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2026-03-18
12:40

A search for lepton-flavour violating $\tau \to 3\mu$ decays with the ATLAS detector
A search for charged lepton flavour violation in $\tau \to 3\mu$ decays is performed in $pp$ collisions at a centre-of-mass energy of 13 TeV using ATLAS data collected between 2016 and 2018, corresponding to an integrated luminosity of 137 $\text{fb}^{-1}$ [...]
CERN-EP-2026-059. - 2026
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2026-03-18
06:17

Laboratory observation of collective beam-plasma instabilities in a relativistic pair jet / Halliday, J W D (U. Oxford (main) ; Rutherford Appleton Laboratory) ; Arrowsmith, C D (U. Oxford (main) ; Unlisted, US) ; Goillot, A M (CERN) ; Bilbao, P J (Unlisted) ; Simon, P (Darmstadt, GSI) ; Stergiou, V (U. Oxford (main) ; CERN) ; Zhang, S (U. Oxford (main)) ; Alexaki, P (CERN ; Athens Natl. Capodistrian U.) ; Bochmann, M (Unlisted, AT) ; Bott, A F A (U. Oxford (main)) et al.
We report on a measurement of collective behavior in a relativistic electron-positron pair plasma produced in the laboratory. [...]
arXiv:2602.16542. - 2026 - 7.
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2026-03-18
06:17

Why (and How) LGADs Work: Ionization, Space Charge, and Gain Saturation / Cartiglia, N (INFN, Turin) ; Altamura, A R (INFN, Turin ; Turin U.) ; Arcidiacono, R (INFN, Turin ; Piemonte Orientale U., Alessandria) ; Durando, M (Turin U.) ; Galletto, S (Turin U.) ; Ferrero, M (INFN, Turin) ; Lanteri, L (INFN, Turin ; Turin U.) ; Losana, A (INFN, Turin ; Turin U.) ; Massaccesi, L (INFN, Turin ; Turin U.) ; Menzio, L (CERN) et al.
The temporal resolution of Low-Gain Avalanche Detectors (LGADs), also known as Ultra-Fast Silicon Detectors (UFSDs), is governed by two contributions: jitter, arising from electronic noise and signal slew rate, and the Landau noise term, arising from the non-uniform energy deposition of minimum ionizing particles (MIPs). [...]
arXiv:2603.10841. - 2026 - 7.
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2026-03-18
06:17

End-to-end optimisation of HEP triggers / Clarke Hall, Noah (U. Coll. London ; CERN) ; Xiotidis, Ioannis (CERN) ; Konstantinidis, Nikos (U. Coll. London ; CERN) ; Miller, David W (CERN ; U. Chicago (main))
High-energy physics experiments face extreme data rates, requiring real-time trigger systems to reduce event throughput while preserving sensitivity to rare processes. [...]
arXiv:2603.08428. - 2026 - 25.
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2026-03-18
06:17

Recent searches for new phenomena with the ATLAS detector / Fawcett, William J (Cambridge U. (main))
Three recently and uniquely interesting searches for new physics performed by the ATLAS collaboration are presented. [...]
2022 - 6.
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2026-03-18
06:17

Experimental characterization of the hierarchy of quantum correlations in top quark pairs / Afik, Yoav (Chicago U., EFI) ; Demina, Regina (Rochester U.) ; Herrera, Alan (Rochester U.) ; Heinz Hindrichs, Otto (Rochester U.) ; de Nova, Juan Ramón Muñoz (CSIC, Madrid ; UCM, Madrid, Dept. Phys.) ; Ravina, Baptiste (CERN)
Recent results from the Large Hadron Collider have demonstrated quantum entanglement of top quark-antiquark pairs using the spin degree of freedom. [...]
arXiv:2602.15115. - 2026 - 11.
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2026-03-18
06:17

AMD Versal AI-Engines for fixed latency environments / Xiotidis, Ioannis (CERN) ; Clarke Hall, Noah (University Coll. London) ; Du, Tianjia (CERN ; Chicago U., EFI) ; Konstantinidis, Nikos (University Coll. London) ; Miller, David (Chicago U., EFI ; Chicago U., KICP)
Complex, high-throughput data acquisition and processing systems, such as those used in high-energy physics experiments, are increasingly moving sophisticated pattern recognition and data compression algorithms closer to the sensors themselves. [...]
arXiv:2603.13852. - 2026 - 9.
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2026-03-18
06:17

Human versus Artificial Inteligence; a significant example in astrophysics, alas / De Rújula, A (U. Autonoma, Madrid (main) ; CERN)
There are two well documented models of gamma ray bursts (GRBs), the "Standard' model and the "Cannonball" model. [...]
arXiv:2601.23205. - 2026 - 4.
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2026-03-18
04:48

Measurement of the $t$-channel single top quark cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV / CMS Collaboration
The single top quark $t$-channel production cross section is measured in proton-proton collisions at the CERN LHC at $\sqrt{s}$ = 5.02 TeV, using data recorded with the CMS detector in 2017, corresponding to an integrated luminosity of 302 pb$^{-1}$, and resulting in the first CMS measurement of the process at that energy. [...]
arXiv:2603.13592 ; CMS-TOP-24-011 ; CERN-EP-2025-289. - 43.
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2026-03-18
04:47