2026-05-30
06:54 |
Upgrade of the CERN cryogenic test facility for the HL-LHC superconducting magnets and superconducting links
/ Pirotte, O (CERN) ; Barbe, T (CERN) ; Buzio, M (CERN) ; Dassa, L (CERN) ; Gahier, V (CERN) ; Guillotin, N (CERN) ; Lees, A (CERN) ; Mangiarotti, F (CERN) ; Mauny, R (CERN) ; Ninet, G (CERN) et al.
New superconducting magnets, based on Nb$_{3}$Sn technology, have been developed for the HL-LHC project, the High-Luminosity upgrade of the LHC (Large Hadron Collider) at Interaction Points 1 and 5. These magnets require thorough testing in cryogenic conditions at 4.5 and 1.9 K before their installation into the LHC. [...]
2026 - 9 p.
- Published in : IOP Conf. Ser. Mater. Sci. Eng.: 1344 (2026) , no. 1, pp. 012141
Fulltext: PDF;
In : 26th Joint Cryogenic Engineering Conference and International Cryogenic Materials Conference, Peppermill Reno Resort, Reno, Nevada, United States, 18 - 22 May 2025, pp.012141
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2026-05-30
06:54 |
How digital twins can help with operator training, an example with ATLAS and CMS detector’s cryogenics at CERN
/ Jimenez, L (CERN) ; Majorel, A (CERN ; GANIL) ; Bradu, B (CERN) ; Gahier, V (CERN)
This paper presents the implementation of a cryogenic process simulator applied to A Toroidal LHC Apparatus (ATLAS) and the Compact Muon Solenoid (CMS) experiments at CERN (European Organisation for Nuclear Research). Building upon the development of a digital twin of the complex LHC accelerator cryogenic system, this work extends its application to the specific needs of the ATLAS and CMS experiments and their dedicated cryogenic systems. [...]
2026 - 9 p.
- Published in : IOP Conf. Ser. Mater. Sci. Eng. 1344 (2026) 012058
Fulltext: PDF;
In : 26th Joint Cryogenic Engineering Conference and International Cryogenic Materials Conference, Peppermill Reno Resort, Reno, Nevada, United States, 18 - 22 May 2025, pp.012058
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2026-05-20
08:58 |
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2026-05-06
06:06 |
FCC― 次世代円形衝突型加速器
/ OIDE, Katsunobu (CERN ; U. Geneva (main) ; KEK, Tsukuba)
FCC is a project for a next generation circular collider based at CERN, as the next step of LEP/LHC experiments.
It will have at least two stages : (i) measurements on electroweak (Z/W), Higgs, tt by e+e－ collision (FCC-ee) and (ii)
energy frontier pp collision (FCC-hh) up to 100 TeV center of mass (CM) energy. Both will be performed by colliders
in the same tunnel with 90–100 km circumference built around the Geneva area across the Swiss-French border..
2022 - 4 p.
- Published in : Vacuum and Surface Science 65 (2022) 556-559
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2026-04-30
08:43 |
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2026-04-28
14:36 |
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2026-04-28
06:21 |
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Basics of RF Electronics
/ Dexter, Amos Christopher (Lancaster U. (main))
The focus of this educational text is selected examples of high-frequency electronic circuits and their components employed for the accurate phasing and synchronisation of accelerator cavities. [...]
arXiv:2602.15205.
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2026 - 38.
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2026-04-23
07:25 |
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2026-04-21
06:41 |
Transition-Edge Sensor Spectrometer for Precision Spectroscopy of Antiprotonic Atoms
/ Morgan, Kelsey (NIST, Boulder) ; Azuma, Toshiyuki (KEK, Tsukuba) ; Baptista, Gonçalo (Paris, Lab. Kastler Brossel) ; Becker, Daniel (Colorado U.) ; Bennett, Douglas (NIST, Boulder) ; Butin, François (CERN) ; Dean, Jonathan W (NIST, Boulder ; Colorado U.) ; Eizenberg, Ofir (Technion) ; Fowler, Joseph W (NIST, Boulder) ; Fujioka, Hiroyuki (ISCT, Tokyo) et al.
antiProtonic Atom X-ray (PAX) spectroscopy is an experiment that aims to test strong-field quantum electrodynamics (QED) effects by performing high-precision X-ray spectroscopy of antiprotonic atoms. PAX will use a low-energy antiproton beam provided by the Extra Low ENergy Antiproton (ELENA) ring at the European Organization for Nuclear Research (CERN) to create antiprotonic atoms. [...]
2026 - 6 p.
- Published in : IEEE Trans. Appl. Supercond. 36 (2026) 2101706
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2026-04-16
16:32 |
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