CERN Accelerating science

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1.
SND@LHC: The Scattering and Neutrino Detector at the LHC / SND@LHC Collaboration
SND@LHC is a compact and stand-alone experiment designed to perform measurements with neutrinos produced at the LHC in the pseudo-rapidity region of ${7.2 < \eta < 8.4}$. The experiment is located 480 m downstream of the ATLAS interaction point, in the TI18 tunnel. [...]
arXiv:2210.02784.- 2024-05-23 - 57 p. - Published in : JINST 19 (2024) P05067 Fulltext: 2210.02784 - PDF; document - PDF;
In : The Large Hadron Collider and The Experiments for Run 3
2.
The SHiP experiment at the proposed CERN SPS Beam Dump Facility / SHiP Collaboration
The Search for Hidden Particles (SHiP) Collaboration has proposed a general-purpose experimental facility operating in beam-dump mode at the CERN SPS accelerator to search for light, feebly interacting particles. The SHiP experiment incorporates two complementary detectors. [...]
arXiv:2112.01487.- 2022-05-26 - 23 p. - Published in : Eur. Phys. J. C 82 (2022) 486 Fulltext: document - PDF; 2112.01487 - PDF;
3.
Reconstruction of 400 GeV/c proton interactions with the SHiP-charm project / SHiP Collaboration
The SHiP-charm project was proposed to measure the associated charm production induced by 400 GeV/c protons in a thick target, including the contribution from cascade production. An optimisation run was performed in July 2018 at CERN SPS using a hybrid setup. [...]
arXiv:2406.04730; CERN-SHiP-NOTE-2020-002.- Geneva : CERN, 2024-06-04 - 10 p. - Published in : Eur. Phys. J. C 84 (2024) 562 Fulltext: Proton_reconstruction_SHiP-charm_v3 - PDF; document - PDF; 2406.04730 - PDF; Publication: PDF;
4.
The Magnet of the Scattering and Neutrino Detector for the SHiP experiment at CERN / SHiP Collaboration
The Search for Hidden Particles (SHiP) experiment proposal at CERN demands a dedicated dipole magnet for its scattering and neutrino detector. This requires a very large volume to be uniformly magnetized at B > 1.2 T, with constraints regarding the inner instrumented volume as well as the external region, where no massive structures are allowed and only an extremely low stray field is admitted. [...]
arXiv:1910.02952.- 2020-01-23 - 25 p. - Published in : JINST 15 (2020) P01027 Fulltext: fulltext1758067 - PDF; 1910.02952 - PDF;

Vegeu també: autors amb noms similars
2 Cavalcante, A
3 Cavalcante, A B R
1 Cavalcante, Ana Barbara R.
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