4 research outputs found
Derivation of the Kinetic Equation for the Density Matrix of Two-Level Particles by the Green’S Function Method
- Publication venue
- 'Pleiades Publishing Ltd'
- Publication date
- Field of study
Organosilicon Derivatives of Sulfur
- Author
- A Almenningen
- A Berger
- A Bygdén
- A Colson
- A Colson
- A Gauthier
- A Gauthier
- A Gauthier
- A Gauthier
- A Haas
- A Haas
- A Ladenburg
- A Ladenburg
- A Stock
- A Weiss
- A Weiss
- A Weiss
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- AA Bugorkova
- AA Bugorkova
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- AF Plate
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- AG Brook
- AG Brook
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- AG Macdiarmid
- AG Macdiarmid
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- AG Macdiarmid
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- AN Egorochkin
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/1971
- Field of study
The ATLAS experiment at the CERN Large Hadron Collider: a description of the detector configuration for Run 3
- Author
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- Abbott B
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- IOP Publishing
- Publication date
- 01/05/2024
- Field of study
Abstract
The ATLAS detector is installed in its experimental cavern
at Point 1 of the CERN Large Hadron Collider. During Run 2 of the
LHC, a luminosity of
ℒ = 2 × 1034 cm-2 s-1 was
routinely achieved at the start of fills, twice the design
luminosity. For Run 3, accelerator improvements, notably luminosity
levelling, allow sustained running at an instantaneous luminosity of
ℒ = 2 × 1034 cm-2 s-1,
with an average of up to 60 interactions per bunch crossing. The
ATLAS detector has been upgraded to recover Run 1 single-lepton
trigger thresholds while operating comfortably under Run 3 sustained
pileup conditions. A fourth pixel layer 3.3 cm from the beam axis
was added before Run 2 to improve vertex reconstruction and
b-tagging performance. New Liquid Argon Calorimeter digital
trigger electronics, with corresponding upgrades to the Trigger and
Data Acquisition system, take advantage of a factor of 10 finer
granularity to improve triggering on electrons, photons, taus, and
hadronic signatures through increased pileup rejection. The inner
muon endcap wheels were replaced by New Small Wheels with Micromegas
and small-strip Thin Gap Chamber detectors, providing both precision
tracking and Level-1 Muon trigger functionality. Trigger coverage of
the inner barrel muon layer near one endcap region was augmented
with modules integrating new thin-gap resistive plate chambers and
smaller-diameter drift-tube chambers. Tile Calorimeter scintillation
counters were added to improve electron energy resolution and
background rejection. Upgrades to Minimum Bias Trigger Scintillators
and Forward Detectors improve luminosity monitoring and enable total
proton-proton cross section, diffractive physics, and heavy ion
measurements. These upgrades are all compatible with operation in
the much harsher environment anticipated after the High-Luminosity
upgrade of the LHC and are the first steps towards preparing ATLAS
for the High-Luminosity upgrade of the LHC. This paper describes
the Run 3 configuration of the ATLAS detector.</jats:p
Recommended from our members
The ATLAS experiment at the CERN Large Hadron Collider: a description of the detector configuration for Run 3
- Author
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- Clawson SE
- Cleland W
- Clemens JC
- Clement C
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- Crespo-Lopez O
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- Curcio F
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- D'Amico V
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- D'Uffizi D
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- Di Ciaccio A
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- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Gregorio G
- Di Luca A
- Di Micco B
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- Di Petrillo KF
- Di Stante L
- Diaconu C
- Dias Do Vale T
- Dias FA
- Diaz Capriles FG
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- Dreyer E
- Drivas-koulouris I
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- Drozdova M
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- Durglishvili A
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- Eggleston MG
- Egidio Purcino De Souza E
- Ehrke LF
- Eigen G
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- Fiore G
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- Fleck I
- Fleischmann P
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- Flierl BM
- Flores Castillo LR
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- Formica A
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Journal of Instrumentation
- Publication date
- 23/05/2024
- Field of study
Abstract
The ATLAS detector is installed in its experimental cavern
at Point 1 of the CERN Large Hadron Collider. During Run 2 of the
LHC, a luminosity of
ℒ = 2 × 1034 cm-2 s-1 was
routinely achieved at the start of fills, twice the design
luminosity. For Run 3, accelerator improvements, notably luminosity
levelling, allow sustained running at an instantaneous luminosity of
ℒ = 2 × 1034 cm-2 s-1,
with an average of up to 60 interactions per bunch crossing. The
ATLAS detector has been upgraded to recover Run 1 single-lepton
trigger thresholds while operating comfortably under Run 3 sustained
pileup conditions. A fourth pixel layer 3.3 cm from the beam axis
was added before Run 2 to improve vertex reconstruction and
b-tagging performance. New Liquid Argon Calorimeter digital
trigger electronics, with corresponding upgrades to the Trigger and
Data Acquisition system, take advantage of a factor of 10 finer
granularity to improve triggering on electrons, photons, taus, and
hadronic signatures through increased pileup rejection. The inner
muon endcap wheels were replaced by New Small Wheels with Micromegas
and small-strip Thin Gap Chamber detectors, providing both precision
tracking and Level-1 Muon trigger functionality. Trigger coverage of
the inner barrel muon layer near one endcap region was augmented
with modules integrating new thin-gap resistive plate chambers and
smaller-diameter drift-tube chambers. Tile Calorimeter scintillation
counters were added to improve electron energy resolution and
background rejection. Upgrades to Minimum Bias Trigger Scintillators
and Forward Detectors improve luminosity monitoring and enable total
proton-proton cross section, diffractive physics, and heavy ion
measurements. These upgrades are all compatible with operation in
the much harsher environment anticipated after the High-Luminosity
upgrade of the LHC and are the first steps towards preparing ATLAS
for the High-Luminosity upgrade of the LHC. This paper describes
the Run 3 configuration of the ATLAS detector.</jats:p