$I_{dAu}$ vs. $p_T^{assoc}$ for different centrality, $p_T^{trig}$ and $\eta^{trig}$ bins.

The ratio of correlation peak widths between $d + Au$ and $p + p$ collisions. Only statistic errors are shown.

The ratio of correlation peak widths between $d + Au$ and $p + p$ collisions. Only statistic errors are shown.

Nuclear modification factor $R_{AA}$ in 10% most central $Au$+$Au$ collisions.

Nuclear modification factor $R_{dA}$ for ($h^+$+$h^-$)/2 in minimum bias $d$+$Au$.

$R_{AA}$ in the 10% most central $Au$+$Au$ collisions.

$R_{dA}$ for ($h^+$+$h^-$)/2 measurement in $d$+$Au$.

$R_{dA}$ for $\pi^0$ measurement in $d$+$Au$.

Ratio of $R_{dA}$ in minimum bias $d$+$Au$ and $R_{pA}$ from neutron tagged $d$+$Au$ collisions for ($h^+$+$h^-$)/2.

Ratio of $R_{dA}$ in minimum bias $d$+$Au$ and $R_{pA}$ from neutron tagged $d$+$Au$ collisions for $\pi^0$

<p>Charged hadron spectra for centrality selected d+Au collisions.</p>

<p>Charged hadron spectra for centrality selected d+Au collisions.</p>

<p>Charged hadron spectra for centrality selected N+Au collisions. All centralities.</p>

<p>Charged hadron spectra for centrality selected N+Au collisions. Centrality A (Central).</p>

<p>Charged hadron spectra for centrality selected N+Au collisions. Centrality B.</p>

<p>Charged hadron spectra for centrality selected N+Au collisions. Centrality C.</p>

<p>Charged hadron spectra for centrality selected N+Au collisions. Centrality D (Peripheral).</p>

<p>$R_{dAu}$ as a function of $p_T$.</p>

<p>$R_{dAu}$ as a function of $p_T$.</p>

<p>$R_{dAu}$ as a function of $p_T$.</p>

<p>$R_{dAu}$ as a function of $p_T$.</p>

<p>$R_{NAu}$ as a function of $p_T$. Centrality A (Peripheral).</p>

<p>$R_{NAu}$ as a function of $p_T$. Centrality B.</p>

<p>$R_{dAu}$ as a function of $p_T$. Centrality C.</p>

<p>$R_{dAu}$ as a function of $p_T$. Centrality D (Central).</p>

<p>$R_{dAu}$ values averaged in three momentum ranges as functions of $\nu−1$. Horizontal bars show the uncertainty in the value of $\nu$ for each centrality class.</p>

<p>$R_{NAu}$ values averaged in three momentum ranges as functions of $\nu−1$. Horizontal bars show the uncertainty in the value of $\nu$ for each centrality class.</p>

<p>Charged hadron spectra for centrality selected d+Au collisions.</p>

Fully corrected assorted $\pi^{0}$-hadron conditional pair distributions for $d$+Au collisions centrality 0-88% and $p$+$p$ collisions. The trigger $\pi^0$s are within 5 < $p_{T,trig}$ < 10 GeV/$c$ and are correlated with hadrons with $p_{T,assoc}$ of 1.5-2 GeV/$c$, 2-3GeV/$c$, 3-4 GeV/$c$, and 4-5 GeV/$c$.

Near- and far-side widths as a function of $p_{T, assoc}$ for charged hadron azimuthal correlations from minimumbias $d$+Au collisions.

Near-side width, far-side width as a function of $p_{T,assoc}$ for a charged pion and neutral pion triggers from the $p_{T,trig}$ range of 5-10 GeV/$c$ in minimum bias $d$+Au collisions.

Near-side width, far-side width as a function of $p_{T,assoc}$ for a charged pion and neutral pion triggers from the $p_{T,trig}$ range of 5-10 GeV/$c$ in minimum bias $d$+Au collisions.

Near- and far-side conditional yields as a function of $p_{T, assoc}$ for charged hadron triggers (2.5−4 GeV/$c$) and associated charged hadrons from $d$+Au collisions.

Near- and far-side conditional yields as a function of $p_{T, assoc}$ for charged hadron triggers (4−6 GeV/$c$) and associated charged hadrons from $d$+Au collisions.

Near- and far-side conditional yields as a function of $p_{T, assoc}$ for charged pion triggers (5−10 GeV/$c$) and associated charged hadrons from minimum-bias $d$+Au collisions.

Near- and far-side conditional yields as a function of $p_{T, assoc}$ for neutral pion triggers (5−10 GeV/$c$) and associated charged hadrons from minimum-bias $d$+Au collisions.

Near- and far-side widths and conditional yields as a function of $N_{coll}$ for charged hadron triggers (2.5−4 GeV/$c$) and associated charged hadrons (1–2.5 GeV/$c$) from $d$+Au collisions.

Near- and far-side widths and conditional yields as a function of centrality for neutral pion triggers (5−10 GeV/$c$) and associated charged hadrons (2–3 GeV/$c$) from $d$+Au collisions.

The extracted $\sqrt{<j^2_T>}$ for minimum-bias $d$+Au collisions from all four dihadron correlations. The trigger $p_T$ ranges are 3 - 5 GeV/$c$, 5 - 10 GeV/$c$ and 5 - 10 GeV/$c$ for $h^{\pm}$ - $h^{\pm}$, $\pi^0$ - $h^{\pm}$ and $\pi^{\pm}$ - $h^{\pm}$ assorted-$p_T$ correlations.

The extracted $\sqrt{<j^2_T>}$ for minimum-bias $d$+Au collisions from all four dihadron correlations. The trigger $p_T$ ranges are 3 - 5 GeV/$c$, 5 - 10 GeV/$c$ and 5 - 10 GeV/$c$ for $h^{\pm}$ - $h^{\pm}$, $\pi^0$ - $h^{\pm}$ and $\pi^{\pm}$ - $h^{\pm}$ assorted-$p_T$ correlations.

The extracted $\sqrt{<j^2_T>}$ for minimum-bias $d$+Au collisions from all four dihadron correlations. The trigger $p_T$ ranges are 3 - 5 GeV/$c$, 5 - 10 GeV/$c$ and 5 - 10 GeV/$c$ for $h^{\pm}$ - $h^{\pm}$, $\pi^0$ - $h^{\pm}$ and $\pi^{\pm}$ - $h^{\pm}$ assorted-$p_T$ correlations.

The extracted $\sqrt{<j^2_T>}$ for minimum-bias $d$+Au collisions from all four dihadron correlations. The trigger $p_T$ ranges are 3 - 5 GeV/$c$, 5 - 10 GeV/$c$ and 5 - 10 GeV/$c$ for $h^{\pm}$ - $h^{\pm}$, $\pi^0$ - $h^{\pm}$ and $\pi^{\pm}$ - $h^{\pm}$ assorted-$p_T$ correlations.

$<sin^2(\phi_{jj})>$ for minimum bias $d$+Au collisions as function of associated particle $p_T$ for $\pi^{\pm}$ - $h^{\pm}$ and $\pi^0$ - $h^{\pm}$ correlations where the trigger particles have a $p_T$ between 5 - 10 GeV/$c$.

$<sin^2(\phi_{jj})>$ for minimum bias $d$+Au collisions as function of associated particle $p_T$ for $\pi^{\pm}$ - $h^{\pm}$ and $\pi^0$ - $h^{\pm}$ correlations where the trigger particles have a $p_T$ between 5 - 10 GeV/$c$.

$<sin^2(\phi_{jj})>$ for minimum bias $d$+Au collisions as function of trigger particle $p_T$ for $\pi^{\pm}$ - $h^{\pm}$ and $\pi^0$ - $h^{\pm}$ correlations.

$<sin^2(\phi_{jj})>$ for minimum bias $d$+Au collisions as function of trigger particle $p_T$ for $\pi^{\pm}$ - $h^{\pm}$ and $\pi^0$ - $h^{\pm}$ correlations.

Near-side and far-side $p_{out}$ distributions for minimum bias $d$+Au collisions obtained from $\pi^{\pm}$ - $h^{\pm}$ correlation. The trigger is 5 < $p_{T,trig}$ < 10 GeV/$c$, the associated particle is 0.5 < $p_{T,assoc}$ < 5.0 GeV/$c$.

Conditional yield as a function of $x_E$ for near-side and far-side for $\pi^{\pm}$ - $h^{\pm}$ and $\pi^0$ - $h^{\pm}$ from minimum-bias $d$+Au collisions.

Conditional yield as a function of $x_E$ for near-side and far-side for $\pi^{\pm}$ - $h^{\pm}$ and $\pi^0$ - $h^{\pm}$ from minimum-bias $d$+Au collisions.

Conditional yield as a function of $x_E$ for near-side and far-side correlations for $\pi^{\pm}$ - $h^{\pm}$ correlations from minimum-bias $d$+Au collisions. The trigger pions are 5 < $p_{T,trig}$ < 6 GeV/$c$.

Conditional yield as a function of $x_E$ for near-side and far-side correlation for $\pi^{\pm}$ - $h^{\pm}$ correlation for several different trigger $p_T$s for minimum-bias $d$+Au collisions.

Far-side conditional yield as a function of $p_{T,trig}$ for different ranges of $x_E$ for $\pi^{\pm}$ - $h^{\pm}$ correlation for minimum-bias $d$+Au collisions.

Far-side conditional yield as a function of $p_{T,trig}$ for different ranges of $x_E$ for $\pi^{\pm}$ - $h^{\pm}$ correlation for minimum-bias $d$+Au collisions.

Far-side conditional yield as a function of $p_{T,trig}$ for different ranges of $x_E$ for $\pi^{\pm}$ - $h^{\pm}$ correlation for minimum-bias $d$+Au collisions.

Far-side conditional yield as a function of $p_{T,trig}$ for different ranges of $x_E$ for $\pi^{\pm}$ - $h^{\pm}$ correlation for minimum-bias $d$+Au collisions.

The comparison of the $\sqrt{<j^2_T>}$ values between $d$+Au and $p$+$p$ for the $\pi^{\pm}$ - $h^{\pm}$ correlations and $\pi^0$ - $h^{\pm}$ correlations. The trigger pion range is 5 - 10 GeV/$c$.

The comparison of the $\sqrt{<j^2_T>}$ values between $d$+Au and $p$+$p$ for the $\pi^{\pm}$ - $h^{\pm}$ correlations and $\pi^0$ - $h^{\pm}$ correlations. The trigger pion range is 5 - 10 GeV/$c$.

Quadrature difference between minimum-bias $d$+Au and $p$+$p$ $<sin^2(\phi_{jj})>$ values.

Quadrature difference between minimum-bias $d$+Au and $p$+$p$ $<sin^2(\phi_{jj})>$ values.

The comparison of the $p_{out}$ distribution at the near-side and far-side between central $d$+Au collisions and $p$+$p$ collisions. Results are obtained for $\pi^{\pm}$ - $h^{\pm}$ correlations with the associated hadron range 0.5 < $p_{T,assoc}$ < 5 GeV/$c$ and trigger pion range of 5 < $p_{T,trig}$ < 10 GeV/$c$.

The comparison of the $x_E$ distribution from $\pi^{\pm}$ - $h^{\pm}$ correlation at the near-side and far-side between minimum bias $d$+Au collisions and $p$+$p$ collisions. The trigger $\pi^{\pm}$ are from 5 - 10 GeV/$c$.

Far-side conditional yield as a function of $p_{T,trig}$ for different ranges of $x_E$ from $p$+$p$ collisions, triggers are $\pi^{\pm}$ from 5 - 10 GeV/$c$.

Far-side conditional yield as a function of $p_{T,trig}$ for different ranges of $x_E$ from $p$+$p$ collisions, triggers are $\pi^{\pm}$ from 5 - 10 GeV/$c$.

Far-side conditional yield as a function of $p_{T,trig}$ for different ranges of $x_E$ from $p$+$p$ collisions, triggers are $\pi^{\pm}$ from 5 - 10 GeV/$c$.

The fitted fractional change in $dN/d_{x_E}$ per unit $p_{T,trig}$ of the far-side conditional yield for different ranges of $x_E$.

Centrality dependent near and far $CY(p_T)$ for $\pi^{\pm}$ - $h^{\pm}$ correlations and $\pi^0$ - $h^{\pm}$ correlations.

Centrality dependent near and far $CY(p_T)$ for $\pi^{\pm}$ - $h^{\pm}$ correlations and $\pi^0$ - $h^{\pm}$ correlations.

Centrality dependence to the ratio of near and far $CY(p_T)$ for $d$+Au to $p$+$p$.

Centrality dependence to the ratio of near and far $CY(p_T)$ for $d$+Au to $p$+$p$.

$\Delta\phi$ distributions for meson triggers with 2.5 < $p_T$ < 4.0 GeV/$c$ and associated charged hadrons with 1.7 < $p_T$ < 2.5 GeV/$c$ for 60-70% centrality in Au+Au collisions.

$\Delta\phi$ distributions for baryon triggers with 2.5 < $p_T$ < 4.0 GeV/$c$ and associated charged hadrons with 1.7 < $p_T$ < 2.5 GeV/$c$ for 60-70% centrality in Au+Au collisions.

Combinatorial Background Levels from Figure 1 Top Panels.

Combinatorial Background Levels from Figure 1 Bottom Panels.

Trigger Particle $v_2$ values.

Partner Particle $v_2$ values.

Yield per trigger for associated charged hadrons between 1.7 < $p_T$ < 2.5 GeV/$c$ for the near- (top) and away- (bottom) side jets.

Yield per trigger for associated charged hadrons between 1.7 < $p_T$ < 2.5 GeV/$c$ for the near- (top) and away- (bottom) side jets.

Uncertainties in Figure 2 as a function of $N_{part}$ and trigger type for AuAu and $d$+Au.

Uncertainties in Figure 2 as a function of $N_{part}$ and trigger type for AuAu and $d$+Au.

$p_T$ spectra of the near side associated charged hadrons corrected to the full jet yield for meson triggers at 2.5 < $p_T$ < 4.0 GeV/$c$ and $|\eta|$ < 0.35 for six centralities in Au+Au and $d$+Au collisions.

$p_T$ spectra of the near side associated charged hadrons corrected to the full jet yield for meson triggers at 2.5 < $p_T$ < 4.0 GeV/$c$ and $|\eta|$ < 0.35 for six centralities in Au+Au and $d$+Au collisions.

$p_T$ spectra of the near side associated charged hadrons corrected to the full jet yield for baryon triggers at 2.5 < $p_T$ < 4.0 GeV/$c$ and $|\eta|$ < 0.35 for six centralities in Au+Au, $d$+Au and $p$+$p$ collisions.

Inverse slopes from the fits in Figure 3.

Inverse slopes from the fits in Figure 3.

Inverse slopes from the fits in Figure 3.

Invariant cross section of $\omega$ production in $p$+$p$ and $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV measured in $\omega \rightarrow \pi^0\pi^+\pi^-$ and $\omega \rightarrow \pi^0\gamma$ decay channels.

Invariant cross section of $\omega$ production in $p$+$p$ and $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV measured in $\omega \rightarrow \pi^0\pi^+\pi^-$ and $\omega \rightarrow \pi^0\gamma$ decay channels.

Invariant cross section of $\omega$ production in $p$+$p$ and $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV measured in $\omega \rightarrow \pi^0\pi^+\pi^-$ and $\omega \rightarrow \pi^0\gamma$ decay channels.

Measured $\omega/{\pi^0}$ vs $p_T$ in $p$+$p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV.

Measured $\omega/{\pi^0}$ vs $p_T$ in $p$+$p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV.

Measured $\omega/{\pi^0}$ vs $p_T$ in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV.

Measured $\omega/{\pi^0}$ vs $p_T$ in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV.

Measured $R_{dA}$ vs $p_T$ for neutral mesons in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV for minimum bias.

Measured $R_{dA}$ vs $p_T$ for neutral mesons in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV for minimum bias.

Measured $R_{dA}$ vs $p_T$ for neutral mesons in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV for 0-20% centrality.

Measured $R_{dA}$ vs $p_T$ for neutral mesons in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV for 0-20% centrality.

Reconstructed $\omega$ mass measured in the $\pi^0\pi^+\pi^-$ decay channel vs $p_T$ in $p$+$p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV.

Reconstructed $\omega$ mass measured in the $\pi^0\pi^+\pi^-$ decay channel vs $p_T$ in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV.

Cross sections at mid-rapidity in $p$+$p$ and $d$+Au collisions as a function of $p_T$.

Cross sections at mid-rapidity in $p$+$p$ and $d$+Au collisions as a function of $p_T$.

Cross sections at mid-rapidity in $p$+$p$ and $d$+Au collisions as a function of $p_T$.

Cross sections at mid-rapidity in $p$+$p$ and $d$+Au collisions as a function of $p_T$.

Nuclear modification factor $R_{dA}$ for $\pi^0$ and $\eta$ in differenet centrality selections and min. bias data.

Nuclear modification factor $R_{dA}$ for $\pi^0$ and $\eta$ in differenet centrality selections and min. bias data.

Nuclear modification factor $R_{dA}$ for $\pi^0$ and $\eta$ in differenet centrality selections and min. bias data.

Measured widths of the near- and away-angle $\pi^0$ - $h^{\pm}$ correlation peaks for various trigger momenta.

Measured widths of the near- and away-angle $\pi^0$ - $h^{\pm}$ correlation peaks for various trigger momenta.

Measured widths of the near- and away-angle $\pi^0$ - $h^{\pm}$ correlation peaks for various trigger momenta.

The $\sigma_N$ and $\sigma_A$ values in GeV/$c$.

The $\sqrt{<p^2_{out}>}$ values in GeV/$c$.

The $\sqrt{<p^2_{out}>}$ values in GeV/$c$.

The $\sqrt{<p^2_{out}>}$ values in GeV/$c$.

The near and away side conditional yield per number of triggers for 1.4 < $p_{Ta}$ < 5.0 GeV/$c$.

The $\sqrt{<j^2_T>}$ values in GeV/$c$.

The $\sqrt{<j^2_T>}$ values in GeV/$c$.

The $\sqrt{<j^2_T>}$ values in GeV/$c$.

The $\sqrt{<j^2_T>}$ values in GeV/$c$.

Measured $x_E$ distributions associated with various transverse momenta of the trigger $\pi^0$.

Measured $x_E$ distributions associated with various transverse momenta of the trigger $\pi^0$.

Measured $x_E$ distributions associated with various transverse momenta of the trigger $\pi^0$.

Measured $x_E$ distributions associated with various transverse momenta of the trigger $\pi^0$.

Measured $x_E$ distributions associated with various transverse momenta of the trigger $\pi^0$.

Extracted values of $D(x)$ parameters according from the fit to the LEP data and power $n$ of the unmeasured final state parton spectra $\Sigma_q(\bar{p_T})$ extracted from the fit to the single inclusive $\pi^0$ invariant cross section for corresponding fragmentation and fixed values of $\sqrt{<k^2_T>}$ = 2.5 GeV/$c$.

The $\bar{x^-1_h}$ $<z_t>$ $\sqrt{<k^2_T>}$ $\sqrt{<k^2_T>}$ values as a function of $p_{Ta}$ for two different trigger $\pi^0$ transverse momentum bins.

The $\bar{x^-1_h}$ $<z_t>$ $\sqrt{<k^2_T>}$ $\sqrt{<k^2_T>}$ values as a function of $p_{Ta}$ for two different trigger $\pi^0$ transverse momentum bins.

Values of $\bar{x^-1_h}$ $<z_t>$ $\sqrt{<k^2_T>}$ and $\sqrt{<k^2_T>}$ for various trigger particle $p_{Tt}$ and associated momenta in 1.4 < $p_{Ta}$ < 5.0 GeV/$c$ region.

The $<z_t>$ and $\bar{x_h}$ values with $p_{Tt}$

The $<z_t>$ and $\bar{x_h}$ values with $p_{Ta}$ for two trigger $\pi^0$ momenta bins.

The $<z_t>$ and $\bar{x_h}$ values with $p_{Ta}$ for two trigger $\pi^0$ momenta bins.