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 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

The measured fiducial cross sections

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 the b-jet multiplicity 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 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 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 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 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 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

The measured fiducial cross sections

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>

Number of signal events expected for 36.1 fb$^{-1}$ at different stages of the event selection for the signal region Rpc2L2bS, in a SUSY scenario where gluinos are produced in pairs and decay directly into the lightest neutralino via an offshell top squark, $\tilde g\to t\bar{t}\tilde{\chi}_1^0$. The masses of the superpartners involved in the process are set to $m(\tilde g)$ = 1500 GeV and $m(\tilde \chi_1^0)$ = 800 GeV. Only statistical uncertainties are shown.

Observed 95% CL exclusion contours on the gluino and lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay into the lightest neutralino via a two-steps cascade, $\tilde g\to q\bar{q}^{'}\tilde{\chi}_1^\pm$ followed by $\tilde{\chi}_1^\pm\to W^\pm\tilde{\chi}_2^0$ and $\tilde{\chi}_2^0\to Z\tilde{\chi}_1^0$.

Expected 95% CL exclusion contours on the gluino and lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay into the lightest neutralino via a two-steps cascade, $\tilde g\to q\bar{q}^{'}\tilde{\chi}_1^\pm$ followed by $\tilde{\chi}_1^\pm\to W^\pm\tilde{\chi}_2^0$ and $\tilde{\chi}_2^0\to Z\tilde{\chi}_1^0$.

Observed 95% CL upper limits on $pp\to \tilde g\tilde g$ production cross-sections in a SUSY scenario where gluinos are produced in pairs and decay into the lightest neutralino via a two-steps cascade, $\tilde g\to q\bar{q}^{'}\tilde{\chi}_1^\pm$ followed by $\tilde{\chi}_1^\pm\to W^\pm\tilde{\chi}_2^0$ and $\tilde{\chi}_2^0\to Z\tilde{\chi}_1^0$. The table also shows the signal acceptance and reconstruction efficiency for the signal region(s) with sensitivity to this scenario.

Number of signal events expected for 36.1 fb$^{-1}$ at different stages of the event selection for the signal region Rpc2L2bH, in a SUSY scenario where gluinos are produced in pairs and decay directly into the lightest neutralino via an offshell top squark, $\tilde g\to t\bar{t}\tilde{\chi}_1^0$. The masses of the superpartners involved in the process are set to $m(\tilde g)$ = 1700 GeV and $m(\tilde \chi_1^0)$ = 200 GeV. Only statistical uncertainties are shown.

Observed 95% CL exclusion contours on the gluino and lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay into the lightest neutralino via a two-steps cascade involving sleptons, $\tilde g\to q\bar{q}\tilde{\chi}_2^0$ followed by $\tilde{\chi}_2^0\to \tilde\ell\ell/\tilde\nu\nu$ and $\tilde\ell/\tilde\nu\to \ell/\nu\tilde{\chi}_1^0$.

Expected 95% CL exclusion contours on the gluino and lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay into the lightest neutralino via a two-steps cascade involving sleptons, $\tilde g\to q\bar{q}\tilde{\chi}_2^0$ followed by $\tilde{\chi}_2^0\to \tilde\ell\ell/\tilde\nu\nu$ and $\tilde\ell/\tilde\nu\to \ell/\nu\tilde{\chi}_1^0$.

Observed 95% CL upper limits on $pp\to \tilde g\tilde g$ production cross-sections in a SUSY scenario where gluinos are produced in pairs and decay into the lightest neutralino via a two-steps cascade involving sleptons, $\tilde g\to q\bar{q}\tilde{\chi}_2^0$ followed by $\tilde{\chi}_2^0\to \tilde\ell\ell/\tilde\nu\nu$ and $\tilde\ell/\tilde\nu\to \ell/\nu\tilde{\chi}_1^0$. The table also shows the signal acceptance and reconstruction efficiency for the signal region(s) with sensitivity to this scenario.

Number of signal events expected for 36.1 fb$^{-1}$ at different stages of the event selection for the signal region Rpc2Lsoft1b, in a SUSY scenario where gluinos are produced in pairs and decay directly into the lightest neutralino via offshell top squark and top quark, $\tilde g\to t\bar{b}W^{-}\tilde{\chi}_1^0$. The masses of the superpartners involved in the process are set to $m(\tilde g)$ = 1200 GeV and $m(\tilde \chi_1^0)$ = 940 GeV. Only statistical uncertainties are shown.

Observed 95% CL exclusion contours on the lightest bottom squark and lightest neutralino masses in a SUSY scenario where pairs of bottom-antibottom squarks are produced and decay into the lightest neutralino via a chargino, $\tilde b^{}_{1}\to t\tilde{\chi}_1^-$ followed by $\tilde{\chi}_1^\pm\to W^\pm\tilde{\chi}_1^0$.

Expected 95% CL exclusion contours on the lightest bottom squark and lightest neutralino masses in a SUSY scenario where pairs of bottom-antibottom squarks are produced and decay into the lightest neutralino via a chargino, $\tilde b^{}_{1}\to t\tilde{\chi}_1^-$ followed by $\tilde{\chi}_1^\pm\to W^\pm\tilde{\chi}_1^0$.

Observed 95% CL upper limits on $pp\to \tilde{b}^{}_1\tilde{b}^{*}_1$ production cross-sections in a SUSY scenario where pairs of bottom-antibottom squarks are produced and decay into the lightest neutralino via a chargino, $\tilde b^{}_{1}\to t\tilde{\chi}_1^-$ followed by $\tilde{\chi}_1^\pm\to W^\pm\tilde{\chi}_1^0$. The table also shows the signal acceptance and reconstruction efficiency for the signal region(s) with sensitivity to this scenario.

Number of signal events expected for 36.1 fb$^{-1}$ at different stages of the event selection for the signal region Rpc2Lsoft2b, in a SUSY scenario where gluinos are produced in pairs and decay directly into the lightest neutralino via offshell top squark and top quark, $\tilde g\to t\bar{b}W^{-}\tilde{\chi}_1^0$. The masses of the superpartners involved in the process are set to $m(\tilde g)$ = 1200 GeV and $m(\tilde \chi_1^0)$ = 900 GeV. Only statistical uncertainties are shown.

Expected 95% CL exclusion contours on the gluino and lightest top squark masses in a SUSY scenario where gluinos are produced in pairs and decay into a top quark and an antitop squark, which in turn decays via non-zero baryon-number-violating RPV couplings $\lambda^{''}_{313}$ or $\lambda^{''}_{323}$, $\tilde g\to \bar{t}\tilde{t}_1$ followed by $\tilde{t}_1\to \bar b\bar d / \bar b \bar s$.

Number of signal events expected for 36.1 fb$^{-1}$ at different stages of the event selection for the signal region Rpc2L0bS, in a SUSY scenario where gluinos are produced in pairs and decay into the lightest neutralino via a two-steps cascade, $\tilde g\to q\bar{q}^{'}\tilde{\chi}_1^\pm$ followed by $\tilde{\chi}_1^\pm\to W^\pm\tilde{\chi}_2^0$ and $\tilde{\chi}_2^0\to Z\tilde{\chi}_1^0$. The masses of the superpartners involved in the process are set to $m(\tilde g)$ = 1200 GeV, $m(\tilde \chi_1^\pm)$ = 1050 GeV, $m(\tilde \chi_2^0)$ = 975 GeV and $m(\tilde \chi_1^0)$ = 900 GeV. Only statistical uncertainties are shown.

Observed 95% CL exclusion contours on the gluino and lightest top squark masses in a SUSY scenario where gluinos are produced in pairs and decay into a top quark and an antitop squark, which in turn decays via non-zero baryon-number-violating RPV couplings $\lambda^{''}_{313}$ or $\lambda^{''}_{323}$, $\tilde g\to \bar{t}\tilde{t}_1$ followed by $\tilde{t}_1\to \bar b\bar d / \bar b \bar s$.

Observed 95% CL upper limits on $pp\to \tilde g\tilde g$ production cross-sections in a SUSY scenario where gluinos are produced in pairs and decay into a top quark and an antitop squark, which in turn decays via non-zero baryon-number-violating RPV couplings $\lambda^{''}_{313}$ or $\lambda^{''}_{323}$, $\tilde g\to \bar{t}\tilde{t}_1$ followed by $\tilde{t}_1\to \bar b\bar d / \bar b \bar s$. The table also shows the signal acceptance and reconstruction efficiency for the signal region(s) with sensitivity to this scenario.

Number of signal events expected for 36.1 fb$^{-1}$ at different stages of the event selection for the signal region Rpc2L0bH, in a SUSY scenario where gluinos are produced in pairs and decay into the lightest neutralino via a two-steps cascade, $\tilde g\to q\bar{q}^{'}\tilde{\chi}_1^\pm$ followed by $\tilde{\chi}_1^\pm\to W^\pm\tilde{\chi}_2^0$ and $\tilde{\chi}_2^0\to Z\tilde{\chi}_1^0$. The masses of the superpartners involved in the process are set to $m(\tilde g)$ = 1600 GeV, $m(\tilde \chi_1^\pm)$ = 850 GeV, $m(\tilde \chi_2^0)$ = 475 GeV and $m(\tilde \chi_1^0)$ = 100 GeV. Only statistical uncertainties are shown.

Observed 95% CL exclusion contours on the gluino and lightest top squark masses in a SUSY scenario where gluinos are produced in pairs and decay into a top quark and an antitop squark, which in turn decays via non-zero baryon-number-violating RPV couplings $\lambda^{''}_{321}$, $\lambda^{''}_{311}$ or $\lambda^{''}_{322}$, $\tilde g\to \bar{t}\tilde{t}_1$ followed by $\tilde{t}_1\to \bar s\bar d /\bar d \bar d/\bar s \bar s$.

Expected 95% CL exclusion contours on the gluino and lightest top squark masses in a SUSY scenario where gluinos are produced in pairs and decay into a top quark and an antitop squark, which in turn decays via non-zero baryon-number-violating RPV couplings $\lambda^{''}_{321}$, $\lambda^{''}_{311}$ or $\lambda^{''}_{322}$, $\tilde g\to \bar{t}\tilde{t}_1$ followed by $\tilde{t}_1\to \bar s\bar d /\bar d \bar d/\bar s \bar s$.

Observed 95% CL upper limits on $pp\to \tilde g\tilde g$ production cross-sections in a SUSY scenario where gluinos are produced in pairs and decay into a top quark and an antitop squark, which in turn decays via non-zero baryon-number-violating RPV couplings $\lambda^{''}_{321}$, $\lambda^{''}_{311}$ or $\lambda^{''}_{322}$, $\tilde g\to \bar{t}\tilde{t}_1$ followed by $\tilde{t}_1\to \bar s\bar d /\bar d \bar d/\bar s \bar s$. The table also shows the signal acceptance and reconstruction efficiency for the signal region(s) with sensitivity to this scenario.

Number of signal events expected for 36.1 fb$^{-1}$ at different stages of the event selection for the signal region Rpc3L0bS, in a SUSY scenario where gluinos are produced in pairs and decay into the lightest neutralino via a two-steps cascade involving sleptons, $\tilde g\to q\bar{q}\tilde{\chi}_2^0$ followed by $\tilde{\chi}_2^0\to \tilde\ell\ell/\tilde\nu\nu$ and $\tilde\ell/\tilde\nu\to \ell/\nu\tilde{\chi}_1^0$. The masses of the superpartners involved in the process are set to $m(\tilde g)$ = 1400 GeV, $m(\tilde \chi_2^0)$ = 1250 GeV, $m(\tilde\ell)=m(\tilde\nu)$ = 1175 GeV and $m(\tilde \chi_1^0)$ = 1100 GeV. Only statistical uncertainties are shown.

Observed 95% CL exclusion contours on the gluino and lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay directly into the lightest neutralino, which in turn decays via non-zero baryon- and lepton-number-violating RPV couplings $\lambda^{'}_{ijk}$, $\tilde g\to q\bar{q}\tilde{\chi}_1^0$ followed by $\tilde{\chi}_1^0\to q\bar{q}^{'}\ell$.

Expected 95% CL exclusion contours on the gluino and lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay directly into the lightest neutralino, which in turn decays via non-zero baryon- and lepton-number-violating RPV couplings $\lambda^{'}_{ijk}$, $\tilde g\to q\bar{q}\tilde{\chi}_1^0$ followed by $\tilde{\chi}_1^0\to q\bar{q}^{'}\ell$.

Observed 95% CL upper limits on $pp\to \tilde g\tilde g$ production cross-sections in a SUSY scenario where gluinos are produced in pairs and decay directly into the lightest neutralino, which in turn decays via non-zero baryon- and lepton-number-violating RPV couplings $\lambda^{'}_{ijk}$, $\tilde g\to q\bar{q}\tilde{\chi}_1^0$ followed by $\tilde{\chi}_1^0\to q\bar{q}^{'}\ell$. The table also shows the signal acceptance and reconstruction efficiency for the signal region(s) with sensitivity to this scenario.

Observed 95% CL exclusion contours on the gluino and lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay directly into a pair of top-antitop quarks and the lightest neutralino, which in turn decays into light quarks via non-zero baryon-number-violating RPV couplings $\lambda^{''}_{ijk}$, $\tilde g\to t\bar{t}\tilde{\chi}_1^0$ followed by $\tilde{\chi}_1^0\to qqq$.

Expected 95% CL exclusion contours on the gluino and lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay directly into a pair of top-antitop quarks and the lightest neutralino, which in turn decays into light quarks via non-zero baryon-number-violating RPV couplings $\lambda^{''}_{ijk}$, $\tilde g\to t\bar{t}\tilde{\chi}_1^0$ followed by $\tilde{\chi}_1^0\to qqq$.

Observed 95% CL upper limits on $pp\to \tilde g\tilde g$ production cross-sections in a SUSY scenario where gluinos are produced in pairs and decay directly into a pair of top-antitop quarks and the lightest neutralino, which in turn decays into light quarks via non-zero baryon-number-violating RPV couplings $\lambda^{''}_{ijk}$, $\tilde g\to t\bar{t}\tilde{\chi}_1^0$ followed by $\tilde{\chi}_1^0\to qqq$. The table also shows the signal acceptance and reconstruction efficiency for the signal region(s) with sensitivity to this scenario.

Number of signal events expected for 36.1 fb$^{-1}$ at different stages of the event selection for the signal region Rpc3L0bH, in a SUSY scenario where gluinos are produced in pairs and decay into the lightest neutralino via a two-steps cascade involving sleptons, $\tilde g\to q\bar{q}\tilde{\chi}_2^0$ followed by $\tilde{\chi}_2^0\to \tilde\ell\ell/\tilde\nu\nu$ and $\tilde\ell/\tilde\nu\to \ell/\nu\tilde{\chi}_1^0$. The masses of the superpartners involved in the process are set to $m(\tilde g)$ = 1800 GeV, $m(\tilde \chi_2^0)$ = 950 GeV, $m(\tilde\ell)=m(\tilde\nu)$ = 475 GeV and $m(\tilde \chi_1^0)$ = 100 GeV. Only statistical uncertainties are shown.

Observed and expected 95% CL upper limits on $pp\to \tilde{t}^{}_\mathrm{1}\tilde{t}^{*}_\mathrm{1}$ production cross-sections in a SUSY scenario where pairs of top-antitop squarks are produced and decay into the lightest neutralino via a two-steps cascade, $\tilde t^{}_{1}\to t\tilde{\chi}_2^0$ followed by $\tilde{\chi}_2^0\to \tilde{\chi}_1^\pm W^\mp$ and $\tilde{\chi}_1^\pm\to f\bar{f^{'}}\tilde{\chi}_1^0$. The lightest chargino and the lightest neutralino are assumed to be nearly mass-degenerate. The table also shows the signal acceptance and reconstruction efficiency for the signal region(s) with sensitivity to this scenario.

Number of signal events expected for 36.1 fb$^{-1}$ at different stages of the event selection for the signal region Rpc2L1bS, in a SUSY scenario where pairs of bottom-antibottom squarks are produced and decay into the lightest neutralino via a chargino, $\tilde b^{}_{1}\to t\tilde{\chi}_1^-$ followed by $\tilde{\chi}_1^\pm\to W^\pm\tilde{\chi}_1^0$. The masses of the superpartners involved in the process are set to $m(\tilde{b}^{}_1)$ = 600 GeV, $m(\tilde \chi_1^\pm)$ = 350 GeV and $m(\tilde \chi_1^0)$ = 250 GeV. Only statistical uncertainties are shown.

Observed and expected 95% CL upper limits on $pp\to \tilde g\tilde g$ production cross-sections in a SUSY scenario with non-universal Higgs masses (NUHM2, see the publication Refs. [31-32]). The table also shows the signal acceptance and reconstruction efficiency for the signal region(s) with sensitivity to this scenario.

Number of signal events expected for 36.1 fb$^{-1}$ at different stages of the event selection for the signal region Rpc2L1bH, in a SUSY scenario where pairs of bottom-antibottom squarks are produced and decay into the lightest neutralino via a chargino, $\tilde b^{}_{1}\to t\tilde{\chi}_1^-$ followed by $\tilde{\chi}_1^\pm\to W^\pm\tilde{\chi}_1^0$. The masses of the superpartners involved in the process are set to $m(\tilde{b}^{}_1)$ = 750 GeV, $m(\tilde \chi_1^\pm)$ = 200 GeV and $m(\tilde \chi_1^0)$ = 100 GeV. Only statistical uncertainties are shown.

Observed and expected 95% CL upper limits on $pp\to \tilde{d}^{}_\mathrm{R}\tilde{d}^{*}_\mathrm{R}$ production cross-sections in a SUSY scenario where gluinos are produced in pairs and decay into a top quark and an antitop squark, which in turn decays via non-zero baryon-number-violating RPV couplings $\lambda^{''}_{313}$ or $\lambda^{''}_{323}$, $\tilde g\to \bar{t}\tilde{t}_1$ followed by $\tilde{t}_1\to \bar b\bar d / \bar b \bar s$. The table also shows the signal acceptance and reconstruction efficiency for the signal region(s) with sensitivity to this scenario.

Number of signal events expected for 36.1 fb$^{-1}$ at different stages of the event selection for the signal region Rpc3LSS1b, in a SUSY scenario where pairs of top-antitop squarks are produced and decay into the lightest neutralino via a two-steps cascade, $\tilde t^{}_{1}\to t\tilde{\chi}_2^0$ followed by $\tilde{\chi}_2^0\to \tilde{\chi}_1^\pm W^\mp$ and $\tilde{\chi}_1^\pm\to f\bar{f^{'}}\tilde{\chi}_1^0$. The lightest chargino and the lightest neutralino are assumed to be nearly mass-degenerate. The masses of the superpartners involved in the process are set to $m(\tilde{t}^{}_1)$ = 700 GeV, $m(\tilde \chi_2^0)$ = 525 GeV, $m(\tilde \chi_1^\pm)\approx m(\tilde \chi_1^0)$ = 425 GeV. Only statistical uncertainties are shown.

Observed and expected 95% CL upper limits on $pp\to \tilde{d}^{}_\mathrm{R}\tilde{d}^{*}_\mathrm{R}$ production cross-sections in a SUSY scenario where gluinos are produced in pairs and decay into a top quark and an antitop squark, which in turn decays via non-zero baryon-number-violating RPV couplings $\lambda^{''}_{321}$, $\lambda^{''}_{311}$ or $\lambda^{''}_{322}$, $\tilde g\to \bar{t}\tilde{t}_1$ followed by $\tilde{t}_1\to \bar s\bar d /\bar d \bar d/\bar s \bar s$. The table also shows the signal acceptance and reconstruction efficiency for the signal region(s) with sensitivity to this scenario.

Number of signal events expected for 36.1 fb$^{-1}$ at different stages of the event selection for the signal region Rpv2L1bH, in a SUSY scenario where gluinos are produced in pairs and decay into a top quark and an antitop squark, which in turn decays via non-zero baryon-number-violating RPV couplings $\lambda^{''}_{321}$, $\lambda^{''}_{311}$ or $\lambda^{''}_{322}$, $\tilde g\to \bar{t}\tilde{t}_1$ followed by $\tilde{t}_1\to \bar s\bar d /\bar d \bar d/\bar s \bar s$. The masses of the superpartners involved in the process are set to $m(\tilde g)$ = 1400 GeV, $m(\tilde{t}^{}_{1})$ = 800 GeV. Only statistical uncertainties are shown.

Number of signal events expected for 36.1 fb$^{-1}$ at different stages of the event selection for the signal region Rpv2L0b, in a SUSY scenario where gluinos are produced in pairs and decay directly into the lightest neutralino, which in turn decays via non-zero baryon- and lepton-number-violating RPV couplings $\lambda^{'}_{ijk}$, $\tilde g\to q\bar{q}\tilde{\chi}_1^0$ followed by $\tilde{\chi}_1^0\to q\bar{q}^{'}\ell$. The masses of the superpartners involved in the process are set to $m(\tilde g)$ = 1400 GeV, $m(\tilde{\chi}_1^0)$ = 500 GeV. Only statistical uncertainties are shown.

Number of signal events expected for 36.1 fb$^{-1}$ at different stages of the event selection for the signal region Rpv2L2bH, in a SUSY scenario where gluinos are produced in pairs and decay directly into a pair of top-antitop quarks and the lightest neutralino, which in turn decays into light quarks via non-zero baryon-number-violating RPV couplings $\lambda^{''}_{ijk}$, $\tilde g\to t\bar{t}\tilde{\chi}_1^0$ followed by $\tilde{\chi}_1^0\to qqq$. The masses of the superpartners involved in the process are set to $m(\tilde g)$ = 1800 GeV, $m(\tilde{\chi}_1^0)$ = 200 GeV. Only statistical uncertainties are shown.

Number of signal events expected for 36.1 fb$^{-1}$ at different stages of the event selection for the signal region Rpv2L2bS, in a SUSY scenario where pairs of down-down squark-rights are produced and decay into a pair of top and bottom quarks via a non-zero baryon-number-violating RPV coupling $\lambda^{''}_{331}$, $\tilde{d}^{}_\mathrm{R}\to \bar t\bar b$. The masses of the superpartners involved in the process are set to $m(\tilde{d}^{}_\mathrm{R})$ = 600 GeV, $m(\tilde g)$ = 2000 GeV. Only statistical uncertainties are shown.

Number of signal events expected for 36.1 fb$^{-1}$ at different stages of the event selection for the signal region Rpv2L1bS, in a SUSY scenario where pairs of down-down squarks are produced and decay into a pair of top and a light quarks via non-zero baryon-number-violating RPV couplings $\lambda^{''}_{321}$ or $\lambda^{''}_{322}$, $\tilde{d}^{}_\mathrm{R}\to \bar t\bar s/\bar t\bar d$. The masses of the superpartners involved in the process are set to $m(\tilde{d}^{}_\mathrm{R})$ = 600 GeV, $m(\tilde g)$ = 2000 GeV. Only statistical uncertainties are shown.

Number of signal events expected for 36.1 fb$^{-1}$ at different stages of the event selection for the signal region Rpv2L1bM, in a SUSY scenario where pairs of down-down squarks are produced and decay into a pair of top and a light quarks via non-zero baryon-number-violating RPV couplings $\lambda^{''}_{321}$ or $\lambda^{''}_{322}$, $\tilde{d}^{}_\mathrm{R}\to \bar t\bar s/\bar t\bar d$. The masses of the superpartners involved in the process are set to $m(\tilde{d}^{}_\mathrm{R})$ = 1000 GeV, $m(\tilde g)$ = 2000 GeV. Only statistical uncertainties are shown.

Sequential impact of each requirement on the number of events passing the selection for the high-$E_T$ analysis.

Sequential impact of each requirement on the number of events passing the selection for the low-$E_T$ analysis.

Application of the modified ABCD method to the final high-$E_T$ and low-$E_T$ selections.

The extrapolated signal efficiencies as a function of proper decay length of the $s$ for several simulated samples in the low-$E_T$ selections.

The extrapolated signal efficiencies as a function of proper decay length of the $s$ for several simulated samples in the high-$E_T$ selections.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 25 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 600 ~\mathrm{GeV}$ and $m_{s} = 150 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 25 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 600 ~\mathrm{GeV}$ and $m_{s} = 150 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 5 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 8 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 15 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 40 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 55 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 200 ~\mathrm{GeV}$ and $m_{s} = 8 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 200 ~\mathrm{GeV}$ and $m_{s} = 25 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 200 ~\mathrm{GeV}$ and $m_{s} = 50 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 400 ~\mathrm{GeV}$ and $m_{s} = 50 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 400 ~\mathrm{GeV}$ and $m_{s} = 100 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 600 ~\mathrm{GeV}$ and $m_{s} = 50 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 1000 ~\mathrm{GeV}$ and $m_{s} = 50 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 1000 ~\mathrm{GeV}$ and $m_{s} = 150 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 1000 ~\mathrm{GeV}$ and $m_{s} = 400 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 5 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 8 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 15 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 40 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 200 ~\mathrm{GeV}$ and $m_{s} = 8 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 200 ~\mathrm{GeV}$ and $m_{s} = 25 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 200 ~\mathrm{GeV}$ and $m_{s} = 50 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 400 ~\mathrm{GeV}$ and $m_{s} = 50 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 400 ~\mathrm{GeV}$ and $m_{s} = 100 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 600 ~\mathrm{GeV}$ and $m_{s} = 50 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 1000 ~\mathrm{GeV}$ and $m_{s} = 50 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 1000 ~\mathrm{GeV}$ and $m_{s} = 150 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 1000 ~\mathrm{GeV}$ and $m_{s} = 400 ~\mathrm{GeV}$.

Expected exclusion regions for the EWK-singlet model with m_S = 300 GeV. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Expected exclusion regions for the EWK-singlet model with m_S = 400 GeV. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Expected exclusion regions for the EWK-singlet model with m_S = 500 GeV. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Expected exclusion regions for the EWK-singlet model for tan &beta; = 1. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Expected exclusion regions for the EWK-singlet model for tan &beta; = 2. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Expected exclusion regions for the EWK-singlet model with tan &beta; = 5.0. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Expected exclusion regions in the hMSSM model

Expected exclusion regions (+1 sigma band) in the hMSSM model

Expected exclusion regions (-1 sigma band) in the hMSSM model

Observed exclusion regions in the EWK-singlet model for m_S= 260 GeV. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Observed exclusion regions for the EWK-singlet model with m_S = 300 GeV. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Observed exclusion regions for the EWK-singlet model with m_S = 400 GeV. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Observed exclusion regions for the EWK-singlet model with m_S = 500 GeV. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Observed exclusion regions for the EWK-singlet model for tan &beta; = 1. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Observed exclusion regions for the EWK-singlet model for tan &beta; = 2. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Observed exclusion regions for the EWK-singlet model with tan &beta; = 5.0. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Observed exclusion regions in the hMSSM model

Signal acceptance times efficiency as a function of &kappa;_&lambda; for the $b\bar{b}b\bar{b}$, $b\bar{b}\tau^{+}\tau^{-}$ and $b\bar{b}\gamma\gamma$ analyses. The $b\bar{b}b\bar{b}$ curve is the average of the 2015 and 2016 curves weighted by the integrated luminosities of the two datasets

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-0 heavy scalar

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-0 heavy scalar

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-0 heavy scalar

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-0 heavy scalar

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-0 heavy scalar

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-0 heavy scalar

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-0 heavy scalar

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-0 heavy scalar

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-0 heavy scalar

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 1

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 1

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 1

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 1

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 1

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 1

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 2

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 2

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 2

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 2

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 2

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 2

Observed 95% CL exclusion limits for simplified models with direct stau pair production in SR-lowMass.

Expected 95% CL exclusion limits for simplified models with direct stau pair production in SR-lowMass.

The observed 95% CL exclusion contours for the combined fit of SR-lowMass and SR-highMass for simplified models with ${\tilde{\tau}}_L {\tilde{\tau}}_L$ only production.

The expected 95% CL exclusion contours for the combined fit of SR-lowMass and SR-highMass for simplified models with ${\tilde{\tau}}_L {\tilde{\tau}}_L$ only production.

The observed upper limits on the model cross-section in units of pb for simplified models with ${\tilde{\tau}}_L {\tilde{\tau}}_L$ only production. Three points at $M({\tilde{\chi}}^{0}_{1})=200GeV$ were removed from the plot but kept in the table because they overlapped with the plot's legend and are far from the exclusion contour.

Observed 95% CL exclusion limits for simplified models with direct stau pair production in SR-highMass.

Expected 95% CL exclusion limits for simplified models with direct stau pair production in SR-highMass.

The $E_{T}^{miss}$ post-fit distributions in the multi-jet background validation region VR-F (highMass). The stacked histograms show the contribution of each relevant SM process. The multi-jet shape is taken from VR-E in the ABCD method and the normalization is determined by the transfer factor $T$ and rescaled by a correction factor determined by the fit. The hatched bands represent the combined statistical and systematic uncertainties in the sum of the SM backgrounds shown. For illustration, the distributions of the SUSY reference points are also shown as dashed lines.

The $m_{T2}$ post-fit distributions in the multi-jet background validation VR-F (highMass). The stacked histograms show the contribution of each relevant SM process. The multi-jet shape is taken from VR-E in the ABCD method and the normalization is determined by the transfer factor $T$ and rescaled by a correction factor determined by the fit. The hatched bands represent the combined statistical and systematic uncertainties in the sum of the SM backgrounds shown. For illustration, the distributions of the SUSY reference points are also shown as dashed lines.

The $E_{T}^{miss}$ post-fit distributions in the multi-jet background validation region VR-F (lowMass). The stacked histograms show the contribution of each relevant SM process. The multi-jet shape is taken from VR-E in the ABCD method and the normalization is determined by the transfer factor $T$ and rescaled by a correction factor determined by the fit. The hatched bands represent the combined statistical and systematic uncertainties in the sum of the SM backgrounds shown. For illustration, the distributions of the SUSY reference points are also shown as dashed lines.

The $m_{T2}$ post-fit distributions in the multi-jet background validation region VR-F (lowMass). The stacked histograms show the contribution of each relevant SM process. The multi-jet shape is taken from VR-E in the ABCD method and the normalization is determined by the transfer factor $T$ and rescaled by a correction factor determined by the fit. The hatched bands represent the combined statistical and systematic uncertainties in the sum of the SM backgrounds shown. For illustration, the distributions of the SUSY reference points are also shown as dashed lines.

Signal acceptance in SR highMass for combined stau final states

Signal acceptance in SR lowMass for combined stau final states

Observed and expected numbers of events in the control and signal regions where all control and signal region bins are included as constraints in the likelihood. The expected event yields of SM processes are given after the background-only fit. The entries marked as "--" are negligible. The uncertainties correspond to the sum in quadrature of statistical and systematic uncertainties. The correlation of systematic uncertainties among control regions and among background processes is fully taken into account.

Cutflow for two reference points (${\tilde{\tau}}^{+}_{R,L} {\tilde{\tau}}^{-}_{R,L}$ production) in SR. The column labelled $N_{weighted}$ shows the results including all correction factors applied to simulation, and is normalised to 139 fb$^{-1}$, while $N_{raw}$ in brackets shows the results for the generated number of events. The quoted uncertainties are statistical only. The "Generator filter" includes the requirements that two $\tau$ in the event have ${p}_{T} > 15$ GeV and $|\eta| <$ 2.6. The "Baseline Cut" includes the requirement of two baseline $\tau$ with a minimum value at 0.01 of the boosted decision tree discriminant (JetBDTSigTransMin $>$ 0.01) and ${p}_{T, \tau_{1}} > 50$ GeV and ${p}_{T, \tau_{2}} > 40$ GeV. At the step "Trigger & offline cuts", the following requirements are applied: the event is recorded using the asymmetric di-$\tau$ trigger (di-$\tau$ $E_{T}^{miss}$ trigger) in SR-lowMass (SR-highMass), and the lepton $p_{T}$ and $E_{T}^{miss}$ are required at plateau.

Signal acceptance*efficiency in SR highMass for combined stau final states

Signal acceptance*efficiency in SR lowMass for combined stau final states

Signal efficiency in SR highMass for combined stau final states

Signal efficiency in SR lowMass for combined stau final states

The post-fit $m_{T2}$ distribution for SR-highMass. The stacked histograms show the expected SM backgrounds. The multi-jet contribution is estimated from data using the ABCD method. The contributions of multi-jet and $W$+jets events are scaled with the corresponding normalization factors derived from the background-only fit. The hatched bands represent the sum in quadrature of systematic and statistical uncertainties of the total SM background. For illustration, the distributions from the SUSY reference points are also shown as dashed lines. The last bin includes the overflow events.

The post-fit $m_{T2}$ distribution for SR-lowMass. The stacked histograms show the expected SM backgrounds. The multi-jet contribution is estimated from data using the ABCD method. The contributions of multi-jet and $W$+jets events are scaled with the corresponding normalization factors derived from the background-only fit. The hatched bands represent the sum in quadrature of systematic and statistical uncertainties of the total SM background. For illustration, the distributions from the SUSY reference points are also shown as dashed lines. The last bin includes the overflow events.

The post-fit yields in the $WVR$, $TVRs$, $ZVRs$ and $VVVRs$. The SM backgrounds other than multi-jet production are estimated from MC simulation. The multi-jet contribution is negligible and is estimated from data using the ABCD method, using CRs obtained with the same technique used for the SRs. The hatched bands represent the combined statistical and systematic uncertainties of the total SM background. For illustration, the distributions of the SUSY reference points are also shown as dashed lines. The lower panels show the ratio of data to the SM background estimate.

The pre-fit $m_{T2}$ distribution in the $WCR$. The SM backgrounds other than multi-jet production are estimated from MC simulation. The multi-jet contribution is estimated from data using the OS--SS method. The hatched bands represent the combined statistical and systematic uncertainties of the total SM background. For illustration, the distributions of the SUSY reference points are also shown as dashed lines.

transmax region : Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

away region : Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

Figure 09b, mean nTracks toward, toward region: Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

transverse region: Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

Figure 09a, mean nTracks transmin, transmin region: Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

transmax region: Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

away region: Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

Figure 10b, mean meanPt toward, toward region : Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

transverse region : Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

Figure 10a, mean meanPt transmin, transmin region : Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

transmax region : Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

away region : Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

Figure 04c from auxiliary figures, mean sumPt toward low thrust, toward region : low thrust ($T<0.75$) Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

transverse region : low thrust ($T<0.75$) Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

Figure 11c, mean sumPt transmin low thrust, transmin region : low thrust ($T<0.75$) Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

transmax region : low thrust ($T<0.75$) Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

away region : low thrust ($T<0.75$) Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

Figure 04a from auxiliary figures, mean nTracks toward low thrust, toward region : low thrust ($T<0.75$) Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

transverse region : low thrust ($T<0.75$) Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

Figure 11a, mean nTracks transmin low thrust, transmin region : low thrust ($T<0.75$) Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

transmax region : low thrust ($T<0.75$) Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

away region : low thrust ($T<0.75$) Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

Figure 06a from auxiliary figures, mean meanPt toward low thrust, toward region : low thrust ($T<0.75$) Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

transverse region : low thrust ($T<0.75$) Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

Figure 12a, mean meanPt transmin low thrust, transmin region : low thrust ($T<0.75$) Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

transmax region : low thrust ($T<0.75$) Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

away region : low thrust ($T<0.75$) Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

Figure 04d from auxiliary figures, mean sumPt toward high thrust, toward region : hight thrust ($0.75\leq T$) Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

transverse region : hight thrust ($0.75\leq T$) Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

Figure 11d, mean sumPt transmin high thrust, transmin region : hight thrust ($0.75\leq T$) Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

transmax region : hight thrust ($0.75\leq T$) Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

away region : hight thrust ($0.75\leq T$) Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

Figure 04b from auxiliary figures, mean nTracks toward high thrust, toward region : hight thrust ($0.75\leq T$) Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

transverse region : hight thrust ($0.75\leq T$) Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

Figure 11b, mean nTracks transmin high thrust, transmin region : hight thrust ($0.75\leq T$) Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

transmax region : hight thrust ($0.75\leq T$) Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

away region : hight thrust ($0.75\leq T$) Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

Figure 06b from auxiliary figures, mean meanPt toward high thrust, toward region : hight thrust ($0.75\leq T$) Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

transverse region : hight thrust ($0.75\leq T$) Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

Figure 12b, mean meanPt transmin high thrust, transmin region : hight thrust ($0.75\leq T$) Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

transmax region : hight thrust ($0.75\leq T$) Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

away region : hight thrust ($0.75\leq T$) Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$0GeV<p_{T}^{Z}<10GeV$

Figure 01a from auxiliary figures, ptSpec toward_zptregion2, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$80GeV<p_{T}^{Z}<120GeV$

Figure 02a from auxiliary figures, ptSpec toward_zptregion7, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$0GeV<p_{T}^{Z}<10GeV$

Figure 04a, ptSpec transmin_zptregion2, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$80GeV<p_{T}^{Z}<120GeV$

Figure 05a, ptSpec transmin_zptregion7, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,toward region,$0GeV<p_{T}^{Z}<10GeV$

Figure 01b from auxiliary figures, nTracks toward_zptregion2, $\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,toward region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,toward region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,toward region,$80GeV<p_{T}^{Z}<120GeV$

Figure 02b from auxiliary figures, nTracks toward_zptregion7, $\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,toward region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,toward region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transverse region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transverse region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transverse region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transverse region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transverse region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transverse region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transverse region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transverse region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmin region,$0GeV<p_{T}^{Z}<10GeV$

Figure 04b, nTracks transmin_zptregion2, $\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmin region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmin region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmin region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmin region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmin region,$80GeV<p_{T}^{Z}<120GeV$

Figure 05b, nTracks transmin_zptregion7, $\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmin region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmin region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmax region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmax region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmax region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmax region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmax region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmax region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmax region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmax region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,away region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,away region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,away region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,away region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,away region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,away region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,away region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,away region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$0GeV<p_{T}^{Z}<10GeV$

Figure 01c from auxiliary figures, sumPt toward_zptregion2, $\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$80GeV<p_{T}^{Z}<120GeV$

Figure 02c from auxiliary figures, sumPt toward_zptregion7, $\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$0GeV<p_{T}^{Z}<10GeV$

Figure 04c, sumPt transmin_zptregion2, $\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$80GeV<p_{T}^{Z}<120GeV$

Figure 05c, sumPt transmin_zptregion7, $\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$0GeV<p_{T}^{Z}<10GeV$

Figure 01d from auxiliary figures, meanPt toward_zptregion2, $\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$80GeV<p_{T}^{Z}<120GeV$

Figure 02d from auxiliary figures, meanPt toward_zptregion7, $\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$0GeV<p_{T}^{Z}<10GeV$

Figure 04d, meanPt transmin_zptregion2, $\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$80GeV<p_{T}^{Z}<120GeV$

Figure 05d, meanPt transmin_zptregion7, $\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$0GeV<p_{T}^{Z}<10GeV$

Figure 03a from auxiliary figures, ptSpec toward_zptregion2 low thrust, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$80GeV<p_{T}^{Z}<120GeV$

Figure 03c from auxiliary figures, ptSpec toward_zptregion7 low thrust, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$0GeV<p_{T}^{Z}<10GeV$

Figure 06a, ptSpec transmin_zptregion2 low thrust, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$80GeV<p_{T}^{Z}<120GeV$

Figure 06c, ptSpec transmin_zptregion7 low thrust, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),toward region,$0GeV<p_{T}^{Z}<10GeV$

Figure 05a from auxiliary figures, nTracks toward_zptregion2 low thrust, $\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),toward region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),toward region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),toward region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),toward region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),toward region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transverse region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transverse region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transverse region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transverse region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transverse region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transverse region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transverse region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transverse region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmin region,$0GeV<p_{T}^{Z}<10GeV$

Figure 07a, nTracks transmin_zptregion2 low thrust, $\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmin region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmin region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmin region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmin region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmin region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmin region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmin region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmax region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmax region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmax region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmax region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmax region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmax region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmax region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmax region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),away region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),away region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),away region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),away region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),away region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),away region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),away region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),away region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),toward region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),toward region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),toward region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),toward region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),toward region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),toward region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transverse region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transverse region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transverse region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transverse region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transverse region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transverse region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transverse region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transverse region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmin region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmin region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmin region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmin region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmin region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmin region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmin region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmin region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmax region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmax region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmax region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmax region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmax region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmax region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmax region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmax region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),away region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),away region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),away region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),away region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),away region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),away region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),away region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),away region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$0GeV<p_{T}^{Z}<10GeV$

Figure 03b from auxiliary figures, ptSpec toward_zptregion2 high thrust, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$80GeV<p_{T}^{Z}<120GeV$

Figure 03d from auxiliary figures, ptSpec toward_zptregion7 high thrust, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$0GeV<p_{T}^{Z}<10GeV$

Figure 06b, ptSpec transmin_zptregion2 high thrust, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$80GeV<p_{T}^{Z}<120GeV$

Figure 06d, ptSpec transmin_zptregion7 high thrust, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),toward region,$0GeV<p_{T}^{Z}<10GeV$

Figure 05b from auxiliary figures, nTracks toward_zptregion2 high thrust, $\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),toward region,$40GeV<p_{T}^{Z}<60GeV$