Abstract

The 8-channel Multiple Use Silicon Photo-multiplier (SiPM) Integrated Circuit (MUSIC) Application specific integrated circuit (ASIC) for SiPM anode readout has been designed for applications where large photo-detection areas are required. MUSIC offers three main features: (1) Sum of the eight input channels using a differential output driver, (2) eight individual single ended (SE) analog outputs, and (3) eight individual SE binary outputs using a time over threshold technique. Each functionality, summation and individual readout includes a selectable dual-gain configuration. Moreover, the signal sum implements a dual-gain output providing a 15-bit dynamic range. The circuit contains a tunable pole zero cancellation of the SiPM recovery time constant to deal with most of the available SiPM devices in the market. Experimental tests show how MUSIC can linearly sum signals from different SiPMs and distinguish even a few photons. Additionally, it provides a single photon output pulse width at half maximum (FWHM) between 5–10 ns for the analog output and a single-photon time resolution (SPTR) around 118 ps sigma using a Hamamatsu SiPM S13360-3075CS for the binary output. Lastly, the summation mode has a power consumption of ≈200 mW, whereas the individual readout consumes ≈30 mW/ch.

Highlights

  • IntroductionThe detection of low intensity light radiation with large efficiency and robust detectors is highly in demand for several applications [1]

  • This paper presents an 8-channel Multiple Use Silicon Photo-multiplier (SiPM) Integrated Circuit (MUSIC) [53] Application specific integrated circuit (ASIC) for SiPM anode readout, which implements all the aforementioned functionalities, and is organized as follows

  • The multiplier (SiPM) Integrated Circuit (MUSIC) ASIC is designed for high speed sampling

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Summary

Introduction

The detection of low intensity light radiation with large efficiency and robust detectors is highly in demand for several applications [1]. A classical example of a Cherenkov detector is the Ring Imaging Cherenkov (RICH) used for particle identification [12,13]. Another example is ground-based Cherenkov telescopes that are employed for high-energy gammaray stereoscopic observations [14,15]. These telescopes focus the flashes of Cherenkov light with nanosecond duration onto fast photo-sensor arrays where the signal is readout [16]. Medical imaging, including technologies such as positron emission tomography (PET) [17,18] and gamma single photon emission computed tomography (SPECT), demand efficient photo-detectors [19,20]

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