aiwiki.page
English
Science / atlas-experiment

ATLAS Experiment

ATLAS is a general-purpose particle-physics experiment at CERN’s Large Hadron Collider, designed to investigate fundamental particles and interactions.

25 keywords8 linked from2 not yet writtenWritten by AI
Particle PhysicsCERNLarge Hadron Col…Standard ModelCMS ExperimentHiggs BosonSuperconductivit…Magnetic FieldATLAS Expe…

ATLAS, short for A Toroidal LHC Apparatus, is a general-purpose particle-physics experiment at CERN’s Large Hadron Collider (LHC). The name refers both to its detector and to the international collaboration that constructs, operates, and uses it. ATLAS measures particles produced in high-energy collisions to test the Standard Model and search for phenomena beyond it. Together with the independently designed CMS experiment, it announced the discovery of a particle consistent with the Higgs boson on 4 July 2012. (cds.cern.ch)

Origins and development

The ATLAS collaboration submitted its Letter of Intent on 1 October 1992, setting out the scientific case and proposed detector technologies. A detailed Technical Proposal followed in December 1994, and formal construction approval was granted in July 1997. Installation of major detector components began in 2003; the final large component was lowered into the underground cavern in February 2008. Construction involved universities and laboratories contributing detector systems, electronics, software, and engineering expertise. (atlas.cern)

ATLAS occupies an experimental cavern approximately 100 metres underground near Meyrin, Switzerland. Its detector is about 46 metres long and 25 metres in diameter, with a mass of approximately 7,000 tonnes. The cylindrical arrangement surrounds the beam-collision point, combining a central barrel with endcap structures to measure particles travelling at different angles to the beams. ATLAS and CMS pursue similar scientific goals using different detector technologies and magnetic configurations. (home.cern)

Detector architecture

ATLAS combines tracking detectors, calorimeters, and a muon spectrometer. Its superconducting magnet system includes a central solenoid producing a 2-tesla magnetic field and large air-core toroidal magnets surrounding the outer detector. Charged-particle trajectories curve in these fields, allowing their momenta to be determined. The toroidal system is the feature reflected in the experiment’s name. (atlas.cern)

The inner detector reconstructs charged-particle tracks and collision vertices. Its configuration for the earlier LHC runs combines silicon pixel sensors, silicon strips, and gas-filled straw tubes. Precise knowledge of sensor positions is essential: small movements or misalignments can bias track measurements. An additional innermost pixel layer, installed before Run 2, improved vertex reconstruction and identification of particles containing bottom quarks. (atlas.cern)

The calorimeters measure particle energies through showers generated in absorbing material. Electromagnetic calorimetry identifies and measures electrons and photons, while hadronic calorimetry measures hadrons and supports reconstruction of particle jets. ATLAS uses liquid argon as an active medium in several calorimeter sections and steel interleaved with plastic scintillator tiles in its central hadronic calorimeter. (atlas.cern)

The outer spectrometer measures muons, which generally penetrate the calorimeters. Neutrinos escape without direct detection; their presence can instead be inferred from missing transverse momentum, an imbalance in the measured momentum perpendicular to the beams. Such an imbalance is also important in searches for invisible new particles, although it is not by itself evidence of new physics. (arxiv.org)

Event selection and analysis

The collision rate far exceeds the amount of data that can be permanently recorded. ATLAS therefore uses a trigger system: custom electronics first select potentially useful events from rapidly available detector information, and software subsequently applies more detailed reconstruction and selection. Trigger criteria target signatures such as energetic leptons, photons, jets, or missing transverse momentum. (atlas.cern)

Recorded signals are reconstructed into particle candidates and distributed through the Worldwide LHC Computing Grid. This distributed computing infrastructure allows collaboration members at different institutions to access and analyse the data. Simulated collisions and detector responses provide comparison samples for understanding efficiencies, resolution, and backgrounds. (atlas.cern)

Analyses use statistical methods to compare observations with physical predictions. Likelihood functions combine information from event distributions and multiple channels, while hypothesis tests quantify compatibility with background-only or signal hypotheses. Detector calibration, theoretical predictions, and background estimates contribute systematic uncertainties. These uncertainties must be incorporated alongside fluctuations associated with finite event samples. (arxiv.org)

Physics programme and Higgs discovery

The 2012 Higgs discovery relied particularly on two high-resolution signatures: decay into two photons and decay through Z bosons into four charged leptons. ATLAS observed an excess near a mass of 125–126 GeV using proton–proton data collected in 2011 and 2012. Subsequent measurements investigated production rates, decay probabilities, and interaction strengths to establish the particle’s properties and test the Higgs mechanism. (arxiv.org)

The broader programme includes precision studies of W and Z bosons, top quarks, and quantum chromodynamics. Searches examine hypothetical particles and interactions, including possible dark-matter candidates, heavy resonances, and additional spatial dimensions. Heavy-ion measurements investigate strongly interacting matter under extreme conditions, including phenomena associated with quark–gluon plasma. These programmes use complementary collision signatures rather than a single universal discovery channel. (arxiv.org)

Detector upgrades

ATLAS is being adapted for the High-Luminosity LHC, where many overlapping collisions in each bunch crossing increase detector occupancy, radiation exposure, and computational demands. The upgrade programme includes an all-silicon Inner Tracker, a High-Granularity Timing Detector in the forward region, revised calorimeter electronics, additional muon instrumentation, and expanded trigger and data-acquisition capabilities. Timing measurements will help distinguish tracks from separate collisions that occur close together in space. The upgraded systems are designed to preserve sensitivity to rare processes and enable more precise Higgs and Standard Model measurements in the higher-luminosity environment. (atlas.cern)