TY - JOUR
T1 - LGAD designs for Future Particle Trackers
AU - Cartiglia, N.
AU - Arcidiacono, R.
AU - Borghi, G.
AU - Boscardin, M.
AU - Costa, M.
AU - Galloway, Z.
AU - Fausti, F.
AU - Ferrero, M.
AU - Ficorella, F.
AU - Mandurrino, M.
AU - Mazza, S.
AU - Olave, E. J.
AU - Paternoster, G.
AU - Siviero, F.
AU - Sadrozinski, H. F.W.
AU - Sola, V.
AU - Staiano, A.
AU - Seiden, A.
AU - Tornago, M.
AU - Zhao, Y.
N1 - Publisher Copyright:
© 2020 The Author(s)
PY - 2020/11/1
Y1 - 2020/11/1
N2 - Several future high-energy physics facilities are currently being planned. The proposed projects include high energy e+e− circular and linear colliders, hadron colliders, and muon colliders, while the Electron–Ion Collider (EIC) is expected to construct at the Brookhaven National Laboratory in the future. Each proposal has its advantages and disadvantages in terms of readiness, cost, schedule, and physics reach, and each proposal requires the design and production of specific new detectors. This paper first presents the performances necessary for future silicon tracking systems at the various new facilities. Then it illustrates a few possibilities for the realization of such silicon trackers. The challenges posed by the future facilities require a new family of silicon detectors, where features such as impact ionization, radiation damage saturation, charge sharing, and analog read-out are exploited to meet these new demands.
AB - Several future high-energy physics facilities are currently being planned. The proposed projects include high energy e+e− circular and linear colliders, hadron colliders, and muon colliders, while the Electron–Ion Collider (EIC) is expected to construct at the Brookhaven National Laboratory in the future. Each proposal has its advantages and disadvantages in terms of readiness, cost, schedule, and physics reach, and each proposal requires the design and production of specific new detectors. This paper first presents the performances necessary for future silicon tracking systems at the various new facilities. Then it illustrates a few possibilities for the realization of such silicon trackers. The challenges posed by the future facilities require a new family of silicon detectors, where features such as impact ionization, radiation damage saturation, charge sharing, and analog read-out are exploited to meet these new demands.
KW - Charge multiplication
KW - Fast detector
KW - LGAD
KW - Low gain
KW - Silicon
UR - https://www.scopus.com/pages/publications/85088920520
U2 - 10.1016/j.nima.2020.164383
DO - 10.1016/j.nima.2020.164383
M3 - Article
SN - 0168-9002
VL - 979
JO - Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
JF - Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
M1 - 164383
ER -