Micromegas detectors

E25675

gaseous particle detector micro-pattern gaseous detector tracking detector

Micromegas detectors are high-granularity gaseous particle detectors that provide precise tracking and fast timing for high-energy physics experiments.

Try in SPARQL Jump to: Surface forms Disambiguation Statements Elicitation Referenced by

All labels observed (7)

Label	Occurrences
MICRO-MEsh GAseous Structure (Micromegas) concept	1
Micromegas detector community	1
Micromegas detectors canonical	1
Micromegas particle detectors	1
bulk Micromegas	1
microbulk Micromegas	1
resistive Micromegas	1

How this entity was disambiguated

This entity first appeared as the object of triple T192702 — resolving that mention is where its identity was fixed. The disambiguator weighed these candidate entities and picked the highlighted one (or “None”, minting a new entity). This is how homonymy is resolved: the same surface form can point to different entities.

NED1 Entity disambiguation (via context triple) gpt-5-mini-2025-08-07

Target entity: Micromegas detectors
Context triple: [COMPASS, uses, Micromegas detectors]

A. Time Projection Chamber
The Time Projection Chamber is a large gaseous detector used in particle physics experiments to track and identify charged particles in three dimensions with high precision.
B. Muon Spectrometer
The Muon Spectrometer is a specialized ALICE detector subsystem designed to identify and measure muons produced in high-energy heavy-ion collisions at the Large Hadron Collider.
C. Electromagnetic Calorimeter
The Electromagnetic Calorimeter is a high-precision detector subsystem used in particle physics experiments to measure the energy and position of electrons and photons produced in high-energy collisions.
D. Zero Degree Calorimeters
Zero Degree Calorimeters are specialized forward detectors used in high-energy nuclear physics experiments to measure neutral particles emitted close to the beam direction, aiding in event characterization and centrality determination.
E. RICH detector
The RICH detector is a ring-imaging Cherenkov device used in the NA62 experiment at CERN to identify charged particles by measuring the Cherenkov light they emit.
F. None of above. chosen
G. Unsure - the case is ambiguous/there is not enough information to decide.

NED2 Entity disambiguation (via description) gpt-5-mini-2025-08-07

Target entity: Micromegas detectors
Target entity description: Micromegas detectors are high-granularity gaseous particle detectors that provide precise tracking and fast timing for high-energy physics experiments.

A. Time Projection Chamber
The Time Projection Chamber is a large gaseous detector used in particle physics experiments to track and identify charged particles in three dimensions with high precision.
B. Muon Spectrometer
The Muon Spectrometer is a specialized ALICE detector subsystem designed to identify and measure muons produced in high-energy heavy-ion collisions at the Large Hadron Collider.
C. Electromagnetic Calorimeter
The Electromagnetic Calorimeter is a high-precision detector subsystem used in particle physics experiments to measure the energy and position of electrons and photons produced in high-energy collisions.
D. Zero Degree Calorimeters
Zero Degree Calorimeters are specialized forward detectors used in high-energy nuclear physics experiments to measure neutral particles emitted close to the beam direction, aiding in event characterization and centrality determination.
E. RICH detector
The RICH detector is a ring-imaging Cherenkov device used in the NA62 experiment at CERN to identify charged particles by measuring the Cherenkov light they emit.
F. None of above. chosen

Statements (54)

Predicate	Object
instanceOf	gaseous particle detector ⓘ micro-pattern gaseous detector ⓘ tracking detector ⓘ
appliedIn	dark matter experiments ⓘ neutrino experiments ⓘ rare event searches ⓘ time projection chambers ⓘ
canBe	bulk Micromegas ⓘ linked to: Micromegas detectors microbulk Micromegas ⓘ linked to: Micromegas detectors resistive Micromegas ⓘ linked to: Micromegas detectors
detects	charged particles ⓘ minimum ionizing particles ⓘ
developedAt	CEA Saclay ⓘ linked to: Commissariat à l’énergie atomique
hasAdvantage	good radiation hardness ⓘ high rate capability ⓘ low ion backflow ⓘ low material budget ⓘ
hasAmplificationGapThickness	about 100 micrometers ⓘ
hasComponent	amplification gap ⓘ drift region ⓘ micromesh electrode ⓘ readout anode ⓘ
hasDriftGapThickness	few millimeters ⓘ
hasGranularity	high ⓘ
hasReadout	analog readout electronics ⓘ digital readout electronics ⓘ
hasSpatialResolution	of order 50–100 micrometers ⓘ
hasTimeResolution	of order few nanoseconds ⓘ
introducedBy	Ioannis Giomataris ⓘ
introducedIn	1996 ⓘ
operatesWith	strong electric field in amplification gap ⓘ uniform electric field in drift region ⓘ
operatingMode	proportional gas amplification ⓘ
provides	fast timing ⓘ precise tracking ⓘ
readoutSegmentation	two-dimensional possible ⓘ
readoutTechnology	segmented anode pads ⓘ segmented anode strips ⓘ
requires	gas mixture ⓘ high-voltage power supply ⓘ
resistiveTechnologyProvides	spark protection ⓘ
signalFormation	electron avalanche in amplification gap ⓘ
typicalGasMixture	argon-based mixture ⓘ neon-based mixture ⓘ
usedFor	X-ray detection ⓘ muon detection ⓘ neutron detection with converters ⓘ precision tracking in collider experiments ⓘ
usedIn	ATLAS New Small Wheel upgrade ⓘ ATLAS experiment at the LHC ⓘ linked to: ATLAS COMPASS experiment at CERN ⓘ linked to: COMPASS experiment T2K near detectors ⓘ linked to: T2K high-energy physics experiments ⓘ
usesMedium	gas ⓘ

How these facts were elicited