Abstract (data abstract)

Measurement of W-boson production at forward rapidity in p-Pb collisions at $\sqrt{s_{NN}} =$ 8.16 TeV and Pb-Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV. The measurement is done in the muon decay channel. The fiducial region is defined by - $\eta$ (pseudorapidity) of muons in $-4.0 < \eta < -2.5$ in the laboratory frame and ALICE reference system - $p_{\rm T}$ (transverse momentum) of muons larger than 10 GeV/$c$ For Pb-Pb collisions the laboratory frame and cms frame coincide. For p-Pb collisions the nucleon-nucleon cms is boosted with respect to the laboratory frame by $\Delta y_{cms} = \pm 0.465$

Cross section in p-Pb

Data from Table 4

10.17182/hepdata.133034.v1/t1

d$\sigma$ / d$y$ of muons from W decays in p-Pb, in full fiducial region
Cross section in p-Pb, rapidity bins

Data from Fig. 3

10.17182/hepdata.133034.v1/t2

d$\sigma$ / d$y$ of muons from W decays in p-Pb, in rapidity bins
Lepton-charge asymmetry in p-Pb

Data from Eq. (5)

10.17182/hepdata.133034.v1/t3

Lepton-charge asymmetry $A_{ch} = \frac{N_{\mu^+} - N_{\mu^-}}{N_{\mu^+} + N_{\mu^-}}$ in p-Pb
Lepton-charge asymmetry in p-Pb, rapidity bins

Data from Fig. 5

10.17182/hepdata.133034.v1/t4

Lepton-charge asymmetry $A_{ch} = \frac{N_{\mu^+} - N_{\mu^-}}{N_{\mu^+} + N_{\mu^-}}$ in p-Pb, in rapidity bins
Nuclear modification factor in p-Pb

Data from Table 5

10.17182/hepdata.133034.v1/t5

Nuclear modification factor $R_{pPb} = \frac{1}{208}\frac{\sigma_{pPb}}{\sigma_{pp}}$ in p-Pb. pp reference from POWHEG+CT10 calculations.
Nuclear modification factor in p-Pb, rapidity bins

Data from Fig. 6

10.17182/hepdata.133034.v1/t6

Nuclear modification factor $R_{pPb} = \frac{1}{208}\frac{\sigma_{pPb}}{\sigma_{pp}}$ in p-Pb, in rapidity bins. pp reference from POWHEG+CT10 calculations.
Multiplicity dependent cross section in p-Pb

Data from Fig. 7

10.17182/hepdata.133034.v1/t7

Cross section vs. multiplicity, scaled with the average number of binary nucleon-nucleon collisions $< N^{\rm mult}_{\rm coll} >$ in p-Pb
Cross section in Pb-Pb

Data from Fig. 8

10.17182/hepdata.133034.v1/t8

$\sigma$ of muons from W decays in Pb-Pb with 0-90% centrality
Lepton charge asymmetry in Pb-Pb

Data from Fig. 8

10.17182/hepdata.133034.v1/t9

Lepton-charge asymmetry $A_{ch} = \frac{N_{\mu^+} - N_{\mu^-}}{N_{\mu^+} + N_{\mu^-}}$ in Pb-Pb with 0-90% centrality
TAA-scaled yield in Pb-Pb

Data from Fig. 10

10.17182/hepdata.133034.v1/t10

Yield of muons from W decays per Minimum Bias (MB) event scaled with the average nuclear overlap $< T_{\rm AA}...
Nuclear modification factor in Pb-Pb

Data from Fig. 12

10.17182/hepdata.133034.v1/t11

Nuclear modification factor $R_{PbPb} = \frac{1}{< T_{\rm AA} >} \frac{N^{\rm MB}_{\mu^\pm \leftarrow W^\pm}}{\sigma_{pp}}$ in Pb-Pb. pp reference from POWHEG+CT10 calculations.
Nuclear modification factor in Pb-Pb in centrality bins

Data from Fig. 12

10.17182/hepdata.133034.v1/t12

Nuclear modification factor $R_{PbPb} = \frac{1}{< T_{\rm AA} >} \frac{N^{\rm MB}_{\mu^\pm \leftarrow W^\pm}}{\sigma_{pp}}$ in Pb-Pb in centrality bins. pp reference...

Cross section in p-Pb

Cross section in p-Pb, rapidity bins

Lepton-charge asymmetry in p-Pb

Lepton-charge asymmetry in p-Pb, rapidity bins

Nuclear modification factor in p-Pb

Nuclear modification factor in p-Pb, rapidity bins

Multiplicity dependent cross section in p-Pb

Cross section in Pb-Pb

Lepton charge asymmetry in Pb-Pb

TAA-scaled yield in Pb-Pb

Nuclear modification factor in Pb-Pb

Nuclear modification factor in Pb-Pb in centrality bins

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