Charged-hadron spectrum in the centrality interval 5-10% for p+Pb, divided by 〈TPPB〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 10-20% for p+Pb, divided by 〈TPPB〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 20-30% for p+Pb, divided by 〈TPPB〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 30-40% for p+Pb, divided by 〈TPPB〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 40-60% for p+Pb, divided by 〈TPPB〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 60-90% for p+Pb, divided by 〈TPPB〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 0-90% for p+Pb, divided by 〈TPPB〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron cross-section in pp collisions. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 0-5% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Charged-hadron spectrum in the centrality interval 5-10% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Charged-hadron spectrum in the centrality interval 10-20% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Charged-hadron spectrum in the centrality interval 20-30% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Charged-hadron spectrum in the centrality interval 30-40% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Charged-hadron spectrum in the centrality interval 40-50% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Charged-hadron spectrum in the centrality interval 50-60% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Charged-hadron spectrum in the centrality interval 60-80% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Charged-hadron cross-section in pp collisions. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 0-5% for Xe+Xe, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 5-10% for Xe+Xe, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 10-20% for Xe+Xe, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 20-30% for Xe+Xe, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 30-40% for Xe+Xe, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 40-50% for Xe+Xe, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 50-60% for Xe+Xe, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 60-80% for Xe+Xe, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-60% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-90% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-90% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Nuclear modification factor in centrality interval 5-10% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Nuclear modification factor in centrality interval 10-20% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Nuclear modification factor in centrality interval 20-30% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Nuclear modification factor in centrality interval 30-40% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Nuclear modification factor in centrality interval 40-50% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Nuclear modification factor in centrality interval 50-60% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Nuclear modification factor in centrality interval 60-80% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Nuclear modification factor in centrality interval 0-5% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-50% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 50-60% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-80% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-60% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-60% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-60% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-60% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-90% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-90% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-90% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-90% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-90% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-90% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-90% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-90% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-50% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-50% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-50% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-50% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 50-60% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 50-60% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 50-60% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 50-60% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-80% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-80% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-80% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-80% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-50% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-50% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-50% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 50-60% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 50-60% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 50-60% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-80% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-80% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-80% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Double differential cross sections for charged particle jets as a function of the jet PT in the |rapidity| range 1.5-1.9, shown separately for the two R values. The first (sys) errors is the correlated efficiency uncertainty and the second (sys) error is the correlated vetex splitting uncertainty. The third (sys) error is the quadratic sum of all the uncorrelated systematic uncertainties.

Multiplicity of charged particles per jet in the |rapidity| range 0.0-1.9 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.0-1.9 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.0-1.9 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.0-1.9 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.0-1.9 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.0-0.5 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.0-0.5 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.0-0.5 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.0-0.5 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.0-0.5 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.5-1.0 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.5-1.0 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.5-1.0 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.5-1.0 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 0.5-1.0 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 1.0-1.5 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 1.0-1.5 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 1.0-1.5 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 1.0-1.5 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 1.0-1.5 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 1.5-1.9 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 1.5-1.9 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 1.5-1.9 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 1.5-1.9 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Multiplicity of charged particles per jet in the |rapidity| range 1.5-1.9 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.0-1.9 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.0-1.9 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.0-1.9 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.0-1.9 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.0-1.9 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.0-0.5 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.0-0.5 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.0-0.5 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.0-0.5 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.0-0.5 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.5-1.0 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.5-1.0 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.5-1.0 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.5-1.0 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 0.5-1.0 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 1.0-1.5 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 1.0-1.5 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 1.0-1.5 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 1.0-1.5 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 1.0-1.5 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 1.5-1.9 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 1.5-1.9 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 1.5-1.9 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 1.5-1.9 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the fragmentation variable Z in the |rapidity| range 1.5-1.9 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.0-1.9 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.0-1.9 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.0-1.9 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.0-1.9 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.0-1.9 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.0-0.5 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.0-0.5 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.0-0.5 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.0-0.5 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.0-0.5 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.5-1.0 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.5-1.0 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.5-1.0 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.5-1.0 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 0.5-1.0 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 1.0-1.5 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 1.0-1.5 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 1.0-1.5 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 1.0-1.5 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 1.0-1.5 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 1.5-1.9 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 1.5-1.9 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 1.5-1.9 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 1.5-1.9 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle PT(rel) wrt anti-kt jets in the |rapidity| range 1.5-1.9 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.0-1.9 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.0-1.9 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.0-1.9 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.0-1.9 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.0-1.9 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.0-0.5 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.0-0.5 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.0-0.5 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.0-0.5 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.0-0.5 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.5-1.0 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.5-1.0 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.5-1.0 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.5-1.0 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 0.5-1.0 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 1.0-1.5 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 1.0-1.5 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 1.0-1.5 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 1.0-1.5 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 1.0-1.5 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 1.5-1.9 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 1.5-1.9 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 1.5-1.9 and transverse momentum 10-15 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 1.5-1.9 and transverse momentum 15-24 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Distribution of the charged particle number density RHO in the |rapidity| range 1.5-1.9 and transverse momentum 24-40 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.

Rapidity distributions for PHI mesons produced in P P collisions.

Integrated yields of PHI and PI mesons and their ratio.

Multiplicity dependence of the PHI/PI ratio in P P collisions.

Centrality dependence of the PHI/PI ratio in the forward hemisphere in P PBcollisions normalised to the average P P values. Here N(C=CD) is the number emi tted in the backward direction in P PB collisions and is essentially related to the mean number of collisions of the projectile in the target.

'PRODUCED PARTICLES' (SEE CONDITIONS).

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