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Related papers: CUORE Opens the Door to Tonne-scale Cryogenics Exp…

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Models for light dark matter particles with masses below 1 GeV/c$^2$ are a natural and well-motivated alternative to so-far unobserved weakly interacting massive particles. Gram-scale cryogenic calorimeters provide the required detector…

A model of a multilayer device with non-trivial geometrical structure and nonlinear dependencies of thermodynamic material properties at cryogenic temperatures is suggested. A considered device, called cryogenic cell, is intended for use in…

Computational Physics · Physics 2015-11-20 Alexander Ayriyan , Jan Busa , Eugeny E. Donets , Hovik Grigorian , Jan Pribis

In-vacuo cryogenic environments are ideal for applications requiring both low temperatures and extremely low particle densities. This enables reaching long storage and coherence times for example in ion traps, essential requirements for…

The understanding of complex and/or large vacuum systems operating at cryogenic temperatures requires a specific knowledge of the vacuum science at such temperatures. At room temperature, molecules with a low binding energy to a surface are…

Instrumentation and Detectors · Physics 2020-06-03 Vincent Baglin

As a step towards the realization of cryogenic-detector experiments to search for neutrinoless double-beta decay (such as CROSS, BINGO, and CUPID), we investigated a batch of 10 Ge light detectors (LDs) assisted by Neganov-Trofimov-Luke…

We discuss the possibility of new generation neutrino and astroparticle physics experiments exploiting the liquid Argon Time Projection Chamber (LAr TPC) technique, following a graded strategy that envisions applications with increasing…

High Energy Physics - Phenomenology · Physics 2009-11-11 A. Ereditato , A. Rubbia

Ultracold molecules represent a fascinating research frontier in physics and chemistry, but it has proven challenging to prepare dense samples at low velocities. Here we present a solution to this goal by a non-conventional approach dubbed…

Atomic Physics · Physics 2018-12-04 Xing Wu , Thomas Gantner , Manuel Koller , Martin Zeppenfeld , Sotir Chervenkov , Gerhard Rempe

Muon ionization cooling provides the only practical solution to prepare high-brilliance beams necessary for a neutrino factory or muon collider. The Muon Ionization Cooling Experiment (MICE), under development at the Rutherford Appleton…

Accelerator Physics · Physics 2008-10-11 Terrence L. Hart , Daniel M. Kaplan

Cryogenics is a pivotal aspect in the development of quantum technologies. Closed-cycle devices have recently emerged as an environmentally friendly and low-maintenance alternative to liquid helium cryostats. Yet the larger level of…

Instrumentation and Detectors · Physics 2023-01-16 Anne Louchet-Chauvet , Thierry Chanelière

Refrigeration is an important enabler for quantum technology. The very low energy of the fundamental excitations typically utilized in quantum technology devices and systems requires temperature well below 1 K. Expensive cryostats are…

Quantum Physics · Physics 2022-09-16 E. Mykkänen , J. S. Lehtinen , A. Ronzani , A. Kemppinen , A. Alkurdi , P. -O. Chapuis , M. Prunnila

Recent studies in quantum computing have shown that quantum error correction with large numbers of physical qubits are limited by ionizing radiation from high-energy particles. Depending on the physical setup of the quantum processor, the…

Quantum Physics · Physics 2023-12-11 Ulascan Sarica

Transition Edge Sensors (TESs) are amongst the most sensitive cryogenic detectors and can be easily optimized for the detection of massive particles or photons ranging from X-rays all the way down to millimetre radiation. Furthermore, TESs…

Instrumentation and Detectors · Physics 2024-11-05 Mario De Lucia , Paolo Dal Bo , Eugenia Di Giorgi , Tommaso Lari , Claudio Puglia , Federico Paolucci

Chapter 9 in High-Luminosity Large Hadron Collider (HL-LHC) : Preliminary Design Report. The Large Hadron Collider (LHC) is one of the largest scientific instruments ever built. Since opening up a new energy frontier for exploration in…

Accelerator Physics · Physics 2017-06-01 S. Claudet , L. Tavian

A detailed description of the CUORICINO $^{130}Te$ neutrinoless double-beta ($\nbb$) decay experiment is given and recent results are reported. CUORICINO is an array of 62 tellurium oxide ($TeO_{2}$) bolometers with an active mass of 40.7…

Quantum technologies promise a radically new way to solve classically intractable computing problems. Superconducting circuits as a platform are at the forefront of this field. The cryogenic operation temperatures of superconducting…

IceTop is a 1 km^2 air shower detector presently under construction as a part of the IceCube Observatory at South Pole. It will consist of 80 detector stations, each equipped with two ice Cherenkov tanks, which cover 1 km^2. In 2008, the…

Astrophysics · Physics 2019-08-13 Stefan Klepser

The future electron-ion collider (EIC) will produce the first-ever high energy collisions between electrons and a wide range of nuclei, opening a new era in the study of cold nuclear matter. Quarks and gluons produced in these collisions…

High Energy Physics - Phenomenology · Physics 2025-10-03 Kyle Devereaux , Wenqing Fan , Weiyao Ke , Kyle Lee , Ian Moult

The energy dependent thermoelectric response of a single molecule contains valuable information about its transmission function and its excited states. However, measuring it requires devices that can efficiently heat up one side of the…

Understanding heat transport is relevant to develop efficient strategies for thermal management in microelectronics for instance, as well as for fundamental science purposes. However, measuring temperatures in nanostructured environments…

We report a study of the CUORE sensitivity to neutrinoless double beta ($0\nu\beta\beta$) decay. We used a Bayesian analysis based on a toy Monte Carlo (MC) approach to extract the exclusion sensitivity to the $0\nu\beta\beta$ decay…

Instrumentation and Detectors · Physics 2017-08-16 CUORE Collaboration , C. Alduino , K. Alfonso , D. R. Artusa , F. T. Avignone , O. Azzolini , T. I. Banks , G. Bari , J. W. Beeman , F. Bellini , G. Benato , A. Bersani , M. Biassoni , A. Branca , C. Brofferio , C. Bucci , A. Camacho , A. Caminata , L. Canonica , X. G. Cao , S. Capelli , L. Cappelli , L. Carbone , L. Cardani , P. Carniti , N. Casali , L. Cassina , D. Chiesa , N. Chott , M. Clemenza , S. Copello , C. Cosmelli , O. Cremonesi , R. J. Creswick , J. S. Cushman , A. D'Addabbo , I. Dafinei , C. J. Davis , S. Dell'Oro , M. M. Deninno , S. Di Domizio , M. L. Di Vacri , A. Drobizhev , D. Q. Fang , M. Faverzani , G. Fernandes , E. Ferri , F. Ferroni , E. Fiorini , M. A. Franceschi , S. J. Freedman , B. K. Fujikawa , A. Giachero , L. Gironi , A. Giuliani , L. Gladstone , P. Gorla , C. Gotti , T. D. Gutierrez , E. E. Haller , K. Han , E. Hansen , K. M. Heeger , R. Hennings-Yeomans , K. P. Hickerson , H. Z. Huang , R. Kadel , G. Keppel , Yu. G. Kolomensky , A. Leder , C. Ligi , K. E. Lim , Y. G. Ma , M. Maino , L. Marini , M. Martinez , R. H. Maruyama , Y. Mei , N. Moggi , S. Morganti , P. J. Mosteiro , T. Napolitano , M. Nastasi , C. Nones , E. B. Norman , V. Novati , A. Nucciotti , T. O'Donnell , J. L. Ouellet , C. E. Pagliarone , M. Pallavicini , V. Palmieri , L. Pattavina , M. Pavan , G. Pessina , V. Pettinacci , G. Piperno , C. Pira , S. Pirro , S. Pozzi , E. Previtali , C. Rosenfeld , C. Rusconi , M. Sakai , S. Sangiorgio , D. Santone , B. Schmidt , J. Schmidt , N. D. Scielzo , V. Singh , M. Sisti , A. R. Smith , L. Taffarello , M. Tenconi , F. Terranova , C. Tomei , S. Trentalange , M. Vignati , S. L. Wagaarachchi , B. S. Wang , H. W. Wang , B. Welliver , J. Wilson , L. A. Winslow , T. Wise , A. Woodcraft , L. Zanotti , G. Q. Zhang , B. X. Zhu , S. Zimmermann , S. Zucchelli
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