Measured jet multiplicity distribution in the $W\mu\nu$+jets control region for the inclusive SR1 selection, compared to the background expectations. The latter include the global normalization factors extracted from the data. Where appropriate, the last bin of the distribution includes overflows.

Measured dilepton invariant mass distribution in the $Z\mu\mu$+jets control region for the inclusive SR1 selection, compared to the background expectations. The latter include the global normalization factors extracted from the data. Where appropriate, the last bin of the distribution includes overflows. P P --> Z0 JET(S) X.

Measured $E_{T}^{miss}$ distribution in the $Z\mu\mu$+jets control region for the inclusive SR1 selection, compared to the background expectations. The latter include the global normalization factors extracted from the data. Where appropriate, the last bin of the distribution includes overflows. P P --> Z0 JET(S) X.

Measured leading jet $p_{T}$ distribution in the $Z\mu\mu$+jets control region for the inclusive SR1 selection, compared to the background expectations. The latter include the global normalization factors extracted from the data. Where appropriate, the last bin of the distribution includes overflows. P P --> Z0 JET(S) X.

Measured jet multiplicity distribution in the $Z\mu\mu$+jets control region for the inclusive SR1 selection, compared to the background expectations. The latter include the global normalization factors extracted from the data. Where appropriate, the last bin of the distribution includes overflows. P P --> Z0 JET(S) X.

Measured transverse mass distribution in the $We\nu$+jets control region for the inclusive SR1 selection, compared to the background expectations. The latter include the global normalization factors extracted from the data. Where appropriate, the last bin of the distribution includes overflows.

Measured $E_{T}^{miss}$ distribution in the $We\nu$+jets control region for the inclusive SR1 selection, compared to the background expectations. The latter include the global normalization factors extracted from the data. Where appropriate, the last bin of the distribution includes overflows.

Measured leading jet $p_{T}$ distribution in the $We\nu$+jets control region for the inclusive SR1 selection, compared to the background expectations. The latter include the global normalization factors extracted from the data. Where appropriate, the last bin of the distribution includes overflows.

Measured jet multiplicity distribution in the $We\nu$+jets control region for the inclusive SR1 selection, compared to the background expectations. The latter include the global normalization factors extracted from the data. Where appropriate, the last bin of the distribution includes overflows.

Measured dilepton invariant mass distribution in the $Zee$+jets control region for the inclusive SR1 selection, compared to the background expectations. The latter include the global normalization factors extracted from the data. Where appropriate, the last bin of the distribution includes overflows.

Measured $E_{T}^{miss}$ distribution in the $Zee$+jets control region for the inclusive SR1 selection, compared to the background expectations. The latter include the global normalization factors extracted from the data. Where appropriate, the last bin of the distribution includes overflows.

Measured leading jet $p_{T}$ distribution in the $Zee$+jets control region for the inclusive SR1 selection, compared to the background expectations. The latter include the global normalization factors extracted from the data. Where appropriate, the last bin of the distribution includes overflows.

Measured jet multiplicity distribution in the $Zee$+jets control region for the inclusive SR1 selection, compared to the background expectations. The latter include the global normalization factors extracted from the data. Where appropriate, the last bin of the distribution includes overflows.

Measured distribution of the jet multiplicity for the SR1 selection compared to the SM expectations. The $Z\nu\nu$+jets contribution is shown as constrained by the $W\mu\nu$+jets control sample. Where appropriate, the last bin of the distribution includes overflows. The distribution of different ADD, WIMP and GMSB scenarios are included.

Measured distribution of $E_{T}^{miss}$ for the SR1 selection compared to the SM expectations. The $Z\nu\nu$+jets contribution is shown as constrained by the $W\mu\nu$+jets control sample. Where appropriate, the last bin of the distribution includes overflows. The distribution of different ADD, WIMP and GMSB scenarios are included.

Measured distribution of leading jet $p_{T}$ for the SR1 selection compared to the SM expectations. The $Z\nu\nu$+jets contribution is shown as constrained by the $W\mu\nu$+jets control sample. Where appropriate, the last bin of the distribution includes overflows. The distribution of different ADD, WIMP and GMSB scenarios are included.

Measured distribution of the leading jet $p_{T}$ to $E_{T}^{miss}$ ratio for the SR1 selection compared to the SM expectations. The $Z\nu\nu$+jets contribution is shown as constrained by the $W\mu\nu$+jets control sample. Where appropriate, the last bin of the distribution includes overflows. The distribution of different ADD, WIMP and GMSB scenarios are included.

Measured distribution of the jet multiplicity for SR7 selection compared to the SM expectations. The $Z\nu\nu$+jets contribution is shown as constrained by the $W\mu\nu$+jets control sample. Where appropriate, the last bin of the distribution includes overflows. The distribution of different ADD, WIMP and GMSB scenarios are included.

Measured distribution of the jet multiplicity for SR7 selection compared to the SM expectations. The $Z\nu\nu$+jets contribution is shown as constrained by the $W\mu\nu$+jets control sample. Where appropriate, the last bin of the distribution includes overflows. The distribution of different ADD, WIMP and GMSB scenarios are included.

Measured distribution of the leading jet $p_T$ for SR7 selection compared to the SM expectations. The $Z\nu\nu$+jets contribution is shown as constrained by the $W\mu\nu$+jets control sample. Where appropriate, the last bin of the distribution includes overflows. The distribution of different ADD, WIMP and GMSB scenarios are included.

Measured distribution of the leading jet $p_T$ for SR9 selection compared to the SM expectations. The $Z\nu\nu$+jets contribution is shown as constrained by the $W\mu\nu$+jets control sample. Where appropriate, the last bin of the distribution includes overflows. The distribution of different ADD, WIMP and GMSB scenarios are included.

Measured distribution of the leading jet $p_T$ to $E_{T}^{miss}$ ratio for SR7 selection compared to the SM expectations. The $Z\nu\nu$+jets contribution is shown as constrained by the $W\mu\nu$+jets control sample. Where appropriate, the last bin of the distribution includes overflows. The distribution of different ADD, WIMP and GMSB scenarios are included.

Measured distribution of the leading jet $p_T$ to $E_{T}^{miss}$ ratio for SR9 selection compared to the SM expectations. The $Z\nu\nu$+jets contribution is shown as constrained by the $W\mu\nu$+jets control sample. Where appropriate, the last bin of the distribution includes overflows. The distribution of different ADD, WIMP and GMSB scenarios are included.

Observed and expected 95$\%$ CL limit on the fundamental Planck scale in $4+n$ dimensions, $M_D$, as a function of the number of extra dimensions. In the figure the two results overlap. The shaded areas around the expected limit indicate the expected $\pm 1\sigma$ and $\pm 2\sigma$ ranges of limits in the absence of a signal. The 95$\%$ CL observed limits after the suppression of the events with $\hat{s} > M_D^2$ is applied (truncated) are also given.

Limits at 95% C.L. on the EFT suppression scale M* as a function of the WIMP mass m_chi, for the scalar operator D1. Results where EFT truncation is applied are also shown for couplings of 1 and the perturbative limit.

Limits at 95% C.L. on the EFT suppression scale M* as a function of the WIMP mass m_chi, for the vector operator D5. Results where EFT truncation is applied are also shown for couplings of 1 and the perturbative limit.

Limits at 95% C.L. on the EFT suppression scale M* as a function of the WIMP mass m_chi, for the axial vector operator D8. Results where EFT truncation is applied are also shown for couplings of 1 and the perturbative limit.

Limits at 95% C.L. on the EFT suppression scale M* as a function of the WIMP mass m_chi, for the tensor operator D9. Results where EFT truncation is applied are also shown for couplings of 1 and the perturbative limit.

Limits at 95% C.L. on the EFT suppression scale M* as a function of the WIMP mass m_chi, for the gluon operator D11. Results where EFT truncation is applied are also shown for couplings of 1 and the perturbative limit.

Limits at 95% C.L. on the EFT suppression scale M* as a function of the WIMP mass m_chi, for the gluon operator C5. Results where EFT truncation is applied are also shown for couplings of 1 and the perturbative limit.

Observed 95% CL limits on the suppression scale M* as a function of the mediator mass Mmed, assuming a Z'-like boson in a simplified model and a DM mass of 50 GeV and 400 GeV. The width of the mediator is varied between Mmed/3 and Mmed/8pi.

Observed 95% CL upper limits on the product of couplings of the simplified model vertex in the plane of mediator and WIMP mass (Mmed versus m_chi).

Upper limits at 90% C.L. on the WIMP-nucleon scattering cross section as a function of m_chi for spin-independent interactions, for a coupling strength of unity or the maximum value that keeps the model within its perturbative regime. The truncation procedure is applied for both cases.

Upper limits at 90% C.L. on the WIMP-nucleon scattering cross section as a function of m_chi for spin-dependent interactions, for a coupling strength of unity or the maximum value that keeps the model within its perturbative regime. The truncation procedure is applied for both cases.

Upper limits at 90% C.L. on the WIMP-nucleon annihilation cross section as a function of m_chi, for a coupling strength of unity or the maximum value that keeps the model within its perturbative regime. The truncation procedure is applied for both cases.

95$\%$ CL lower limits on the gravitino mass $m_{\tilde{G}}$ as a function of the squark mass $m_{\tilde{q}}$ for degenerate squark/gluino masses.

95$\%$ CL lower limits on the gravitino mass $m_{\tilde{G}}$ as a function of the squark mass $m_{\tilde{q}}$ for non-degenerate squark/gluino masses: $ m_{\tilde{g}} = 1/2 \times m_{\tilde{q}}$.

95$\%$ CL lower limits on the gravitino mass $m_{\tilde{G}}$ as a function of the squark mass $m_{\tilde{q}}$ for non-degenerate squark/gluino masses: $ m_{\tilde{g}} = 1/4 \times m_{\tilde{q}}$.

95$\%$ CL lower limits on the gravitino mass $m_{\tilde{G}}$ as a function of the squark mass $m_{\tilde{q}}$ for non-degenerate squark/gluino masses: $ m_{\tilde{g}} = 2 \times m_{\tilde{q}}$.

95$\%$ CL lower limits on the gravitino mass $m_{\tilde{G}}$ as a function of the squark mass $m_{\tilde{q}}$ for non-degenerate squark/gluino masses: $ m_{\tilde{g}} = 4 \times m_{\tilde{q}}$.

Observed and expected 95$\%$ CL upper limit on $\sigma \times {\rm{BR}}(H \to {\rm{invisible}})$ as a function of the Higgs boson mass.

Limits at 95% C.L. on the EFT suppression scale M* as a function of the WIMP mass m_chi, for the scalar operator C1. Results where EFT truncation is applied are also shown for couplings of 1 and the perturbative limit.

The acceptance-corrected excess dielectron mass spectra, normalized to the charged particle multiplicity at mid-rapidity dNch/dy, in Au+Au collisions at $\sqrt{s_{NN}}$ = 19.6 GeV. The dNch/dy values in Au+Au collisions at $\sqrt{s_{NN}}$ = 19.6 GeV are from Ref. [38]. The normalization uncertainty from the STAR measured dN/dy is about 10%, which is not shown in the table.

The acceptance-corrected excess dielectron mass spectra, normalized to the charged particle multiplicity at mid-rapidity dNch/dy, in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The dNch/dy values in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV are from Ref. [39]. The normalization uncertainty from the STAR measured dN/dy is about 10%, which is not shown in the table.

Integrated yields of the normalized dilepton excesses for 0.4 < $M^{ll}$ < 0.75 GeV/c$^2$ as a function of dNch/dy. From top to bottom: 0-80% Au+Au collisions at $\sqrt{s_{NN}}$ = 19.6 GeV, then 0-10%, 10-40%, 40-80% and 0-80% Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV.

Diffractive DIS dijet cross section measured differentially as a function of $\log x_P$. The global normalisation uncertainty of $7.8\%$ is not listed explicitly but is included in the total systematic uncertainty. The last two column show the correction factors for hadronisation and QED radiation, respectively. (Note: assume typo in Table 2 that $x_P$ really means $\log x_P$.).

Diffractive DIS dijet cross section measured differentially as a function of $z_P$. The global normalisation uncertainty of $7.8\%$ is not listed explicitly but is included in the total systematic uncertainty. The last two column show the correction factors for hadronisation and QED radiation, respectively.

Diffractive DIS dijet cross section measured differentially as a function of $p^{\ast}_{T,1}$.

Diffractive DIS dijet cross section measured differentially as a function of $p^{\ast}_{T,2}$.

Diffractive DIS dijet cross section measured differentially as a function of $\langle p^{\ast}_{T}\rangle$.

Diffractive DIS dijet cross section measured differentially as a function of $\Delta\eta^{\ast}$.

Diffractive DIS dijet cross section measured differentially as a function of $z_P$ and $Q^2$.

Diffractive DIS dijet cross section measured differentially as a function of $p^{\ast}_{\rm T,1}$ and $Q^2$.

Lower limits at 95% CL on the mass of $H_{\mathrm{L}}^{\pm \pm}$ and $H_{\mathrm{R}}^{\pm \pm}$ bosons, assuming a 100% branching ratio to $e^{\pm}e^{\pm}$, $e^{\pm}/\mu^{\pm}$ and $\mu^{\pm}\mu^{\pm}$ pairs. The $1\sigma$ variations are also shown for the expected limits.

Asymmetry results on $\vec e-^2$H parity-violating scattering from the PVDIS experiment at JLab, for RES IV settings.

Asymmetry results on $\vec e-^2$H parity-violating scattering from the PVDIS experiment at JLab, for RES III settings.

The fiducial efficiency for electrons and taus in different $\eta$ ranges ($\epsilon_{\mathrm{fid}}(\eta)$). For electrons from tau decays, the $\eta$ is that of the electron, not the tau. The uncertainties shown reflect the statistical uncertainties of the simulated samples only. UPDATE (18 MAY 2015): Updated fiducial lepton efficiencies.

Expected and observed event yields for the $H_{\mathrm{T}}^{\mathrm{leptons}}$ signal regions.

Expected and observed event yields for the minimum $p_{\mathrm{T}}^{\ell}$ signal regions.

Expected and observed event yields for the $b$-tag signal regions.

Expected and observed event yields for the inclusive $m_{\mathrm{eff}}$ signal regions.

Expected and observed event yields for the high-$E_{\mathrm{T}}^{\mathrm{miss}}$, $m_{\mathrm{eff}}$ signal regions.

Expected and observed event yields for the high-$m_{\mathrm{T}}^{W}$, $m_{\mathrm{eff}}$ signal regions.

Expected and observed event yields for the high-$H_{\mathrm{T}}^{\mathrm{jets}}$, $E_{\mathrm{T}}^{\mathrm{miss}}$ signal regions.

Expected and observed event yields for the low-$H_{\mathrm{T}}^{\mathrm{jets}}$, $E_{\mathrm{T}}^{\mathrm{miss}}$ signal regions.

Expected and observed limits, and corresponding $p$-values and significances (in standard deviations), for signal regions based on cuts on $H_{\mathrm{T}}^{\mathrm{leptons}}$.

Expected and observed limits, and corresponding $p$-values and significances (in standard deviations), for signal regions based on cuts on $p_{\mathrm{T}}^{\ell\mathrm{,min}}$.

Expected and observed limits, and corresponding $p$-values and significances (in standard deviations), for signal regions based on cuts on the number of $b$-tagged jets.

Expected and observed limits, and corresponding $p$-values and significances (in standard deviations), for signal regions based on cuts on $m_{\mathrm{eff}}$.

Expected and observed limits, and corresponding $p$-values and significances (in standard deviations), for signal regions based on cuts on $m_{\mathrm{eff}}$ [GeV]. All these signal regions have an additional requirement of $E_{\mathrm{T}}^{\mathrm{miss}}\geq 100$ GeV.

Expected and observed limits, and corresponding $p$-values and significances (in standard deviations), for signal regions based on cuts on $m_{\mathrm{eff}}$ [GeV]. All these signal regions have an additional requirement of $m_{\mathrm{T}}^{W}\geq 100$ GeV.

Expected and observed limits, and corresponding $p$-values and significances (in standard deviations), for signal regions based on cuts on $E_{\mathrm{T}}^{\mathrm{miss}}$. All these signal regions have an additional requirement of $H_{\mathrm{T}}^{\mathrm{jets}}\geq 150$ GeV.

Expected and observed limits, and corresponding $p$-values and significances (in standard deviations), for signal regions based on cuts on $E_{\mathrm{T}}^{\mathrm{miss}}$. All these signal regions have an additional requirement of $H_{\mathrm{T}}^{\mathrm{jets}} < 150$ GeV.

Trans.min. scalar pT sum density vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum density vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity density vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity density vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Away charged multiplicity density vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity density vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 0 - 5 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 5 - 10 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 10 - 20 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 20 - 50 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 50 - 110 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 110 - 500 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity density vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 0 - 5 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 5 - 10 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 10 - 20 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 20 - 50 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 50 - 110 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 110 - 500 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 0 - 5 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 5 - 10 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 10 - 20 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 20 - 50 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 50 - 110 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 110 - 500 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 0 - 5 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 5 - 10 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 10 - 20 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 20 - 50 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 50 - 110 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 110 - 500 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 0 - 5 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 5 - 10 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 10 - 20 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 20 - 50 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 50 - 110 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 110 - 500 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 0 - 5 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 5 - 10 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 10 - 20 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 20 - 50 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 50 - 110 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 110 - 500 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards <mean pT(charged)> vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse <mean pT(charged)> vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Away <mean pT(charged)> vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Towards <mean pT(charged)> vs charged multiplicity, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse <mean pT(charged)> vs charged multiplicity, Born leptons : Statistical and systematic errors are added in quadrature.

Away <mean pT(charged)> vs charged multiplicity, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 0 - 5 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 5 - 10 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 10 - 20 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 20 - 50 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 50 - 110 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 110 - 500 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.diff. scalar pT sum density vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.diff. charged multiplicity density vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 0 - 5 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 5 - 10 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 10 - 20 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 20 - 50 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 50 - 110 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 110 - 500 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Away scalar pT sum density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Away charged multiplicity density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 0 - 5 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 5 - 10 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 10 - 20 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 20 - 50 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 50 - 110 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 110 - 500 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 0 - 5 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 5 - 10 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 10 - 20 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 20 - 50 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 50 - 110 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 110 - 500 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 0 - 5 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 5 - 10 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 10 - 20 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 20 - 50 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 50 - 110 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 110 - 500 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 0 - 5 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 5 - 10 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 10 - 20 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 20 - 50 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 50 - 110 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 110 - 500 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 0 - 5 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 5 - 10 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 10 - 20 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 20 - 50 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 50 - 110 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 110 - 500 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 0 - 5 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 5 - 10 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 10 - 20 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 20 - 50 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 50 - 110 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 110 - 500 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards <mean pT(charged)> vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse <mean pT(charged)> vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Away <mean pT(charged)> vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards <mean pT(charged)> vs charged multiplicity, dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse <mean pT(charged)> vs charged multiplicity, dressed leptons : Statistical and systematic errors are added in quadrature.

Away <mean pT(charged)> vs charged multiplicity, dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 0 - 5 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 5 - 10 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 10 - 20 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 20 - 50 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 50 - 110 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 110 - 500 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.diff. scalar pT sum density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.diff. charged multiplicity density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 0 - 5 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 5 - 10 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 10 - 20 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 20 - 50 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 50 - 110 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 110 - 500 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Reconstructed $\cos\theta^*$ distributions for data and the SM background estimate in the dimuon channel.

Reconstructed $A_{\rm FB}$ distributions for data and the SM background estimate as a function of dielectron mass.

Reconstructed $A_{\rm FB}$ distributions for data and the SM background estimate as a function of dimuon mass.

Summary of 95% C.L. lower exclusion limits on $\Lambda$ for the combined dilepton contact interaction search, using a uniform positive prior in 1/$\Lambda^2$.

Summary of 95% C.L. lower exclusion limits on $M_{\rm S}$ for the combined dilepton ADD large extra dimensions search, using a uniform positive prior in 1/$M_{\rm S}^8$.

Reconstructed $\cos\theta^*$ distributions for data and the SM background estimate in the electron channel.

Reconstructed $\cos\theta^*$ distributions for data and the SM background estimate in the muon channel.