Showing 10 of 10000 results
Phys. Rev. Lett. 14, 408 (1965)
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We report the direct virtual photon invariant yields in the transverse momentum ranges $1\!<\!p_{T}\!<\!3$ GeV/$c$ and $5\!<\!p_T\!<\!10$ GeV/$c$ at mid-rapidity derived from the dielectron invariant mass continuum region $0.10<M_{ee}<0.28$ GeV/$c^{2}$ for 0-80\% minimum-bias Au+Au collisions at $\sqrt{s_{NN}}=200$ GeV. A clear excess in the invariant yield compared to the number-of-binary-collisions ($N_{bin}$) scaled $p+p$ reference is observed in the $p_T$ range $1\!<\!p_{T}\!<\!3$ GeV/$c$. For $p_T\!>6$ GeV/$c$ the production follows $N_{bin}$ scaling. Model calculations with contributions from thermal radiation and initial hard parton scattering are consistent within uncertainties with the direct virtual photon invariant yield.
Measurements are reported of the normalized differential cross sections for top quark pair production with respect to four kinematic event variables: the missing transverse energy; the scalar sum of the jet transverse momentum (pT); the scalar sum of the pT of all objects in the event; and the pT of leptonically decaying W bosons from top quark decays. The data sample, collected using the CMS detector at the LHC, consists of 5.0 inverse femtobarns of proton-proton collisions at sqrt(s) = 7 TeV and 19.7 inverse femtobarns at sqrt(s) = 8 TeV. Top quark pair events containing one electron or muon are selected. The results are presented after correcting for detector effects to allow direct comparison with theoretical predictions. No significant deviations from the predictions of several standard model event simulation generators are observed.
Normalized $t\bar{t}$ differential cross section measurements with respect to the $E^{miss}_{T}$ variable at a center-of-mass energy of 7 TeV (combination of electron and muon channels).
Normalized $t\bar{t}$ differential cross section measurements with respect to the $H_T$ variable at a center-of-mass energy of 7 TeV (combination of electron and muon channels).
Normalized $t\bar{t}$ differential cross section measurements with respect to the $S_T$ variable at a center-of-mass energy of 7 TeV (combination of electron and muon channels).
Normalized $t\bar{t}$ differential cross section measurements with respect to the $p^{W}_{T}$ variable at a center-of-mass energy of 7 TeV (combination of electron and muon channels).
Normalized $t\bar{t}$ differential cross section measurements with respect to the $E^{miss}_{T}$ variable at a center-of-mass energy of 8 TeV (combination of electron and muon channels).
Normalized $t\bar{t}$ differential cross section measurements with respect to the HT variable at a center-of-mass energy of 8 TeV (combination of electron and muon channels).
Normalized $t\bar{t}$ differential cross section measurements with respect to the $S_T$ variable at a center-of-mass energy of 8 TeV (combination of electron and muon channels).
Normalized $t\bar{t}$ differential cross section measurements with respect to the $p^{W}_{T}$ variable at a center-of-mass energy of 8 TeV (combination of electron and muon channels).
Covariance matrix for the normalized $t\bar{t}$ differential cross section measurements with respect to the $E_{T}^{miss}$ variable at a center-of-mass energy of 7 TeV. Both statistical and systematic effects are considered.
Covariance matrix for the normalized $t\bar{t}$ differential cross section measurements with respect to the $H_{T}$ variable at a center-of-mass energy of 7 TeV. Both statistical and systematic effects are considered.
Covariance matrix for the normalized $t\bar{t}$ differential cross section measurements with respect to the $S_{T}$ variable at a center-of-mass energy of 7 TeV. Both statistical and systematic effects are considered.
Covariance matrix for the normalized $t\bar{t}$ differential cross section measurements with respect to the $p^{W}_{T}$ variable at a center-of-mass energy of 7 TeV. Both statistical and systematic effects are considered.
Covariance matrix for the normalized $t\bar{t}$ differential cross section measurements with respect to the $E_{T}^{miss}$ variable at a center-of-mass energy of 8 TeV. Both statistical and systematic effects are considered.
Covariance matrix for the normalized $t\bar{t}$ differential cross section measurements with respect to the $H_{T}$ variable at a center-of-mass energy of 8 TeV. Both statistical and systematic effects are considered.
Covariance matrix for the normalized $t\bar{t}$ differential cross section measurements with respect to the $S_{T}$ variable at a center-of-mass energy of 8 TeV. Both statistical and systematic effects are considered.
Covariance matrix for the normalized $t\bar{t}$ differential cross section measurements with respect to the $p^{W}_{T}$ variable at a center-of-mass energy of 8 TeV. Both statistical and systematic effects are considered.
The result of a search for pair production of the supersymmetric partner of the Standard Model bottom quark ($\tilde{b}_1$) is reported. The search uses 3.2 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}=$13 TeV collected by the ATLAS experiment at the Large Hadron Collider in 2015. Bottom squarks are searched for in events containing large missing transverse momentum and exactly two jets identified as originating from $b$-quarks. No excess above the expected Standard Model background yield is observed. Exclusion limits at 95% confidence level on the mass of the bottom squark are derived in phenomenological supersymmetric $R$-parity-conserving models in which the $\tilde{b}_1$ is the lightest squark and is assumed to decay exclusively via $\tilde{b}_1 \rightarrow b \tilde{\chi}_1^0$, where $\tilde{\chi}_1^0$ is the lightest neutralino. The limits significantly extend previous results; bottom squark masses up to 800 (840) GeV are excluded for the $\tilde{\chi}_1^0$ mass below 360 (100) GeV whilst differences in mass above 100 GeV between the $\tilde{b}_1$ and the $\tilde{\chi}_1^0$ are excluded up to a $\tilde{b}_1$ mass of 500 GeV.
Expected exclusion limit at 95% CL in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the sbottom pair production scenario.
Observed exclusion limit at 95% CL in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the sbottom pair production scenario.
Signal region (SR) providing the best expected sensitivity in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane.
Cross-section upper limit in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the best expected signal region.
Cross-section upper limit in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the SRA250 signal region.
Cross-section upper limit in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the SRA350 signal region.
Cross-section upper limit in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the SRA450 signal region.
Cross-section upper limit in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the SRB signal region.
Expected CLs values in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the best expected signal region.
Expected CLs values in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the SRA250 signal region.
Expected exclusion limit at 95% CL in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the sbottom pair production scenario, for signal region SRA250.
Observed exclusion limit at 95% CL in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the sbottom pair production scenario, for signal region SRA250.
Expected CLs values in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the SRA350 signal region.
Expected exclusion limit at 95% CL in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the sbottom pair production scenario, for signal region SRA350.
Observed exclusion limit at 95% CL in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the sbottom pair production scenario, for signal region SRA350.
Expected CLs values in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the SRA450 signal region.
Expected exclusion limit at 95% CL in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the sbottom pair production scenario, for signal region SRA450.
Observed exclusion limit at 95% CL in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the sbottom pair production scenario, for signal region SRA450.
Expected CLs values in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the SRB signal region.
Expected exclusion limit at 95% CL in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the sbottom pair production scenario, for signal region SRB.
Observed exclusion limit at 95% CL in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the sbottom pair production scenario, for signal region SRB.
Observed CLs values in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the best expected signal region.
Observed CLs values in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the SRA250 signal region.
Observed CLs values in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the SRA350 signal region.
Observed CLs values in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the SRA450 signal region.
Observed CLs values in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the SRB signal region.
Signal efficiency (in %) in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the sbottom pair production scenario, for the best expected signal region.
Signal efficiency (in %) in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the sbottom pair production scenario, for the SRA250 signal region.
Signal efficiency (in %) in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the sbottom pair production scenario, for the SRA350 signal region.
Signal efficiency (in %) in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the sbottom pair production scenario, for the SRA450 signal region.
Signal efficiency (in %) in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the sbottom pair production scenario, for the SRB signal region.
Signal acceptance (in %) in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the sbottom pair production scenario, for the best expected signal region.
Signal acceptance (in %) in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the sbottom pair production scenario, for the SRA250 signal region.
Signal acceptance (in %) in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the sbottom pair production scenario, for the SRA350 signal region.
Signal acceptance (in %) in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the sbottom pair production scenario, for the SRA450 signal region.
Signal acceptance (in %) in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane for the sbottom pair production scenario, for the SRB signal region.
Total experimental systematic uncertainty in percent on the signal efficiency times acceptance in the $m(\tilde b_1)$-$m(\tilde\chi^0_1)$ plane. The best expected signal region selection is used per point.
The inclusive J/$\psi$ production has been studied in Pn-Pb and pp collisions at the centre-of-mass energy per nucleon pair $\sqrt{s_{\rm NN}}=5.02$ TeV, using the ALICE detector at the CERN LHC. The J/$\psi$ meson is reconstructed, in the centre-of-mass rapidity interval $2.5<y<4$ and in the transverse-momentum range $p_{\rm T}<12$ GeV/$c$, via its decay to a muon pair. In this Letter, we present results on the inclusive J/$\psi$ cross section in pp collisions at $\sqrt{s}=5.02$ TeV and on the nuclear modification factor $R_{\rm AA}$. The latter is presented as a function of the centrality of the collision and, for central collisions, as a function of the transverse momentum $p_{\rm T}$ of the J/$\psi$. The measured $R_{\rm AA}$ values indicate a suppression of the J/$\psi$ in nuclear collisions and are then compared to our previous results obtained in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76$ TeV. The ratio of the $R_{\rm AA}$ values at the two energies is also computed and compared to calculations of statistical and dynamical models. The numerical value of the ratio for central events (0-10\% centrality) is $1.17 \pm 0.04 {\rm{(stat)}}\pm 0.20 {\rm{(syst)}}$. In central events, as a function of $p_{\rm T}$, a slight increase of $R_{\rm AA}$ with collision energy is visible in the region $2<p_{\rm T}<6$ GeV/$c$. Theoretical calculations provide a good description of the measurements, within uncertainties.
Differential cross section ${\rm d}^2\sigma^{\rm pp}_{{\rm J}/\psi}/{\rm d}y{\rm d}p_{\rm T}$ for inclusive J/$\psi$ cross section in pp collisions at $\sqrt{s}=5.02$ TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a $p_{\rm T}$-correlated systematic uncertainty.
The nuclear modification factor for inclusive J/$\psi$ production, as a function of centrality, at $\sqrt{s_{\rm NN}}=5.02$ TeV. The widths of the centrality classes used are 2% from 0 to 12%, then 3% up to 30% and 5% for more peripheral collisions. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a centrality-correlated systematic uncertainty.
Centrality dependence (with 10% width centrality classes) of the inclusive J/$\psi$ $R_{\rm AA}$ for $0.3<p_{\rm T}<8$ GeV/$c$. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a centrality-correlated systematic uncertainty.
Centrality dependence (with 10% width centrality classes) of the ratio of the inclusive J/$\psi$ $R_{\rm AA}$ for $0.3<p_{\rm T}<8$ GeV/$c$ at $\sqrt{s_{NN}}$=5.02 and 2.76 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a centrality-correlated systematic uncertainty.
Transverse momentum dependence (in 0-20% centrality class) of the inclusive J/$\psi$ $R_{\rm AA}$. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a $p_{\rm T}$-correlated systematic uncertainty.
Transverse momentum dependence (in 0-20% centrality class) of the double ratio of the inclusive J/$\psi$ $R_{\rm AA}$ at $\sqrt{s_{NN}}$= 5.02 and 2.76 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a $p_{\rm T}$-correlated systematic uncertainty.
Two-particle pseudorapidity correlations are measured in $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV Pb+Pb, $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV $p$+Pb, and $\sqrt{s}$ = 13 TeV $pp$ collisions at the LHC, with total integrated luminosities of approximately 7 $\mu\mathrm{b}^{-1}$, 28 $\mathrm{nb}^{-1}$, and 65 $\mathrm{nb}^{-1}$, respectively. The correlation function $C_{\rm N}(\eta_1,\eta_2)$ is measured as a function of event multiplicity using charged particles in the pseudorapidity range $|\eta|<2.4$. The correlation function contains a significant short-range component, which is estimated and subtracted. After removal of the short-range component, the shape of the correlation function is described approximately by $1+\langle{a_1^2}\rangle \eta_1\eta_2$ in all collision systems over the full multiplicity range. The values of $\sqrt{\langle{a_1^2}\rangle}$ are consistent between the opposite-charge pairs and same-charge pairs, and for the three collision systems at similar multiplicity. The values of $\sqrt{\langle{a_1^2}\rangle}$ and the magnitude of the short-range component both follow a power-law dependence on the event multiplicity. The $\eta$ distribution of the short-range component, after symmetrizing the proton and lead directions in $p$+Pb collisions, is found to be smaller than that in $pp$ collisions with comparable multiplicity.
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (260<=Nch<300)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (260<=Nch<300)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (240<=Nch<260)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (240<=Nch<260)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (220<=Nch<240)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (220<=Nch<240)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (200<=Nch<220)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (200<=Nch<220)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (180<=Nch<200)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (180<=Nch<200)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (160<=Nch<180)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (160<=Nch<180)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (140<=Nch<160)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (140<=Nch<160)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (120<=Nch<140)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (120<=Nch<140)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (100<=Nch<120)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (100<=Nch<120)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (80<=Nch<100)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (80<=Nch<100)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (60<=Nch<80)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (60<=Nch<80)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (40<=Nch<60)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (40<=Nch<60)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (20<=Nch<40)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (20<=Nch<40)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (10<=Nch<20)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (10<=Nch<20)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (260<=Nch<300)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (260<=Nch<300)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (240<=Nch<260)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (240<=Nch<260)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (220<=Nch<240)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (220<=Nch<240)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (200<=Nch<220)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (200<=Nch<220)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (180<=Nch<200)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (180<=Nch<200)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (160<=Nch<180)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (160<=Nch<180)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (140<=Nch<160)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (140<=Nch<160)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (120<=Nch<140)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (120<=Nch<140)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (100<=Nch<120)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (100<=Nch<120)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (80<=Nch<100)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (80<=Nch<100)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (60<=Nch<80)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (60<=Nch<80)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (40<=Nch<60)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (40<=Nch<60)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (20<=Nch<40)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (20<=Nch<40)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (10<=Nch<20)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (10<=Nch<20)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (260<=Nch<300)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (260<=Nch<300)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (240<=Nch<260)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (240<=Nch<260)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (220<=Nch<240)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (220<=Nch<240)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (200<=Nch<220)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (200<=Nch<220)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (180<=Nch<200)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (180<=Nch<200)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (160<=Nch<180)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (160<=Nch<180)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (140<=Nch<160)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (140<=Nch<160)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (120<=Nch<140)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (120<=Nch<140)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (100<=Nch<120)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (100<=Nch<120)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (80<=Nch<100)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (80<=Nch<100)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (60<=Nch<80)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (60<=Nch<80)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (40<=Nch<60)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (40<=Nch<60)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (20<=Nch<40)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (20<=Nch<40)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (10<=Nch<20)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (10<=Nch<20)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (260<=Nch<300)
C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (260<=Nch<300)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (240<=Nch<260)
C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (240<=Nch<260)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (220<=Nch<240)
C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (220<=Nch<240)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (200<=Nch<220)
C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (200<=Nch<220)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (180<=Nch<200)
C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (180<=Nch<200)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (160<=Nch<180)
C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (160<=Nch<180)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (140<=Nch<160)
C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (140<=Nch<160)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (120<=Nch<140)
SRC(eta_1, eta_2) for pp, pT>0.2GeV, (10<=Nch<20)
C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (140<=Nch<160)
C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (140<=Nch<160)
C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (120<=Nch<140)
C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (120<=Nch<140)
C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (100<=Nch<120)
C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (100<=Nch<120)
C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (80<=Nch<100)
C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (80<=Nch<100)
C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (60<=Nch<80)
C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (60<=Nch<80)
C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (40<=Nch<60)
C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (40<=Nch<60)
C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (20<=Nch<40)
C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (20<=Nch<40)
C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (10<=Nch<20)
C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (10<=Nch<20)
<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, w SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, w SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, w SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, w SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, w SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, w SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, w SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, w SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 100<=Nch<120, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 100<=Nch<120, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 100<=Nch<120, w SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 100<=Nch<120, w SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 100<=Nch<120, w SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 100<=Nch<120, w SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 80<=Nch<100, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 80<=Nch<100, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 80<=Nch<100, w SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 80<=Nch<100, w SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 80<=Nch<100, w SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 80<=Nch<100, w SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 60<=Nch<80, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 60<=Nch<80, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 60<=Nch<80, w SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 60<=Nch<80, w SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 60<=Nch<80, w SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 60<=Nch<80, w SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 40<=Nch<60, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 40<=Nch<60, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 40<=Nch<60, w SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 40<=Nch<60, w SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 40<=Nch<60, w SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 40<=Nch<60, w SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 20<=Nch<40, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 20<=Nch<40, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 20<=Nch<40, w SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 20<=Nch<40, w SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 20<=Nch<40, w SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 20<=Nch<40, w SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 10<=Nch<20, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 10<=Nch<20, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 10<=Nch<20, w SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 10<=Nch<20, w SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 10<=Nch<20, w SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 10<=Nch<20, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, wo SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, wo SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, wo SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, wo SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, wo SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, wo SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, wo SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, wo SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, wo SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, wo SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, wo SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, wo SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 100<=Nch<120, wo SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 100<=Nch<120, wo SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 100<=Nch<120, wo SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 100<=Nch<120, wo SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 100<=Nch<120, wo SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 100<=Nch<120, wo SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 80<=Nch<100, wo SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 80<=Nch<100, wo SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 80<=Nch<100, wo SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 80<=Nch<100, wo SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 80<=Nch<100, wo SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 80<=Nch<100, wo SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 60<=Nch<80, wo SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 60<=Nch<80, wo SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 60<=Nch<80, wo SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 60<=Nch<80, wo SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 60<=Nch<80, wo SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 60<=Nch<80, wo SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 40<=Nch<60, wo SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 40<=Nch<60, wo SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 40<=Nch<60, wo SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 40<=Nch<60, wo SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 40<=Nch<60, wo SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 40<=Nch<60, wo SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 20<=Nch<40, wo SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 20<=Nch<40, wo SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 20<=Nch<40, wo SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 20<=Nch<40, wo SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 20<=Nch<40, wo SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 20<=Nch<40, wo SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 10<=Nch<20, wo SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 10<=Nch<20, wo SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 10<=Nch<20, wo SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 10<=Nch<20, wo SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 10<=Nch<20, wo SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 10<=Nch<20, wo SRC, all pairs
a1 from fit C_N^sub(eta-) for Pb+Pb, pT>0.5GeV
a1 from fit C_N^sub(eta-) for Pb+Pb, pT>0.2GeV
a1 from fit C_N^sub(eta+) for Pb+Pb, pT>0.5GeV
a1 from fit C_N^sub(eta+) for Pb+Pb, pT>0.2GeV
a1 from fit r_N^sub(eta) for Pb+Pb, pT>0.5GeV
a1 from fit r_N^sub(eta) for Pb+Pb, pT>0.2GeV
a1 from fit C_N^sub(eta1, eta2) for Pb+Pb, pT>0.5GeV
a1 from fit C_N^sub(eta1, eta2) for Pb+Pb, pT>0.2GeV
a1 from fit C_N^sub(eta-) for p+Pb, pT>0.5GeV
a1 from fit C_N^sub(eta-) for p+Pb, pT>0.2GeV
a1 from fit C_N^sub(eta+) for p+Pb, pT>0.5GeV
a1 from fit C_N^sub(eta+) for p+Pb, pT>0.2GeV
a1 from fit r_N^sub(eta) for p+Pb, pT>0.5GeV
a1 from fit r_N^sub(eta) for p+Pb, pT>0.2GeV
a1 from fit C_N^sub(eta1, eta2) for p+Pb, pT>0.5GeV
a1 from fit C_N^sub(eta1, eta2) for p+Pb, pT>0.2GeV
a1 from fit C_N^sub(eta-) for pp, pT>0.5GeV
a1 from fit C_N^sub(eta-) for pp, pT>0.2GeV
a1 from fit C_N^sub(eta+) for pp, pT>0.5GeV
a1 from fit C_N^sub(eta+) for pp, pT>0.2GeV
a1 from fit r_N^sub(eta) for pp, pT>0.5GeV
a1 from fit r_N^sub(eta) for pp, pT>0.2GeV
a1 from fit C_N^sub(eta1, eta2) for pp, pT>0.5GeV
a1 from fit C_N^sub(eta1, eta2) for pp, pT>0.2GeV
SRC for Pb+Pb, pT>0.5GeV, all pairs
SRC for Pb+Pb, pT>0.2GeV, all pairs
SRC for Pb+Pb, pT>0.5GeV, opposite pairs
SRC for Pb+Pb, pT>0.2GeV, opposite pairs
SRC for Pb+Pb, pT>0.5GeV, same pairs
SRC for Pb+Pb, pT>0.2GeV, same pairs
SRC for p+Pb, pT>0.5GeV, all pairs
SRC for p+Pb, pT>0.2GeV, all pairs
SRC for p+Pb, pT>0.5GeV, opposite pairs
SRC for p+Pb, pT>0.2GeV, opposite pairs
SRC for p+Pb, pT>0.5GeV, same pairs
SRC for p+Pb, pT>0.2GeV, same pairs
SRC for pp, pT>0.5GeV, all pairs
SRC for pp, pT>0.2GeV, all pairs
SRC for pp, pT>0.5GeV, opposite pairs
SRC for pp, pT>0.2GeV, opposite pairs
SRC for pp, pT>0.5GeV, same pairs
SRC for pp, pT>0.2GeV, same pairs
SRC for Pb+Pb, pT>0.5GeV
SRC for Pb+Pb, pT>0.2GeV
SRC for p+Pb, pT>0.5GeV
SRC for p+Pb, pT>0.2GeV
SRC for pp, pT>0.5GeV
SRC for pp, pT>0.2GeV
a1 for Pb+Pb, pT>0.5GeV
a1 for Pb+Pb, pT>0.2GeV
a1 for p+Pb, pT>0.5GeV
High statistics measurements of the photon asymmetry $\mathrm{\Sigma}$ for the $\overrightarrow{\gamma}$p$\rightarrow\pi^{0}$p reaction have been made in the center of mass energy range W=1214-1450 MeV. The data were measured with the MAMI A2 real photon beam and Crystal Ball/TAPS detector systems in Mainz, Germany. The results significantly improve the existing world data and are shown to be in good agreement with previous measurements, and with the MAID, SAID, and Bonn-Gatchina predictions. We have also combined the photon asymmetry results with recent cross-section measurements from Mainz to calculate the profile functions, $\check{\mathrm{\Sigma}}$ (= $\sigma_{0}\mathrm{\Sigma}$), and perform a moment analysis. Comparison with calculations from the Bonn-Gatchina model shows that the precision of the data is good enough to further constrain the higher partial waves, and there is an indication of interference between the very small $F$-waves and the $N(1520) 3/2^{-}$ and $N(1535) 1/2^{-}$ resonances.
Photon beam asymmetry Sigma at W=1.2159988 GeV
Photon beam asymmetry Sigma at W=1.2194968 GeV
Photon beam asymmetry Sigma at W=1.2225014 GeV
Photon beam asymmetry Sigma at W=1.2254987 GeV
Photon beam asymmetry Sigma at W=1.2290003 GeV
Photon beam asymmetry Sigma at W=1.2324995 GeV
Photon beam asymmetry Sigma at W=1.2355029 GeV
Photon beam asymmetry Sigma at W=1.2389989 GeV
Photon beam asymmetry Sigma at W=1.2425001 GeV
Photon beam asymmetry Sigma at W=1.2455020 GeV
Photon beam asymmetry Sigma at W=1.2484967 GeV
Photon beam asymmetry Sigma at W=1.2514991 GeV
Photon beam asymmetry Sigma at W=1.2550029 GeV
Photon beam asymmetry Sigma at W=1.2584969 GeV
Photon beam asymmetry Sigma at W=1.2614979 GeV
Photon beam asymmetry Sigma at W=1.2644992 GeV
Photon beam asymmetry Sigma at W=1.2675008 GeV
Photon beam asymmetry Sigma at W=1.2705027 GeV
Photon beam asymmetry Sigma at W=1.2739984 GeV
Photon beam asymmetry Sigma at W=1.2774992 GeV
Photon beam asymmetry Sigma at W=1.2804996 GeV
Photon beam asymmetry Sigma at W=1.2835003 GeV
Photon beam asymmetry Sigma at W=1.2864940 GeV
Photon beam asymmetry Sigma at W=1.2895026 GeV
Photon beam asymmetry Sigma at W=1.2924970 GeV
Photon beam asymmetry Sigma at W=1.2954989 GeV
Photon beam asymmetry Sigma at W=1.2989995 GeV
Photon beam asymmetry Sigma at W=1.3024980 GeV
Photon beam asymmetry Sigma at W=1.3054984 GeV
Photon beam asymmetry Sigma at W=1.3084992 GeV
Photon beam asymmetry Sigma at W=1.3115002 GeV
Photon beam asymmetry Sigma at W=1.3145016 GeV
Photon beam asymmetry Sigma at W=1.3175032 GeV
Photon beam asymmetry Sigma at W=1.3204980 GeV
Photon beam asymmetry Sigma at W=1.3235001 GeV
Photon beam asymmetry Sigma at W=1.3265026 GeV
Photon beam asymmetry Sigma at W=1.3294983 GeV
Photon beam asymmetry Sigma at W=1.3325013 GeV
Photon beam asymmetry Sigma at W=1.3354976 GeV
Photon beam asymmetry Sigma at W=1.3385012 GeV
Photon beam asymmetry Sigma at W=1.3414981 GeV
Photon beam asymmetry Sigma at W=1.3445022 GeV
Photon beam asymmetry Sigma at W=1.3474997 GeV
Photon beam asymmetry Sigma at W=1.3504974 GeV
Photon beam asymmetry Sigma at W=1.3535024 GeV
Photon beam asymmetry Sigma at W=1.3565007 GeV
Photon beam asymmetry Sigma at W=1.3594993 GeV
Photon beam asymmetry Sigma at W=1.3624982 GeV
Photon beam asymmetry Sigma at W=1.3654974 GeV
Photon beam asymmetry Sigma at W=1.3684968 GeV
Photon beam asymmetry Sigma at W=1.3714966 GeV
Photon beam asymmetry Sigma at W=1.3744966 GeV
Photon beam asymmetry Sigma at W=1.3774969 GeV
Photon beam asymmetry Sigma at W=1.3804974 GeV
Photon beam asymmetry Sigma at W=1.3834983 GeV
Photon beam asymmetry Sigma at W=1.3864994 GeV
Photon beam asymmetry Sigma at W=1.3890010 GeV
Photon beam asymmetry Sigma at W=1.3914981 GeV
Photon beam asymmetry Sigma at W=1.3945022 GeV
Photon beam asymmetry Sigma at W=1.3974998 GeV
Photon beam asymmetry Sigma at W=1.4004978 GeV
Photon beam asymmetry Sigma at W=1.4035026 GeV
Photon beam asymmetry Sigma at W=1.4065011 GeV
Photon beam asymmetry Sigma at W=1.4094998 GeV
Photon beam asymmetry Sigma at W=1.4119939 GeV
Photon beam asymmetry Sigma at W=1.4144969 GeV
Photon beam asymmetry Sigma at W=1.4174985 GeV
Photon beam asymmetry Sigma at W=1.4205005 GeV
Photon beam asymmetry Sigma at W=1.4235027 GeV
Photon beam asymmetry Sigma at W=1.4259986 GeV
Photon beam asymmetry Sigma at W=1.4284967 GeV
Photon beam asymmetry Sigma at W=1.4315018 GeV
Photon beam asymmetry Sigma at W=1.4345006 GeV
Photon beam asymmetry Sigma at W=1.4374997 GeV
Photon beam asymmetry Sigma at W=1.4399974 GeV
Photon beam asymmetry Sigma at W=1.4424973 GeV
Photon beam asymmetry Sigma at W=1.4454993 GeV
Photon beam asymmetry Sigma at W=1.4485015 GeV
At sufficiently high temperature and energy density, nuclear matter undergoes a transition to a phase in which quarks and gluons are not confined: the Quark-Gluon Plasma (QGP) [1]. Such an extreme state of strongly-interacting QCD (Quantum Chromo-Dynamics) matter is produced in the laboratory with high-energy collisions of heavy nuclei, where an enhanced production of strange hadrons is observed [2-6]. Strangeness enhancement, originally proposed as a signature of QGP formation in nuclear collisions [7], is more pronounced for multi-strange baryons. Several effects typical of heavy-ion phenomenology have been observed in high-multiplicity proton-proton (pp) collisions [8,9]. Yet, enhanced production of multi-strange particles has not been reported so far. Here we present the first observation of strangeness enhancement in high-multiplicity pp collisions. We find that the integrated yields of strange and multi-strange particles relative to pions increases significantly with the event charged-particle multiplicity. The measurements are in remarkable agreement with p-Pb collision results [10,11] indicating that the phenomenon is related to the final system created in the collision. In high-multiplicity events strangeness production reaches values similar to those observed in Pb-Pb collisions, where a QGP is formed.
$K^{0}_{S}$ transverse momentum spectrum: V0M Class I (pp at $\sqrt{s}=7$ TeV).
$K^{0}_{S}$ transverse momentum spectrum: V0M Class II (pp at $\sqrt{s}=7$ TeV).
$K^{0}_{S}$ transverse momentum spectrum: V0M Class III (pp at $\sqrt{s}=7$ TeV).
$K^{0}_{S}$ transverse momentum spectrum: V0M Class IV (pp at $\sqrt{s}=7$ TeV).
$K^{0}_{S}$ transverse momentum spectrum: V0M Class V (pp at $\sqrt{s}=7$ TeV).
$K^{0}_{S}$ transverse momentum spectrum: V0M Class VI (pp at $\sqrt{s}=7$ TeV).
$K^{0}_{S}$ transverse momentum spectrum: V0M Class VII (pp at $\sqrt{s}=7$ TeV).
$K^{0}_{S}$ transverse momentum spectrum: V0M Class VIII (pp at $\sqrt{s}=7$ TeV).
$K^{0}_{S}$ transverse momentum spectrum: V0M Class IX (pp at $\sqrt{s}=7$ TeV).
$K^{0}_{S}$ transverse momentum spectrum: V0M Class X (pp at $\sqrt{s}=7$ TeV).
$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class I (pp at $\sqrt{s}=7$ TeV).
$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class II (pp at $\sqrt{s}=7$ TeV).
$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class III (pp at $\sqrt{s}=7$ TeV).
$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class IV (pp at $\sqrt{s}=7$ TeV).
$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class V (pp at $\sqrt{s}=7$ TeV).
$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class VI (pp at $\sqrt{s}=7$ TeV).
$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class VII (pp at $\sqrt{s}=7$ TeV).
$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class VIII (pp at $\sqrt{s}=7$ TeV).
$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class IX (pp at $\sqrt{s}=7$ TeV).
$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class X (pp at $\sqrt{s}=7$ TeV).
$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class I (pp at $\sqrt{s}=7$ TeV).
$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class II (pp at $\sqrt{s}=7$ TeV).
$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class III (pp at $\sqrt{s}=7$ TeV).
$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class IV (pp at $\sqrt{s}=7$ TeV).
$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class V (pp at $\sqrt{s}=7$ TeV).
$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class VI (pp at $\sqrt{s}=7$ TeV).
$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class VII (pp at $\sqrt{s}=7$ TeV).
$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class VIII (pp at $\sqrt{s}=7$ TeV).
$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class IX (pp at $\sqrt{s}=7$ TeV).
$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class X (pp at $\sqrt{s}=7$ TeV).
$\Omega^{-}+\bar{\Omega}^{+}$ transverse momentum spectrum: V0M Class I+II (pp at $\sqrt{s}=7$ TeV).
$\Omega^{-}+\bar{\Omega}^{+}$ transverse momentum spectrum: V0M Class III+IV (pp at $\sqrt{s}=7$ TeV).
$\Omega^{-}+\bar{\Omega}^{+}$ transverse momentum spectrum: V0M Class V+VI (pp at $\sqrt{s}=7$ TeV).
$\Omega^{-}+\bar{\Omega}^{+}$ transverse momentum spectrum: V0M Class VII+VIII (pp at $\sqrt{s}=7$ TeV).
$\Omega^{-}+\bar{\Omega}^{+}$ transverse momentum spectrum: V0M Class IX+X (pp at $\sqrt{s}=7$ TeV).
$2K^{0}_{S}/(\pi^{+}+\pi^{-})$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of the average charged particle multiplicity density at midrapidity.
$(\Lambda+\bar{\Lambda})/(\pi^{+}+\pi^{-})$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of the average charged particle multiplicity density at midrapidity.
$(\Xi^{-}+\bar{\Xi}^{+})/(\pi^{+}+\pi^{-})$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of the average charged particle multiplicity density at midrapidity.
$(\Omega^{-}+\bar{\Omega}^{+})/(\pi^{+}+\pi^{-})$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of the average charged particle multiplicity density at midrapidity.
$\pi^{+}+\pi^{-}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).
$p+\bar{p}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).
$K^{0}_{S}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).
$\Lambda+\bar{\Lambda}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).
$\Xi^{-}+\bar{\Xi}^{+}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).
$\Omega^{-}+\bar{\Omega}^{+}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).
$(\Lambda+\bar{\Lambda})/2K^{0}_{S}$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of charged particle multiplicity density at midrapidity.
$(p+\bar{p})/(\pi^{+}+\pi^{-})$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of charged particle multiplicity density at midrapidity.
$(2K^{0}_{S})/(\pi^{+}+\pi^{-})$ double-ratio vs multiplicity for pp collisions at $\sqrt{s}=7$ TeV.
$(\Lambda+\bar{\Lambda})/(\pi^{+}+\pi^{-})$ double-ratio vs multiplicity for pp collisions at $\sqrt{s}=7$ TeV.
$(\Xi^{-}+\bar{\Xi}^{+})/(\pi^{+}+\pi^{-})$ double-ratio vs multiplicity for pp collisions at $\sqrt{s}=7$ TeV.
$(\Omega^{-}+\bar{\Omega}^{+})/(\pi^{+}+\pi^{-})$ double-ratio vs multiplicity for pp collisions at $\sqrt{s}=7$ TeV.
Event multiplicity classes, their corresponding fraction of the INEL>0 cross-section and their corresponding average charged particle density at midrapidity ($|\eta|<0.5$). The value of in the inclusive (INEL>0) class is 5.96 $\pm$ 0.23. The uncertainties are the quadratic sum of statistical and systematic contributions.
The process $e^+e^-\to\omega\eta\pi^0$ is studied in the energy range $1.45-2.00$ GeV using data with an integrated luminosity of 33 pb$^{-1}$ accumulated by the SND detector at the $e^+e^-$ collider VEPP-2000. The $e^+e^-\to\omega\eta\pi^0$ cross section is measured for the first time. The cross section has a threshold near 1.75 GeV. Its value is about 2 nb in the energy range $1.8-2.0$ GeV. The dominant intermediate state for the process $e^+e^- \to \omega\eta\pi^0$ is found to be $\omega a_0(980)$.
The energy interval, integrated luminosity ($L$), number of selected events ($N$), estimated number of background events ($N_{bkg}$), detection efficiency for $e^+e^-\to\omega\eta\pi^0\to 7\gamma$ events ($\epsilon$), radiative correction ($\delta+1$), and $e^+e^-\to\omega\eta\pi^0$ Born cross section ($\sigma$). The shown cross-section errors are statistical. The systematic error is 4.2%. The 90% confidence level upper limits are listed for the first two energy intervals.
The elliptic, triangular, quadrangular and pentagonal anisotropic flow coefficients for $\pi^{\pm}$, $\mathrm{K}^{\pm}$ and p+$\overline{\mathrm{p}}$ in Pb-Pb collisions at $\sqrt{s_\mathrm{{NN}}} = 2.76$ TeV were measured with the ALICE detector at the Large Hadron Collider. The results were obtained with the Scalar Product method, correlating the identified hadrons with reference particles from a different pseudorapidity region. Effects not related to the common event symmetry planes (non-flow) were estimated using correlations in pp collisions and were subtracted from the measurement. The obtained flow coefficients exhibit a clear mass ordering for transverse momentum ($p_{\mathrm{T}}$) values below $\approx$ 3 GeV/$c$. In the intermediate $p_{\mathrm{T}}$ region ($3 < p_{\mathrm{T}} < 6$ GeV/$c$), particles group at an approximate level according to the number of constituent quarks, suggesting that coalescence might be the relevant particle production mechanism in this region. The results for $p_{\mathrm{T}} < 3$ GeV/$c$ are described fairly well by a hydrodynamical model (iEBE-VISHNU) that uses initial conditions generated by A Multi-Phase Transport model (AMPT) and describes the expansion of the fireball using a value of 0.08 for the ratio of shear viscosity to entropy density ($\eta/s$), coupled to a hadronic cascade model (UrQMD). Finally, expectations from AMPT alone fail to quantitatively describe the measurements for all harmonics throughout the measured transverse momentum region. However, the comparison to the AMPT model highlights the importance of the late hadronic rescattering stage to the development of the observed mass ordering at low values of $p_{\mathrm{T}}$ and of coalescence as a particle production mechanism for the particle type grouping at intermediate values of $p_{\mathrm{T}}$ for all harmonics.
pion <uQ>2 as a function of pT in pp collision.
kaon <uQ>2 as a function of pT in pp collision.
proton <uQ>2 as a function of pT in pp collision.
pion <uQ>3 as a function of pT in pp collision.
kaon <uQ>3 as a function of pT in pp collision.
proton <uQ>3 as a function of pT in pp collision.
pion <uQ>4 as a function of pT in pp collision.
kaon <uQ>4 as a function of pT in pp collision.
proton <uQ>4 as a function of pT in pp collision.
pion <uQ>5 as a function of pT in pp collision.
kaon <uQ>5 as a function of pT in pp collision.
proton <uQ>5 as a function of pT in pp collision.
pion <uQ>2 as a function of pT for centrality: 0-1%.
pion <uQ>2 as a function of pT for centrality: 20-30%.
pion <uQ>2 as a function of pT for centrality: 40-50%.
kaon <uQ>2 as a function of pT for centrality: 0-1%.
kaon <uQ>2 as a function of pT for centrality: 20-30%.
kaon <uQ>2 as a function of pT for centrality: 40-50%.
proton <uQ>2 as a function of pT for centrality: 0-1%.
proton <uQ>2 as a function of pT for centrality: 20-30%.
proton <uQ>2 as a function of pT for centrality: 40-50%.
pion <uQ>3 as a function of pT for centrality: 0-1%.
pion <uQ>3 as a function of pT for centrality: 20-30%.
pion <uQ>3 as a function of pT for centrality: 40-50%.
kaon <uQ>3 as a function of pT for centrality: 0-1%.
kaon <uQ>3 as a function of pT for centrality: 20-30%.
kaon <uQ>3 as a function of pT for centrality: 40-50%.
proton <uQ>3 as a function of pT for centrality: 0-1%.
proton <uQ>3 as a function of pT for centrality: 20-30%.
proton <uQ>3 as a function of pT for centrality: 40-50%.
pion <uQ>4 as a function of pT for centrality: 0-1%.
pion <uQ>4 as a function of pT for centrality: 20-30%.
pion <uQ>4 as a function of pT for centrality: 40-50%.
kaon <uQ>4 as a function of pT for centrality: 0-1%.
kaon <uQ>4 as a function of pT for centrality: 20-30%.
kaon <uQ>4 as a function of pT for centrality: 40-50%.
proton <uQ>4 as a function of pT for centrality: 0-1%.
proton <uQ>4 as a function of pT for centrality: 20-30%.
proton <uQ>4 as a function of pT for centrality: 40-50%.
pion <uQ>5 as a function of pT for centrality: 0-1%.
pion <uQ>5 as a function of pT for centrality: 20-30%.
pion <uQ>5 as a function of pT for centrality: 40-50%.
kaon <uQ>5 as a function of pT for centrality: 0-1%.
kaon <uQ>5 as a function of pT for centrality: 20-30%.
kaon <uQ>5 as a function of pT for centrality: 40-50%.
proton <uQ>5 as a function of pT for centrality: 0-1%.
proton <uQ>5 as a function of pT for centrality: 20-30%.
proton <uQ>5 as a function of pT for centrality: 40-50%.
pion v2 as a function of pT for centrality: 0-1%.
pion v2 as a function of pT for centrality: 0-5%.
pion v2 as a function of pT for centrality: 5-10%.
pion v2 as a function of pT for centrality: 10-20%.
pion v2 as a function of pT for centrality: 20-30%.
pion v2 as a function of pT for centrality: 30-40%.
pion v2 as a function of pT for centrality: 40-50%.
kaon v2 as a function of pT for centrality: 0-1%.
kaon v2 as a function of pT for centrality: 0-5%.
kaon v2 as a function of pT for centrality: 5-10%.
kaon v2 as a function of pT for centrality: 10-20%.
kaon v2 as a function of pT for centrality: 20-30%.
kaon v2 as a function of pT for centrality: 30-40%.
kaon v2 as a function of pT for centrality: 40-50%.
proton v2 as a function of pT for centrality: 0-1%.
proton v2 as a function of pT for centrality: 0-5%.
proton v2 as a function of pT for centrality: 5-10%.
proton v2 as a function of pT for centrality: 10-20%.
proton v2 as a function of pT for centrality: 20-30%.
proton v2 as a function of pT for centrality: 30-40%.
proton v2 as a function of pT for centrality: 40-50%.
pion v3 as a function of pT for centrality: 0-1%.
pion v3 as a function of pT for centrality: 0-5%.
pion v3 as a function of pT for centrality: 5-10%.
pion v3 as a function of pT for centrality: 10-20%.
pion v3 as a function of pT for centrality: 20-30%.
pion v3 as a function of pT for centrality: 30-40%.
pion v3 as a function of pT for centrality: 40-50%.
kaon v3 as a function of pT for centrality: 0-1%.
kaon v3 as a function of pT for centrality: 0-5%.
kaon v3 as a function of pT for centrality: 5-10%.
kaon v3 as a function of pT for centrality: 10-20%.
kaon v3 as a function of pT for centrality: 20-30%.
kaon v3 as a function of pT for centrality: 30-40%.
kaon v3 as a function of pT for centrality: 40-50%.
proton v3 as a function of pT for centrality: 0-1%.
proton v3 as a function of pT for centrality: 0-5%.
proton v3 as a function of pT for centrality: 5-10%.
proton v3 as a function of pT for centrality: 10-20%.
proton v3 as a function of pT for centrality: 20-30%.
proton v3 as a function of pT for centrality: 30-40%.
proton v3 as a function of pT for centrality: 40-50%.
pion v4 as a function of pT for centrality: 0-1%.
pion v4 as a function of pT for centrality: 0-5%.
pion v4 as a function of pT for centrality: 5-10%.
pion v4 as a function of pT for centrality: 10-20%.
pion v4 as a function of pT for centrality: 20-30%.
pion v4 as a function of pT for centrality: 30-40%.
pion v4 as a function of pT for centrality: 40-50%.
kaon v4 as a function of pT for centrality: 0-1%.
kaon v4 as a function of pT for centrality: 0-5%.
kaon v4 as a function of pT for centrality: 5-10%.
kaon v4 as a function of pT for centrality: 10-20%.
kaon v4 as a function of pT for centrality: 20-30%.
kaon v4 as a function of pT for centrality: 30-40%.
kaon v4 as a function of pT for centrality: 40-50%.
proton v4 as a function of pT for centrality: 0-1%.
proton v4 as a function of pT for centrality: 0-5%.
proton v4 as a function of pT for centrality: 5-10%.
proton v4 as a function of pT for centrality: 10-20%.
proton v4 as a function of pT for centrality: 20-30%.
proton v4 as a function of pT for centrality: 30-40%.
proton v4 as a function of pT for centrality: 40-50%.
pion v5 as a function of pT for centrality: 0-1%.
pion v5 as a function of pT for centrality: 0-5%.
pion v5 as a function of pT for centrality: 5-10%.
pion v5 as a function of pT for centrality: 10-20%.
pion v5 as a function of pT for centrality: 20-30%.
pion v5 as a function of pT for centrality: 30-40%.
pion v5 as a function of pT for centrality: 40-50%.
kaon v5 as a function of pT for centrality: 0-1%.
kaon v5 as a function of pT for centrality: 0-5%.
kaon v5 as a function of pT for centrality: 5-10%.
kaon v5 as a function of pT for centrality: 10-20%.
kaon v5 as a function of pT for centrality: 20-30%.
kaon v5 as a function of pT for centrality: 30-40%.
kaon v5 as a function of pT for centrality: 40-50%.
proton v5 as a function of pT for centrality: 0-1%.
proton v5 as a function of pT for centrality: 0-5%.
proton v5 as a function of pT for centrality: 5-10%.
proton v5 as a function of pT for centrality: 10-20%.
proton v5 as a function of pT for centrality: 20-30%.
proton v5 as a function of pT for centrality: 30-40%.
proton v5 as a function of pT for centrality: 40-50%.
pion delta2 as a function of pT for centrality: 0-1%.
pion delta2 as a function of pT for centrality: 0-5%.
pion delta2 as a function of pT for centrality: 5-10%.
pion delta2 as a function of pT for centrality: 10-20%.
pion delta2 as a function of pT for centrality: 20-30%.
pion delta2 as a function of pT for centrality: 30-40%.
pion delta2 as a function of pT for centrality: 40-50%.
kaon delta2 as a function of pT for centrality: 0-1%.
kaon delta2 as a function of pT for centrality: 0-5%.
kaon delta2 as a function of pT for centrality: 5-10%.
kaon delta2 as a function of pT for centrality: 10-20%.
kaon delta2 as a function of pT for centrality: 20-30%.
kaon delta2 as a function of pT for centrality: 30-40%.
kaon delta2 as a function of pT for centrality: 40-50%.
proton delta2 as a function of pT for centrality: 0-1%.
proton delta2 as a function of pT for centrality: 0-5%.
proton delta2 as a function of pT for centrality: 5-10%.
proton delta2 as a function of pT for centrality: 10-20%.
proton delta2 as a function of pT for centrality: 20-30%.
proton delta2 as a function of pT for centrality: 30-40%.
proton delta2 as a function of pT for centrality: 40-50%.
pion delta3 as a function of pT for centrality: 0-1%.
pion delta3 as a function of pT for centrality: 0-5%.
pion delta3 as a function of pT for centrality: 5-10%.
pion delta3 as a function of pT for centrality: 10-20%.
pion delta3 as a function of pT for centrality: 20-30%.
pion delta3 as a function of pT for centrality: 30-40%.
pion delta3 as a function of pT for centrality: 40-50%.
kaon delta3 as a function of pT for centrality: 0-1%.
kaon delta3 as a function of pT for centrality: 0-5%.
kaon delta3 as a function of pT for centrality: 5-10%.
kaon delta3 as a function of pT for centrality: 10-20%.
kaon delta3 as a function of pT for centrality: 20-30%.
kaon delta3 as a function of pT for centrality: 30-40%.
kaon delta3 as a function of pT for centrality: 40-50%.
proton delta3 as a function of pT for centrality: 0-1%.
proton delta3 as a function of pT for centrality: 0-5%.
proton delta3 as a function of pT for centrality: 5-10%.
proton delta3 as a function of pT for centrality: 10-20%.
proton delta3 as a function of pT for centrality: 20-30%.
proton delta3 as a function of pT for centrality: 30-40%.
proton delta3 as a function of pT for centrality: 40-50%.
pion delta4 as a function of pT for centrality: 0-1%.
pion delta4 as a function of pT for centrality: 0-5%.
pion delta4 as a function of pT for centrality: 5-10%.
pion delta4 as a function of pT for centrality: 10-20%.
pion delta4 as a function of pT for centrality: 20-30%.
pion delta4 as a function of pT for centrality: 30-40%.
pion delta4 as a function of pT for centrality: 40-50%.
kaon delta4 as a function of pT for centrality: 0-1%.
kaon delta4 as a function of pT for centrality: 0-5%.
kaon delta4 as a function of pT for centrality: 5-10%.
kaon delta4 as a function of pT for centrality: 10-20%.
kaon delta4 as a function of pT for centrality: 20-30%.
kaon delta4 as a function of pT for centrality: 30-40%.
kaon delta4 as a function of pT for centrality: 40-50%.
proton delta4 as a function of pT for centrality: 0-1%.
proton delta4 as a function of pT for centrality: 0-5%.
proton delta4 as a function of pT for centrality: 5-10%.
proton delta4 as a function of pT for centrality: 10-20%.
proton delta4 as a function of pT for centrality: 20-30%.
proton delta4 as a function of pT for centrality: 30-40%.
proton delta4 as a function of pT for centrality: 40-50%.
pion delta5 as a function of pT for centrality: 0-1%.
pion delta5 as a function of pT for centrality: 0-5%.
pion delta5 as a function of pT for centrality: 5-10%.
pion delta5 as a function of pT for centrality: 10-20%.
pion delta5 as a function of pT for centrality: 20-30%.
pion delta5 as a function of pT for centrality: 30-40%.
pion delta5 as a function of pT for centrality: 40-50%.
kaon delta5 as a function of pT for centrality: 0-1%.
kaon delta5 as a function of pT for centrality: 0-5%.
kaon delta5 as a function of pT for centrality: 5-10%.
kaon delta5 as a function of pT for centrality: 10-20%.
kaon delta5 as a function of pT for centrality: 20-30%.
kaon delta5 as a function of pT for centrality: 30-40%.
kaon delta5 as a function of pT for centrality: 40-50%.
proton delta5 as a function of pT for centrality: 0-1%.
proton delta5 as a function of pT for centrality: 0-5%.
proton delta5 as a function of pT for centrality: 5-10%.
proton delta5 as a function of pT for centrality: 10-20%.
proton delta5 as a function of pT for centrality: 20-30%.
proton delta5 as a function of pT for centrality: 30-40%.
proton delta5 as a function of pT for centrality: 40-50%.
pion Integrated v2 as a function of centrality percentile:.
kaon Integrated v2 as a function of centrality percentile:.
proton Integrated v2 as a function of centrality percentile:.
pion Integrated v3 as a function of centrality percentile:.
kaon Integrated v3 as a function of centrality percentile:.
proton Integrated v3 as a function of centrality percentile:.
pion Integrated v4 as a function of centrality percentile:.
kaon Integrated v4 as a function of centrality percentile:.
proton Integrated v4 as a function of centrality percentile:.
pion Integrated v5 as a function of centrality percentile:.
kaon Integrated v5 as a function of centrality percentile:.
proton Integrated v5 as a function of centrality percentile:.
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