The systematic uncertainty on the unfolded distribution as a function of minimax-mbl, broken down by components.

The covariance matrix for the unfolded, normalized data in bins of minimax-mbl shown in Figure 2. Redundant entries are suppressed.

Leading lepton transverse momentum distribution for events passing the signal selection in bins of minimax-mbl. The data here are not unfolded.

Sub-leading lepton transverse momentum distribution for events passing the signal selection in bins of minimax-mbl. The data here are not unfolded.

Leading lepton pseudorapidity distribution for events passing the signal selection in bins of minimax-mbl. The data here are not unfolded.

Sub-leading lepton pseudorapidity distribution for events passing the signal selection in bins of minimax-mbl. The data here are not unfolded.

Leading b-jet transverse momentum distribution for events passing the signal selection in bins of minimax-mbl. The data here are not unfolded.

Sub-leading b-jet transverse momentum distribution for events passing the signal selection in bins of minimax-mbl. The data here are not unfolded.

Leading b-jet pseudorapidity distribution for events passing the signal selection in bins of minimax-mbl. The data here are not unfolded.

Sub-leading b-jet pseudorapidity distribution for events passing the signal selection in bins of minimax-mbl. The data here are not unfolded.

The detector-level minimax-m(bl) distribution for events entering the Z+jets control region.

The detector-level minimax-m(bl) distribution for events entering the same-sign lepton control region.

Normalized differential cross section, $(1/\sigma_\text{fid})d\sigma_\text{fid}/d\log(m_{bb}/p_\text{T})$, as a function of $\log(m_{bb}/p_\text{T})$ for $m_{bb}$ the invariant mass of the two b-jets.

Measured and expected differential cross-section $\text{d}\sigma / \text{d} m_{4l}$ as a function of $m_{4l}$ in bin of 50$< p_{T}^{4l} <$100 GeV

Measured and expected differential cross-section $\text{d}\sigma / \text{d} m_{4l}$ as a function of $m_{4l}$ in bin of 100$< p_{T}^{4l} <$600 GeV

Measured and expected double differential cross-section $\text{d}\sigma / \text{d} m_{4l}$ as a function of $m_{4l}$ in bin of 0.0$< y_{4l} <$0.4

Measured and expected double differential cross-section $\text{d}\sigma / \text{d} m_{4l}$ as a function of $m_{4l}$ in bin of 0.4$< y_{4l} <$0.8

Measured and expected double differential cross-section $\text{d}\sigma / \text{d} m_{4l}$ as a function of $m_{4l}$ in bin of 0.8$< y_{4l} <$1.2

Measured and expected double differential cross-section $\text{d}\sigma / \text{d} m_{4l}$ as a function of $m_{4l}$ in bin of 1.2$< y_{4l} <$2.5

Measured and expected double differential cross-section $\text{d}\sigma / \text{d} m_{4l}$ as a function of $m_{4l}$ for MELA$<$1.4 bin

Measured and expected double differential cross-section $\text{d}\sigma / \text{d} m_{4l}$ as a function of $m_{4l}$ for MELA$>$1.4 bin

Measured and expected double differential cross-section $\text{d}\sigma / \text{d} m_{4l}$ as a function of $m_{4l}$ for $\mu\mu\mu\mu$ events

Measured and expected double differential cross-section $\text{d}\sigma / \text{d} m_{4l}$ as a function of $m_{4l}$ for $eeee$ events

Measured and expected double differential cross-section $\text{d}\sigma / \text{d} m_{4l}$ as a function of $m_{4l}$ for $ee\mu\mu$ events

Systematic covariance matrix for the differential $m_{4l}$ distribution.

Statistical covariance matrix for the differential $m_{4l}$ distribution.

Background covariance matrix for the differential $m_{4l}$ distribution.

Systematic covariance matrix for the differential $m_{4l}$-$p_{T}^{4l}$ distribution.<br><br> Bins labelled 1-9 correspond to the 0$< p_{T}^{4l} < $20 GeV bin with $m_{4l}$ values as listed in Table 2.<br> Bins labelled 10-16 correspond to the 20$< p_{T}^{4l} <$50 GeV bin with $m_{4l}$ values as listed in Table 3.<br> Bins labelled 17-23 correspond to the 50$< p_{T}^{4l} <$100 GeV bin with $m_{4l}$ values as listed in Table 4.<br> Bins labelled 24-30 correspond to the 100$< p_{T}^{4l} <$600 GeV bin with $m_{4l}$ values as listed in Table 5.

Statistical covariance matrix for the differential $m_{4l}$-$p_{T}^{4l}$ distribution. <br><br> Bins labelled 1-9 correspond to the 0$< p_{T}^{4l} < $20 GeV bin with $m_{4l}$ values as listed in Table 2.<br> Bins labelled 10-16 correspond to the 20$< p_{T}^{4l} <$50 GeV bin with $m_{4l}$ values as listed in Table 3.<br> Bins labelled 17-23 correspond to the 50$< p_{T}^{4l} <$100 GeV bin with $m_{4l}$ values as listed in Table 4.<br> Bins labelled 24-30 correspond to the 100$< p_{T}^{4l} <$600 GeV bin with $m_{4l}$ values as listed in Table 5.

Background covariance matrix for the differential $m_{4l}$-$p_{T}^{4l}$ distribution. <br><br> Bins labelled 1-9 correspond to the 0$< p_{T}^{4l} < $20 GeV bin with $m_{4l}$ values as listed in Table 2.<br> Bins labelled 10-16 correspond to the 20$< p_{T}^{4l} <$50 GeV bin with $m_{4l}$ values as listed in Table 3.<br> Bins labelled 17-23 correspond to the 50$< p_{T}^{4l} <$100 GeV bin with $m_{4l}$ values as listed in Table 4.<br> Bins labelled 24-30 correspond to the 100$< p_{T}^{4l} <$600 GeV bin with $m_{4l}$ values as listed in Table 5.

Systematic covariance matrix for the differential $m_{4l}$-$y_{4l}$ distribution. <br><br> Bins labelled 1-9 correspond to the 0.0$< y_{4l} < $0.4 bin with $m_{4l}$ values as listed in Table 6.<br> Bins labelled 10-18 correspond to the 0.4$< y_{4l} <$0.8 bin with $m_{4l}$ values as listed in Table 7.<br> Bins labelled 19-26 correspond to the 0.8$< y_{4l} <$1.2 bin with $m_{4l}$ values as listed in Table 8.<br> Bins labelled 27-34 correspond to the 1.2$< y_{4l} <$2.5 bin with $m_{4l}$ values as listed in Table 9.

Statistical covariance matrix for the differential $m_{4l}$-$y_{4l}$ distribution. <br><br> Bins labelled 1-9 correspond to the 0.0$< y_{4l} < $0.4 bin with $m_{4l}$ values as listed in Table 6.<br> Bins labelled 10-18 correspond to the 0.4$< y_{4l} <$0.8 bin with $m_{4l}$ values as listed in Table 7.<br> Bins labelled 19-26 correspond to the 0.8$< y_{4l} <$1.2 bin with $m_{4l}$ values as listed in Table 8.<br> Bins labelled 27-34 correspond to the 1.2$< y_{4l} <$2.5 bin with $m_{4l}$ values as listed in Table 9.

Background covariance matrix for the differential $m_{4l}$-$y_{4l}$ distribution. <br><br> Bins labelled 1-9 correspond to the 0.0$< y_{4l} < $0.4 bin with $m_{4l}$ values as listed in Table 6.<br> Bins labelled 10-18 correspond to the 0.4$< y_{4l} <$0.8 bin with $m_{4l}$ values as listed in Table 7.<br> Bins labelled 19-26 correspond to the 0.8$< y_{4l} <$1.2 bin with $m_{4l}$ values as listed in Table 8.<br> Bins labelled 27-34 correspond to the 1.2$< y_{4l} <$2.5 bin with $m_{4l}$ values as listed in Table 9.

Systematic covariance matrix for the differential $m_{4l}$-MELA distribution. <br><br> Bins labelled 1-7 correspond to the MELA$<$ 0.4 bin with $m_{4l}$ values as listed in Table 10.<br> Bins labelled 8-12 correspond to the MELA$>$ 0.4 bin with $m_{4l}$ values as listed in Table 11.

Statistical covariance matrix for the differential $m_{4l}$-MELA distribution. <br><br> Bins labelled 1-7 correspond to the MELA$<$ 0.4 bin with $m_{4l}$ values as listed in Table 10.<br> Bins labelled 8-12 correspond to the MELA$>$ 0.4 bin with $m_{4l}$ values as listed in Table 11.

Background covariance matrix for the differential $m_{4l}$-MELA distribution. <br><br> Bins labelled 1-7 correspond to the MELA$<$ 0.4 bin with $m_{4l}$ values as listed in Table 10.<br> Bins labelled 8-12 correspond to the MELA$>$ 0.4 bin with $m_{4l}$ values as listed in Table 11.

Systematic covariance matrix for the differential $m_{4l}$-lepton flavour distribution. <br><br> Bins labelled 1-9 correspond to $\mu\mu\mu\mu$ events with $m_{4l}$ values as listed in Table 12.<br> Bins labelled 10-18 correspond to $eeee$ events with $m_{4l}$ values as listed in Table 13.<br> Bins labelled 19-27 correspond to $\mu\mu\mu\mu$ events with $m_{4l}$ values as listed in Table 14.<br>

Statistical covariance matrix for the differential $m_{4l}$-lepton flavour distribution. <br><br> Bins labelled 1-9 correspond to $\mu\mu\mu\mu$ events with $m_{4l}$ values as listed in Table 12.<br> Bins labelled 10-18 correspond to $eeee$ events with $m_{4l}$ values as listed in Table 13.<br> Bins labelled 19-27 correspond to $\mu\mu\mu\mu$ events with $m_{4l}$ values as listed in Table 14.<br>

Background covariance matrix for the differential $m_{4l}$-lepton flavour distribution. <br><br> Bins labelled 1-9 correspond to $\mu\mu\mu\mu$ events with $m_{4l}$ values as listed in Table 12.<br> Bins labelled 10-18 correspond to $eeee$ events with $m_{4l}$ values as listed in Table 13.<br> Bins labelled 19-27 correspond to $\mu\mu\mu\mu$ events with $m_{4l}$ values as listed in Table 14.<br>

Dijet mass distribution for the b-tagged category. Data, estimated background and uncertainties are shown. Events are collected using the combined trigger and contain a $E_T^{\gamma} > 95$ GeV photon and two $p_T^{jet} > 65$ GeV jets.

Upper limits on Gaussian-shape contributions to the dijet mass distributions from the flavour-inclusive category and masses below 450 GeV, for which the single-photon trigger was used.

Upper limits on Gaussian-shape contributions to the dijet mass distributions from the flavour-inclusive category and masses above 450 GeV, for which the combined trigger was used.

Upper limits on Gaussian-shape contributions to the dijet mass distributions from the b-tagged category and masses below 450 GeV, for which the single-photon trigger was used.

Upper limits on Gaussian-shape contributions to the dijet mass distributions from the b-tagged category and masses above 450 GeV, for which the combined trigger was used.

Kinematic acceptance values predicted for the $Z'$ model as a function of mass $m_{Z'}$ for the flavour-inclusive category using the single-photon trigger.

Kinematic acceptance values predicted for the $Z'$ model as a function of mass $m_{Z'}$ for the flavour-inclusive category using the combined trigger.

Kinematic acceptance values predicted for the $Z'$ model as a function of mass $m_{Z'}$ for the b-tagged category using the single-photon trigger.

Kinematic acceptance values predicted for the $Z'$ model as a function of mass $m_{Z'}$ for the b-tagged category using the combined trigger.

Reconstruction efficiency for $Z'$ model, flavour inclusive category, single-photon trigger.

Reconstruction efficiency for $Z'$ model, flavour inclusive category, combined trigger.

Reconstruction efficiency for $Z'$ model, b-tagged category, single-photon trigger.

Reconstruction efficiency for $Z'$ model, b-tagged category, combined trigger.

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (240<=Nch<260)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (220<=Nch<240)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (220<=Nch<240)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (200<=Nch<220)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (200<=Nch<220)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (180<=Nch<200)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (180<=Nch<200)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (160<=Nch<180)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (160<=Nch<180)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (140<=Nch<160)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (140<=Nch<160)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (120<=Nch<140)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (120<=Nch<140)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (100<=Nch<120)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (100<=Nch<120)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (80<=Nch<100)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (80<=Nch<100)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (60<=Nch<80)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (60<=Nch<80)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (40<=Nch<60)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (40<=Nch<60)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (20<=Nch<40)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (20<=Nch<40)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (10<=Nch<20)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (10<=Nch<20)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (260<=Nch<300)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (260<=Nch<300)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (240<=Nch<260)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (240<=Nch<260)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (220<=Nch<240)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (220<=Nch<240)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (200<=Nch<220)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (200<=Nch<220)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (180<=Nch<200)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (180<=Nch<200)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (160<=Nch<180)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (160<=Nch<180)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (140<=Nch<160)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (140<=Nch<160)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (120<=Nch<140)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (120<=Nch<140)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (100<=Nch<120)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (100<=Nch<120)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (80<=Nch<100)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (80<=Nch<100)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (60<=Nch<80)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (60<=Nch<80)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (40<=Nch<60)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (40<=Nch<60)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (20<=Nch<40)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (20<=Nch<40)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (10<=Nch<20)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (10<=Nch<20)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (260<=Nch<300)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (260<=Nch<300)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (240<=Nch<260)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (240<=Nch<260)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (220<=Nch<240)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (220<=Nch<240)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (200<=Nch<220)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (200<=Nch<220)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (180<=Nch<200)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (180<=Nch<200)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (160<=Nch<180)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (160<=Nch<180)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (140<=Nch<160)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (140<=Nch<160)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (120<=Nch<140)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (120<=Nch<140)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (100<=Nch<120)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (100<=Nch<120)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (80<=Nch<100)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (80<=Nch<100)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (60<=Nch<80)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (60<=Nch<80)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (40<=Nch<60)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (40<=Nch<60)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (20<=Nch<40)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (20<=Nch<40)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (10<=Nch<20)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (10<=Nch<20)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (260<=Nch<300)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (260<=Nch<300)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (240<=Nch<260)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (240<=Nch<260)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (220<=Nch<240)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (220<=Nch<240)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (200<=Nch<220)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (200<=Nch<220)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (180<=Nch<200)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (180<=Nch<200)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (160<=Nch<180)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (160<=Nch<180)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (140<=Nch<160)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (140<=Nch<160)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (120<=Nch<140)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (120<=Nch<140)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (100<=Nch<120)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (100<=Nch<120)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (80<=Nch<100)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (80<=Nch<100)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (60<=Nch<80)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (60<=Nch<80)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (40<=Nch<60)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (40<=Nch<60)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (20<=Nch<40)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (20<=Nch<40)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (10<=Nch<20)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (10<=Nch<20)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (260<=Nch<300)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (260<=Nch<300)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (240<=Nch<260)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (240<=Nch<260)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (220<=Nch<240)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (220<=Nch<240)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (200<=Nch<220)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (200<=Nch<220)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (180<=Nch<200)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (180<=Nch<200)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (160<=Nch<180)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (160<=Nch<180)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (140<=Nch<160)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (140<=Nch<160)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (120<=Nch<140)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (120<=Nch<140)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (100<=Nch<120)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (100<=Nch<120)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (80<=Nch<100)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (80<=Nch<100)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (60<=Nch<80)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (60<=Nch<80)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (40<=Nch<60)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (40<=Nch<60)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (20<=Nch<40)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (20<=Nch<40)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (10<=Nch<20)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (10<=Nch<20)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (260<=Nch<300)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (260<=Nch<300)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (240<=Nch<260)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (240<=Nch<260)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (220<=Nch<240)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (220<=Nch<240)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (200<=Nch<220)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (200<=Nch<220)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (180<=Nch<200)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (180<=Nch<200)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (160<=Nch<180)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (160<=Nch<180)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (140<=Nch<160)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (140<=Nch<160)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (120<=Nch<140)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (120<=Nch<140)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (100<=Nch<120)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (100<=Nch<120)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (80<=Nch<100)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (80<=Nch<100)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (60<=Nch<80)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (60<=Nch<80)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (40<=Nch<60)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (40<=Nch<60)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (20<=Nch<40)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (20<=Nch<40)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (10<=Nch<20)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (10<=Nch<20)

C_N(eta_1, eta_2) for pp, pT>0.5GeV, (140<=Nch<160)

C_N(eta_1, eta_2) for pp, pT>0.2GeV, (140<=Nch<160)

C_N(eta_1, eta_2) for pp, pT>0.5GeV, (120<=Nch<140)

C_N(eta_1, eta_2) for pp, pT>0.2GeV, (120<=Nch<140)

C_N(eta_1, eta_2) for pp, pT>0.5GeV, (100<=Nch<120)

C_N(eta_1, eta_2) for pp, pT>0.2GeV, (100<=Nch<120)

C_N(eta_1, eta_2) for pp, pT>0.5GeV, (80<=Nch<100)

C_N(eta_1, eta_2) for pp, pT>0.2GeV, (80<=Nch<100)

C_N(eta_1, eta_2) for pp, pT>0.5GeV, (60<=Nch<80)

C_N(eta_1, eta_2) for pp, pT>0.2GeV, (60<=Nch<80)

C_N(eta_1, eta_2) for pp, pT>0.5GeV, (40<=Nch<60)

C_N(eta_1, eta_2) for pp, pT>0.2GeV, (40<=Nch<60)

C_N(eta_1, eta_2) for pp, pT>0.5GeV, (20<=Nch<40)

C_N(eta_1, eta_2) for pp, pT>0.2GeV, (20<=Nch<40)

C_N(eta_1, eta_2) for pp, pT>0.5GeV, (10<=Nch<20)

C_N(eta_1, eta_2) for pp, pT>0.2GeV, (10<=Nch<20)

SRC(eta_1, eta_2) for pp, pT>0.5GeV, (140<=Nch<160)

SRC(eta_1, eta_2) for pp, pT>0.2GeV, (140<=Nch<160)

SRC(eta_1, eta_2) for pp, pT>0.5GeV, (120<=Nch<140)

SRC(eta_1, eta_2) for pp, pT>0.2GeV, (120<=Nch<140)

SRC(eta_1, eta_2) for pp, pT>0.5GeV, (100<=Nch<120)

SRC(eta_1, eta_2) for pp, pT>0.2GeV, (100<=Nch<120)

SRC(eta_1, eta_2) for pp, pT>0.5GeV, (80<=Nch<100)

SRC(eta_1, eta_2) for pp, pT>0.2GeV, (80<=Nch<100)

SRC(eta_1, eta_2) for pp, pT>0.5GeV, (60<=Nch<80)

SRC(eta_1, eta_2) for pp, pT>0.2GeV, (60<=Nch<80)

SRC(eta_1, eta_2) for pp, pT>0.5GeV, (40<=Nch<60)

SRC(eta_1, eta_2) for pp, pT>0.2GeV, (40<=Nch<60)

SRC(eta_1, eta_2) for pp, pT>0.5GeV, (20<=Nch<40)

SRC(eta_1, eta_2) for pp, pT>0.2GeV, (20<=Nch<40)

SRC(eta_1, eta_2) for pp, pT>0.5GeV, (10<=Nch<20)

SRC(eta_1, eta_2) for pp, pT>0.2GeV, (10<=Nch<20)

C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (140<=Nch<160)

C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (140<=Nch<160)

C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (120<=Nch<140)

C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (120<=Nch<140)

C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (100<=Nch<120)

C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (100<=Nch<120)

C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (80<=Nch<100)

C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (80<=Nch<100)

C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (60<=Nch<80)

C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (60<=Nch<80)

C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (40<=Nch<60)

C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (40<=Nch<60)

C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (20<=Nch<40)

C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (20<=Nch<40)

C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (10<=Nch<20)

C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (10<=Nch<20)

<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, w SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, w SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, w SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, w SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, w SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, w SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, w SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, w SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 100<=Nch<120, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 100<=Nch<120, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 100<=Nch<120, w SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 100<=Nch<120, w SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 100<=Nch<120, w SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 100<=Nch<120, w SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 80<=Nch<100, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 80<=Nch<100, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 80<=Nch<100, w SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 80<=Nch<100, w SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 80<=Nch<100, w SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 80<=Nch<100, w SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 60<=Nch<80, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 60<=Nch<80, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 60<=Nch<80, w SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 60<=Nch<80, w SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 60<=Nch<80, w SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 60<=Nch<80, w SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 40<=Nch<60, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 40<=Nch<60, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 40<=Nch<60, w SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 40<=Nch<60, w SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 40<=Nch<60, w SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 40<=Nch<60, w SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 20<=Nch<40, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 20<=Nch<40, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 20<=Nch<40, w SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 20<=Nch<40, w SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 20<=Nch<40, w SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 20<=Nch<40, w SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 10<=Nch<20, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 10<=Nch<20, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 10<=Nch<20, w SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 10<=Nch<20, w SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 10<=Nch<20, w SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 10<=Nch<20, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 100<=Nch<120, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 100<=Nch<120, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 100<=Nch<120, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 100<=Nch<120, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 100<=Nch<120, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 100<=Nch<120, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 80<=Nch<100, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 80<=Nch<100, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 80<=Nch<100, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 80<=Nch<100, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 80<=Nch<100, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 80<=Nch<100, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 60<=Nch<80, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 60<=Nch<80, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 60<=Nch<80, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 60<=Nch<80, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 60<=Nch<80, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 60<=Nch<80, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, wo SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, wo SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, wo SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, wo SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, wo SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, wo SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, wo SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, wo SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 100<=Nch<120, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 100<=Nch<120, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 100<=Nch<120, wo SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 100<=Nch<120, wo SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 100<=Nch<120, wo SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 100<=Nch<120, wo SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 80<=Nch<100, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 80<=Nch<100, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 80<=Nch<100, wo SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 80<=Nch<100, wo SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 80<=Nch<100, wo SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 80<=Nch<100, wo SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 60<=Nch<80, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 60<=Nch<80, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 60<=Nch<80, wo SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 60<=Nch<80, wo SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 60<=Nch<80, wo SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 60<=Nch<80, wo SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 40<=Nch<60, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 40<=Nch<60, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 40<=Nch<60, wo SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 40<=Nch<60, wo SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 40<=Nch<60, wo SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 40<=Nch<60, wo SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 20<=Nch<40, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 20<=Nch<40, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 20<=Nch<40, wo SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 20<=Nch<40, wo SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 20<=Nch<40, wo SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 20<=Nch<40, wo SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 10<=Nch<20, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 10<=Nch<20, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 10<=Nch<20, wo SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 10<=Nch<20, wo SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 10<=Nch<20, wo SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 10<=Nch<20, wo SRC, all pairs

a1 from fit C_N^sub(eta-) for Pb+Pb, pT>0.5GeV

a1 from fit C_N^sub(eta-) for Pb+Pb, pT>0.2GeV

a1 from fit C_N^sub(eta+) for Pb+Pb, pT>0.5GeV

a1 from fit C_N^sub(eta+) for Pb+Pb, pT>0.2GeV

a1 from fit r_N^sub(eta) for Pb+Pb, pT>0.5GeV

a1 from fit r_N^sub(eta) for Pb+Pb, pT>0.2GeV

a1 from fit C_N^sub(eta1, eta2) for Pb+Pb, pT>0.5GeV

a1 from fit C_N^sub(eta1, eta2) for Pb+Pb, pT>0.2GeV

a1 from fit C_N^sub(eta-) for p+Pb, pT>0.5GeV

a1 from fit C_N^sub(eta-) for p+Pb, pT>0.2GeV

a1 from fit C_N^sub(eta+) for p+Pb, pT>0.5GeV

a1 from fit C_N^sub(eta+) for p+Pb, pT>0.2GeV

a1 from fit r_N^sub(eta) for p+Pb, pT>0.5GeV

a1 from fit r_N^sub(eta) for p+Pb, pT>0.2GeV

a1 from fit C_N^sub(eta1, eta2) for p+Pb, pT>0.5GeV

a1 from fit C_N^sub(eta1, eta2) for p+Pb, pT>0.2GeV

a1 from fit C_N^sub(eta-) for pp, pT>0.5GeV

a1 from fit C_N^sub(eta-) for pp, pT>0.2GeV

a1 from fit C_N^sub(eta+) for pp, pT>0.5GeV

a1 from fit C_N^sub(eta+) for pp, pT>0.2GeV

a1 from fit r_N^sub(eta) for pp, pT>0.5GeV

a1 from fit r_N^sub(eta) for pp, pT>0.2GeV

a1 from fit C_N^sub(eta1, eta2) for pp, pT>0.5GeV

a1 from fit C_N^sub(eta1, eta2) for pp, pT>0.2GeV

SRC for Pb+Pb, pT>0.5GeV, all pairs

SRC for Pb+Pb, pT>0.2GeV, all pairs

SRC for Pb+Pb, pT>0.5GeV, opposite pairs

SRC for Pb+Pb, pT>0.2GeV, opposite pairs

SRC for Pb+Pb, pT>0.5GeV, same pairs

SRC for Pb+Pb, pT>0.2GeV, same pairs

SRC for p+Pb, pT>0.5GeV, all pairs

SRC for p+Pb, pT>0.2GeV, all pairs

SRC for p+Pb, pT>0.5GeV, opposite pairs

SRC for p+Pb, pT>0.2GeV, opposite pairs

SRC for p+Pb, pT>0.5GeV, same pairs

SRC for p+Pb, pT>0.2GeV, same pairs

SRC for pp, pT>0.5GeV, all pairs

SRC for pp, pT>0.2GeV, all pairs

SRC for pp, pT>0.5GeV, opposite pairs

SRC for pp, pT>0.2GeV, opposite pairs

SRC for pp, pT>0.5GeV, same pairs

SRC for pp, pT>0.2GeV, same pairs

SRC for Pb+Pb, pT>0.5GeV

SRC for Pb+Pb, pT>0.2GeV

SRC for p+Pb, pT>0.5GeV

SRC for p+Pb, pT>0.2GeV

SRC for pp, pT>0.5GeV

SRC for pp, pT>0.2GeV

a1 for Pb+Pb, pT>0.5GeV

a1 for Pb+Pb, pT>0.2GeV

a1 for p+Pb, pT>0.5GeV

a1 for p+Pb, pT>0.2GeV

a1 for pp, pT>0.5GeV

a1 for pp, pT>0.2GeV

f(eta+) for p+Pb

f(eta+) for symmetrized p+Pb

f(eta+) for pp

f(eta+) for Pb+Pb

Relative differential cross section as a function of the b-jet multiplicity in emu channel

Relative differential cross section as a function of H_T in emu channel

Relative differential cross section as a function of H_T in emu channel

Relative differential cross section as a function of H_Thad in emu channel

Relative differential cross section as a function of H_Thad in emu channel

Relative differential cross section as a function of H_T in leptons+jets channel

Relative differential cross section as a function of H_T in leptons+jets channel

Relative differential cross section as a function of H_Thad in leptons+jets channel

Relative differential cross section as a function of H_Thad in leptons+jets channel

Relative differential cross section as a function of pT of leading b-jet in emu channel

Relative differential cross section as a function of pT of leading b-jet in emu channel

Relative differential cross section as a function of pT of sub-leading b-jet in emu channel

Relative differential cross section as a function of pT of sub-leading b-jet in emu channel

Relative differential cross section as a function of pT of third-leading b-jet in emu channel

Relative differential cross section as a function of pT of third-leading b-jet in emu channel

Relative differential cross section as a function of pT of leading b-jet in lepton+jets channel

Relative differential cross section as a function of pT of leading b-jet in lepton+jets channel

Relative differential cross section as a function of pT of sub-leading b-jet in lepton+jets channel

Relative differential cross section as a function of pT of sub-leading b-jet in lepton+jets channel

Relative differential cross section as a function of pT of third-leading b-jet in lepton+jets channel

Relative differential cross section as a function of pT of third-leading b-jet in lepton+jets channel

Relative differential cross section as a function of pT of fourth-leading b-jet in lepton+jets channel

Relative differential cross section as a function of pT of fourth-leading b-jet in lepton+jets channel

Relative differential cross section as a function of invarant mass of two highest pT b-jets in emu channel

Relative differential cross section as a function of invarant mass of two highest pT b-jets in emu channel

Relative differential cross section as a function of pT of two highest pT b-jets in emu channel

Relative differential cross section as a function of pT of two highest pT b-jets in emu channel

Relative differential cross section as a function of deltaR of two highest pT b-jets in emu channel

Relative differential cross section as a function of deltaR of two highest pT b-jets in emu channel

Relative differential cross section as a function of invariant mass of two highest pT b-jets in lepton+jets channel

Relative differential cross section as a function of invariant mass of two highest pT b-jets in lepton+jets channel

Relative differential cross section as a function of pT of two highest pT b-jets in lepton+jets channel

Relative differential cross section as a function of pT of two highest pT b-jets in lepton+jets channel

Relative differential cross section as a function of deltaR of two highest pT b-jets in lepton+jets channel

Relative differential cross section as a function of deltaR of two highest pT b-jets in lepton+jets channel

Relative differential cross section as a function of invariant mass of two closest b-jets in deltaR in emu channel

Relative differential cross section as a function of invariant mass of two closest b-jets in deltaR in emu channel

Relative differential cross section as a function of pT of two closest b-jets in deltaR in emu channel

Relative differential cross section as a function of pT of two closest b-jets in deltaR in emu channel

Relative differential cross section as a function of deltaR of two closest b-jets in deltaR in emu channel

Relative differential cross section as a function of deltaR of two closest b-jets in deltaR in emu channel

Relative differential cross section as a function of invariant mass of two closest b-jets in deltaR in lepton+jets channel

Relative differential cross section as a function of invariant mass of two closest b-jets in deltaR in lepton+jets channel

Relative differential cross section as a function of pT of two closest b-jets in deltaR in lepton+jets channel

Relative differential cross section as a function of pT of two closest b-jets in deltaR in lepton+jets channel

Relative differential cross section as a function of deltaR of two closest b-jets in deltaR in lepton+jets channel

Relative differential cross section as a function of deltaR of two closest b-jets in deltaR in lepton+jets channel

Photon-jet pT balance distributions (1/Ng)(dN/dxJg) in pp events (blue, reproduced on all panels) and Pb+Pb events (red) with each panel denoting a different centrality selection. These panels show results with pTg = 158-200 GeV. Total systematic uncertainties are shown as boxes, while statistical uncertainties are shown with vertical bars.

Selected comparisons of the nominal results in pp (blue) and 0-10% Pb+Pb (red) collisions with the central values obtained using a different photon-jet signal definition. Comparison of the nominal results (with DeltaPhi > 7pi/8) with those obtained using DeltaPhi > 3pi/4 for the pTg = 63.1-79.6 GeV range. Boxes indicate total systematic uncertainties, while vertical bars indicate statistical uncertainties.

Selected comparisons of the nominal results in pp (blue) and 0-10% Pb+Pb (red) collisions with the central values obtained using a different photon-jet signal definition. Comparison of the nominal results (inclusive jet selection) with those obtained using a photon-plus-leading-jet selection for the pTg = 100-158 GeV range. Boxes indicate total systematic uncertainties, while vertical bars indicate statistical uncertainties.

Comparison of the distribution of the scalar sum of small-$R$ jet and lepton transverse momenta, $S_T$, between data and the background prediction in the signal region of the pair-production (PP) $\geq 3\ell$ channel. The background prediction is shown post-fit, i.e. after the fit to the data $S_T$ distributions under the background-only hypothesis. The last bin contains the overflow. An example distribution for a $B\bar B$ signal in the singlet model with $m_B$ = 900 GeV is overlaid.

Comparison of the distribution of the invariant mass of the $Z$ boson candidate and the highest-$p_T$ top-tagged large-$R$ jet, $m_{Zt}$, between data and the background prediction in the signal region of the single-production (SP) 2$\ell$ channel. The background prediction is shown post-fit, i.e. after the fit to the data $m_{Zt}$ distributions under the background-only hypothesis. The last bin contains the overflow. An example distribution for a single-$T$-quark signal with $m_T$ = 900 GeV and $\kappa_T = 0.5$ is overlaid.

Comparison of the distribution of the scalar sum of small-$R$ jet and lepton transverse momenta, $S_T$, between data and the background prediction in the signal region of the single-production (SP) $\geq 3\ell$ channel. The background prediction is shown post-fit, i.e. after the fit to the data $S_T$ distributions under the background-only hypothesis. The last bin contains the overflow. An example distribution for a single-$T$-quark signal with $m_T$ = 900 GeV and $\kappa_T$ = 0.5 is overlaid.

Upper limits at 95$\%$ CL on the cross section of vector-like quark pair production (PP) for $T\bar T$ in the singlet model. The expected limits are shown for the combination of the channels, as are the observed limits.

Upper limits at 95$\%$ CL on the cross section of vector-like quark pair production (PP) for $B\bar B$ in the singlet model. The expected limits are shown for the combination of the channels, as are the observed limits.

Upper limits at 95$\%$ CL on the cross section of vector-like quark pair production (PP) for $T\bar T$ in the doublet model. The expected limits are shown for the combination of the channels, as are the observed limits.

Upper limits at 95$\%$ CL on the cross section of vector-like quark pair production (PP) for $B\bar B$ in the doublet model. The expected limits are shown for the combination of the channels, as are the observed limits.

Upper limits at 95$\%$ CL on the cross section of vector-like quark pair production (PP) for $T\bar T$ with a BR of 100$\%$ to $Zt$. The expected limits are shown for the combination of the channels, as are the observed limits.

Upper limits at 95$\%$ CL on the cross section of vector-like quark pair production (PP) for $B\bar B$ with a BR of 100$\%$ to $Zb$. The expected limits are shown for the combination of the channels, as are the observed limits.

Expected 95$\%$ CL lower limits from the combination of the pair-production channels on the mass of vector-like quarks for all combinations of BRs for $T\rightarrow Zt$, $T\rightarrow Ht$, $T\rightarrow Wb$, adding up to unity.

Observed 95$\%$ CL lower limits from the combination of the pair-production channels on the mass of vector-like quarks for all combinations of BRs for $T\rightarrow Zt$, $T\rightarrow Ht$, $T\rightarrow Wb$, adding up to unity.

Expected 95$\%$ CL lower limits from the combination of the pair-production channels on the mass of vector-like quarks for all combinations of BRs for $B\rightarrow Zb$, $B\rightarrow Hb$, $B\rightarrow Wt$, adding up to unity.

Observed 95$\%$ CL lower limits from the combination of the pair-production channels on the mass of vector-like quarks for all combinations of BRs for $B\rightarrow Zb$, $B\rightarrow Hb$, $B\rightarrow Wt$, adding up to unity.

Upper limits at 95$\%$ CL on the cross section times BR to $Zt$ of single production (SP) of a $T$-quark. The expected limits are shown for the combination of the channels, as are the observed limits. The expected cross section times BR to $Zt$ for single-$T$-quark production is also shown for a coupling $\kappa_T = 0.5$, which corresponds to a coupling of $c_W = \sqrt{c^2_{W,L} + c^2_{W,R}} = 0.45$ from Ref. [14]. The BR assumed here corresponds to the singlet benchmark model, i.e. $\approx 25\%$.

Expected and observed 95$\%$ CL limits from the combination of the single-production channels on the coupling of the $T$ quark to SM particles, $c_W = \sqrt c^2_L + c^2_R$, assuming the singlet-model BR of $\approx 25\%$, as a function of the mass of the $T$ quark, $m_T$. Values of $c_W$ larger than the observed limit are excluded.

Expected and observed 95$\%$ CL limits from the combination of the single-production channels on the mixing angle in the singlet model between the $T$ quark and the top quark, $|\sin\theta_L|$, as a function of the mass of the $T$ quark, $m_T$. Values of $|\sin\theta_L|$ enclosed by the observed limit are excluded, i.e. for $m_T$ larger than $\approx 1200$ GeV, no value of $|\sin\theta_L|$ is excluded.

Expected lower limit from the combination of the single-production channels on the mass of the $T$ quark as a function of the couplings of the $T$ quark to the $W$ boson, $\sqrt c^2_L + c^2_R$, and to the $Z$ boson, $\sqrt c^2_L + c^2_R$ with the assumption of equal BRs for $T\rightarrow Zt$ and $T\rightarrow Ht$ in the limit of large $T$-quark masses.

Observed lower limit from the combination of the single-production channels on the mass of the $T$ quark as a function of the couplings of the $T$ quark to the $W$ boson, $\sqrt c^2_L + c^2_R$, and to the $Z$ boson, $\sqrt c^2_L + c^2_R$ with the assumption of equal BRs for $T\rightarrow Zt$ and $T\rightarrow Ht$ in the limit of large $T$-quark masses.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow T\bar T)$ for the combination of the pair-production channels for all combinations of BRs for $T\rightarrow Zt$, $T\rightarrow Ht$, $T\rightarrow Wb$ adding up to unity for a $T$-quark mass of 500 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow T\bar T)$ for the combination of the pair-production channels for all combinations of BRs for $T\rightarrow Zt$, $T\rightarrow Ht$, $T\rightarrow Wb$ adding up to unity for a $T$-quark mass of 600 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow T\bar T)$ for the combination of the pair-production channels for all combinations of BRs for $T\rightarrow Zt$, $T\rightarrow Ht$, $T\rightarrow Wb$ adding up to unity for a $T$-quark mass of 700 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow T\bar T)$ for the combination of the pair-production channels for all combinations of BRs for $T\rightarrow Zt$, $T\rightarrow Ht$, $T\rightarrow Wb$ adding up to unity for a $T$-quark mass of 750 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow T\bar T)$ for the combination of the pair-production channels for all combinations of BRs for $T\rightarrow Zt$, $T\rightarrow Ht$, $T\rightarrow Wb$ adding up to unity for a $T$-quark mass of 800 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow T\bar T)$ for the combination of the pair-production channels for all combinations of BRs for $T\rightarrow Zt$, $T\rightarrow Ht$, $T\rightarrow Wb$ adding up to unity for a $T$-quark mass of 850 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow T\bar T)$ for the combination of the pair-production channels for all combinations of BRs for $T\rightarrow Zt$, $T\rightarrow Ht$, $T\rightarrow Wb$ adding up to unity for a $T$-quark mass of 900 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow T\bar T)$ for the combination of the pair-production channels for all combinations of BRs for $T\rightarrow Zt$, $T\rightarrow Ht$, $T\rightarrow Wb$ adding up to unity for a $T$-quark mass of 950 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow T\bar T)$ for the combination of the pair-production channels for all combinations of BRs for $T\rightarrow Zt$, $T\rightarrow Ht$, $T\rightarrow Wb$ adding up to unity for a $T$-quark mass of 1000 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow T\bar T)$ for the combination of the pair-production channels for all combinations of BRs for $T\rightarrow Zt$, $T\rightarrow Ht$, $T\rightarrow Wb$ adding up to unity for a $T$-quark mass of 1050 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow T\bar T)$ for the combination of the pair-production channels for all combinations of BRs for $T\rightarrow Zt$, $T\rightarrow Ht$, $T\rightarrow Wb$ adding up to unity for a $T$-quark mass of 1100 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow T\bar T)$ for the combination of the pair-production channels for all combinations of BRs for $T\rightarrow Zt$, $T\rightarrow Ht$, $T\rightarrow Wb$ adding up to unity for a $T$-quark mass of 1150 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow T\bar T)$ for the combination of the pair-production channels for all combinations of BRs for $T\rightarrow Zt$, $T\rightarrow Ht$, $T\rightarrow Wb$ adding up to unity for a $T$-quark mass of 1200 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow T\bar T)$ for the combination of the pair-production channels for all combinations of BRs for $T\rightarrow Zt$, $T\rightarrow Ht$, $T\rightarrow Wb$ adding up to unity for a $T$-quark mass of 1300 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow T\bar T)$ for the combination of the pair-production channels for all combinations of BRs for $T\rightarrow Zt$, $T\rightarrow Ht$, $T\rightarrow Wb$ adding up to unity for a $T$-quark mass of 1400 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow B\bar B)$ for the combination of the pair-production channels for all combinations of BRs for $B\rightarrow Zb$, $B\rightarrow Hb$, $B\rightarrow Wt$ adding up to unity for a $B$-quark mass of 500 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow B\bar B)$ for the combination of the pair-production channels for all combinations of BRs for $B\rightarrow Zb$, $B\rightarrow Hb$, $B\rightarrow Wt$ adding up to unity for a $B$-quark mass of 600 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow B\bar B)$ for the combination of the pair-production channels for all combinations of BRs for $B\rightarrow Zb$, $B\rightarrow Hb$, $B\rightarrow Wt$ adding up to unity for a $B$-quark mass of 700 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow B\bar B)$ for the combination of the pair-production channels for all combinations of BRs for $B\rightarrow Zb$, $B\rightarrow Hb$, $B\rightarrow Wt$ adding up to unity for a $B$-quark mass of 750 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow B\bar B)$ for the combination of the pair-production channels for all combinations of BRs for $B\rightarrow Zb$, $B\rightarrow Hb$, $B\rightarrow Wt$ adding up to unity for a $B$-quark mass of 800 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow B\bar B)$ for the combination of the pair-production channels for all combinations of BRs for $B\rightarrow Zb$, $B\rightarrow Hb$, $B\rightarrow Wt$ adding up to unity for a $B$-quark mass of 850 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow B\bar B)$ for the combination of the pair-production channels for all combinations of BRs for $B\rightarrow Zb$, $B\rightarrow Hb$, $B\rightarrow Wt$ adding up to unity for a $B$-quark mass of 900 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow B\bar B)$ for the combination of the pair-production channels for all combinations of BRs for $B\rightarrow Zb$, $B\rightarrow Hb$, $B\rightarrow Wt$ adding up to unity for a $B$-quark mass of 950 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow B\bar B)$ for the combination of the pair-production channels for all combinations of BRs for $B\rightarrow Zb$, $B\rightarrow Hb$, $B\rightarrow Wt$ adding up to unity for a $B$-quark mass of 1000 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow B\bar B)$ for the combination of the pair-production channels for all combinations of BRs for $B\rightarrow Zb$, $B\rightarrow Hb$, $B\rightarrow Wt$ adding up to unity for a $B$-quark mass of 1050 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow B\bar B)$ for the combination of the pair-production channels for all combinations of BRs for $B\rightarrow Zb$, $B\rightarrow Hb$, $B\rightarrow Wt$ adding up to unity for a $B$-quark mass of 1100 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow B\bar B)$ for the combination of the pair-production channels for all combinations of BRs for $B\rightarrow Zb$, $B\rightarrow Hb$, $B\rightarrow Wt$ adding up to unity for a $B$-quark mass of 1150 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow B\bar B)$ for the combination of the pair-production channels for all combinations of BRs for $B\rightarrow Zb$, $B\rightarrow Hb$, $B\rightarrow Wt$ adding up to unity for a $B$-quark mass of 1200 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow B\bar B)$ for the combination of the pair-production channels for all combinations of BRs for $B\rightarrow Zb$, $B\rightarrow Hb$, $B\rightarrow Wt$ adding up to unity for a $B$-quark mass of 1300 GeV.

Observed upper limits at 95$\%$ CL on $\sigma(pp\rightarrow B\bar B)$ for the combination of the pair-production channels for all combinations of BRs for $B\rightarrow Zb$, $B\rightarrow Hb$, $B\rightarrow Wt$ adding up to unity for a $B$-quark mass of 1400 GeV.

Observed upper limits at 95$\%$ CL on the cross section times BR to $Zt$ as a function of the vector-like $T$-quark mass and coupling $\kappa_T$ for the combination of the SP $2\ell$ and SP $\geq 3\ell$ channels.

Signal cutflows for the $B\bar B$ process in the singlet model in the PP $2\ell$ $0-1$J channel in the 0-large-$R$ jet SR. Only statistical uncertainties are shown.

Signal cutflows for the $B\bar B$ process in the singlet model in the PP $2\ell$ $0-1$J channel in the 1-large-$R$ jet SR. Only statistical uncertainties are shown.

Signal cutflows for the $B\bar B$ process in the doublet model in the PP $2\ell$ $0-1$J channel in the 0-large-$R$ jet SR. Only statistical uncertainties are shown.

Signal cutflows for the $B\bar B$ process in the doublet model in the PP $2\ell$ $0-1$J channel in the 1-large-$R$ jet SR. Only statistical uncertainties are shown.

Signal cutflows for the $B\bar B$ process in the case of 100$\%$ BR for $B \rightarrow Zb$ in the PP $2\ell$ $0-1$J channel in the 0-large-$R$ jet SR. Only statistical uncertainties are shown.

Signal cutflows for the $B\bar B$ process in the case of 100$\%$ BR for $B \rightarrow Zb$ in the PP $2\ell$ $0-1$J channel in the 1-large-$R$ jet SR. Only statistical uncertainties are shown.

Signal cutflows for the $T\bar T$ process in the singlet model in the PP $2\ell$ $0-1$J channel in the 0-large-$R$ jet SR. Only statistical uncertainties are shown.

Signal cutflows for the $T\bar T$ process in the singlet model in the PP $2\ell$ $0-1$J channel in the 1-large-$R$ jet SR. Only statistical uncertainties are shown.

Signal cutflows for the $T\bar T$ process in the doublet model in the PP $2\ell$ $0-1$J channel in the 0-large-$R$ jet SR. Only statistical uncertainties are shown.

Signal cutflows for the $T\bar T$ process in the doublet model in the PP $2\ell$ $0-1$J channel in the 1-large-$R$ jet SR. Only statistical uncertainties are shown.

Signal cutflows for the $T\bar T$ process in the case of 100$\%$ BR for $T \rightarrow Zt$ in the PP $2\ell$ $0-1$J channel in the 0-large-$R$ jet SR. Only statistical uncertainties are shown.

Signal cutflows for the $T\bar T$ process in the case of 100$\%$ BR for $T \rightarrow Zt$ in the PP $2\ell$ $0-1$J channel in the 1-large-$R$ jet SR. Only statistical uncertainties are shown.

Signal cutflows for the $T\bar T$ process in the singlet model in the PP $2\ell$ $\geq 2$J channel. Only statistical uncertainties are shown.

Signal cutflows for the $B\bar B$ process in the singlet model in the PP $2\ell$ $\geq 2$J channel. Only statistical uncertainties are shown.

Signal cutflows for the $T\bar T$ process in the doublet model in the PP $2\ell$ $\geq 2$J channel. Only statistical uncertainties are shown.

Signal cutflows for the $B\bar B$ process in the doublet model in the PP $2\ell$ $\geq 2$J channel. Only statistical uncertainties are shown.

Signal cutflows for the $T\bar T$ process in the case of 100$\%$ BR for $T \rightarrow Zt$ in the PP $2\ell$ $\geq 2$J channel. Only statistical uncertainties are shown.

Signal cutflows for the $B\bar B$ process in the case of 100$\%$ BR for $B \rightarrow Zb$ in the PP $2\ell$ $\geq 2$J channel. Only statistical uncertainties are shown.

Signal cutflows for the $T\bar T$ process in the singlet model in the PP $\geq 3\ell$ channel. Only statistical uncertainties are shown.

Signal cutflows for the $B\bar B$ process in the singlet model in the PP $\geq 3\ell$ channel. Only statistical uncertainties are shown.

Signal cutflows for the $T\bar T$ process in the doublet model in the PP $\geq 3\ell$ channel. Only statistical uncertainties are shown.

Signal cutflows for the $B\bar B$ process in the doublet model in the PP $\geq 3\ell$ channel. Only statistical uncertainties are shown.

Signal cutflows for the $T\bar T$ process in the case of 100$\%$ BR for $T \rightarrow Zt$ in the PP $\geq 3\ell$ channel. Only statistical uncertainties are shown.

Signal cutflows for the $B\bar B$ process in the case of 100$\%$ BR for $B \rightarrow Zb$ in the PP $\geq 3\ell$ channel. Only statistical uncertainties are shown.

Signal cutflows for single-$T$-quark production with $\kappa_T = 0.5$ in the SP $2\ell$ channel. Only statistical uncertainties are shown.

Signal cutflows for single-$T$-quark production with $\kappa_T = 0.5$ in the SP $\geq 3\ell$ channel. Only statistical uncertainties are shown.

Signal efficiencies in $\%$ in the PP $2\ell$ $0-1$J channel in the 0-large-$R$ jet SR. Uncertainties are statistical only.

Signal efficiencies in $\%$ in the PP $2\ell$ $0-1$J channel in the 1-large-$R$ jet SR. Uncertainties are statistical only.

Signal efficiencies in $\%$ in the PP $2\ell$ $\geq 2$J channel. Uncertainties are statistical only.

Signal efficiencies in $\%$ in the PP $\geq 3\ell$ channel. Uncertainties are statistical only.

Signal efficiencies in $\%$ in the SP $2\ell$ channel for $\kappa_T = 0.5$. Uncertainties are statistical only.

Signal efficiencies in $\%$ in the SP $\geq 3\ell$ channel for $\kappa_T = 0.5$. Uncertainties are statistical only.