Production of inclusive $\Upsilon$(1S) and $\Upsilon$(2S) in p-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV

Abelev, Betty Bezverkhny; Adam, Jaroslav; Adamova, Dagmar; Aggarwal, Madan Mohan; Aglieri Rinella, Gianluca; Agnello, Michelangelo; Agostinelli, Andrea; Agrawal, Neelima; Ahammed, Zubayer; Ahmad, Nazeer

doi:10.1016/j.physletb.2014.11.041

Production of inclusive $\Upsilon$ (1S) and $\Upsilon$ (2S) in p-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV

ALICE

Collaboration

Oct 8, 2014

13 pages

Published in:

Phys.Lett.B 740 (2015) 105-117

Published: Nov 19, 2014

e-Print:

1410.2234 [nucl-ex]

DOI:

10.1016/j.physletb.2014.11.041

Report number:

CERN-PH-EP-2014-196,
ALICE-PUBLIC-2014-002

Experiments:

CERN-LHC-ALICE

View in:

datasets

reference search103 citations

Citations per year

Abstract: (Elsevier)

We report on the production of inclusive ϒ (1S) and ϒ (2S) in p–Pb collisions at sNN=5.02 TeV at the LHC. The measurement is performed with the ALICE detector at backward ( −4.46

Note:

23 pages, 5 captioned figures, 1 table, authors from page 18, published version, figures at http://aliceinfo.cern.ch/ArtSubmission/node/824

shadowing
p nucleus: scattering
lead
rapidity dependence
nucleon nucleon
CERN LHC Coll
Upsilon(9460): suppression
parton: energy loss
ALICE
nuclear matter: effect

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Figures(8)

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Production of inclusive Υ\UpsilonΥ(1S) and Υ\UpsilonΥ(2S) in p-Pb collisions at sNN=5.02\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}sNN​​=5.02 TeV

Citations per year

Production of inclusive $\Upsilon$ (1S) and $\Upsilon$ (2S) in p-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV