The dynamic range of LZ

Published 18 February 2016 © 2016 IOP Publishing Ltd and Sissa Medialab srl
, , Light Detection in Noble Elements (LIDINE 2015) Citation J. Yin 2016 JINST 11 C02054 DOI 10.1088/1748-0221/11/02/C02054

1748-0221/11/02/C02054

Abstract

The electronics of the LZ experiment, the 7-tonne dark matter detector to be installed at the Sanford Underground Research Facility (SURF), is designed to permit studies of physics where the energies deposited range from 1 keV of nuclear-recoil energy up to 3,000 keV of electron-recoil energy. The system is designed to provide a 70% efficiency for events that produce three photoelectrons in the photomultiplier tubes (PMTs). This corresponds approximately to the lowest energy threshold achievable in multi-tonne time-projection chambers, and drives the noise specifications for the front end. The upper limit of the LZ dynamic range is defined to accommodate the electroluminescence (S2) signals. The low-energy channels of the LZ amplifiers provide the dynamic range required for the tritium and krypton calibrations. The high-energy channels provide the dynamic range required to measure the activated Xe lines.

Export citation and abstract BibTeX RIS

10.1088/1748-0221/11/02/C02054