001     889109
005     20210128101610.0
024 7 _ |2 Handle
|a 2128/26655
037 _ _ |a FZJ-2021-00039
100 1 _ |0 P:(DE-HGF)0
|a Aidala, C. A.
|b 0
245 _ _ |a The LHCSpin Project
260 _ _ |a New York, N.Y.
|b Allerton Press
|c 2018
336 7 _ |0 PUB:(DE-HGF)25
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|a Preprint
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|s 1609852743_16410
336 7 _ |2 ORCID
|a WORKING_PAPER
336 7 _ |0 28
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336 7 _ |2 BibTeX
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336 7 _ |2 DataCite
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520 _ _ |a LHCSpin aims at installing a polarized gas target in front of the LHCb spectrometer, bringing, for the first time, polarized physics to the LHC. The project will benefit from the experience achieved with the installation of an unpolarized gas target at LHCb during the LHC Long Shutdown 2. LHCb will then become the first experiment simultaneously running in collider and fixed-target mode with polarized targets, opening a whole new range of explorations to its exceptional spectrometer. LHCSpin will offer a unique opportunity to probe polarized quark and gluon parton distributions in nucleons and nuclei, especially at high $x$ and intermediate $Q^2$, where experimental data are still largely missing. Beside standard collinear parton distribution functions (PDFs), LHCSpin will make it possible to study multidimensional polarized parton distributions that depend also on parton transverse momentum. The study of the multidimensional partonic structure of the nucleon, particularly including polarization effects, can test our knowledge of QCD at an unprecedented level of sophistication, both in the perturbative and nonperturbative regime. At the same time, an accurate knowledge of hadron structure is necessary for precision measurements of Standard Model (SM) observables and discovery of physics beyond the SM. Due to the intricate nature of the strong interaction, it is indispensable to perform the widest possible suite of experimental measurements. It will be ideal to have two new projects complementing each other: a new facility for polarized electron-proton collisions and a new facility for polarized proton-proton collisions. LHCSpin stands out at the moment as the most promising candidate for the second type of project, going beyond the kinematic coverage and the accuracy of the existent experiments, especially on the heavy-quark sector.
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|a Bacchetta, A.
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|a Boglione, M.
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|a Bozzi, G.
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|a Carassiti, V.
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|a Ciullo, Giuseppe
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|a D'Alesio, U.
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|a Di Nezza, P.
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|a Lenisa, Paolo
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|a Liuti, S.
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|a Metz, Lisa Maria
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|a Mulder, P. J.
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|a Pisano, C.
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|a Steffens, Jennifer
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