The dihadron correlated yield normalized per radian per unit of pseudorapidity as function of $\Delta\eta$ in d+Au collisions on the away side (|$\Delta\phi$ - $\pi$| < $\pi$/3). Shown is the high FTPC-Au activity data. Trigger and associated particles have 1 < $p_T$ < 3 GeV/c and |$\eta$| < 1.

The dihadron correlated yield normalized per radian per unit of pseudorapidity as function of $\Delta\eta$ in d+Au collisions on the away side (|$\Delta\phi$ - $\pi$| < $\pi$/3). Shown is the high-activity data after subtracting the unscaled low-activity data. Trigger and associated particles have 1 < $p_T$ < 3 GeV/c and |$\eta$| < 1.

The dihadron correlated yield normalized per radian per unit of pseudorapidity as function of $\Delta\eta$ in d+Au collisions on the away side (|$\Delta\phi$ - $\pi$| < $\pi$/3). Shown is the high-activity data after subtracting the unscaled low-activity data. Trigger and associated particles have 1 < $p_T$ < 3 GeV/c and |$\eta$| < 1.

The dihadron correlated yield normalized per radian per unit of pseudorapidity as function of $\Delta\eta$ in d+Au collisions on the near (|$\Delta\phi$| < $\pi$/3) side. Shown is the high-activity data after subtracting the unscaled low-activity data. Trigger and associated particles have 1 < $p_T$ < 3 GeV/c and |$\eta$| < 1.

The dihadron correlated yield normalized per radian per unit of pseudorapidity as function of $\Delta\eta$ in d+Au collisions on the near (|$\Delta\phi$| < $\pi$/3, solid circles) and away side (|$\Delta\phi$ - $\pi$| < $\pi$/3, open circles). Shown are the (a) low and (b) high FTPC-Au activity data, and the high-activity data after subtracting the (c) unscaled. Trigger and associated particles have 1 < $p_T$ < 3 GeV/c and |$\eta$| < 1.

(a) The near-side jetlike correlated yield obtained from Gaussian fit as in Fig. 1 as function of the uncorrected dN/d$\eta$ at midrapidity measured in the TPC. Two event selections are used: FTPC-Au multiplicity and ZDC-Au energy. The curve is the result from a HIJING calculation.

(a) The near-side jetlike correlated yield obtained from Gaussian fit as in Fig. 1 as function of the uncorrected dN/d$\eta$ at midrapidity measured in the TPC. Two event selections are used: FTPC-Au multiplicity and ZDC-Au energy. The curve is the result from a HIJING calculation.

$p_T^{(a)}$ dependence. The ratio of the correlated yields in high over low FTPC-Au multiplicity events as a function of $p_T^{(a)}$ $p_T^{(t)}$ where $p_T^{(a)}$ $p_T^{(t)}$ is fixed.

$p_T^{(a)}$ dependence. The ratio of the correlated yields in high over low FTPC-Au multiplicity events as a function of $p_T^{(a)}$ $p_T^{(t)}$ where $p_T^{(a)}$ $p_T^{(t)}$ is fixed.

(a) The dihadron correlated yield normalized per radian per unit of pseudorapidity as a function of $\Delta\phi$ in d+Au collisions at high (0-20%) FTPC-Au multiplicities. Trigger and associated particles are 1 < $p_T$ < 3 GeV/c within 0.5 < |$\Delta\eta$| < 0.7. ZYAM positions are indicated with arrows.

(a) The dihadron correlated yield normalized per radian per unit of pseudorapidity as a function of $\Delta\phi$ in d+Au collisions at low (40-100%) FTPC-Au multiplicities. Trigger and associated particles are 1 < $p_T$ < 3 GeV/c within 0.5 < |$\Delta\eta$| < 0.7. ZYAM positions are indicated with arrows.multiplicity versus $\Delta\phi$.

The raw associated yield at high FTPC-Au multiplicity minus the unscaled ZYAM-subtracted correlated yields at low FTPC-Au multiplicity versus $\Delta\phi$.

The raw associated yield at high FTPC-Au multiplicity minus the scaled ZYAM-subtracted correlated yields at low FTPC-Au multiplicity versus $\Delta\phi$.

Inclusive jet $A_{LL}$ vs. parton jet $p_T$ for 0.5<|eta|<1.0.

The uncertainties on the parton jet pT values are strongly correlated across the bins. The point-to-point statistical and systematic uncertainties on the measured A_LL values given above are only weakly correlated among the bins. The correlation matrix for the quadrature sum of the point-to-point statistical and systematic uncertainties is given below. In that matrix, the order of the rows and columns matches the bin numbering above. In addition to the point-to-point statistical and systematic uncertainties, there are two systematic uncertainties that are common to all the measured A_LL values (and not included in the systematic uncertainty numbers quoted above): (a) +/-0.0005 vertical shift uncertainty from relative luminosity and (b) +/-6.5% vertical scale uncertainty from polarization.

$A_{LL}$ model predictions for |eta|<0.5.

$A_{LL}$ model predictions for 0.5<|eta|<1.0.

Mean $p_T$, leading in-jet charged particle.

Mean $p_T$, charged particle jets, $p^{ch.jet}_T > 5$ GeV, $|\eta^{ch.jet}| < 1.9$.

Charged jet rate, $p^\text{ch.jet}_T > 5$ GeV, $|\eta^{ch.jet}| < 1.9$.

Charged jet rate, $p^\text{ch.jet}_T > 30$ GeV, $|\eta^{ch.jet}| < 1.9$.

Jet $p_T$ spectrum, $|\eta^{ch.jet}| < 1.9$, $10 < N_\text{ch} \le 30$.

Jet $p_T$ spectrum, $|\eta^{ch.jet}| < 1.9$, $30 < N_\text{ch} \le 50$.

Jet $p_T$ spectrum, $|\eta^{ch.jet}| < 1.9$, $50 < N_\text{ch} \le 80$.

Jet $p_T$ spectrum, $|\eta^{ch.jet}| < 1.9$, $80 < N_\text{ch} \le 110$.

Jet $p_T$ spectrum, $|\eta^{ch.jet}| < 1.9$, $110 < N_\text{ch} \le 140$.

Intrajet ring $p_{T}$ density, $10 < N_\text{ch} \le 30$.

Intrajet ring $p_{T}$ density, $30 < N_\text{ch} \le 50$.

Intrajet ring $p_{T}$ density, $50 < N_\text{ch} \le 80$.

Intrajet ring $p_{T}$ density, $80 < N_\text{ch} \le 110$.

Intrajet ring $p_{T}$ density, $110 < N_\text{ch} \le 140$.

PT dependences of the differential multiplicities for 0.0080 < x_Bjorken < 0.0120 and 1.00 < Q^2 < 1.50 GeV^2 for Positive hadrons.

PT dependences of the differential multiplicities for 0.0080 < x_Bjorken < 0.0120 and 1.50 < Q^2 < 2.10 GeV^2 for Positive hadrons.

PT dependences of the differential multiplicities for 0.0120 < x_Bjorken < 0.0180 and 1.00 < Q^2 < 1.50 GeV^2 for Positive hadrons.

PT dependences of the differential multiplicities for 0.0120 < x_Bjorken < 0.0180 and 1.50 < Q^2 < 2.50 GeV^2 for Positive hadrons.

PT dependences of the differential multiplicities for 0.0120 < x_Bjorken < 0.0180 and 2.50 < Q^2 < 3.50 GeV^2 for Positive hadrons.

PT dependences of the differential multiplicities for 0.0180 < x_Bjorken < 0.0250 and 1.00 < Q^2 < 1.50 GeV^2 for Positive hadrons.

PT dependences of the differential multiplicities for 0.0180 < x_Bjorken < 0.0250 and 1.50 < Q^2 < 2.50 GeV^2 for Positive hadrons.

PT dependences of the differential multiplicities for 0.0180 < x_Bjorken < 0.0250 and 2.50 < Q^2 < 3.50 GeV^2 for Positive hadrons.

PT dependences of the differential multiplicities for 0.0180 < x_Bjorken < 0.0250 and 3.50 < Q^2 < 5.00 GeV^2 for Positive hadrons.

PT dependences of the differential multiplicities for 0.0250 < x_Bjorken < 0.0350 and 1.00 < Q^2 < 1.20 GeV^2 for Positive hadrons.

PT dependences of the differential multiplicities for 0.0250 < x_Bjorken < 0.0400 and 1.20 < Q^2 < 1.50 GeV^2 for Positive hadrons.

PT dependences of the differential multiplicities for 0.0250 < x_Bjorken < 0.0400 and 1.50 < Q^2 < 2.50 GeV^2 for Positive hadrons.

PT dependences of the differential multiplicities for 0.0250 < x_Bjorken < 0.0400 and 2.50 < Q^2 < 3.50 GeV^2 for Positive hadrons.

PT dependences of the differential multiplicities for 0.0250 < x_Bjorken < 0.0400 and 3.50 < Q^2 < 6.00 GeV^2 for Positive hadrons.

PT dependences of the differential multiplicities for 0.0400 < x_Bjorken < 0.0500 and 1.50 < Q^2 < 2.50 GeV^2 for Positive hadrons.

PT dependences of the differential multiplicities for 0.0400 < x_Bjorken < 0.0700 and 2.50 < Q^2 < 3.50 GeV^2 for Positive hadrons.

PT dependences of the differential multiplicities for 0.0400 < x_Bjorken < 0.0700 and 3.50 < Q^2 < 6.00 GeV^2 for Positive hadrons.

PT dependences of the differential multiplicities for 0.0400 < x_Bjorken < 0.0700 and 6.00 < Q^2 < 10.00 GeV^2 for Positive hadrons.

PT dependences of the differential multiplicities for 0.0700 < x_Bjorken < 0.1200 and 3.50 < Q^2 < 6.00 GeV^2 for Positive hadrons.

PT dependences of the differential multiplicities for 0.0700 < x_Bjorken < 0.1200 and 6.00 < Q^2 < 10.00 GeV^2 for Positive hadrons.

PT dependences of the differential multiplicities for 0.0045 < x_Bjorken < 0.0060 and 1.00 < Q^2 < 1.25 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0060 < x_Bjorken < 0.0080 and 1.00 < Q^2 < 1.30 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0060 < x_Bjorken < 0.0080 and 1.30 < Q^2 < 1.70 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0080 < x_Bjorken < 0.0120 and 1.00 < Q^2 < 1.50 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0080 < x_Bjorken < 0.0120 and 1.50 < Q^2 < 2.10 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0120 < x_Bjorken < 0.0180 and 1.00 < Q^2 < 1.50 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0120 < x_Bjorken < 0.0180 and 1.50 < Q^2 < 2.50 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0120 < x_Bjorken < 0.0180 and 2.50 < Q^2 < 3.50 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0180 < x_Bjorken < 0.0250 and 1.00 < Q^2 < 1.50 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0180 < x_Bjorken < 0.0250 and 1.50 < Q^2 < 2.50 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0180 < x_Bjorken < 0.0250 and 2.50 < Q^2 < 3.50 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0180 < x_Bjorken < 0.0250 and 3.50 < Q^2 < 5.00 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0250 < x_Bjorken < 0.0350 and 1.00 < Q^2 < 1.20 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0250 < x_Bjorken < 0.0400 and 1.20 < Q^2 < 1.50 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0250 < x_Bjorken < 0.0400 and 1.50 < Q^2 < 2.50 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0250 < x_Bjorken < 0.0400 and 2.50 < Q^2 < 3.50 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0250 < x_Bjorken < 0.0400 and 3.50 < Q^2 < 6.00 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0400 < x_Bjorken < 0.0500 and 1.50 < Q^2 < 2.50 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0400 < x_Bjorken < 0.0700 and 2.50 < Q^2 < 3.50 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0400 < x_Bjorken < 0.0700 and 3.50 < Q^2 < 6.00 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0400 < x_Bjorken < 0.0700 and 6.00 < Q^2 < 10.00 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0700 < x_Bjorken < 0.1200 and 3.50 < Q^2 < 6.00 GeV^2 for Negative hadrons.

PT dependences of the differential multiplicities for 0.0700 < x_Bjorken < 0.1200 and 6.00 < Q^2 < 10.00 GeV^2 for Negative hadrons.

Fitted average PTs for positive hadrons.

Fitted average PTs for negative hadrons.

(Color online.) $J/\psi$ RAA versus pT for several centrality bins for Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The statistical (systematic) uncertainties are shown with vertical bars (open boxes). The filled boxes about unity on the right show the size of the normalization uncertainty. PHENIX low-$p_{T}$ $J/\psi$ results [6] and STAR high-$p_{T}$ results in Cu+Cu collisions [15] are shown for comparison. The curves are from the predictions by Model I (Liu et al.) [11] and Model II (Zhao et al.) [12].

(Color online) $R_{AA}$ versus $N_{part}$ for high-$p_{T}$ $J/\psi$ in comparison with a) low-$p_{T}$ $J/\psi$ data from PHENIX [6], and high-$p_{T}$ $\pi^{\pm}$ from STAR [41, 42], and b) high-$p_{T}$ $J/\psi$ from CMS [8]. The statistical (systematic) uncertainties are shown in vertical bars (boxes). The shaded green band about unity shows the systematic uncertainties from $N_{bin}$ and the box about unity on the right shows the $R_{AA}$ normalization uncertainty from the statistical and global systematic uncertainties of the $p+p$ reference data. The percentage in the top horizontal axis of (a) and (b) refer to the collision centrality for high-$p_{T}$ $J/\psi$ data at the RHIC and LHC, respectively.

Toward $\sum p_\perp$ density vs $p_\perp^{\mu\mu}$.

Transverse $\sum p_\perp$ density vs $p_\perp^{\mu\mu}$.

Away $\sum p_\perp$ density vs $p_\perp^{\mu\mu}$.

Toward $\langle p_\perp \rangle$ vs $p_\perp^{\mu\mu}$.

Transverse $\langle p_\perp \rangle$ vs $p_\perp^{\mu\mu}$.

Away $\langle p_\perp \rangle$ vs $p_\perp^{\mu\mu}$.

Towards $+$ transverse $N_\text{chg}$ density vs $m_{\mu\mu}$, $p_\perp^{\mu\mu} < 5$ GeV.

Towards $+$ transverse $\sum p_\perp$ density vs $m_{\mu\mu}$, $p_\perp^{\mu\mu} < 5$ GeV.

Towards $+$ transverse $\langle p_\perp \rangle$ vs $m_{\mu\mu}$, $p_\perp^{\mu\mu} < 5$ GeV.

Toward $N_\text{chg}$.

Transverse $N_\text{chg}$.

Away $N_\text{chg}$.

Toward $p_\perp$.

Transverse $p_\perp$.

Away $p_\perp$.

Transverse $N_\text{chg}$, $p_\perp(\mu\mu) < 5$ GeV.

Transverse $p_\perp$, $p_\perp(\mu\mu) < 5$ GeV.

(Color online) Distribution of the product of the TPC reconstructed charge sign and 1/$p_{T}$ for candidates satisfying all the W signal selection criteria and $E^{e}_{T}$ > 25 GeV.

(Color online) Distributions of the invariant mass of pairs of oppositely charged $e^{\pm}$ candidates after sequentially applying the selection criteria described in Sec. IV A to both $e^{\pm}$ candidates.

(Color online) Distributions of the invariant mass of $Z/\gamma^{*} \to e^{+}e^{−}$ candidate events satisfying all selection criteria described in Sec. IVC. The $Z/\gamma^{*} \to e^{+}e^{−}$ MC distribution (dashed line) is shown for comparison. Note the larger bin widths relative to Fig. 7

(Color online) $E^{e}_{T}$ distribution of $W^{+}$ (top) and $W^{−}$ (bottom) candidate events, background components, and $W \to e\nu$ MC signal for comparison. Note the factor of two difference in the vertical scales.

(Color online) $E^{e}_{T}$ distribution of $W^{+}$ (top) and $W^{−}$ (bottom) candidate events, background components, and $W \to e\nu$ MC signal for comparison. Note the factor of two difference in the vertical scales.

(Color online) Lepton pseudorapidity distribution of $W^{+}$ (left) and $W^{−}$ (right) candidate events, background components, and $W \to e\nu$ MC signal for comparison.

(Color online) Lepton pseudorapidity distribution of $W^{+}$ (left) and $W^{−}$ (right) candidate events, background components, and $W \to e\nu$ MC signal for comparison.

(Color online) W cross section ratio, $R_{W}$, for the two $e^{\pm}$ pseudorapidity bins. Theory calculations at NLO from the fewz program using the MSTW08 and CTEQ 6.6 PDF sets (with 90% confidence level error eigenvector uncertainties) are shown for comparison.

Fully corrected average charged particle scalar PT Sum per unit of pseudorapidity and per radian as a function of the leading track-jet transverse momentum for proton-proton collisions at a centre-of-mass energy of 0.9 TeV.

Fully corrected average charged particle scalar PT Sum per unit of pseudorapidity and per radian as a function of the leading track-jet transverse momentum for proton-proton collisions at a centre-of-mass energy of 7 TeV.

Ratio of the fully corrected average charged particle scalar PT Sum at 7 TeV to that at 0.9 TeV.

Normalized multiplicity distribution of charged particles produced in proton-proton collisions at a center-of-mass energy of 0.9 TeV with the leading track-jet transverse momentum > 3 GeV.

Normalized multiplicity distribution of charged particles produced in proton-proton collisions at a center-of-mass energy of 7 TeV with the leading track-jet transverse momentum > 3 GeV.

Normalized multiplicity distribution of charged particles produced in proton-proton collisions at a center-of-mass energy of 7 TeV with the leading track-jet transverse momentum > 20 GeV.

Normalized scalar PT Sum distribution of charged particles produced in proton-proton collisions at a center-of-mass energy of 0.9 TeV with the leading track-jet transverse momentum > 3 GeV.

Normalized scalar PT Sum distribution of charged particles produced in proton-proton collisions at a center-of-mass energy of 7 TeV with the leading track-jet transverse momentum > 3 GeV.

Normalized scalar PT Sum distribution of charged particles produced in proton-proton collisions at a center-of-mass energy of 7 TeV with the leading track-jet transverse momentum > 20 GeV.

PT distribution of charged particles produced in proton-proton collisions at a center-of-mass energy of 0.9 TeV with the leading track-jet transverse momentum > 3 GeV.

PT distribution of charged particles produced in proton-proton collisions at a center-of-mass energy of 7 TeV with the leading track-jet transverse momentum > 3 GeV.

PT distribution of charged particles produced in proton-proton collisions at a center-of-mass energy of 7 TeV with the leading track-jet transverse momentum > 20 GeV.

The transverse momentum production spectra per NSD event spectra for LAMBDA mesons at 0.9 and 7 TeV.

The rapidity production spectra per NSD event spectra for XI- mesons at 0.9 and 7 TeV.

The transverse momentum production spectra per NSD event spectra for XI- mesons at 0.9 and 7 TeV.

Ratio of production rates per NSD event for LAMBDA and KS events as a function of transverse momentum.

Ratio of production rates per NSD event for XI- and LAMBDA events as a function of transverse momentum.

Ratio of production rates per NSD event for LAMBDA and KS events as a function of rapidity.

Ratio of production rates per NSD event for XI- and LAMBDA events as a function of rapidity.

Results from fitting the Tsallis function to the data at 0.9 TeV. See text of paper for details.

Results from fitting the Tsallis function to the data at 7 TeV. See text of paper for details.

Mean PT obtained from the DN/DPT distributions.

The central rapidity production rate and the integrated yields per NSD event at 0.9 TeV for |rapidity| < 2.

The central rapidity production rate and the integrated yields per NSD event at 7 TeV for |rapidity| < 2.

Mean transverse momentum as a function of the mass of the emitted particle.