Abstract

A measurement of $W^\pm$ boson production in lead-lead collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV is reported using data recorded by the ATLAS experiment at the LHC in 2015, corresponding to a total integrated luminosity of $0.49\;\mathrm{nb^{-1}}$. The $W^\pm$ bosons are reconstructed in the electron or muon leptonic decay channels. Production yields of leptonically decaying $W^\pm$ bosons, normalised by the total number of minimum-bias events and the nuclear thickness function, are measured within a fiducial region defined by the detector acceptance and the main kinematic requirements. These normalised yields are measured separately for $W^+$ and $W^-$ bosons, and are presented as a function of the absolute value of pseudorapidity of the charged lepton and of the collision centrality. The lepton charge asymmetry is also measured as a function of the absolute value of lepton pseudorapidity. In addition, nuclear modification factors are calculated using the $W^\pm$ boson production cross-sections measured in $pp$ collisions. The results are compared with predictions based on next-to-leading-order calculations with CT14 parton distribution functions as well as with predictions obtained with the EPPS16 and nCTEQ15 nuclear parton distribution functions. No dependence of normalised production yields on centrality and a good agreement with predictions are observed for mid-central and central collisions. For peripheral collisions, the data agree with predictions within 1.7 (0.9) standard deviations for $W^-$ ($W^+$) bosons.

Figure 10a

Data from Figure 10 (left).

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Differential normalised production yields for $W^+$ bosons as a function of absolute pseudorapidity of the charged lepton for the combined...
Figure 10b

Data from Figure 10 (right).

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Differential normalised production yields for $W^-$ bosons as a function of absolute pseudorapidity of the charged lepton for the combined...
Figure 11

Data from Figure 11.

10.17182/hepdata.91908.v1/t3

Combined result for lepton charge asymmetry.
Figure 12

Data from Figure 12.

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Normalised production yields of $W^+$ and $W^-$ bosons as a function of $⟨N_{\mathrm{part}}⟩$ shown for the combination of electron and...
Figure 13a

Data from Figure 13 (left).

10.17182/hepdata.91908.v1/t5

Normalised production yields for $W^+$ bosons as a function of $⟨N_{\mathrm{part}}⟩$ for geometric parameters obtained with the MCGlauber v2.4 and...
Figure 13b

Data from Figure 13 (right).

10.17182/hepdata.91908.v1/t6

Normalised production yields for $W^-$ bosons as a function of $⟨N_{\mathrm{part}}⟩$ for geometric parameters obtained with the MCGlauber v2.4 and...
Figure 14

Data from Figure 14.

10.17182/hepdata.91908.v1/t7

Nuclear modification factor $R_{\mathrm{AA}}$ obtained from the fiducial $W^+$ and $W^-$ boson production yields as a function of $⟨N_{\mathrm{part}}⟩$.
Auxiliary 1

The covariance matrix for the data from Figure 10.

10.17182/hepdata.91908.v1/t8

The covariance matrix of the differential normalised production yields for $W^+$ bosons. Systematic uncertainties related to $T_{\mathrm{AA}}$ (1.6%) are not...
Auxiliary 2

The covariance matrix for the data from Figure 10.

10.17182/hepdata.91908.v1/t9

The covariance matrix of the differential normalised production yields for $W^-$ bosons. Systematic uncertainties related to $T_{\mathrm{AA}}$ (1.6%) are not...
Auxiliary 3

The covariance matrix for the data from Figure 11.

10.17182/hepdata.91908.v1/t10

The covariance matrix of the lepton charge asymmetry.

Figure 10a

Figure 10b

Figure 11

Figure 12

Figure 13a

Figure 13b

Figure 14

Auxiliary 1

Auxiliary 2

Auxiliary 3

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