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References - Bogoliubov Laboratory of Theoretical Physics - JINR

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Table 1: Status <strong>of</strong> the DY experiments<br />

Experiment Status Remarks<br />

CERN: E615 Finished Fixed target mode. Unpolarized target and beam<br />

CERN: NA10,38,50 Finished Fixed target mode. Unpolarized tergat and beam<br />

FERMILAB: E886,906 Running Fixed target mode. Unpolarized target and beam<br />

RHIC: STAR,PHENIX Running up to ? Collider mode. Detector upgrade for DY studies<br />

polarized beams<br />

GSI: PANDA Plan > 2016 Fixed target mode. Unpolarized<br />

GSI: PAX Plan > 2016 Collider mode. Polarized beams.<br />

Problem with anti-proton beam polarization<br />

CERN: COMPASS Plan > 2011 Fixed target mode. Polarized beam.<br />

Valence PDFs<br />

J-PARC Plan > 2011 Fixed target mode. Unpolarized beam and<br />

target, s ∼ 60 − 100GeV 2<br />

SPASCHARM Plan ? Fixed target mode. Unpolarized beam and<br />

target, s ∼ 140GeV 2 2<br />

SPD-NICA Plan > 2014 Collider mode. s ∼ 670GeV 2 ,high<br />

luminosity, polarized proton and deuteron<br />

beams, energy scan.<br />

Table 2: The estimation <strong>of</strong> the cross-sections and number <strong>of</strong> DY events for NICA and PAX kinematics<br />

σDY total, nb L, cm −2 s −1 Thousands events<br />

PAX, √ s =14.6GeV ∼ 2 ∼ 10 3 0 ∼ 10<br />

NICA, √ s =20GeV ∼ 1 ∼ 10 3 0 ∼ 5<br />

PAX, √ s =26GeV ∼ 1.3 ∼ 10 3 0 ∼ 7<br />

– J/ψ production processes with unpolarized and single polarized pp and pd<br />

collisions, which can not be completely duplicated by other experiments (COMPASS [1],<br />

RHIC [2], PAX [3] and J-PARC [4], as it is seen from Table 1.<br />

First, at COMPASS and J-PARC the fixed target mode with unpolarized beam and<br />

polarized target is only possible. As it will be shown later, for this option the transversity<br />

and Boer-Mulders PDFs are hardly accessible for pp and pd collisions. COMPASS can<br />

reach the transversity via π − p collisions. However, in this case the unknown pion PDFs<br />

will be involved, introducing the additional theoretical uncertainty [5].<br />

Second, PAX plans to access transversity via measurements <strong>of</strong> double polarized DY<br />

processes, which will very difficult because <strong>of</strong> the antiproton polarization problems [3].<br />

Third, the RHIC experiments cover the kinematical region different from the respective<br />

region covered by NICA.<br />

Fourth, the advantage <strong>of</strong> NICA in comparison with all above mentioned experiments<br />

is that only NICA can provide an access to transversity, Boer-Mulders and Sivers PDFs<br />

for both u and d flavors.<br />

The Table 2 shows the estimation <strong>of</strong> the cross-sections and possible statistics for DY<br />

events, which can be collected with SPD at NICA during one month in comparison with<br />

those from the PAX proposal.<br />

To estimate the possible precision <strong>of</strong> measurements <strong>of</strong> the asymmetries the set <strong>of</strong><br />

267

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