Application of the DRS chip for fast waveform digitizing

By S. Ritt, R. Dinapoli, U. Hartmann. 2010

276 citations recorded by the source corpus.

Subfields: Biomedical Engineering, Electrical and Electronic Engineering

View Paper: https://www.semanticscholar.org/paper/ec1a72d96fa92ea520b25451dfc3f569f7bce451

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In Electrical and Electronic Engineering

1. G. Lanfranchi
2. Giovanni Signorelli
3. Mattias Marklund
4. Padma Kant Shukla

Citations in the corpus

• Search for the lepton flavour violating decay μ+→e+γ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mu ^+ \rightarrow (2016, unknown): “2.8 Front-end electronics The digitisation and data acquisition system for MEG uses a custom, high frequency digitiser based on the switched capacitor array technique, the Domino Ring Sampler 4 (DRS4) [22].”
• A facility to Search for Hidden Particles (SHiP) at the CERN SPS (2015, methodology): “The DRS4 (Domino Ring Sampler, 4-th generation) is a switched capacitor array capable of sampling 8 differential input channels at a sampling rate up to 5 GS/s [143].”
• The design of the MEG II experiment (2018, methodology): “The amplified and shaped waveforms are digitised at a sampling frequency of 2 GSPS by the DRS4 chips on the WDBs for a detailed offline analysis of the pulses in order to compute the precise signal times.”
• MEG Upgrade Proposal (2013, unknown): “The active target will be made from an array of 240 (0.25 × 0.25 mm2) multi-clad BCF12 (from SaintGobain) square fibres, with a peak emission at 435 nm, a light yield of about 8000 ph/MeV, a trapping efficiency of ≈ 7%, an attenuation length of 2.7 m and a decay time of 3.2 ns.”
• Any Light Particle Search II -- Technical Design Report (2013, methodology): “For the initial setup and tests an already available DRS-4 board of the ETH Zürich with 4 channels in self-triggering mode can be used [117] as well.”
• Design and operation of FACT - the first G-APD Cherenkov telescope (2013, methodology): “In this way, a precise relative timing between all channels of about 300 ps is possible [21] (depending on the sampling frequency), provided that the fixed-aperture jitter of the DRS 4 is calibrated.”