Difference between revisions of "CORE Overview"
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| − | COmpact detectoR for the Electron ion collider (CORE) | + | ==COmpact detectoR for the Electron ion collider (CORE)== |
| − | + | [[File:CORE_Logo.png|right|logo: CORE_Logo.png, pdf]] <br /> | |
| − | + | General principles: | |
| + | *A detector built within and around a compact solenoid can enable the full EIC physics program | ||
**Compact size reduces cost and enables investments in key technologies for critical subsystems | **Compact size reduces cost and enables investments in key technologies for critical subsystems | ||
| − | **Compact longitudinal size allows option of moving Final Focus Quadrupoles closer to the Interaction Point (IP) | + | ***Compact longitudinal size allows option of moving Final Focus Quadrupoles closer to the Interaction Point (IP) |
*** Enables higher luminosity and higher far-forward angular acceptance | *** Enables higher luminosity and higher far-forward angular acceptance | ||
| − | **High performance Particle ID is enabled by the past decade of EIC Generic Detector R&D | + | *An all-Si digital tracker based on Monolithic Active Pixel Sensors (MAPS) technology fulfills the tracking requirements |
| − | ** | + | *High performance Particle ID is enabled by the past decade of EIC Generic Detector R&D |
| + | ** DIRC with focussing optics for hadron PID in `Barrel' region | ||
| + | ** Dual RICH (aerogel + heavy gas) for hadron PID in `ion-Endcap' region | ||
| + | ** LGAD TOF in electron Endcap | ||
| + | *High Performance EMCal | ||
| + | ** High resolution PbWO4 for –3.5 < η < 0 | ||
| + | ** W-Shashlik for 0 ≤ η < 3.5 | ||
| + | *Hadronic Calorimetry adapted to EIC kinematics/multiplicity | ||
| + | ** High granularity total absorption HCal in forward (ion) direction | ||
| + | ** Modest granularity (BELLE-II style) muon and K-Long ID in remainder of solenoid flux return | ||
Latest revision as of 17:30, 27 January 2022
COmpact detectoR for the Electron ion collider (CORE)
General principles:
- A detector built within and around a compact solenoid can enable the full EIC physics program
- Compact size reduces cost and enables investments in key technologies for critical subsystems
- Compact longitudinal size allows option of moving Final Focus Quadrupoles closer to the Interaction Point (IP)
- Enables higher luminosity and higher far-forward angular acceptance
- Compact size reduces cost and enables investments in key technologies for critical subsystems
- An all-Si digital tracker based on Monolithic Active Pixel Sensors (MAPS) technology fulfills the tracking requirements
- High performance Particle ID is enabled by the past decade of EIC Generic Detector R&D
- DIRC with focussing optics for hadron PID in `Barrel' region
- Dual RICH (aerogel + heavy gas) for hadron PID in `ion-Endcap' region
- LGAD TOF in electron Endcap
- High Performance EMCal
- High resolution PbWO4 for –3.5 < η < 0
- W-Shashlik for 0 ≤ η < 3.5
- Hadronic Calorimetry adapted to EIC kinematics/multiplicity
- High granularity total absorption HCal in forward (ion) direction
- Modest granularity (BELLE-II style) muon and K-Long ID in remainder of solenoid flux return
