SPD: Difference between revisions

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The goal of the studies at SPD is measurement of different spin observables in polarized p–p, d–d and p–d collisions sensitive to the polarized gluonic structure of the nucleon..
The goal of the studies at SPD is measurement of different spin observables in polarized p–p, d–d and p–d collisions sensitive to the polarized gluonic structure of the nucleon..
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[http://spd.jinr.ru/ '''Official web page''']


[http://spd.jinr.ru/wp-content/uploads/2023/03/TechnicalDesignReport_SPD2023.pdf '''T'''echnical '''D'''esign '''R'''eport]  Version 1.00 (February 12, 2023)
* [http://spd.jinr.ru/ '''Official web page''']
 
* [http://spd.jinr.ru/wp-content/uploads/2023/03/TechnicalDesignReport_SPD2023.pdf '''T'''echnical '''D'''esign '''R'''eport]  Version 1.00 (February 12, 2023)
[[SPD componets ID convention|'''Components ID conventions''']]
* [[SPD componets ID convention|'''Components ID conventions''']]


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Revision as of 10:19, 11 December 2023

SPD NICA logo.png

The Spin Physics Detector (SPD) is one of the two large experimental facility at the NICA collider. The collaboration includes 300 scientists from 23 institutes from 10 countries and individual contributors.

The goal of the studies at SPD is measurement of different spin observables in polarized p–p, d–d and p–d collisions sensitive to the polarized gluonic structure of the nucleon..



Subdetectors

Range (muon) System

Magnetic system

Electromagnetic Calorimeter

Time-of-Flight system

Aerogel counters

Straw Tracker

Beam-Beam Counter

Silicon Vertex Detector

Micromegas-based Central Tracker

Zero Degree Calorimeter

Beam pipe and BBC MCP detector


Detector Control System

Data Acquisition System

Computing and offline software

Online data filter

Offline software

Databases