Fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction off protons with a Soeding-inspired analytic function --- statistical correlations only. Only one half of the (symmetric) matrix is stored.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction off protons, differential in the dipion mass and in bins of $W$. The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction off protons, differential in the dipion mass and in bins of $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction off protons, in bins of the photon-proton energy $W$. The cross section is defined as the integral of the relativistic Breit Wigner resonance in the dipion mass over the range $2m_\pi<m_{\pi\pi}<1.53$ GeV. The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction off protons in bins of the photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction cross sections off protons as a function of energy. Parameters with subscript "el" and "pd" correspond to elastic and proton-dissociative cross sections, respectively.

Fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction cross sections off protons as a function of energy --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Fit of elastic $\rho^0(770)$ photoproduction cross section off protons as a function of energy (various experiments)

Fit of elastic $\rho^0(770)$ photoproduction cross sections off protons as a function of energy (various experiments) --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction cross section off protons, double-differential in the dipion mass and the momentum transfer $\vert t\vert$. The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction cross section off protons, double-differential in the dipion mass and the momentum transfer $\vert t\vert$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction off protons, single-differential in the momentum transfer $\vert t\vert$. The cross section is defined as the integral of the relativistic Breit Wigner resonance in the dipion mass over the range $2m_\pi<m_{\pi\pi}<1.53$ GeV. The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction off protons, single differential in the momentum transfer $\vert t\vert$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$. Parameters with subscript "el" and "pd" correspond to elastic and proton-dissociative cross sections, respectively.

Fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction double-differenial cross section off protons, as a function of the dipion mass and the momentum transfer $\vert t\vert$, in bins of the photon-proton energy $W$ The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction double-differenial cross section off protons, as a function of the dipion mass and the momentum transfer $\vert t\vert$, in bins of the photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction off protons, single-differential in the momentum transfer $\vert t\vert$, in bins of the photon-proton energy $W$. The cross section is defined as the integral of the relativistic Breit Wigner resonance in the dipion mass over the range $2m_\pi<m_{\pi\pi}<1.53$ GeV. The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction cross section off protons, single differential in the momentum transfer $\vert t\vert$ and in bins of the photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Regge fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ and photon-proton energy $W$. Parameters with subscript "el" and "pd" correspond to elastic and proton-dissociative cross sections, respectively.

Regge fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ and photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Fit of $b$-slopes in elastic ($m_Y=m_p$) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ in bins of photon-proton energy $W$.

Fit of $b$-slopes in elastic ($m_Y=m_p$) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ in bins of photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Fit of Pomeron trajectories in elastic ($m_Y=m_p$) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ in bins of photon-proton energy $W$.

Fit of Pomeron trajectories in elastic ($m_Y=m_p$) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ in bins of photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Transverse mass $m_T$ spectrum at midrapidity of $\phi$ mesons produced in minimum bias p+p collisions at beam momentum of 158 GeV/c. $m_0$ is the PDG mass of the $\phi$ meson.

Transverse mass $m_T$ spectrum at midrapidity of $\phi$ mesons produced in minimum bias p+p collisions at beam momentum of 80 GeV/c. $m_0$ is the PDG mass of the $\phi$ meson.

Dependence of the slope parameter $T$ of the transverse momentum spectrum on rapidity $y$, of $\phi$ mesons produced in minimum bias p+p collisions at beam momentum of 158 GeV/c.

Dependence of the slope parameter $T$ of the transverse momentum spectrum on rapidity $y$, of $\phi$ mesons produced in minimum bias p+p collisions at beam momentum of 80 GeV/c.

Dependence of the width $\sigma_y$ of the rapidity distributions on $p_T$, of $\phi$ mesons produced in minimum bias p+p collisions at beam momentum of 158 GeV/c.

Dependence of the width $\sigma_y$ of the rapidity distributions on $p_T$, of $\phi$ mesons produced in minimum bias p+p collisions at beam momentum of 80 GeV/c.

Rapidity spectrum of $\phi$ mesons produced in minimum bias p+p collisions at beam momentum of 158 GeV/c.

Rapidity spectrum of $\phi$ mesons produced in minimum bias p+p collisions at beam momentum of 80 GeV/c.

Rapidity spectrum of $\phi$ mesons produced in minimum bias p+p collisions at beam momentum of 40 GeV/c.

Energy dependence of ratios of total yields of $\phi$ mesons to mean total yields of pions produced in in minimum bias p+p collisions at CERN SPS energies.

Energy dependence of double ratios of total yields of $\phi$ mesons to mean total yields of pions in central Pb+Pb collisions over minimum bias p+p collisions at CERN SPS energies.

Energy dependence of total yields of $\phi$ mesons produced in minimum bias p+p collisions at CERN SPS energies.

Energy dependence of midrapidity yields of $\phi$ mesons produced in minimum bias p+p collisions at CERN SPS energies.

Widths of rapidity distributions of $\phi$ mesons produced in minimum bias p+p collisions at CERN SPS energies, as a function of beam rapidity.

Example of $\Lambda$ signal for 0-40% most central events, over mixed-event background for the bin $-0.05 < y_{cm} < 0.05$ and reduced transverse masses between $100-150 MeV/c^{2}$.

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $K^{0}_{S}$ for the 0-40% most central events.

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $K^{0}_{S}$ for the 0-40% most central events. NOTE: The spectra are not scaled by $1/N_{Events}$! To compare the data, divide by $N_{Events} = 2.1997626 x 10^{9}$

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $\Lambda$ for the 0-40% most central events.

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $\Lambda$ for the 0-40% most central events. NOTE: The spectra are not scaled by $1/N_{Events}$! To compare the data, divide by $N_{Events} = 2.1997626 x 10^{9}$

Rapidity distribution of $K^{0}_{S}$

Rapidity distribution of $K^{0}_{S}$

Rapidity distribution of $\Lambda$

Rapidity distribution of $\Lambda$

Compilation of mid-rapidity yields for central Au+Au collisions as a function of $\sqrt{s_{NN}}$ of $K^{0}_{S}$ and $\Lambda$.

Compilation of mid-rapidity yields for central Au+Au collisions as a function of $\sqrt{s_{NN}}$ of $K^{0}_{S}$ and $\Lambda$.

Multiplicities per mean number of participants $Mult/\langle A_{Part}\rangle$ as a function of $\langle A_{Part}\rangle$

Multiplicities per mean number of participants $Mult/\langle A_{Part}\rangle$ as a function of $\langle A_{Part}\rangle$

Multiplicities per mean number of participants $Mult/\langle A_{Part}\rangle$ as a function of $\langle A_{Part}\rangle$ for $K^{0}_{S}$

Multiplicities per mean number of participants $Mult/\langle A_{Part}\rangle$ as a function of $\langle A_{Part}\rangle$ for $K^{0}_{S}$

Multiplicities per mean number of participants $Mult/\langle A_{Part}\rangle$ as a function of $\langle A_{Part}\rangle$ for $\Lambda$

Multiplicities per mean number of participants $Mult/\langle A_{Part}\rangle$ as a function of $\langle A_{Part}\rangle$ for $\Lambda$

Comparison of the shape of the rapidity distribution of $K^{0}_{S}$ to various transport model versions.

Comparison of the shape of the rapidity distribution of $K^{0}_{S}$ to various transport model versions.

Comparison of the shape of the rapidity distribution of $\Lambda$ to various transport model versions.

Comparison of the shape of the rapidity distribution of $\Lambda$ to various transport model versions.

Comparison of the shape of the $p_{t}$-spectra for $\pm0.15$ rapidity units around mid-rapidity of $K^{0}_{S}$ to various transport model versions.

Comparison of the shape of the $p_{t}$-spectra for $\pm0.15$ rapidity units around mid-rapidity of $K^{0}_{S}$ to various transport model versions.

Comparison of the shape of the $p_{t}$-spectra for $\pm0.15$ rapidity units around mid-rapidity of $\Lambda$ to various transport model versions.

Comparison of the shape of the $p_{t}$-spectra for $\pm0.15$ rapidity units around mid-rapidity of $\Lambda$ to various transport model versions.

Differential yield of $K^{0}_{S}$ as function of rapdidity and reduced transverse mass for the four centrality classes.

Differential yield of $K^{0}_{S}$ as function of rapdidity and reduced transverse mass for the four centrality classes. NOTE: The spectra are not scaled by $1/N_{Events}$! To compare the data, divide by $N_{Events} = 5.64247975 x 10^{8} (0 - 10\%)$, $5.85743394 x 10^{8} (10 - 20\%)$, $5.76369451 x 10^{8} (20 - 30\%)$ or $4.73401752 x 10^{8} (30 - 40\%)$

Differential yield of $\Lambda$ as function of rapdidity and reduced transverse mass for the four centrality classes.

Differential yield of $\Lambda$ as function of rapdidity and reduced transverse mass for the four centrality classes. NOTE: The spectra are not scaled by $1/N_{Events}$! To compare the data, divide by $N_{Events} = 5.64247975 x 10^{8} (0 - 10\%)$, $5.85743394 x 10^{8} (10 - 20\%)$, $5.76369451 x 10^{8} (20 - 30\%)$ or $4.73401752 x 10^{8} (30 - 40\%)$

$K^{0}_{S}$ and $\Lambda$ multiplicities in full phase space and inverse slopes at mid-rapidity $T_{Eff}$ for a given centrality.

$K^{0}_{S}$ and $\Lambda$ multiplicities in full phase space and inverse slopes at mid-rapidity $T_{Eff}$ for a given centrality.

Value of the parameter $\alpha$ extracted for $K^{+}$, $K^{-}$, $K^{0}_{S}$, $\Lambda$ and $\Phi$, as displayed in Figure 5 - Global $Mult/\langle A_{Part}\rangle$ Fit

Value of the parameter $\alpha$ extracted for $K^{+}$, $K^{-}$, $K^{0}_{S}$, $\Lambda$ and $\Phi$, as displayed in Figure 5 - Global $Mult/\langle A_{Part}\rangle$ Fit

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 120 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 120 to 140 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 160 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 160 to 180 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 200 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 200 to 220 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 340 to 380 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 120 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 120 to 140 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 160 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 160 to 180 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 200 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 200 to 220 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 340 to 380 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 120 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 120 to 140 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 160 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 160 to 180 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 200 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 200 to 220 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 340 to 380 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 120 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 120 to 140 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 160 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 160 to 180 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 200 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 200 to 220 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 340 to 380 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 120 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 120 to 140 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 160 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 160 to 180 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 200 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 200 to 220 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 340 to 380 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 120 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 120 to 140 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 160 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 160 to 180 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 200 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 200 to 220 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 340 to 380 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 120 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 120 to 140 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 160 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 160 to 180 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 200 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 200 to 220 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 340 to 380 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 120 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 120 to 140 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 160 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 160 to 180 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 200 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 200 to 220 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 340 to 380 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 120 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 120 to 140 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 160 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 160 to 180 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 200 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 200 to 220 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 340 to 380 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 120 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 120 to 140 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 160 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 160 to 180 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 200 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 200 to 220 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 340 to 380 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 120 to 180 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 280 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 120 to 180 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 280 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 120 to 180 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 280 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 120 to 180 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 280 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 120 to 180 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 280 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 120 to 180 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 280 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 120 to 180 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 280 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 120 to 180 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 280 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 120 to 180 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 280 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 120 to 180 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 280 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 100 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 300 to 380 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 100 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 300 to 380 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 100 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 300 to 380 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 100 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 300 to 380 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 100 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 300 to 380 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 100 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.

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$K^{+}$ signal and the corresponding background fit for the region covering mid-rapidity and $m_{t}−m_{0}$ between 25 and 50 $MeV/c^{2}$.

$K^{+}$ signal and the corresponding background fit for the region covering mid-rapidity and $m_{t}−m_{0}$ between 25 and 50 $MeV/c^{2}$.

$K^{+}$ signal and the corresponding background fit for the region covering mid-rapidity and $m_{t}−m_{0}$ between 25 and 50 $MeV/c^{2}$.

$K^{-}$ signal and the corresponding background fit for the region covering mid-rapidity and $m_{t}−m_{0}$ between 50 and 75 $MeV/c^{2}$.

$K^{-}$ signal and the corresponding background fit for the region covering mid-rapidity and $m_{t}−m_{0}$ between 50 and 75 $MeV/c^{2}$.

$K^{-}$ signal and the corresponding background fit for the region covering mid-rapidity and $m_{t}−m_{0}$ between 50 and 75 $MeV/c^{2}$.

$K^{+}K^{-}$ invariant mass distribution for the mid-rapidity region and $m_{t}−m_{0}$ between 0 and 100 $MeV/c^{2}$ after subtraction of the background.

$K^{+}K^{-}$ invariant mass distribution for the mid-rapidity region and $m_{t}−m_{0}$ between 0 and 100 $MeV/c^{2}$ after subtraction of the background.

$K^{+}K^{-}$ invariant mass distribution for the mid-rapidity region and $m_{t}−m_{0}$ between 0 and 100 $MeV/c^{2}$ after subtraction of the background.

Rapidity distributions of $K^{-}$ and $\phi$ as well as extracted inverse slope parameters obtained from the Boltzmann fits to the the $m_{t}$ spectra.

Rapidity distributions of $K^{-}$ and $\phi$ as well as extracted inverse slope parameters obtained from the Boltzmann fits to the the $m_{t}$ spectra.

Rapidity distributions of $K^{-}$ and $\phi$ as well as extracted inverse slope parameters obtained from the Boltzmann fits to the the $m_{t}$ spectra.

$K^{-}$ transverse-mass spectrum around mid-rapidity

$K^{-}$ transverse-mass spectrum around mid-rapidity

$K^{-}$ transverse-mass spectrum around mid-rapidity

Multiplicity ratio $\phi/K^{-}$ as function of $\sqrt{s_{NN}}$ for central heavy-ion collisions.

Multiplicity ratio $\phi/K^{-}$ as function of $\sqrt{s_{NN}}$ for central heavy-ion collisions.

Multiplicity ratio $\phi/K^{-}$ as function of $\sqrt{s_{NN}}$ for central heavy-ion collisions.

Multiplicities and effective inverse slopes $T_{eff}$ at mid-rapidity for given centrality classes.

Multiplicities and effective inverse slopes $T_{eff}$ at mid-rapidity for given centrality classes.

Multiplicities and effective inverse slopes $T_{eff}$ at mid-rapidity for given centrality classes.

Multiplicity ratios for given centrality classes.

Multiplicity ratios for given centrality classes.

Multiplicity ratios for given centrality classes.

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $K^{+}$ for the 0-40% most central events.

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $K^{+}$ for the 0-40% most central events.

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $K^{+}$ for the 0-40% most central events.

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $K^{-}$ for the 0-40% most central events.

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $K^{-}$ for the 0-40% most central events.

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $K^{-}$ for the 0-40% most central events.

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $\phi$ for the 0-40% most central events.

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $\phi$ for the 0-40% most central events.

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $\phi$ for the 0-40% most central events.

Rapidity distribution of $K^{+}$ for the 0-40% most central events.

$R_{pPb}$ as a function of $p_{T}$ integrated over rapidity range $-1.8<y*<1.3$ for the 0--90% centrality interval for the three geometric models: (a) Glauber, (b) Glauber-Gribov with $\omega_{\sigma}=0.11$ and (c) Glauber-Gribov with $\omega_{\sigma}=0.2$.

$R_{pPb}$ values as a function of $p_{T}$ in the 0--90% centrality interval averaged over $|y*|<0.5$.The $\langle T_{Pb} \rangle$ value for the ATLAS centrality correction is calculated with the Glauber model. The total systematic uncertainties, which include the uncertainty in $\langle T_{Pb} \rangle$, are indicated by lines of the same colour. Strict quantitative agreement is not expected as each measurement uses different rapidity intervals for the centrality determination and apply different event selection criteria to reject diffractive collisions.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields integrated over $-1.8<y*<1.3$ for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields integrated over $-1.8<y*<1.3$ for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields integrated over $-1.8<y*<1.3$ for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{CP}$ as a function of $p_{T}$ extracted from the invariant yields integrated over $|\eta|<2.3$ for seven centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{CP}$ as a function of $p_{T}$ extracted from the invariant yields integrated over $|\eta|<2.3$ for seven centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{CP}$ as a function of $p_{T}$ extracted from the invariant yields integrated over $|\eta|<2.3$ for seven centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $p_{T}$ extracted from the invariant yields for six rapidity ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

$R_{pPb}$ as a function of $y*$ extracted from the invariant yields for eight $p_{T}$ ranges, for eight centrality intervals, and for different geometrical models used to calculate $\langle T_{Pb} \rangle$.

The jet-like yield in $\mid\Delta\eta\mid<$0.78 as a function of $p_T^{trigger}$ for $K_S^0$-h and $\Lambda$-h correlations for 1.5 GeV/$c$ < $p_T^{associated}$ < $p_T^{trigger}$ in minimum bias $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Statistical errors listed in table. 5.4% systematic error on all points.

The jet-like yield in $\mid\Delta\eta\mid<$0.78 as a function of $p_T^{trigger}$ for $K_S^0$-h and $\Lambda$-h correlations for 1.5 GeV/$c$ < $p_T^{associated}$ < $p_T^{trigger}$ in 0-60% Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 GeV. Statistical errors listed in table. 5.4% systematic error on all points.

The jet-like yield in $\mid\Delta\eta\mid<$0.78 as a function of $p_T^{trigger}$ for $K_S^0$-h and $\Lambda$-h correlations for 1.5 GeV/$c$ < $p_T^{associated}$ < $p_T^{trigger}$ in 40-80% Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Statistical errors listed in table. 5.4% systematic error on all points.

The jet-like yield in $\mid\Delta\eta\mid<$0.78 as a function of $p_T^{trigger}$ for $K_S^0$-h and $\Lambda$-h correlations for 1.5 GeV/$c$ < $p_T^{associated}$ < $p_T^{trigger}$ in 0-12% Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Statistical errors listed in table. 5.4% systematic error on all points.

Centrality dependence of the jet-like yield of $K_S^0$-h and $\Lambda$-h correlations for 3 < $p_T^{trigger}$ < 6 GeV/$c$ and 1.5 GeV/$c$ < $p_T^{associated}$ < $p_T^{trigger}$ in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 GeV. 5.4% systematic error on all points.

Centrality dependence of the jet-like yield of $K_S^0$-h and $\Lambda$-h correlations for 3 < $p_T^{trigger}$ < 6 GeV/$c$ and 1.5 GeV/$c$ < $p_T^{associated}$ < $p_T^{trigger}$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. 5.4% systematic error on all points.

Centrality dependence of the jet-like yield of $K_S^0$-h and $\Lambda$-h correlations for 3 < $p_T^{trigger}$ < 6 GeV/$c$ and 1.5 GeV/$c$ < $p_T^{associated}$ < $p_T^{trigger}$ in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. 5.4% systematic error on all points.

Centrality dependence of the jet-like yield of $K_S^0$-h and $\Lambda$-h correlations for 3 < $p_T^{trigger}$ < 6 GeV/$c$ and 1.5 GeV/$c$ < $p_T^{associated}$ < $p_T^{trigger}$ in minimum bias $d$+Au and 0-60% central Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 GeV. 5.4% systematic error on all points.

Average of relative D$^{0}$, D$^{+}$ and D*$^{+}$ meson yields for the sum of particles and antiparticles in several multiplicity and PT(D) intervals for p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV as a function of the relative charged-particle multiplicity at central rapidity. The values are reported together with their uncertainties, which are quoted in the order: statistical, systematic and feed-down contribution uncertainties. The yields reported here are per inelastic event. The global normalisation uncertainty of $3.1\%$ is not shown.

Average of relative D$^{0}$, D$^{+}$ and D*$^{+}$ meson yields for the sum of particles and antiparticles in several multiplicity and PT(D) intervals for p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV as a function of the relative average multiplicity in the VZERO detector, $N_{V0A} \big/ \langle N_{V0A} \rangle$. The uncertainties are shown in the following order: statistical, systematic, and feed-down contribution uncertainties. The global normalisation uncertainty of $3.1\%$ is not shown. The yields reported here are normalised to the inelastic cross section. For $1 < PT(D) < 2$ GeV/c and $12 < PT(D) < 24$ GeV/c, the final two multiplicity intervals are merged.

Xi pt spectrum in 20-40% multiplicity class.

Xi pt spectrum in 40-60% multiplicity class.

Xi pt spectrum in 60-80% multiplicity class.

Xi pt spectrum in 80-100% multiplicity class.

Omega pt spectrum in 0-5% multiplicity class.

Omega pt spectrum in 5-10% multiplicity class.

Omega pt spectrum in 10-20% multiplicity class.

Omega pt spectrum in 20-40% multiplicity class.

Omega pt spectrum in 40-60% multiplicity class.

Omega pt spectrum in 60-80% multiplicity class.

Omega pt spectrum in 80-100% multiplicity class.

Mean pT of XI- in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV for each V0A multiplicity event class.

Mean pT of XIBAR+ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV for each V0A multiplicity event class.

Mean pT of OMEGA- in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV for each V0A multiplicity event class.

Mean pT of OMEGABAR+ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV for each V0A multiplicity event class.

XiMinus yield as a function of charged particle multiplicity per unit pseudorapidity.

XiPlus yield as a function of charged particle multiplicity per unit pseudorapidity.

OmegaMinus yield as a function of charged particle multiplicity per unit pseudorapidity.

OmegaPlus yield as a function of charged particle multiplicity per unit pseudorapidity.

Xi/pi ratio as a function of charged particle multiplicity per unit pseudorapidity.

Omega/pi ratio as a function of charged particle multiplicity per unit pseudorapidity.