The project CUPID ¹⁾ is an upgrade of the CUORE experiment, aiming at searching for neutrinoless double beta (0νββ) decay with Li₂MoO₄ scintillating crystals enriched in ¹⁰⁰Mo. The crystals are operated as cryogenic detectors in the zero-background condition for its entire life cycle, which provides the fastest increase of sensitivity over the data collection time. The zero background condition is achievable via the particle discrimination in the scintillation channel.

Neutrinos have been postulated almost a century ago, and over 60 years have passed since their discovery. Over the past decades, neutrinos of different origins have been measured, including solar, atmospheric, reactor and supernova neutrinos, providing an impressive amount of information on their sources, as well as on the Standard Model of particle physics. Nevertheless, the experimental evidence of non-zero neutrino masses provided by the oscillation experiments unambiguously indicates the existence of new physics beyond the Standard Model. In parallel, several open questions tantalize the physics community since decades:

• What are the fundamental symmetries of the Standard Model, and their corresponding conserved quantities?
• What is the origin of the asymmetry between the amount of Matter and that of Anti-Matter in the Universe?
• Why is the mass of neutrinos much smaller than that of the other leptons?

A possible answer to these questions can be provided by 0νββ decay.

0νββ decay is a process in which a nucleus (A,Z) decays to (A,Z+2) with the simultaneous emission of two electrons, without any counterbalancing emission of antiparticles. Since the introduction of the Fermi theory of β decay, this would be the first example of a process that does not conserve the difference between the number of particles and antiparticles. In the framework of the Standard Model, 0νββ decay is a process that violates the lepton number L, and, more fundamentally, the difference between the baryon and lepton number B-L. Hence, the observation of 0νββ decay would simultaneously prove that the conservation of B-L is only approximate and that the Standard Model is thus just an approximate version of a broader theory, and provide an unequivocal evidence for the existence of matter creating processes. 0νββ is only possible if neutrinos have a Majorana mass component: in this framework, the mass of the three known (light) left-handed neutrinos could be generated by some heavy right-handed partner via the so-called see-saw mechanism, which naturally accounts for the smallness of neutrino masses in comparison to the Higgs-generated masses of all other known particles.

0νββ decay is a 3 body decay, with the available energy shared between the daughter nucleus and the two emitted electrons. Given its much larger mass, the daughter nucleus is subject to a negligible recoil. Moreover, for most detector technologies the two emitted electrons are not distinguishable, so only their sum energy is measurable. The experimental signature of 0νββ decay is thus an excess at the Q-value of the reaction, corresponding to the mass difference between the parent and daughter atom.

On the other hand, 2νββ decay is a 5 body decay, with again a negligible nuclear recoil. In this case, the two antineutrinos escape undetected, so only a fraction of the Q-value is shared between the electrons. The signature in this case is therefore a continuum from zero to the Q-value.

Decay scheme of 2νββ (top) and 0νββ decay (bottom). The two processes share the same parent and daughter nucleus, but differ for the number of emitted partiles, and consequently their energy.	The measurable sum electron spectrum is a continuum for 2νββ decay, and an excess at Qββ for 0νββ decay.

The first experimental attempts to detect 0νββ decay are date back to the 1940s. Over the decades, many different technologies have been developed to search for this process on a variety of candidate isotopes. Presently, CUORE²⁾ is one of the most sensitive experiments in the field. It is located at the Laboratori Nazionali del Gran Sasso (LNGS) of INFN, in the Abruzzo region in central Italy. CUORE is composed of 988 TeO₂ crystals operated as cryogenic calorimeters at a temperature of 10-15 mK. The crystals act simultaneously as detectors and source of 0νββ decay: in fact, they contain the ββ decay isotope ¹³⁰Te, that contributes to ~27% of the crystal mass.

The Gran Sasso National Park, below which the underground lab of LNGS is located.	The CUORE detectors right after their installation in the cryostat.

The detectors are operated in the largest dilution refrigerator ever build³⁾.

The future of the CUORE experiment is the CUPID project, whose goal is to measure the 0υ2β decay in the ¹⁰⁰Mo isotope instead of ¹³⁰Te used in CUORE using 1500 Li₂ MoO₄ crystals . The main reason for the change in the target material is due to the scintillating properties of the Li₂ MoO₄ which are necessary for the particle identification.

The CUPID crystal will be placed inside the CUORE cryostat arranged as in the sketch shown below.

The CUPID crystals are operated as cryogenic calorimeters, each equipped with a cryogenic light detector. A particle interaction in the crystal produces a phonon and light signal (see figure below), the latter one is used to discriminate α background from the electrons events.