From 22475ebbfc748f05caf4c12102c46648db7822d9 Mon Sep 17 00:00:00 2001 From: Lucia Morganti <lucia.morganti@cnaf.infn.it> Date: Mon, 13 May 2019 09:32:27 +0200 Subject: [PATCH] Add new file for cupid --- contributions/cupid/main.tex | 60 ++++++++++++++++++++++++++++++++++++ 1 file changed, 60 insertions(+) create mode 100644 contributions/cupid/main.tex diff --git a/contributions/cupid/main.tex b/contributions/cupid/main.tex new file mode 100644 index 0000000..eaaf716 --- /dev/null +++ b/contributions/cupid/main.tex @@ -0,0 +1,60 @@ +\documentclass[a4paper]{jpconf} +\usepackage{graphicx} + +\bibliographystyle{iopart-num} +%\usepackage{citesort} + +\begin{document} +\title{CUPID-0 experiment} + +\author{CUPID-0 collaboration} + +%\address{} + +\ead{stefano.pirro@lngs.infn.it} + +\begin{abstract} +With their excellent energy resolution, efficiency, and intrinsic radio-purity, cryogenic calorimeters are primed for the search of neutrino-less double beta decay (0$\nu$DBD). +CUPID-0 is an array of 24 Zn$^{82}$Se scintillating bolometers used to search for 0$\nu$DBD of $^{82}$Se. +It is the first large mass 0$\nu$DBD experiment exploiting a double read-out technique: the heat signal to accurately measure particle energies and the light signal to identify the particle type. +The CUPID-0 is in data taking since March 2017 and obtained several outstanding scientific results. +The configuration of the CUPID-0 data processing environment on the CNAF computing cluster has been used for the analysis of the first period of data taking. +\end{abstract} + +\section{The experiment} +Neutrino-less Double Beta Decay (0$\nu$DBD) is a hypothesized nuclear transition in which a nucleus decays emitting only two electrons. +This process can not be accommodated in the Standard Model, as the absence of emitted neutrinos would violate the lepton number conservation. +Among the several experimental approaches proposed for the search of 0$\nu$DBD, cryogenic calorimeters (bolometers) stand out for the possibility of achieving excellent energy resolution ($\sim$0.1\%), efficiency ($\ge$80\%) and intrinsic radio-purity. Moreover, the crystals that are operated as bolometers can be grown starting from most of the 0$\nu$DBD emitters, enabling the test of different nuclei. +The state of the art of the bolometric technique is represented by CUORE, an experiment composed of 988 bolometers for a total mass of 741 kg, presently in data taking at Laboratori Nazionali del Gran Sasso. +The ultimate limit of the CUORE background suppression resides in the presence of $\alpha$-decaying isotopes located in the detector structure. +The CUPID-0 project \cite{Azzolini:2018dyb,Azzolini:2018tum} was born to overcome the actual limits. +The main breakthrough of CUPID-0 is the addition of independent devices to measure the light signals emitted from scintillation in ZnSe bolometers. + The different properties of the light emission of electrons and $\alpha$ particles will enable event-by-event rejection of $\alpha$ interactions, suppressing the overall background in the region of interest for 0$\nu$DBD of at least one order of magnitude. +The detector is composed by 26 ZnSe ultra-pure $\sim$ 500g bolometers, enriched at 95\% in $^{82}$Se, the 0$\nu$DBD emitter, and faced to Ge disks light detector operated as bolometers. +CUPID-0 is hosted in a dilution refrigerator at the Laboratori Nazionali del Gran Sasso and started the data taking in March 2017. +The first scientific run (i.e.,~ Phase I) ended in December 2018, collecting 9.95 kg$\times$y of ZnSe exposure. +Such data were used to calculate a new limits on the $^{82}$Se 0$\nu$DBD~\cite{Azzolini:2018dyb,Azzolini:2018oph} and to develop a full background model of the experiment~\cite{Azzolini:2019nmi}. +Phase II will start in June 2019 with an improved detector configuration. + +\section{CUPID-0 computing model and the role of CNAF} +The CUPID-0 computing model is similar to the CUORE one, being the only difference in the sampling frequency and working point of the light detector bolometers. +The full data stream is saved in root files, and a derivative trigger is software generated with a channel dependent threshold. +%Raw data are saved in Root files and contain events in correspondence with energy releases occurred in the bolometers. +Each event contains the waveform of the triggering bolometer and those geometrically close to it, plus some ancillary information. +The non-event-based information is stored in a PostgreSQL database that is also accessed by the offline data analysis software. +The data taking is arranged in runs, each run lasting about two days. +Details of the CUPID-0 data acquisition and control system can be found in \cite{DiDomizio:2018ldc}. +Raw data are transferred from the DAQ computers (LNGS) to the permanent storage area (located at CNAF) at the end of each run. +A full copy of data is also preserved on tape. + +The data analysis flow consists of two steps; in the first level analysis, the event-based quantities are evaluated, while in the second level analysis the energy spectra are produced. +The analysis software is organized in sequences. +Each sequence consists of a collection of modules that scan the events in the Root files sequentially, evaluate some relevant quantities and store them back in the events. +The analysis flow consists of several key steps that can be summarized in pulse amplitude estimation, detector gain correction, energy calibration and search for events in coincidence among multiple bolometers. +The new tools developed for CUPID-0 to handle the light signals are introduced in \cite{Azzolini:2018yye,Beretta:2019bmm}. +The main instance of the database was located at CNAF and the full analysis framework was used to analyze data until November 2017. A web page for offline reconstruction monitoring was maintained. +%During 2017 a more intense usage of the CNAF resources is expected, both in terms of computing resourced and storage space. + +\section*{References} +\bibliography{cupid-biblio} +\end{document} -- GitLab