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Aidala, C.; Akiba, Y.; Alfred, M.; Andrieux, V.; Apadula, N.; Asano, H.; Azmoun, B.; Babintsev, V.; Bagoly, A.; Bandara, N. S.; Barish, K. N.; Bathe, S.; Bazilevsky, A.; Beaumier, M.; Belmont, R.; Berdnikov, A.; Berdnikov, Y.; Blau, D.; Boër, M.; Bok, Jeongsu; Brooks, M. L.; Bryslawskyj, J.; Bumazhnov, V.; Campbell, S.; Roman, V. Canoa; Cervantes, R.; Y., C.; Chiu, M.; Choi, I. J.; Choi, J.; Citron, Z. H.; Connors, M.; Cronin, N.; Csanád, M.; Csörgő, T.; Danley, T. W.; Daugherity, M.; David, G.; DeBlasio, K.; Dehmelt, K.; Denisov, A.; Deshpande, A.; Desmond, E. J.; Dion, A.; Dixit, Dhruv Utpalkumar; H., J.; Drees, A.; Drees, K. A.; Durham, J. M.; Durum, A.; Enokizono, A.; En’yo, H.; Esumi, S.; Fadem, B.; Fan, W.; Feege, N.; Fields, D. E.; Finger, M.; Fokin, S.; Frantz, J. E.; Franz, A.; Frawley, A. D.; Fukuda, Y.; Gal, C.; Gallus, P.; Garg, P.; Ge, H.; Giordano, F.; Goto, Y.; Grau, N.; Greene, S.; Perdekamp, M. Grosse; Gunji, T.; Guragain, H.; Hachiya, T.; Haggerty, J. S.; Hahn, K. I.; Hamagaki, H.; Hamilton, H. F.; Han, S. Y.; Hanks, J.; Hasegawa, S.; Haseler, T. O. S.; He, X.; Hemmick, T. K.; Hill, J. C.; Hill, K. K.; Hodges, A.; Hollis, R. S.; Homma, K.; Hong, B.; Hoshino, T.; Hotvedt, N.; Huang, J.; Huang, S.; Imai, K.; Inaba, M.; Iordanova, A.; Isenhower, D.; Ivanishchev, D.; Jacak, B. V.; Jezghani, M.; Ji, Z.; Jiang, X.; Johnson, B. M.; Jouan, D.; Jumper, D. S.; Kang, J. H.; Kapukchyan, D.; Karthas, S.; Kawall, D.; Kazantsev, A. V.; Khachatryan, V.; Khanzadeev, A.; Kim, C.; Kim, E.-J.; Kim, M.; Kincses, D.; Kistenev, E.; Klatsky, J.; Kline, P.; Koblesky, T.; Kotov, D.; Kudo, S.; Kurita, K.; Kwon, Y.; Lajoie, J. G.; Lebedev, A.; Lee, S.; Lee, S. H.; Leitch, M. J.; Leung, Y. H.; Lewis, N. A.; Li, X.; Lim, Sanghoon; Liu, M. X.; Loggins, V.-R.; Lökòs, S.; Lovasz, K.; Lynch, D.; Majoros, T.; Makdisi, Y. I.; Makek, M.; Manko, V.; Mannel, E.; McCumber, M.; McGaughey, P. L.; McGlinchey, D.; McKinney, C.; Mendoza, M.; Mignerey, A. C.; Mihalik, D. E.; Milov, A.; Mishra, D.; Mitchell, J. T.; Mitsuka, G.; Miyasaka, S.; Mizuno, S.; Montuenga, P.; Moon, T.; Morrison, D. P.; Morrow, S. I.; Murakami, T.; Murata, J.; Nagai, K.; Nagashima, K.; Nagashima, T.; Nagle, J. L.; Nagy, M. I.; Nakagawa, I.; Nakano, K.; Nattrass, C.; Niida, T.; Nouicer, R.; Novák, T.; Novitzky, N.; Nyanin, A. S.; O’Brien, E.; Ogilvie, C. A.; Koop, J. D. Orjuela; Osborn, J. D.; Öskarsson, A.; Ottino, G. J.; Ozawa, K.; Pantuev, V.; Papavassiliou, V.; Park, J. S.; Park, S.; Pate, S. F.; Patel, M.; Peng, W.; Perepelitsa, D. V.; Perera, G. D. N.; Peressounko, D. Yu.; PerezLara, C. E.; Perry, J.; Petti, R.; Phipps, M. W.; Pinkenburg, C.; Pisani, R. P.; Purschke, M. L.; Radzevich, P. V.; Read, K. F.; Reynolds, D.; Riabov, V.; Riabov, Y.; Richford, D.; Rinn, Timothy Thomas; Rolnick, S. D.; Rosati, M.; Rowan, Z.; Runchey, J.; Safonov, A.; Sakaguchi, T.; Sako, H.; Samsonov, V.; Sarsour, M.; Sato, Susumu; Schaefer, B.; Schmoll, B. K.; Sedgwick, K.; Seidl, R.; Sen, A.; Seto, R.; Sexton, A.; Sharma, D.; Shein, I.; Shibata, T. A.; Shigaki, K.; Shimomura, M.; Shioya, T.; Shukla, P.; Sickles, A. M.; Silva, C. L.; Silvermyr, D.; Singh, B. K.; Singh, C. P.; Singh, V. K.; Skoby, M. J.; Slunečka, M.; Snowball, M.; Soltz, R. A.; Sondheim, W. E.; Sörensen, S.; Sourikova, I. V.; Stankus, P. W.; Stoll, S. P.; Sugitate, T.; Sukhanov, A.; Sumita, T.; Sun, J.; Sun, Z.; Sziklai, J.; Tanida, K.; Tannenbaum, M. J.; Tarafdar, S.; Taranenko, A.; Tarnai, G.; Tieulent, R.; Timilsina, A.; Todoroki, T.; Tomášek, M.; Towell, C. L.; Towell, R. S.; Tserruya, I.; Ueda, Y.; Ujvári, B.; Hecke, H. W. van; Velkovska, J.; Virius, M.; Vrba, V.; Vukman, N.; Wang, X. R.; Watanabe, Y.; Wong, C. P.; Woody, C. L.; Xu, C.; Xu, Qingyang; Xue, L.; Yalcin, S.; Yamaguchi, Y.; Yamamoto, Hiroshi; Yanovich, A.; Yoo, J.; Yoon, I.; Yu, H.; Yushmanov, I. E.; Zajc, W. A.; Zelenski, A.; Zharko, S.; Zou, L.

doi:10.1103/physrevd.98.012006

Cited by 21 publications

(19 citation statements)

References 62 publications

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“…Let us recall that nearly nothing is known from the experimental side about the gluon Sivers function (see e.g. the review [52] and recent measurements [26,53,54,55]). The polarisation of not only hydrogen but also deuterium and helium targets allows for an even more ambitious spin program bearing on the neutron and spin 1 bound states (see e.g.…”

Section: Unraveling the Nucleon Spinmentioning

confidence: 99%

“…33(a) shows the estimated uncertainties at AFTER@LHC for the Υ A N as a function of x F in pp collisions at √ s = 115 GeV, while Fig. 33(b) shows the projected uncertainties for J/ψ compared to already existing measurements at √ s = 200 GeV [26,55]. With the expected charmonium yields [293] these results are only limited by the systematic uncertainties, and can thus give a very precise access to the gluon content of the proton over a much wider x range than at RHIC.…”

Section: Gluon Sivers Effectmentioning

confidence: 99%

“…In any case, the precise measurements performed within the AFTER@LHC programme can give us a handle to discriminate the discussed scenarios. [26,55] and predictions by the generalised parton model (GPM) and the color gauge invariant (CGI) version of the GPM model [283]. The quarkonium states are assumed to be measured in a di-muon channel with a LHCb-like detector.…”

Section: Gluon Sivers Effectmentioning

confidence: 99%

“…The production of C-even states can fruitfully be investigated [58,297,298,59]. With an LHCb-like detector 41 Figure 34: Statistical-precision projections for J/ψ A N as a function of x F compared to the existing measurements [26,55] for AFTER@ALICE µ . The J/ψ di-muon spectrum is assumed to be measured in the Muon Spectrometer of the ALICE detector.…”

Section: Gluon Sivers Effectmentioning

confidence: 99%

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Studies of various physics effects on an on-axis LHCD experiment using numerical tools

et al. 2018

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We review the context, the motivations and the expected performances of a comprehensive and ambitious fixed-target program using the multi-TeV proton and ion LHC beams. We also provide a detailed account of the different possible technical implementations ranging from an internal wire target to a full dedicated beam line extracted with a bent crystal. The possibilities offered by the use of the ALICE and LHCb detectors in the fixed-target mode are also reviewed.

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Section: Unraveling the Nucleon Spinmentioning

confidence: 99%

Section: Gluon Sivers Effectmentioning

confidence: 99%

Section: Gluon Sivers Effectmentioning

confidence: 99%

Section: Gluon Sivers Effectmentioning

confidence: 99%

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Studies of various physics effects on an on-axis LHCD experiment using numerical tools

et al. 2018

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“…Maximized and constrained J/ψ Sivers SSAs for the GPM and CGI-PGM, compared to RHIC data[8] (upper panels) and predicted for LHC fixed-target energies (lower panels). See text for details.…”

mentioning

confidence: 99%

Quarkonium production and TMDs at LHC

Murgia¹,

D’Alesio²,

Pisano³

et al. 2019

Proceedings of XXVII International Workshop on Deep-Inelastic Scattering and Related Subjects — PoS(DIS2019)

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In this contribution we briefly discuss an ongoing phenomenological programme on quarkonium production in unpolarized and polarized proton-proton collisions in a fixed target setup at LHCb, the LHCSpin project. Within a TMD approach, we aim at considering in particular: the relative role of the NRQCD color-singlet and color-octet production mechanisms, both for unpolarized and polarized quarkonium production; the study of azimuthal and transverse single-spin asymmetries as a phenomenological tool for learning about the almost unknown gluon Sivers function; the role of initial-and final-state interactions for spin asymmetries.

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