cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.156764.v1/t11
title: "Table 3" of "Search for jet quenching with dijets from high-multiplicity pPb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV"

description: Mean xj ratio, $\langle x_{j} \rangle$, in the range $10-60$ as unfolded for different multiplicities, for different leading and subleading jet combinations for the midrapidity, forward, and backward regions
description: The first measurement of the dijet transverse momentum balance ($x_{j}$) in proton-lead (pPb) collisions at nucleon-nucleon center-of–mass energy $\sqrt{s_{\text{\tiny NN}}} = $8.16$~\text{TeV}$ is presented. The analysis uses data collected with the CMS detector in 2016, corresponding to an integrated luminosity of 174.6$~\text{nb}^\text{$-$1}$. The average values and distributions of $x_{j}$ are measured as functions of the event charged-particle multiplicity for various combinations of the pseudorapidity regions in which the two jets are found. These different configurations enable measurements of distinct nucleon momentum fractions x in both proton- and lead-going directions. Thanks to high-multiplicity triggers, designed for probing potential jet-quenching effects, we reached a charged-particle multiplicity as high as 400. Collective behavior of the outgoing particles was previously observed in very high multiplicity pPb events, possibly indicating the formation of small quark-gluon plasma (QGP) droplets. The ratio of $x_{j}$ for high multiplicity to low-multiplicity events is used to quantify possible medium effects. The results are found to be consistent with simulations of the hard-scattering process that do not include (QGP) production. These measurements provide a limit on medium-induced energy loss of 1.26% at the 90% confidence level in terms of subleading jet's transverse momentum in high multiplicity pPb events.
DOI: 10.17182/hepdata.156764.v1/t12
title: "Table 4a" of "Search for jet quenching with dijets from high-multiplicity pPb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV"

description: The reconstructed (raw) dijet balance distribution, $(1/N_{dijet})(dN_{dijet}/dx_{j})$, as function of $x_{j}$ for the $10-60$, $60-120$, $120-185$, $185-250$ and $250-400$ multiplicity ranges with both jets at the midrapidity regions.
description: The first measurement of the dijet transverse momentum balance ($x_{j}$) in proton-lead (pPb) collisions at nucleon-nucleon center-of–mass energy $\sqrt{s_{\text{\tiny NN}}} = $8.16$~\text{TeV}$ is presented. The analysis uses data collected with the CMS detector in 2016, corresponding to an integrated luminosity of 174.6$~\text{nb}^\text{$-$1}$. The average values and distributions of $x_{j}$ are measured as functions of the event charged-particle multiplicity for various combinations of the pseudorapidity regions in which the two jets are found. These different configurations enable measurements of distinct nucleon momentum fractions x in both proton- and lead-going directions. Thanks to high-multiplicity triggers, designed for probing potential jet-quenching effects, we reached a charged-particle multiplicity as high as 400. Collective behavior of the outgoing particles was previously observed in very high multiplicity pPb events, possibly indicating the formation of small quark-gluon plasma (QGP) droplets. The ratio of $x_{j}$ for high multiplicity to low-multiplicity events is used to quantify possible medium effects. The results are found to be consistent with simulations of the hard-scattering process that do not include (QGP) production. These measurements provide a limit on medium-induced energy loss of 1.26% at the 90% confidence level in terms of subleading jet's transverse momentum in high multiplicity pPb events.
DOI: 10.17182/hepdata.156764.v1/t14
title: "Table 4c" of "Search for jet quenching with dijets from high-multiplicity pPb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV"

description: The reconstructed (raw) dijet balance distribution, $(1/N_{dijet})(dN_{dijet}/dx_{j})$, as function of $x_{j}$ for the $10-60$, $60-120$, $120-185$, $185-250$ and $250-400$ multiplicity ranges with leading and subleading jets at midrapidity and backward regions, respectively.
description: The first measurement of the dijet transverse momentum balance ($x_{j}$) in proton-lead (pPb) collisions at nucleon-nucleon center-of–mass energy $\sqrt{s_{\text{\tiny NN}}} = $8.16$~\text{TeV}$ is presented. The analysis uses data collected with the CMS detector in 2016, corresponding to an integrated luminosity of 174.6$~\text{nb}^\text{$-$1}$. The average values and distributions of $x_{j}$ are measured as functions of the event charged-particle multiplicity for various combinations of the pseudorapidity regions in which the two jets are found. These different configurations enable measurements of distinct nucleon momentum fractions x in both proton- and lead-going directions. Thanks to high-multiplicity triggers, designed for probing potential jet-quenching effects, we reached a charged-particle multiplicity as high as 400. Collective behavior of the outgoing particles was previously observed in very high multiplicity pPb events, possibly indicating the formation of small quark-gluon plasma (QGP) droplets. The ratio of $x_{j}$ for high multiplicity to low-multiplicity events is used to quantify possible medium effects. The results are found to be consistent with simulations of the hard-scattering process that do not include (QGP) production. These measurements provide a limit on medium-induced energy loss of 1.26% at the 90% confidence level in terms of subleading jet's transverse momentum in high multiplicity pPb events.
DOI: 10.17182/hepdata.156764.v1/t15
title: "Table 4d" of "Search for jet quenching with dijets from high-multiplicity pPb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV"

description: The reconstructed (raw) dijet balance distribution, $(1/N_{dijet})(dN_{dijet}/dx_{j})$, as function of $x_{j}$ for the $10-60$, $60-120$, $120-185$, $185-250$ and $250-400$ multiplicity ranges with leading and subleading jets at forward and midrapidity regions, respectively.
description: The first measurement of the dijet transverse momentum balance ($x_{j}$) in proton-lead (pPb) collisions at nucleon-nucleon center-of–mass energy $\sqrt{s_{\text{\tiny NN}}} = $8.16$~\text{TeV}$ is presented. The analysis uses data collected with the CMS detector in 2016, corresponding to an integrated luminosity of 174.6$~\text{nb}^\text{$-$1}$. The average values and distributions of $x_{j}$ are measured as functions of the event charged-particle multiplicity for various combinations of the pseudorapidity regions in which the two jets are found. These different configurations enable measurements of distinct nucleon momentum fractions x in both proton- and lead-going directions. Thanks to high-multiplicity triggers, designed for probing potential jet-quenching effects, we reached a charged-particle multiplicity as high as 400. Collective behavior of the outgoing particles was previously observed in very high multiplicity pPb events, possibly indicating the formation of small quark-gluon plasma (QGP) droplets. The ratio of $x_{j}$ for high multiplicity to low-multiplicity events is used to quantify possible medium effects. The results are found to be consistent with simulations of the hard-scattering process that do not include (QGP) production. These measurements provide a limit on medium-induced energy loss of 1.26% at the 90% confidence level in terms of subleading jet's transverse momentum in high multiplicity pPb events.
DOI: 10.17182/hepdata.156764.v1/t16
title: "Table 4e" of "Search for jet quenching with dijets from high-multiplicity pPb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV"

description: The reconstructed (raw) dijet balance distribution, $(1/N_{dijet})(dN_{dijet}/dx_{j})$, as function of $x_{j}$ for the $10-60$, $60-120$, $120-185$, $185-250$ and $250-400$ multiplicity ranges with leading and subleading jets at backward and midrapidity regions, respectively.
description: The first measurement of the dijet transverse momentum balance ($x_{j}$) in proton-lead (pPb) collisions at nucleon-nucleon center-of–mass energy $\sqrt{s_{\text{\tiny NN}}} = $8.16$~\text{TeV}$ is presented. The analysis uses data collected with the CMS detector in 2016, corresponding to an integrated luminosity of 174.6$~\text{nb}^\text{$-$1}$. The average values and distributions of $x_{j}$ are measured as functions of the event charged-particle multiplicity for various combinations of the pseudorapidity regions in which the two jets are found. These different configurations enable measurements of distinct nucleon momentum fractions x in both proton- and lead-going directions. Thanks to high-multiplicity triggers, designed for probing potential jet-quenching effects, we reached a charged-particle multiplicity as high as 400. Collective behavior of the outgoing particles was previously observed in very high multiplicity pPb events, possibly indicating the formation of small quark-gluon plasma (QGP) droplets. The ratio of $x_{j}$ for high multiplicity to low-multiplicity events is used to quantify possible medium effects. The results are found to be consistent with simulations of the hard-scattering process that do not include (QGP) production. These measurements provide a limit on medium-induced energy loss of 1.26% at the 90% confidence level in terms of subleading jet's transverse momentum in high multiplicity pPb events.
DOI: 10.17182/hepdata.156764.v1/t9
title: "Table 2d" of "Search for jet quenching with dijets from high-multiplicity pPb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV"

description: The ratio of unfolded dijet balance distribution to the lower multiplicity range, $10-60$, as function of $x_{j}$ for the $60-120$, $120-185$, $185-250$ and $250-400$ ranges with leading and subleading jets at forward and midrapidity regions, respectively.
description: The first measurement of the dijet transverse momentum balance ($x_{j}$) in proton-lead (pPb) collisions at nucleon-nucleon center-of–mass energy $\sqrt{s_{\text{\tiny NN}}} = $8.16$~\text{TeV}$ is presented. The analysis uses data collected with the CMS detector in 2016, corresponding to an integrated luminosity of 174.6$~\text{nb}^\text{$-$1}$. The average values and distributions of $x_{j}$ are measured as functions of the event charged-particle multiplicity for various combinations of the pseudorapidity regions in which the two jets are found. These different configurations enable measurements of distinct nucleon momentum fractions x in both proton- and lead-going directions. Thanks to high-multiplicity triggers, designed for probing potential jet-quenching effects, we reached a charged-particle multiplicity as high as 400. Collective behavior of the outgoing particles was previously observed in very high multiplicity pPb events, possibly indicating the formation of small quark-gluon plasma (QGP) droplets. The ratio of $x_{j}$ for high multiplicity to low-multiplicity events is used to quantify possible medium effects. The results are found to be consistent with simulations of the hard-scattering process that do not include (QGP) production. These measurements provide a limit on medium-induced energy loss of 1.26% at the 90% confidence level in terms of subleading jet's transverse momentum in high multiplicity pPb events.
DOI: 10.17182/hepdata.156764.v1/t13
title: "Table 4b" of "Search for jet quenching with dijets from high-multiplicity pPb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV"

description: The reconstructed (raw) dijet balance distribution, $(1/N_{dijet})(dN_{dijet}/dx_{j})$, as function of $x_{j}$ for the $10-60$, $60-120$, $120-185$, $185-250$ and $250-400$ multiplicity ranges with leading and subleading jets at midrapidity and forward regions, respectively.
description: The first measurement of the dijet transverse momentum balance ($x_{j}$) in proton-lead (pPb) collisions at nucleon-nucleon center-of–mass energy $\sqrt{s_{\text{\tiny NN}}} = $8.16$~\text{TeV}$ is presented. The analysis uses data collected with the CMS detector in 2016, corresponding to an integrated luminosity of 174.6$~\text{nb}^\text{$-$1}$. The average values and distributions of $x_{j}$ are measured as functions of the event charged-particle multiplicity for various combinations of the pseudorapidity regions in which the two jets are found. These different configurations enable measurements of distinct nucleon momentum fractions x in both proton- and lead-going directions. Thanks to high-multiplicity triggers, designed for probing potential jet-quenching effects, we reached a charged-particle multiplicity as high as 400. Collective behavior of the outgoing particles was previously observed in very high multiplicity pPb events, possibly indicating the formation of small quark-gluon plasma (QGP) droplets. The ratio of $x_{j}$ for high multiplicity to low-multiplicity events is used to quantify possible medium effects. The results are found to be consistent with simulations of the hard-scattering process that do not include (QGP) production. These measurements provide a limit on medium-induced energy loss of 1.26% at the 90% confidence level in terms of subleading jet's transverse momentum in high multiplicity pPb events.
DOI: 10.17182/hepdata.156764.v1/t17
title: "Table 5a" of "Search for jet quenching with dijets from high-multiplicity pPb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV"

description: The ratio of reconstructed (raw) dijet balance distribution to the lower multiplicity range, $10-60$, as function of $x_{j}$ for the $60-120$, $120-185$, $185-250$ and $250-400$ ranges with both jets at the midrapidity regions.
description: The first measurement of the dijet transverse momentum balance ($x_{j}$) in proton-lead (pPb) collisions at nucleon-nucleon center-of–mass energy $\sqrt{s_{\text{\tiny NN}}} = $8.16$~\text{TeV}$ is presented. The analysis uses data collected with the CMS detector in 2016, corresponding to an integrated luminosity of 174.6$~\text{nb}^\text{$-$1}$. The average values and distributions of $x_{j}$ are measured as functions of the event charged-particle multiplicity for various combinations of the pseudorapidity regions in which the two jets are found. These different configurations enable measurements of distinct nucleon momentum fractions x in both proton- and lead-going directions. Thanks to high-multiplicity triggers, designed for probing potential jet-quenching effects, we reached a charged-particle multiplicity as high as 400. Collective behavior of the outgoing particles was previously observed in very high multiplicity pPb events, possibly indicating the formation of small quark-gluon plasma (QGP) droplets. The ratio of $x_{j}$ for high multiplicity to low-multiplicity events is used to quantify possible medium effects. The results are found to be consistent with simulations of the hard-scattering process that do not include (QGP) production. These measurements provide a limit on medium-induced energy loss of 1.26% at the 90% confidence level in terms of subleading jet's transverse momentum in high multiplicity pPb events.
DOI: 10.17182/hepdata.156764.v1/t18
title: "Table 5b" of "Search for jet quenching with dijets from high-multiplicity pPb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV"

description: The ratio of reconstructed (raw) dijet balance distribution to the lower multiplicity range, $10-60$, as function of $x_{j}$ for the $60-120$, $120-185$, $185-250$ and $250-400$ ranges with leading and subleading jets at midrapidity and forward regions, respectively.
description: The first measurement of the dijet transverse momentum balance ($x_{j}$) in proton-lead (pPb) collisions at nucleon-nucleon center-of–mass energy $\sqrt{s_{\text{\tiny NN}}} = $8.16$~\text{TeV}$ is presented. The analysis uses data collected with the CMS detector in 2016, corresponding to an integrated luminosity of 174.6$~\text{nb}^\text{$-$1}$. The average values and distributions of $x_{j}$ are measured as functions of the event charged-particle multiplicity for various combinations of the pseudorapidity regions in which the two jets are found. These different configurations enable measurements of distinct nucleon momentum fractions x in both proton- and lead-going directions. Thanks to high-multiplicity triggers, designed for probing potential jet-quenching effects, we reached a charged-particle multiplicity as high as 400. Collective behavior of the outgoing particles was previously observed in very high multiplicity pPb events, possibly indicating the formation of small quark-gluon plasma (QGP) droplets. The ratio of $x_{j}$ for high multiplicity to low-multiplicity events is used to quantify possible medium effects. The results are found to be consistent with simulations of the hard-scattering process that do not include (QGP) production. These measurements provide a limit on medium-induced energy loss of 1.26% at the 90% confidence level in terms of subleading jet's transverse momentum in high multiplicity pPb events.
DOI: 10.17182/hepdata.156764.v1/t19
title: "Table 5c" of "Search for jet quenching with dijets from high-multiplicity pPb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV"

description: The ratio of reconstructed (raw) dijet balance distribution to the lower multiplicity range, $10-60$, as function of $x_{j}$ for the $60-120$, $120-185$, $185-250$ and $250-400$ ranges with leading and subleading jets at midrapidity and backward regions, respectively.
description: The first measurement of the dijet transverse momentum balance ($x_{j}$) in proton-lead (pPb) collisions at nucleon-nucleon center-of–mass energy $\sqrt{s_{\text{\tiny NN}}} = $8.16$~\text{TeV}$ is presented. The analysis uses data collected with the CMS detector in 2016, corresponding to an integrated luminosity of 174.6$~\text{nb}^\text{$-$1}$. The average values and distributions of $x_{j}$ are measured as functions of the event charged-particle multiplicity for various combinations of the pseudorapidity regions in which the two jets are found. These different configurations enable measurements of distinct nucleon momentum fractions x in both proton- and lead-going directions. Thanks to high-multiplicity triggers, designed for probing potential jet-quenching effects, we reached a charged-particle multiplicity as high as 400. Collective behavior of the outgoing particles was previously observed in very high multiplicity pPb events, possibly indicating the formation of small quark-gluon plasma (QGP) droplets. The ratio of $x_{j}$ for high multiplicity to low-multiplicity events is used to quantify possible medium effects. The results are found to be consistent with simulations of the hard-scattering process that do not include (QGP) production. These measurements provide a limit on medium-induced energy loss of 1.26% at the 90% confidence level in terms of subleading jet's transverse momentum in high multiplicity pPb events.
DOI: 10.17182/hepdata.156764.v1/t20
title: "Table 5d" of "Search for jet quenching with dijets from high-multiplicity pPb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV"

description: The ratio of reconstructed (raw) dijet balance distribution to the lower multiplicity range, $10-60$, as function of $x_{j}$ for the $60-120$, $120-185$, $185-250$ and $250-400$ ranges with leading and subleading jets at forward and midrapidity regions, respectively.
description: The first measurement of the dijet transverse momentum balance ($x_{j}$) in proton-lead (pPb) collisions at nucleon-nucleon center-of–mass energy $\sqrt{s_{\text{\tiny NN}}} = $8.16$~\text{TeV}$ is presented. The analysis uses data collected with the CMS detector in 2016, corresponding to an integrated luminosity of 174.6$~\text{nb}^\text{$-$1}$. The average values and distributions of $x_{j}$ are measured as functions of the event charged-particle multiplicity for various combinations of the pseudorapidity regions in which the two jets are found. These different configurations enable measurements of distinct nucleon momentum fractions x in both proton- and lead-going directions. Thanks to high-multiplicity triggers, designed for probing potential jet-quenching effects, we reached a charged-particle multiplicity as high as 400. Collective behavior of the outgoing particles was previously observed in very high multiplicity pPb events, possibly indicating the formation of small quark-gluon plasma (QGP) droplets. The ratio of $x_{j}$ for high multiplicity to low-multiplicity events is used to quantify possible medium effects. The results are found to be consistent with simulations of the hard-scattering process that do not include (QGP) production. These measurements provide a limit on medium-induced energy loss of 1.26% at the 90% confidence level in terms of subleading jet's transverse momentum in high multiplicity pPb events.
DOI: 10.17182/hepdata.156764.v1/t21
title: "Table 5e" of "Search for jet quenching with dijets from high-multiplicity pPb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV"

description: The ratio of reconstructed (raw) dijet balance distribution to the lower multiplicity range, $10-60$, as function of $x_{j}$ for the $60-120$, $120-185$, $185-250$ and $250-400$ ranges with leading and subleading jets at backward and midrapidity regions, respectively.
description: The first measurement of the dijet transverse momentum balance ($x_{j}$) in proton-lead (pPb) collisions at nucleon-nucleon center-of–mass energy $\sqrt{s_{\text{\tiny NN}}} = $8.16$~\text{TeV}$ is presented. The analysis uses data collected with the CMS detector in 2016, corresponding to an integrated luminosity of 174.6$~\text{nb}^\text{$-$1}$. The average values and distributions of $x_{j}$ are measured as functions of the event charged-particle multiplicity for various combinations of the pseudorapidity regions in which the two jets are found. These different configurations enable measurements of distinct nucleon momentum fractions x in both proton- and lead-going directions. Thanks to high-multiplicity triggers, designed for probing potential jet-quenching effects, we reached a charged-particle multiplicity as high as 400. Collective behavior of the outgoing particles was previously observed in very high multiplicity pPb events, possibly indicating the formation of small quark-gluon plasma (QGP) droplets. The ratio of $x_{j}$ for high multiplicity to low-multiplicity events is used to quantify possible medium effects. The results are found to be consistent with simulations of the hard-scattering process that do not include (QGP) production. These measurements provide a limit on medium-induced energy loss of 1.26% at the 90% confidence level in terms of subleading jet's transverse momentum in high multiplicity pPb events.