Search arXivSearch

arXiv · 2605.24272

Characterization of Aluminum Microwave SQUID Multiplexers for CE$ν$NS Detection

James Amidei·Antoine Armatol·Corinne Augier·Louis Bailly-Salins·Guillaume Baulieu·Laurent Bergé·Julien Billard·Juliette Blé·Gaby Brenot·Guillaume Bres·Jean-Louis Bret·Alexandre Broniatowski·Martino Calvo·Antonella Cavanna·Antoine Cazes·Emanuela Celi·David Chaize·Mohammed Chala·Maurice Chapellier·Luke Chaplinsky·Ran Chen·Ion Cojocari·Jules Colas·Laurent Couraud·Elspeth Cudmore·Maryvonne De Jesus·Pierre de Marcillac·Nicole Dombrowski·Louis Dumoulin·Alan Durnez·Romain Faure·Sylvain Ferriol·Enectali Figueroa-Feliciano·Joseph A. Formaggio·Stephane Fuard·Jules Gascon·Cloé Girard-Carillo·Andrea Giuliani·Corinne Goy·Cyrille Guerin·Leïla Haegel·Patrick M. Harrington·Scott A. Hertel·Cyrus F. Hirjibehedin·Christophe Hoarau·Ziqing Hong·Daemon Howard·Jean-Christophe Ianigro·Yong Jin·Alexandre Juillard·Dimitar Karaivanov·Temirlan Khussainov·Andrew Kubik·Jacob Lamblin·Tatiana Le Bellec·Laetitia Leroy·Mingyu Li·Alexey Lubashevskiy·Stefanos Marnieros·Romain Martin·Nicolas Martini·Julien Minet·Alessandro Monfardini·Franck Mounier·Bethany M. Niedzielski·Valentina Novati·Wiliam D. Oliver·Emiliano Olivieri·H. Douglas Pinckney·Denys V. Poda·Dmitrii Ponomarev·Jean-Sébastien Real·Faith C. Reyes·Alejandro Rodriguez·Sergey Rozov·Irina Rozova·Brianna Ryan·Deeksha Sabhari·Silvia Scorza·Kyle Serniak·Renaud Serra·Yegor Shevchik·Torsten Soldner·Hannah Stickler·Caitlyn Stone-Whitehead·Christian Ulysse·Wouter Van De Pontseele·Sergey Vasilyev·Paul Vittaz·Steven Weber·Evan Wolfe·Wayne Woods·Evgeny Yakushev·Jiatong Yang·Daniya Zinatulina

Abstract

We present the design, fabrication, and characterization of an aluminum-based six-channel microwave SQUID multiplexer ($μ$MUX) prototype for transition-edge sensor (TES) readout in the RICOCHET experiment. The device consists of aluminum coplanar-waveguide resonators and RF SQUIDs with Dolan-style Al/AlO$_x$/Al Josephson junctions. By measuring the resonator scattering parameters at a range of probe tone frequencies, powers, and flux bias points, we demonstrate agreement between the device response and existing multiplexer models. We also characterize the noise performance in both open-loop and flux-ramping modes. With a high electron mobility transistor (HEMT) amplifier, open-loop measurements yield a flux sensitivity of 1-1.5 $μΦ_0/\sqrt{Hz}$. With flux-ramp modulation, low-frequency 1/f noise is suppressed, and the flux sensitivity is around 3-4 $μΦ_0/\sqrt{Hz}$, corresponding to a current sensitivity of 24-33 $pA/\sqrt{Hz}$ at the input coil. We further demonstrate a reduction in readout noise by incorporating a Josephson traveling-wave parametric amplifier (JTWPA) between the $μ$MUX and the HEMT. This achieves an open-loop flux sensitivity of 0.3-0.6 $μΦ_0/\sqrt{Hz}$ and an effective system noise temperature below 1 K. These results establish aluminum $μ$MUX devices as a viable and extensible readout technology for low-noise cryogenic detector arrays.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

James Amidei, Antoine Armatol, Corinne Augier, Louis Bailly-Salins, Guillaume Baulieu, Laurent Bergé, Julien Billard, Juliette Blé, Gaby Brenot, Guillaume Bres, Jean-Louis Bret, Alexandre Broniatowski, Martino Calvo, Antonella Cavanna, Antoine Cazes, Emanuela Celi, David Chaize, Mohammed Chala, Maurice Chapellier, Luke Chaplinsky, Ran Chen, Ion Cojocari, Jules Colas, Laurent Couraud, Elspeth Cudmore, Maryvonne De Jesus, Pierre de Marcillac, Nicole Dombrowski, Louis Dumoulin, Alan Durnez, Romain Faure, Sylvain Ferriol, Enectali Figueroa-Feliciano, Joseph A. Formaggio, Stephane Fuard, Jules Gascon, Cloé Girard-Carillo, Andrea Giuliani, Corinne Goy, Cyrille Guerin, Leïla Haegel, Patrick M. Harrington, Scott A. Hertel, Cyrus F. Hirjibehedin, Christophe Hoarau, Ziqing Hong, Daemon Howard, Jean-Christophe Ianigro, Yong Jin, Alexandre Juillard, Dimitar Karaivanov, Temirlan Khussainov, Andrew Kubik, Jacob Lamblin, Tatiana Le Bellec, Laetitia Leroy, Mingyu Li, Alexey Lubashevskiy, Stefanos Marnieros, Romain Martin, Nicolas Martini, Julien Minet, Alessandro Monfardini, Franck Mounier, Bethany M. Niedzielski, Valentina Novati, Wiliam D. Oliver, Emiliano Olivieri, H. Douglas Pinckney, Denys V. Poda, Dmitrii Ponomarev, Jean-Sébastien Real, Faith C. Reyes, Alejandro Rodriguez, Sergey Rozov, Irina Rozova, Brianna Ryan, Deeksha Sabhari, Silvia Scorza, Kyle Serniak, Renaud Serra, Yegor Shevchik, Torsten Soldner, Hannah Stickler, Caitlyn Stone-Whitehead, Christian Ulysse, Wouter Van De Pontseele, Sergey Vasilyev, Paul Vittaz, Steven Weber, Evan Wolfe, Wayne Woods, Evgeny Yakushev, Jiatong Yang, Daniya Zinatulina. 2026-05-22. Characterization of Aluminum Microwave SQUID Multiplexers for CE$ν$NS Detection. https://arxiv.org/abs/2605.24272

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

TCAD + Allpi$\text{x}^2$ Simulation study of MALTA2, a Depleted Monolithic Active Pixel Sensor for future tracking

In this work, a hybrid simulation framework combining TCAD and Allpi$\text{x}^2$ is presented to investigate the sensor properties of MALTA2, a depleted monolithic active pixel sensor designed for future tracking. The study starts from 3D modeling and transient simulations in TCAD, with generic doping profiles and simple well structures. The resulting doping profiles and electric field are extracted and fed into Allpi$\text{x}^2$ for high-statistics Monte Carlo simulations in both DUT-only and full-telescope mode. Simulations reveal a strong dependence of sensor performance, specifically the detection efficiency and cluster size, on the doping concentration of the N-type blanket at the sensor surface. The doping concentration is then optimized by comparing simulations with measurement data. The active depth of the depleted region of the MALTA2 sensor is estimated in both simulations and measurements using a grazing angle method, in which the sensor is positioned at various inclinations relative to the beam, covering angles from 0 to 60 degrees. Excellent agreement on active depth is obtained with the optimal doping concentration, showing a deviation of 2\% from the measured value at a threshold of 450\,$\text{e}^-$. Consequently, the framework offers a generic toolkit for sensor studies without requiring proprietary information.

physics.ins-det

A compact fibre-coupled active beamstop for fast time-resolved monitoring of synchrotron X-ray beams

We have developed a compact fibre-coupled active beamstop for simultaneous interception and time-resolved monitoring of the direct X-ray beam in synchrotron diffraction experiments. The complete beamstop tip has a maximum transverse dimension of 1 mm and incorporates a 700 $μ$m-wide Ce:YAG scintillator. The scintillator converts the intercepted X-rays into visible light, which is transported through a multimode optical fibre to a silicon photodiode at the bottom of the blade that is connected to a dedicated fast amplifier electronics. Tests with a pulsed laser yielded a system decay time of 69.4 ns, consistent with reported luminescence decay times for Ce:YAG. Measurements at the P14.EH2 end station of PETRA III demonstrated the detection of individual bunch signals separated by 192 ns in the 40-bunch operating mode. The active beamstop also provided an in-situ timing signal for synchronising an experimental sequence with the approximately 190 $μ$s transmission window of a mechanical X-ray chopper. The device therefore combines a compact obstruction of the direct beam with fast monitoring of X-ray timing and flux during diffraction data acquisition.

physics.ins-det

Charge-Carrier transport simulations in diamond detectors with electric-field-dependent mobility and charge-collection-distance-based trapping

Diamond detectors are attractive for operation in harsh radiation environments because they combine radiation tolerance, fast signal formation, and low leakage current. Realistic detector-response simulations require an accurate description of charge-carrier mobility and trapping, which determine both signal amplitude and timing. In this work, we extend \allpix{}, a modular end-to-end detector simulation framework, with diamond-specific transport models. The implementation includes field-dependent mobility parameterizations for electrons and holes and an effective trapping model based on the charge collection distance (CCD), providing a detector-level interface to material quality and radiation-damage measurements. The mobility description is validated in the negligible-trapping limit using single-crystalline CVD diamond by comparing simulated drift velocities and transient-current signals with published reference data. For polycrystalline CVD diamond, the CCD-based trapping model is evaluated using experimentally measured CCD values and compared with laboratory transient-current-technique waveforms. The simulations reproduce the measured drift-velocity behavior in scCVD and the reduced charge collection and degraded transient response observed in pcCVD. The presented implementation enables detector-level studies of charge collection, pulse formation, and timing performance in diamond sensors using experimentally accessible transport and trapping parameters, and provides a practical framework for simulation-driven detector development and radiation-damage studies.

physics.ins-det