000889109 001__ 889109
000889109 005__ 20210128101610.0
000889109 0247_ $$2Handle$$a2128/26655
000889109 037__ $$aFZJ-2021-00039
000889109 1001_ $$0P:(DE-HGF)0$$aAidala, C. A.$$b0
000889109 245__ $$aThe LHCSpin Project
000889109 260__ $$aNew York, N.Y.$$bAllerton Press$$c2018
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000889109 520__ $$aLHCSpin aims at installing a polarized gas target in front of the LHCb spectrometer, bringing, for the first time, polarized physics to the LHC. The project will benefit from the experience achieved with the installation of an unpolarized gas target at LHCb during the LHC Long Shutdown 2. LHCb will then become the first experiment simultaneously running in collider and fixed-target mode with polarized targets, opening a whole new range of explorations to its exceptional spectrometer. LHCSpin will offer a unique opportunity to probe polarized quark and gluon parton distributions in nucleons and nuclei, especially at high $x$ and intermediate $Q^2$, where experimental data are still largely missing. Beside standard collinear parton distribution functions (PDFs), LHCSpin will make it possible to study multidimensional polarized parton distributions that depend also on parton transverse momentum. The study of the multidimensional partonic structure of the nucleon, particularly including polarization effects, can test our knowledge of QCD at an unprecedented level of sophistication, both in the perturbative and nonperturbative regime. At the same time, an accurate knowledge of hadron structure is necessary for precision measurements of Standard Model (SM) observables and discovery of physics beyond the SM. Due to the intricate nature of the strong interaction, it is indispensable to perform the widest possible suite of experimental measurements. It will be ideal to have two new projects complementing each other: a new facility for polarized electron-proton collisions and a new facility for polarized proton-proton collisions. LHCSpin stands out at the moment as the most promising candidate for the second type of project, going beyond the kinematic coverage and the accuracy of the existent experiments, especially on the heavy-quark sector.
000889109 536__ $$0G:(DE-HGF)POF3-612$$a612 - Cosmic Matter in the Laboratory (POF3-612)$$cPOF3-612$$fPOF III$$x0
000889109 7001_ $$0P:(DE-HGF)0$$aBacchetta, A.$$b1
000889109 7001_ $$0P:(DE-HGF)0$$aBoglione, M.$$b2
000889109 7001_ $$0P:(DE-HGF)0$$aBozzi, G.$$b3
000889109 7001_ $$0P:(DE-HGF)0$$aCarassiti, V.$$b4
000889109 7001_ $$0P:(DE-HGF)0$$aChiosso, M.$$b5
000889109 7001_ $$0P:(DE-HGF)0$$aCimino, R.$$b6
000889109 7001_ $$0P:(DE-Juel1)131116$$aCiullo, Giuseppe$$b7
000889109 7001_ $$0P:(DE-HGF)0$$aContalbrigo, M.$$b8
000889109 7001_ $$0P:(DE-HGF)0$$aD'Alesio, U.$$b9
000889109 7001_ $$0P:(DE-HGF)0$$aDi Nezza, P.$$b10
000889109 7001_ $$0P:(DE-Juel1)131141$$aEngels, Ralf W.$$b11$$eCorresponding author$$ufzj
000889109 7001_ $$0P:(DE-Juel1)131170$$aGrigoryev, Kirill$$b12$$ufzj
000889109 7001_ $$0P:(DE-HGF)0$$aKeller, D.$$b13
000889109 7001_ $$0P:(DE-Juel1)162122$$aLenisa, Paolo$$b14
000889109 7001_ $$0P:(DE-HGF)0$$aLiuti, S.$$b15
000889109 7001_ $$0P:(DE-Juel1)172807$$aMetz, Lisa Maria$$b16
000889109 7001_ $$0P:(DE-HGF)0$$aMulder, P. J.$$b17
000889109 7001_ $$0P:(DE-HGF)0$$aMurgia, F.$$b18
000889109 7001_ $$0P:(DE-Juel1)131267$$aNass, Alexander$$b19$$ufzj
000889109 7001_ $$0P:(DE-HGF)0$$aPanzieri, D.$$b20
000889109 7001_ $$0P:(DE-HGF)0$$aPappalardo, L. L.$$b21
000889109 7001_ $$0P:(DE-HGF)0$$aPasquini, B.$$b22
000889109 7001_ $$0P:(DE-HGF)0$$aPisano, C.$$b23
000889109 7001_ $$0P:(DE-HGF)0$$aRadici, M.$$b24
000889109 7001_ $$0P:(DE-Juel1)131297$$aRathmann, Frank$$b25$$ufzj
000889109 7001_ $$0P:(DE-HGF)0$$aReggiani, D.$$b26
000889109 7001_ $$0P:(DE-HGF)0$$aSchlegel, M.$$b27
000889109 7001_ $$0P:(DE-HGF)0$$aScopetta, S.$$b28
000889109 7001_ $$0P:(DE-Juel1)156206$$aSteffens, Jennifer$$b29$$ufzj
000889109 7001_ $$0P:(DE-HGF)0$$aVasilyev, A.$$b30
000889109 773__ $$p10$$v1
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000889109 9141_ $$y2020
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