Abstract
The field covered in this paper will be restricted to fixed-target reac- tions, the probe being real or virtual photons. Multi GeV will mean here photon energy below 10 GeV, because above the effect of the Lorentz boost will confirm all the particles in the forward direction and hadrons win develop hadronic showers in matter. This win imply a completely different design of a detector. Finaly multihadron win start at 2 particles. After some considerations on the physical motivation, I will discuss the main characteristics of the detectors, then I will give some examples of the detection set-up presently under development around electron accelerators and propose some concluding remarks.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a callDisclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.
