements of diboson production with the ATLAS detector
... of new resonances decaying into bosons or of other non-SM contributions and scenarios; furthermore, diboson final states are one of the irreducible SM backgrounds to the Higgs boson ... See full document
12
Searches for Dark Matter at the ATLAS experiment
... Interaction of particles mediating between Dark Matter and Standard Model particles can be de- scribed by contact operators in the framework of an e ff ective field theory (EFT) Refs. [10–12] in cases where they are too ... See full document
6
Search for a standard model Higgs Boson in the ZH -> vvbb channel with the ATLAS Detector
... ATLAS calorimetry systems are situated outside of the 2 T solenoid field surrounding the ID. There are two types of calorimeter in the ATLAS detector. The electromagnetic (EM) calorimeter measures ... See full document
154
Searches for New Physics with Lepton Flavours and Multi-lepton Final States in ATLAS
... The ATLAS result [3] is based on an analysis of collisions where an isolated electron and muon are reconstructed, with an invariant mass compat- ible with the Z -boson ... See full document
7
Dark Matter Searches with the ATLAS detector
... Searches for DM plus a detectable SM particle are referred to as ‘Mono-X’ searches, where ‘X’ is the SM particle being produced in conjunction with the DM particle(s). In Mono-X searches, the presence of DM is inferred ... See full document
11
A Search For Nothing: Dark Matter And Invisible Decays Of The Higgs Boson At The Atlas Detector
... to account for energy losses in the tracker and additional corrections are applied to calibrate the electron’s energy. The exact procedure is described fully in [79]. Due to the necessity of tracking information, ... See full document
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