V1Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-2% having the associated particle PT in the range 0.25-0.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V1Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-2% having the associated particle PT in the range 1-1.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V1Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-10% having the associated particle PT in the range 0.25-0.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V1Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-10% having the associated particle PT in the range 1-1.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V1Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-10% having the associated particle PT in the range 2-2.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V1Delta coefficients as a function of the trigger particle PT for events in the centrality class 40-50% having the associated particle PT in the range 0.25-0.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V1Delta coefficients as a function of the trigger particle PT for events in the centrality class 40-50% having the associated particle PT in the range 1-1.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V1Delta coefficients as a function of the trigger particle PT for events in the centrality class 40-50% having the associated particle PT in the range 2-2.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V2Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-2% having the associated particle PT in the range 0.25-0.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V2Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-2% having the associated particle PT in the range 1-1.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V2Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-10% having the associated particle PT in the range 0.25-0.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V2Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-10% having the associated particle PT in the range 1-1.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V2Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-10% having the associated particle PT in the range 2-2.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V2Delta coefficients as a function of the trigger particle PT for events in the centrality class 40-50% having the associated particle PT in the range 0.25-0.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V2Delta coefficients as a function of the trigger particle PT for events in the centrality class 40-50% having the associated particle PT in the range 1-1.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V2Delta coefficients as a function of the trigger particle PT for events in the centrality class 40-50% having the associated particle PT in the range 2-2.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V3Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-2% having the associated particle PT in the range 0.25-0.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V3Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-2% having the associated particle PT in the range 1-1.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V3Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-10% having the associated particle PT in the range 0.25-0.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V3Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-10% having the associated particle PT in the range 1-1.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V3Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-10% having the associated particle PT in the range 2-2.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V3Delta coefficients as a function of the trigger particle PT for events in the centrality class 40-50% having the associated particle PT in the range 0.25-0.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V3Delta coefficients as a function of the trigger particle PT for events in the centrality class 40-50% having the associated particle PT in the range 1-1.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V3Delta coefficients as a function of the trigger particle PT for events in the centrality class 40-50% having the associated particle PT in the range 2-2.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V4Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-2% having the associated particle PT in the range 0.25-0.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V4Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-2% having the associated particle PT in the range 1-1.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V4Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-10% having the associated particle PT in the range 0.25-0.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V4Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-10% having the associated particle PT in the range 1-1.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V4Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-10% having the associated particle PT in the range 2-2.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V4Delta coefficients as a function of the trigger particle PT for events in the centrality class 40-50% having the associated particle PT in the range 0.25-0.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V4Delta coefficients as a function of the trigger particle PT for events in the centrality class 40-50% having the associated particle PT in the range 1-1.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V4Delta coefficients as a function of the trigger particle PT for events in the centrality class 40-50% having the associated particle PT in the range 2-2.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V5Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-2% having the associated particle PT in the range 0.25-0.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V5Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-2% having the associated particle PT in the range 1-1.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V5Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-10% having the associated particle PT in the range 0.25-0.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V5Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-10% having the associated particle PT in the range 1-1.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V5Delta coefficients as a function of the trigger particle PT for events in the centrality class 0-10% having the associated particle PT in the range 2-2.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V5Delta coefficients as a function of the trigger particle PT for events in the centrality class 40-50% having the associated particle PT in the range 0.25-0.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V5Delta coefficients as a function of the trigger particle PT for events in the centrality class 40-50% having the associated particle PT in the range 1-1.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V5Delta coefficients as a function of the trigger particle PT for events in the centrality class 40-50% having the associated particle PT in the range 2-2.5 GeV. Note that in the paper the data are plotted multiplied by 100.

V1Delta for all pt combinations for the centrality classes 0-10% and 40-50%.

V2Delta for all pt combinations for the centrality classes 0-10% and 40-50%.

V3Delta for all pt combinations for the centrality classes 0-10% and 40-50%.

V4Delta for all pt combinations for the centrality classes 0-10% and 40-50%.

V5Delta for all pt combinations for the centrality classes 0-10% and 40-50%.

The global fit paramter v_2{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 0-2%.

The global fit paramter v_2{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 2-10%.

The global fit paramter v_2{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 10-20%.

The global fit paramter v_2{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 20-30%.

The global fit paramter v_2{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 30-40%.

The global fit paramter v_2{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 40-50%.

The global fit paramter v_3{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 0-2%.

The global fit paramter v_3{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 2-10%.

The global fit paramter v_3{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 10-20%.

The global fit paramter v_3{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 20-30%.

The global fit paramter v_3{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 30-40%.

The global fit paramter v_3{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 40-50%.

The global fit paramter v_4{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 0-2%.

The global fit paramter v_4{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 2-10%.

The global fit paramter v_4{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 10-20%.

The global fit paramter v_4{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 20-30%.

The global fit paramter v_4{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 30-40%.

The global fit paramter v_4{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 40-50%.

The global fit paramter v_5{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 0-2%.

The global fit paramter v_5{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 2-10%.

The global fit paramter v_5{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 10-20%.

The global fit paramter v_5{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 20-30%.

The global fit paramter v_5{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 30-40%.

The global fit paramter v_5{GF} vs. the trigger particle PT for fit range of 0.25-15 GeV/c for the centrality class 40-50%.

The global fit paramter v_1{GF} vs. the trigger particle PT for fit range of 0.25-5 GeV/c for the centrality class 0-20%.

The global fit paramter v_1{GF} vs. the trigger particle PT for fit range of 0.25-5 GeV/c for the centrality class 40-50%.

The global fit paramter v_2{GF} vs. the trigger particle PT for fit range of 0.25-5 GeV/c for the centrality class 0-20%.

The global fit paramter v_2{GF} vs. the trigger particle PT for fit range of 0.25-5 GeV/c for the centrality class 40-50%.

The global fit paramter v_3{GF} vs. the trigger particle PT for fit range of 0.25-5 GeV/c for the centrality class 0-20%.

The global fit paramter v_3{GF} vs. the trigger particle PT for fit range of 0.25-5 GeV/c for the centrality class 40-50%.

The global fit paramter v_4{GF} vs. the trigger particle PT for fit range of 0.25-5 GeV/c for the centrality class 0-20%.

The global fit paramter v_4{GF} vs. the trigger particle PT for fit range of 0.25-5 GeV/c for the centrality class 40-50%.

The global fit paramter v_5{GF} vs. the trigger particle PT for fit range of 0.25-5 GeV/c for the centrality class 0-20%.

The global fit paramter v_5{GF} vs. the trigger particle PT for fit range of 0.25-5 GeV/c for the centrality class 40-50%.

The global fit paramter v_1{GF} vs. the trigger particle PT for fit range of 5-15 GeV/c for the centrality class 0-20%.

The global fit paramter v_1{GF} vs. the trigger particle PT for fit range of 5-15 GeV/c for the centrality class 40-50%.

The global fit paramter v_2{GF} vs. the trigger particle PT for fit range of 5-15 GeV/c for the centrality class 0-20%.

The global fit paramter v_2{GF} vs. the trigger particle PT for fit range of 5-15 GeV/c for the centrality class 40-50%.

The global fit paramter v_3{GF} vs. the trigger particle PT for fit range of 5-15 GeV/c for the centrality class 0-20%.

The global fit paramter v_3{GF} vs. the trigger particle PT for fit range of 5-15 GeV/c for the centrality class 40-50%.

The global fit paramter v_4{GF} vs. the trigger particle PT for fit range of 5-15 GeV/c for the centrality class 0-20%.

The global fit paramter v_4{GF} vs. the trigger particle PT for fit range of 5-15 GeV/c for the centrality class 40-50%.

The global fit paramter v_5{GF} vs. the trigger particle PT for fit range of 5-15 GeV/c for the centrality class 0-20%.

The global fit paramter v_5{GF} vs. the trigger particle PT for fit range of 5-15 GeV/c for the centrality class 40-50%.

The global fit paramter v_1{GF} vs. the trigger particle PT for fit range of 0.25-1 GeV/c for the centrality class 0-10%.

The global fit paramter v_1{GF} vs. the trigger particle PT for fit range of 0.25-1 GeV/c for the centrality class 40-50%.

The global fit paramter v_2{GF} vs. the trigger particle PT for fit range of 0.25-1 GeV/c for the centrality class 0-10%.

The global fit paramter v_2{GF} vs. the trigger particle PT for fit range of 0.25-1 GeV/c for the centrality class 40-50%.

The global fit paramter v_1{GF} vs. the trigger particle PT for fit range of 2-4 GeV/c for the centrality class 0-10%.

The global fit paramter v_1{GF} vs. the trigger particle PT for fit range of 2-4 GeV/c for the centrality class 40-50%.

The global fit paramter v_2{GF} vs. the trigger particle PT for fit range of 2-4 GeV/c for the centrality class 0-10%.

The global fit paramter v_2{GF} vs. the trigger particle PT for fit range of 2-4 GeV/c for the centrality class 40-50%.

Elliptic flow versus $p_{T}$ for charged hadrons from Cu+Cu collisions at 0–60% centrality at $\sqrt{s_{NN}}$ = 22.4 GeV measured with the subevent method with a pseudorapidity gap of 0.3 units compared with previously published STAR results for 200 and 62.4 GeV Cu+Cu [27] measured with full TPC event plane method $v_{2}${TPC} and full FTPC event plane method $v_{2}${FTPC}. The error bars are statistical. Results are also compared to $v_{2}$($p_{T}$) model calculations.

Elliptic flow $v_{2}(\eta)$ for charged hadrons fromCu+Cu collisions at 0–60% centrality at $\sqrt{s_{NN}}$ = 22.4 GeV. The present STAR results are compared to the measurement from the PHOBOS [29] collaboration for Cu+Cu at 22.4 GeV. The PHOBOS results include statistical and systematic errors whereas the STAR results are plotted with statistical uncertainties only, and systematic errors are discussed in Section III C. Results are also compared to $v_{2}(\eta)$ calculations from the indicated models.

Elliptic flow $v_{2}${TPC} and $v_{2}${4} as a function of centrality for charged hadrons from Cu+Cu collisions at 0 − 60% centrality at $\sqrt{s_{NN}}$ = 22.4 GeV, compared with previously published results from the STAR collaboration at 200 GeV and 62.4 GeV.

FIG. 1. (Color online) Perspective views of $2 \mathrm{D}$ charge-independent angular correlations $\Delta \rho / \sqrt{\rho_{\mathrm{ref}}}$ on $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ for Au-Au collisions at $\sqrt{s_{N N}}=200$ and $62 \mathrm{GeV}$ (top and bottom rows, respectively). Centrality increases left to right from most peripheral to most central. Corrected total cross-section fractions are (left to right) $84 \%-93 \%, 55 \%-64 \%, 18 \%-28 \%,$ and $0 \%-5 \%$ for the $200-\mathrm{GeV}$ data and $84 \%-95 \%, 56 \%-65 \%$ $18 \%-28 \%,$ and $0 \%-5 \%$ for the $62 \mathrm{GeV}$ data (see Tables III and IV).

FIG. 1. (Color online) Perspective views of $2 \mathrm{D}$ charge-independent angular correlations $\Delta \rho / \sqrt{\rho_{\mathrm{ref}}}$ on $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ for Au-Au collisions at $\sqrt{s_{N N}}=200$ and $62 \mathrm{GeV}$ (top and bottom rows, respectively). Centrality increases left to right from most peripheral to most central. Corrected total cross-section fractions are (left to right) $84 \%-93 \%, 55 \%-64 \%, 18 \%-28 \%,$ and $0 \%-5 \%$ for the $200-\mathrm{GeV}$ data and $84 \%-95 \%, 56 \%-65 \%$ $18 \%-28 \%,$ and $0 \%-5 \%$ for the $62 \mathrm{GeV}$ data (see Tables III and IV).

FIG. 1. (Color online) Perspective views of $2 \mathrm{D}$ charge-independent angular correlations $\Delta \rho / \sqrt{\rho_{\mathrm{ref}}}$ on $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ for Au-Au collisions at $\sqrt{s_{N N}}=200$ and $62 \mathrm{GeV}$ (top and bottom rows, respectively). Centrality increases left to right from most peripheral to most central. Corrected total cross-section fractions are (left to right) $84 \%-93 \%, 55 \%-64 \%, 18 \%-28 \%,$ and $0 \%-5 \%$ for the $200-\mathrm{GeV}$ data and $84 \%-95 \%, 56 \%-65 \%$ $18 \%-28 \%,$ and $0 \%-5 \%$ for the $62 \mathrm{GeV}$ data (see Tables III and IV).

FIG. 1. (Color online) Perspective views of $2 \mathrm{D}$ charge-independent angular correlations $\Delta \rho / \sqrt{\rho_{\mathrm{ref}}}$ on $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ for Au-Au collisions at $\sqrt{s_{N N}}=200$ and $62 \mathrm{GeV}$ (top and bottom rows, respectively). Centrality increases left to right from most peripheral to most central. Corrected total cross-section fractions are (left to right) $84 \%-93 \%, 55 \%-64 \%, 18 \%-28 \%,$ and $0 \%-5 \%$ for the $200-\mathrm{GeV}$ data and $84 \%-95 \%, 56 \%-65 \%$ $18 \%-28 \%,$ and $0 \%-5 \%$ for the $62 \mathrm{GeV}$ data (see Tables III and IV).

FIG. 1. (Color online) Perspective views of $2 \mathrm{D}$ charge-independent angular correlations $\Delta \rho / \sqrt{\rho_{\mathrm{ref}}}$ on $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ for Au-Au collisions at $\sqrt{s_{N N}}=200$ and $62 \mathrm{GeV}$ (top and bottom rows, respectively). Centrality increases left to right from most peripheral to most central. Corrected total cross-section fractions are (left to right) $84 \%-93 \%, 55 \%-64 \%, 18 \%-28 \%,$ and $0 \%-5 \%$ for the $200-\mathrm{GeV}$ data and $84 \%-95 \%, 56 \%-65 \%$ $18 \%-28 \%,$ and $0 \%-5 \%$ for the $62 \mathrm{GeV}$ data (see Tables III and IV).

FIG. 2. (Color online) Fit decomposition of the $46 \%-56 \%$ centrality data for 62 -GeV Au-Au collisions. The top panels show from left to right the corrected data, model fit, fit residuals (data - model), and same-side 2D Gaussian. The bottom panels similarly show the away-side azimuth dipole, the nonjet azimuth quadrupole, the 1D $\eta_{\Delta}$ Gaussian, and the 2D exponential. This centrality is just below the sharp transition at $v_{\text {trans }}=3$. Fit residuals (c) are scaled up eightfold relative to the data.

FIG. 3. Fit parameters for $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ correlation data from Au-Au collisions at $\sqrt{s_{N N}}=62$ (open symbols) and 200 GeV (solid symbols) versus centrality measure $\nu$ computed at fixed energy $(200 \mathrm{GeV})$. The SS $2 \mathrm{D}$ Gaussian amplitudes, $\eta_{\Delta}$ widths, and $\phi_{\Delta}$ widths are shown in the left, center, and right panels, respectively of the top row. The bottom row shows from left to right the amplitudes for the dipole, quadrupole, and SS peak width aspect ratio $\sigma_{\eta_{\Delta}} / \sigma_{\phi_{\Delta}} .$ Fitting errors are indicated by error bars where larger than the symbols. Solid lines connect the points for clarity. The dotted and dashed curves indicate Glauber linear superposition estimates for 62 - and 200 -GeV peak amplitudes respectively, as discussed in the text. The quadrupole data are consistent with Ref. [60]. The hatched regions indicate the full range of systematic uncertainties listed in Appendix F. The vertical dark bands indicate estimated $v$ equivalents for $N-N$ collisions and $b=0$ Au-Au collisions.

FIG. 3. Fit parameters for $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ correlation data from Au-Au collisions at $\sqrt{s_{N N}}=62$ (open symbols) and 200 GeV (solid symbols) versus centrality measure $\nu$ computed at fixed energy $(200 \mathrm{GeV})$. The SS $2 \mathrm{D}$ Gaussian amplitudes, $\eta_{\Delta}$ widths, and $\phi_{\Delta}$ widths are shown in the left, center, and right panels, respectively of the top row. The bottom row shows from left to right the amplitudes for the dipole, quadrupole, and SS peak width aspect ratio $\sigma_{\eta_{\Delta}} / \sigma_{\phi_{\Delta}} .$ Fitting errors are indicated by error bars where larger than the symbols. Solid lines connect the points for clarity. The dotted and dashed curves indicate Glauber linear superposition estimates for 62 - and 200 -GeV peak amplitudes respectively, as discussed in the text. The quadrupole data are consistent with Ref. [60]. The hatched regions indicate the full range of systematic uncertainties listed in Appendix F. The vertical dark bands indicate estimated $v$ equivalents for $N-N$ collisions and $b=0$ Au-Au collisions.

FIG. 3. Fit parameters for $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ correlation data from Au-Au collisions at $\sqrt{s_{N N}}=62$ (open symbols) and 200 GeV (solid symbols) versus centrality measure $\nu$ computed at fixed energy $(200 \mathrm{GeV})$. The SS $2 \mathrm{D}$ Gaussian amplitudes, $\eta_{\Delta}$ widths, and $\phi_{\Delta}$ widths are shown in the left, center, and right panels, respectively of the top row. The bottom row shows from left to right the amplitudes for the dipole, quadrupole, and SS peak width aspect ratio $\sigma_{\eta_{\Delta}} / \sigma_{\phi_{\Delta}} .$ Fitting errors are indicated by error bars where larger than the symbols. Solid lines connect the points for clarity. The dotted and dashed curves indicate Glauber linear superposition estimates for 62 - and 200 -GeV peak amplitudes respectively, as discussed in the text. The quadrupole data are consistent with Ref. [60]. The hatched regions indicate the full range of systematic uncertainties listed in Appendix F. The vertical dark bands indicate estimated $v$ equivalents for $N-N$ collisions and $b=0$ Au-Au collisions.

FIG. 3. Fit parameters for $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ correlation data from Au-Au collisions at $\sqrt{s_{N N}}=62$ (open symbols) and 200 GeV (solid symbols) versus centrality measure $\nu$ computed at fixed energy $(200 \mathrm{GeV})$. The SS $2 \mathrm{D}$ Gaussian amplitudes, $\eta_{\Delta}$ widths, and $\phi_{\Delta}$ widths are shown in the left, center, and right panels, respectively of the top row. The bottom row shows from left to right the amplitudes for the dipole, quadrupole, and SS peak width aspect ratio $\sigma_{\eta_{\Delta}} / \sigma_{\phi_{\Delta}} .$ Fitting errors are indicated by error bars where larger than the symbols. Solid lines connect the points for clarity. The dotted and dashed curves indicate Glauber linear superposition estimates for 62 - and 200 -GeV peak amplitudes respectively, as discussed in the text. The quadrupole data are consistent with Ref. [60]. The hatched regions indicate the full range of systematic uncertainties listed in Appendix F. The vertical dark bands indicate estimated $v$ equivalents for $N-N$ collisions and $b=0$ Au-Au collisions.

FIG. 3. Fit parameters for $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ correlation data from Au-Au collisions at $\sqrt{s_{N N}}=62$ (open symbols) and 200 GeV (solid symbols) versus centrality measure $\nu$ computed at fixed energy $(200 \mathrm{GeV})$. The SS $2 \mathrm{D}$ Gaussian amplitudes, $\eta_{\Delta}$ widths, and $\phi_{\Delta}$ widths are shown in the left, center, and right panels, respectively of the top row. The bottom row shows from left to right the amplitudes for the dipole, quadrupole, and SS peak width aspect ratio $\sigma_{\eta_{\Delta}} / \sigma_{\phi_{\Delta}} .$ Fitting errors are indicated by error bars where larger than the symbols. Solid lines connect the points for clarity. The dotted and dashed curves indicate Glauber linear superposition estimates for 62 - and 200 -GeV peak amplitudes respectively, as discussed in the text. The quadrupole data are consistent with Ref. [60]. The hatched regions indicate the full range of systematic uncertainties listed in Appendix F. The vertical dark bands indicate estimated $v$ equivalents for $N-N$ collisions and $b=0$ Au-Au collisions.

FIG. 3. Fit parameters for $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ correlation data from Au-Au collisions at $\sqrt{s_{N N}}=62$ (open symbols) and 200 GeV (solid symbols) versus centrality measure $\nu$ computed at fixed energy $(200 \mathrm{GeV})$. The SS $2 \mathrm{D}$ Gaussian amplitudes, $\eta_{\Delta}$ widths, and $\phi_{\Delta}$ widths are shown in the left, center, and right panels, respectively of the top row. The bottom row shows from left to right the amplitudes for the dipole, quadrupole, and SS peak width aspect ratio $\sigma_{\eta_{\Delta}} / \sigma_{\phi_{\Delta}} .$ Fitting errors are indicated by error bars where larger than the symbols. Solid lines connect the points for clarity. The dotted and dashed curves indicate Glauber linear superposition estimates for 62 - and 200 -GeV peak amplitudes respectively, as discussed in the text. The quadrupole data are consistent with Ref. [60]. The hatched regions indicate the full range of systematic uncertainties listed in Appendix F. The vertical dark bands indicate estimated $v$ equivalents for $N-N$ collisions and $b=0$ Au-Au collisions.

FIG. 4. (Color online) (a) 2D data histogram from $0 \%-5 \%$ central 200 GeV Au-Au collisions $[(0,0)$ bin suppressed]. (b) Additional model component fitted to the $2 \mathrm{D}$ histogram and consisting of an AS azimuth dipole modulated by function $F\left(\eta_{\Delta}\right)$ described in the text. (c) Fit residuals including the new model component. (d) Data histogram in the first panel minus the additional model component and fitted offset. Remaining structure is described accurately by an AS dipole and SS 2D Gaussian.

FIG. 9. (a) Amplitude of SS 2D peak (jet-correlated pairs per final-state hadron) for data (solid points), GLS extrapolation from $p$ - $p$ data (dashed curve) and from the HIJING Monte Carlo (open points, dotted curve). (b) Single-particle production extrapolated from $p-p$ data (dashed curve, GLS), and from more-central Au-Au data (solid line) and HIJING (dash-dotted line, open points). (c) Single-particle hard-component production per $N-N$ binary collision from $p-p$ data, from more-central Au-Au data and from HIJING (open points). (d) Jet-correlated pair production (SS 2D peak) per $N-N$ binary collision extrapolated from $p-p$ data (GLS), and from Au-Au data (solid points) and HIJING (open points).

FIG. 9. (a) Amplitude of SS 2D peak (jet-correlated pairs per final-state hadron) for data (solid points), GLS extrapolation from $p$ - $p$ data (dashed curve) and from the HIJING Monte Carlo (open points, dotted curve). (b) Single-particle production extrapolated from $p-p$ data (dashed curve, GLS), and from more-central Au-Au data (solid line) and HIJING (dash-dotted line, open points). (c) Single-particle hard-component production per $N-N$ binary collision from $p-p$ data, from more-central Au-Au data and from HIJING (open points). (d) Jet-correlated pair production (SS 2D peak) per $N-N$ binary collision extrapolated from $p-p$ data (GLS), and from Au-Au data (solid points) and HIJING (open points).

FIG. 9. (a) Amplitude of SS 2D peak (jet-correlated pairs per final-state hadron) for data (solid points), GLS extrapolation from $p$ - $p$ data (dashed curve) and from the HIJING Monte Carlo (open points, dotted curve). (b) Single-particle production extrapolated from $p-p$ data (dashed curve, GLS), and from more-central Au-Au data (solid line) and HIJING (dash-dotted line, open points). (c) Single-particle hard-component production per $N-N$ binary collision from $p-p$ data, from more-central Au-Au data and from HIJING (open points). (d) Jet-correlated pair production (SS 2D peak) per $N-N$ binary collision extrapolated from $p-p$ data (GLS), and from Au-Au data (solid points) and HIJING (open points).

FIG. 9. (a) Amplitude of SS 2D peak (jet-correlated pairs per final-state hadron) for data (solid points), GLS extrapolation from $p$ - $p$ data (dashed curve) and from the HIJING Monte Carlo (open points, dotted curve). (b) Single-particle production extrapolated from $p-p$ data (dashed curve, GLS), and from more-central Au-Au data (solid line) and HIJING (dash-dotted line, open points). (c) Single-particle hard-component production per $N-N$ binary collision from $p-p$ data, from more-central Au-Au data and from HIJING (open points). (d) Jet-correlated pair production (SS 2D peak) per $N-N$ binary collision extrapolated from $p-p$ data (GLS), and from Au-Au data (solid points) and HIJING (open points).

FIG. 11. (Color online) (Left) Uncorrected angular correlations from 62-GeV $37 \%-46 \%$ central Au-Au collisions showing pileup distortions, especially evident as the W-shaped nonuniformity of the AS ridge on $\eta_{\Delta}$. (Right) The same data with pileup correction applied.

Covariance matrix values between the rapidity bins for the electrons data sample.

Covariance matrix values between the rapidity bins for the combined data sample.

Covariance matrix values between the QT bins for the muons data sample.

Covariance matrix values between the QT bins for the electrons data sample.

Covariance matrix values between the QT bins for the combined data sample.

Ratio of deuterons to protons for polar angle 65-90 deg.

Ratio of deuterons to protons for polar angle 90-125 deg.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 3 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 5 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 8 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 12.9 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 12 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in P Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI+ Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 15 GeV.

The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI- Aluminium interactions at a beam energy of 15 GeV.

The ratio of away-side yields in Lead-Lead/Proton-Proton collisions in the peripheral region.

The ratio between near-side central/peripheral yields in Lead-Lead collisions.

The ratio between away-side central/peripheral yields in Lead-Lead collisions.

The ratio of the cross section for Z+ n jet production over the cross section for Z production in the muon channel.

The ratio of the cross section for W+ n jet production over the cross section for W+n-1jet production in the electron channel.

The ratio of the cross section for W+ n jet production over the cross section for W+n-1jet production in the muon channel.

The ratio of the cross section for Z+ n jet production over the cross section for Z+n-1jet production in the electron channel.

The ratio of the cross section for Z+ n jet production over the cross section for Z+n-1jet production in the muon channel.

Measured diphoton differential cross sections as a function of the azimuthal angle between the two photons for the two pseusdorapidity ranges.

Measured diphoton differential cross sections as a function of |cos(theta*)| of the diphotons for the two pseusdorapidity ranges.