ZEUS
The ZEUS detector comprised many different detector components, including a depleted uranium plastic-scintillator calorimeter, a central tracking detector (which was a wire chamber), a silicon microvertex detector and muon chambers. In addition, a solenoid provided a 1.43 T magnetic field. The ZEUS detector measured 12 m × 11 m × 20 m and weighed 3600 tons.
Like its partner experiment H1, the ZEUS experiment studied the internal structure of the proton through measurements of deep inelastic scattering by colliding leptons (electrons or positrons) with protons in the interaction point of ZEUS. These measurements were also used to test and study the Standard Model of particle physics as well as to search for particles beyond the Standard Model, laying the foundation to much of the science done at the Large Hadron Collider (LHC) at the CERN particle physics laboratory today.
Background
The German national laboratory DESY was founded in 1959 and started operating its first particle accelerator in 1964. Since then, it has been a highly regarded center for particle physics, photon science, astroparticle physics, and the development, construction and operation of particle accelerators. The design effort for ZEUS can be traced back to 1982. A Letter of Intent was submitted in 1985. The ZEUS detector was operational with the first collisions of the HERA collider in 1992. The last electron–proton collisions at ZEUS were recorded on 30 June 2007. The other multi-purpose experiment at the HERA collider was the competing H1 experiment. Since May 2012, the former ZEUS detector hall has been used as a lab space for the international European XFEL project.
Detector
The main components of the ZEUS detector were the tracking components, the calorimeter and the muon detectors. The purpose of the ZEUS detector was to collect data to allow the reconstruction of physics events in a consistent way so they can be analyzed.
Calorimeter
The ZEUS Calorimeter was a uranium scintillator based sampling calorimeter and divided into three main sections: the BCAL (Barrel CALorimeter), FCAL (Forward CALorimeter), and RCAL (Rear CALorimeter). Each section was subdivided transversely into towers, and longitudinally into EMC (Electro-Magnetic Calorimeter) or HAC (HAdronic Calorimeter). The smallest subdivision in the calorimeter was called a cell. Each cell was read out by two photomultiplier tubes (PMTs), which helped ensure that there were no holes in the coverage if one of the two PMTs failed.
Uranium was chosen as an absorber so that the calorimeter would be compensating. Electrons and photons deposit energy differently from hadrons, but in a compensating calorimeter the response (e) for an electromagnetic cascade is equal to the response (h) for a hadronic cascade of the same energy (i.e. e/h = 1). In the ZEUS calorimeter neutral pions interacted with uranium atoms to produce slow-moving neutrons which were captured by the scintillator and increased the hadronic signal. Another advantage of using uranium as the absorber was that the natural radioactivity allowed the calorimeter's sensitivity to be conveniently monitored.
Notes
- ^ "Institutes taking part in the ZEUS Collaboration". The ZEUS Experiment.
- ^ "HERA pointing the way" (PDF). DESY. Retrieved 4 May 2023.
- ^ "Heuer, Rolf and Wagner, Alrecht: HERA leaves a rich legacy of knowledge". CERN Courier. Retrieved 4 May 2023.
- ^ Electron-Proton Interaction Experiment (PDF) (Technical report). FermiLab. May 1982.
- ^ ZEUS Collaboration: K. Edwards; Edwards, K.; Kapitza, H. (June 1985). ZEUS: A Detector for HERA, Letter of Intent (Report).
- ^ Harris, David (September 2007). "The End of the HERA Era". Symmetry Magazine. 04 (7). Retrieved 10 November 2011.
- ^ "Research at Hamburg's Deepest Scientific Workplace Resumes". European XFEL. Retrieved 15 July 2015.
- ^ "The ZEUS Detector: Status Report 1993". The ZEUS Experiment.
- ^ Bock, Rudolf K. (9 April 1998). "Compensating Calorimeter". Retrieved 10 November 2011.