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Cryogenic detectors

Silicon arrays for dark matter and neutrinos

A silicon wafer carved into dozens of cubes, each read by a superconducting resonator, listens for collisions of a few tens of eV.

The physics.

A phonon-mediated kinetic inductance detector arrayLeft: a silicon wafer carved into cubes that stay joined to a thin common disk; superconducting resonators on the disk sit under each cube. A particle hits one cube and the phonons it creates reach the resonator. Right: the resonance dip in microwave transmission moves to lower frequency after the hit. particle silicon cubes carved in one waferphonons reach aluminium resonators (KIDs) on the disk frequencytransmission beforeafter a hit
A hit in one cube sends phonons to its resonator, and the resonance moves to lower frequency. Schematic, not to scale.

Light dark matter and co­her­ent elastic neu­tri­no–nucleus scatter­ing (CEνNS) leave the same faint trace: a nucleus recoil­ing with tens to hun­dreds of elec­tron­volts. Measur­ing it takes calo­rim­e­ters cooled to mil­li­kelvin tem­per­a­tures, where the heat ca­pac­i­ty of a crystal is tiny and a small energy deposit gives a mea­sur­able signal.

In BULLKID the energy is read through phonons. The recoil creates phonons that spread through the silicon ab­sorb­er and reach a thin alu­min­ium film, a super­conduct­ing res­o­na­tor. They break Cooper pairs, the kinetic in­duc­tance of the film rises and its res­o­nance moves to lower fre­quen­cy: a kinetic in­duc­tance de­tec­tor (KID). Many res­o­na­tors at dif­fer­ent fre­quen­cies are read on a single line by micro­wave multi­plexing.

The array is carved from one thick silicon wafer. Deep cuts divide it into cubes but stop short of the back, leaving a thin common disk that holds them and carries the KIDs: no glue and no in­di­vid­u­al holders, and the neigh­bours of each cube act as a veto against back­ground from outside.

We dice the arrays in Ferrara. DANAE and BULLKID-DM scale the concept to sixteen wafers, over 2,000 el­e­ments and about 800 g at the Gran Sasso lab­o­ra­to­ries; for NUCLEUS, which will measure CEνNS at the Chooz reactor, we machine the ger­ma­nium veto and the silicon holders.

What we have shown.

BULLKID carves a single silicon wafer into a mono­lithic array of ab­sorb­ers, each read by a kinetic in­duc­tance de­tec­tor, with no extra sup­ports or wiring: the first 60-element pro­to­type reached 26 eV base­line resolu­tion. DANAE and BULLKID-DM scale this to sixteen wafers, over 2,000 el­e­ments and about 800 g at the Gran Sasso lab­o­ra­to­ries. For NUCLEUS, which will measure co­her­ent neu­tri­no–nucleus scatter­ing at the Chooz reactor, we machine the ger­ma­nium veto and silicon holders.

26 eV

Baseline energy resolution of the first BULLKID prototype: 64 cubes of 5.4 × 5.4 × 5 mm³ carved in a 3-inch, 5 mm thick silicon wafer.

Applied Physics Letters 121 (2022)

112 eV

First observation of a nuclear-recoil peak induced by neutron capture, a new way to calibrate low-threshold detectors, in a NUCLEUS CaWO₄ detector.

Physical Review Letters 130 (2023)

Read first.

  1. BULLKID: Monolithic array of particle absorbers sensed by kinetic inductance detectorsCruciani A., Bandiera L., Calvo M. … Guidi V., Romagnoni M., Mazzolari A. et al. · Applied Physics Letters 121 (2022)
  2. Low-energy spectrum of the BULLKID detector array operated on surfaceDelicato D., Ahmad A., Bandiera L. … Guidi V., Romagnoni M., Mazzolari A. et al. · European Physical Journal C 84 (2024)
  3. Energy calibration of bulk events in the BULLKID detectorFolcarelli M., Delicato D., Acevedo-Rentería A. … Bandiera L., Guidi V., Malagutti L. et al. · European Physical Journal C 86 (2026)
  4. Germanium target sensed by phonon-mediated kinetic inductance detectorsDelicato D., Angelone D., Bandiera L. … Guidi V., Romagnoni M., Mazzolari A. et al. · Applied Physics Letters 126 (2025)
  5. Nucleus: Searching for Coherent Neutrino Nucleus Scattering at Lowest EnergiesKluck H., Angloher G., Bento A. … Guidi V., Mazzolari A. et al. · Journal of Low Temperature Physics 209 (2022)
  6. Observation of a Nuclear Recoil Peak at the 100 eV Scale Induced by Neutron CaptureAbele H., Angloher G., Bento A. … Mazzolari A., Romagnoni M. et al. · Physical Review Letters 130 (2023)

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