cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.5281/zenodo.17504147
title: Datos del diagnóstico de las personas creadoras y promotoras culturales independientes del municipio de Guadalajara (2025)

description: Data generated from the questionnaire applied to municipal cultural spaces and the participatory diagnosis. They allow characterization of spaces and analysis of sustainability, networks, and cultural participation.
description: Datos generados a partir del cuestionario aplicado a los espacios culturales municipales y del diagnóstico participativo. Permiten caracterizar espacios y analizar sostenibilidad, redes y participación cultural.
description: Dados gerados a partir do questionário aplicado aos espaços culturais municipais e do diagnóstico participativo. Permitem caracterizar espaços e analisar sustentabilidade, redes e participação cultural.
DOI: 10.17182/hepdata.138430.v1/t10
title: "Table2_6" of "Measurements of azimuthal anisotropies at forward and backward rapidity with muons in high-multiplicity p-Pb collisions at $\sqrt{s_{\rm NN}} = 8.16$ TeV"

description: Inclusive muon $v_{2}^{\mu}$ as a function of $p_{\mathrm{T}}$ is measured by two-particle correlation method at forward rapidities in high-multiplicity (0$-$20%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$= 8.16 TeV. The event activity is estimated with the ZDC estimator.
description: The azimuthal anisotropy of inclusive muons produced in p--Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV is measured by using the ALICE detector at the LHC. The measurement of the second-order Fourier coefficient of the particle azimuthal distribution, $v_2$, is performed as a function of transverse momentum $p_{\rm T}$ in the 0$-$20% high-multiplicity interval at both forward ($2.03 &lt; y_{\mathrm{cms}} &lt; 3.53$) and backward ($-4.46 &lt; y_{\mathrm{cms}} &lt; -2.96$) rapidities over a wide $p_{\rm T}$ range, $0.5 &lt; p_{\rm T} &lt; 10$ GeV/$c$, in which a dominant contribution of muons from heavy-flavour hadron decays is expected at $p_{\rm T} &gt; 2$ GeV/$c$. The $v_2$ coefficient of inclusive muons is extracted using two different techniques, namely two-particle cumulants, used for the first time for heavy-flavour measurements, and forward--central two-particle correlations. A positive $v_2$ is measured at both forward and backward rapidities with a significance larger than 4.7$\sigma$ and 7.6$\sigma$, respectively, in the interval $2
DOI: 10.17182/hepdata.138430.v1/t12
title: "Table2_8" of "Measurements of azimuthal anisotropies at forward and backward rapidity with muons in high-multiplicity p-Pb collisions at $\sqrt{s_{\rm NN}} = 8.16$ TeV"

description: Inclusive muon $v_{2}^{\mu}$ as a function of $p_{\mathrm{T}}$ is measured by two-particle correlation method at backward rapidities in high-multiplicity (0$-$20%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$= 8.16 TeV. The event activity is estimated with the ZDC estimator.
description: The azimuthal anisotropy of inclusive muons produced in p--Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV is measured by using the ALICE detector at the LHC. The measurement of the second-order Fourier coefficient of the particle azimuthal distribution, $v_2$, is performed as a function of transverse momentum $p_{\rm T}$ in the 0$-$20% high-multiplicity interval at both forward ($2.03 &lt; y_{\mathrm{cms}} &lt; 3.53$) and backward ($-4.46 &lt; y_{\mathrm{cms}} &lt; -2.96$) rapidities over a wide $p_{\rm T}$ range, $0.5 &lt; p_{\rm T} &lt; 10$ GeV/$c$, in which a dominant contribution of muons from heavy-flavour hadron decays is expected at $p_{\rm T} &gt; 2$ GeV/$c$. The $v_2$ coefficient of inclusive muons is extracted using two different techniques, namely two-particle cumulants, used for the first time for heavy-flavour measurements, and forward--central two-particle correlations. A positive $v_2$ is measured at both forward and backward rapidities with a significance larger than 4.7$\sigma$ and 7.6$\sigma$, respectively, in the interval $2
DOI: 10.17182/hepdata.138430.v1/t6
title: "Table2_2" of "Measurements of azimuthal anisotropies at forward and backward rapidity with muons in high-multiplicity p-Pb collisions at $\sqrt{s_{\rm NN}} = 8.16$ TeV"

description: Inclusive muon $v_{2}^{\mu}$ as a function of $p_{\mathrm{T}}$ is measured by two-particle cumulant method at forward rapidities in high-multiplicity (0$-$20%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$= 8.16 TeV. The event activity is estimated with the ZDC estimator.
description: The azimuthal anisotropy of inclusive muons produced in p--Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV is measured by using the ALICE detector at the LHC. The measurement of the second-order Fourier coefficient of the particle azimuthal distribution, $v_2$, is performed as a function of transverse momentum $p_{\rm T}$ in the 0$-$20% high-multiplicity interval at both forward ($2.03 &lt; y_{\mathrm{cms}} &lt; 3.53$) and backward ($-4.46 &lt; y_{\mathrm{cms}} &lt; -2.96$) rapidities over a wide $p_{\rm T}$ range, $0.5 &lt; p_{\rm T} &lt; 10$ GeV/$c$, in which a dominant contribution of muons from heavy-flavour hadron decays is expected at $p_{\rm T} &gt; 2$ GeV/$c$. The $v_2$ coefficient of inclusive muons is extracted using two different techniques, namely two-particle cumulants, used for the first time for heavy-flavour measurements, and forward--central two-particle correlations. A positive $v_2$ is measured at both forward and backward rapidities with a significance larger than 4.7$\sigma$ and 7.6$\sigma$, respectively, in the interval $2
DOI: 10.17182/hepdata.138430.v1/t7
title: "Table2_3" of "Measurements of azimuthal anisotropies at forward and backward rapidity with muons in high-multiplicity p-Pb collisions at $\sqrt{s_{\rm NN}} = 8.16$ TeV"

description: Inclusive muon $v_{2}^{\mu}$ as a function of $p_{\mathrm{T}}$ is measured by two-particle cumulant method at backward rapidities in high-multiplicity (0$-$20%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$= 8.16 TeV. The event activity is estimated with the CL1 estimator.
description: The azimuthal anisotropy of inclusive muons produced in p--Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV is measured by using the ALICE detector at the LHC. The measurement of the second-order Fourier coefficient of the particle azimuthal distribution, $v_2$, is performed as a function of transverse momentum $p_{\rm T}$ in the 0$-$20% high-multiplicity interval at both forward ($2.03 &lt; y_{\mathrm{cms}} &lt; 3.53$) and backward ($-4.46 &lt; y_{\mathrm{cms}} &lt; -2.96$) rapidities over a wide $p_{\rm T}$ range, $0.5 &lt; p_{\rm T} &lt; 10$ GeV/$c$, in which a dominant contribution of muons from heavy-flavour hadron decays is expected at $p_{\rm T} &gt; 2$ GeV/$c$. The $v_2$ coefficient of inclusive muons is extracted using two different techniques, namely two-particle cumulants, used for the first time for heavy-flavour measurements, and forward--central two-particle correlations. A positive $v_2$ is measured at both forward and backward rapidities with a significance larger than 4.7$\sigma$ and 7.6$\sigma$, respectively, in the interval $2
DOI: 10.17182/hepdata.138430.v1/t8
title: "Table2_4" of "Measurements of azimuthal anisotropies at forward and backward rapidity with muons in high-multiplicity p-Pb collisions at $\sqrt{s_{\rm NN}} = 8.16$ TeV"

description: Inclusive muon $v_{2}^{\mu}$ as a function of $p_{\mathrm{T}}$ is measured by two-particle cumulant method at backward rapidities in high-multiplicity (0$-$20%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$= 8.16 TeV. The event activity is estimated with the ZDC estimator.
description: The azimuthal anisotropy of inclusive muons produced in p--Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV is measured by using the ALICE detector at the LHC. The measurement of the second-order Fourier coefficient of the particle azimuthal distribution, $v_2$, is performed as a function of transverse momentum $p_{\rm T}$ in the 0$-$20% high-multiplicity interval at both forward ($2.03 &lt; y_{\mathrm{cms}} &lt; 3.53$) and backward ($-4.46 &lt; y_{\mathrm{cms}} &lt; -2.96$) rapidities over a wide $p_{\rm T}$ range, $0.5 &lt; p_{\rm T} &lt; 10$ GeV/$c$, in which a dominant contribution of muons from heavy-flavour hadron decays is expected at $p_{\rm T} &gt; 2$ GeV/$c$. The $v_2$ coefficient of inclusive muons is extracted using two different techniques, namely two-particle cumulants, used for the first time for heavy-flavour measurements, and forward--central two-particle correlations. A positive $v_2$ is measured at both forward and backward rapidities with a significance larger than 4.7$\sigma$ and 7.6$\sigma$, respectively, in the interval $2
DOI: 10.17182/hepdata.135830.v1/t1
title: "Psi(2S) vs mult., pp" of "Measurement of $\psi$(2S) production as a function of charged-particle pseudorapidity density in pp collisions at $\sqrt{s}$ = 13 TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV with ALICE at the LHC"

description: Ratio of measured PSI(2S) cross section in charged-particle multiplicity intervals and integrated in multiplicity.
description: CERN-LHC. Measurement of J/psi and Psi(2S) yields and their ratio as a function of charged-particle multiplicity in pp collisions at 13 TeV and p-Pb collisions at 8.16 TeV.

Quarkonia:
- in their dimuon decay
- pT&gt;0

Charged-particle multiplicity in |eta|&lt;1.0, pT&gt;0

Measurements reported in the INEL&gt;0 event class.
DOI: 10.17182/hepdata.135830.v1/t2
title: "Psi(2S) vs mult., pPb, 2.03 &lt; y &lt; 3.53" of "Measurement of $\psi$(2S) production as a function of charged-particle pseudorapidity density in pp collisions at $\sqrt{s}$ = 13 TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV with ALICE at the LHC"

description: Ratio of measured PSI(2S) cross section in charged-particle multiplicity intervals and integrated in multiplicity.
description: CERN-LHC. Measurement of J/psi and Psi(2S) yields and their ratio as a function of charged-particle multiplicity in pp collisions at 13 TeV and p-Pb collisions at 8.16 TeV.

Quarkonia:
- in their dimuon decay
- pT&gt;0

Charged-particle multiplicity in |eta|&lt;1.0, pT&gt;0

Measurements reported in the INEL&gt;0 event class.
DOI: 10.17182/hepdata.133562.v1/t1
title: "Table 1" of "Measurement of inclusive and leading subjet fragmentation in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Inclusive subjet $z_r$ in pp collisions for $r=0.1$
$80
description: No data abstract available.
DOI: 10.17182/hepdata.134258.v1/t1
title: "Figure 2.1" of "Elliptic flow of charged particles at midrapidity relative to the spectator plane in Pb-Pb and Xe-Xe collisions"

description: Centrality dependence of $v_2\{\Psi_{\mathrm{SP}}\}$, $v_2\{2,|\Delta\eta|&gt;1\}$, and $v_2\{4\}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76~\mathrm{TeV}$.
description: Measurements of the elliptic flow coefficient relative to the collision plane defined by the spectator neutrons $v_2\{\Psi_\mathrm{SP}\}$ in collisions of Pb ions at center-of-mass energy per nucleon-nucleon pair $\sqrt{s_\mathrm{NN}}=2.76$ TeV and Xe ions at $\sqrt{s_\mathrm{NN}}=5.44$ TeV are reported. The results are presented for charged particles produced at midrapidity as a function of centrality and transverse momentum for the $5-70\%$ and $0.2-6\ \mathrm{GeV}/c$ ranges, respectively. The ratio between $v_2\{\Psi_\mathrm{SP}\}$ and the elliptic flow coefficient relative to the participant plane $v_2\{4\}$, estimated using four-particle correlations, deviates by up to $20\%$ from unity depending on centrality. This observation differs strongly from the magnitude of the corresponding eccentricity ratios predicted by the TRENTo and the elliptic power models of initial state fluctuations that are tuned to describe the participant plane anisotropies. The differences can be interpreted as a decorrelation of the neutron spectator plane and the reaction plane because of fragmentation of the remnants from the colliding nuclei, which points to an incompleteness of current models describing the initial state fluctuations. A significant transverse momentum dependence of the ratio $v_2\{\Psi_\mathrm{SP}\}/v_2\{4\}$ is observed in all but the most central collisions, which may help to understand whether momentum anisotropies at low and intermediate transverse momentum have a common origin in initial state fluctuations. The ratios of $v_2\{\Psi_\mathrm{SP}\}$ and $v_2\{4\}$ to the corresponding initial state eccentricities for Xe--Xe and Pb--Pb collisions at similar initial entropy density show a difference of $(7.0\pm0.9)\%$ with an additional variation of $+1.8\%$ when including RHIC data in the TRENTo parameter extraction. These observations provide new experimental constraints for viscous effects in the hydrodynamic modeling of the expanding quark--gluon plasma produced in heavy-ion collisions at the LHC.
DOI: 10.17182/hepdata.134258.v1/t2
title: "Figure 2.2" of "Elliptic flow of charged particles at midrapidity relative to the spectator plane in Pb-Pb and Xe-Xe collisions"

description: Centrality dependence of $v_2\{\Psi_{\mathrm{SP}}\}$, $v_2\{2,|\Delta\eta|&gt;1\}$, and $v_2\{4\}$ in Xe-Xe collisions at $\sqrt{s_{\mathrm{NN}}}=5.44~\mathrm{TeV}$.
description: Measurements of the elliptic flow coefficient relative to the collision plane defined by the spectator neutrons $v_2\{\Psi_\mathrm{SP}\}$ in collisions of Pb ions at center-of-mass energy per nucleon-nucleon pair $\sqrt{s_\mathrm{NN}}=2.76$ TeV and Xe ions at $\sqrt{s_\mathrm{NN}}=5.44$ TeV are reported. The results are presented for charged particles produced at midrapidity as a function of centrality and transverse momentum for the $5-70\%$ and $0.2-6\ \mathrm{GeV}/c$ ranges, respectively. The ratio between $v_2\{\Psi_\mathrm{SP}\}$ and the elliptic flow coefficient relative to the participant plane $v_2\{4\}$, estimated using four-particle correlations, deviates by up to $20\%$ from unity depending on centrality. This observation differs strongly from the magnitude of the corresponding eccentricity ratios predicted by the TRENTo and the elliptic power models of initial state fluctuations that are tuned to describe the participant plane anisotropies. The differences can be interpreted as a decorrelation of the neutron spectator plane and the reaction plane because of fragmentation of the remnants from the colliding nuclei, which points to an incompleteness of current models describing the initial state fluctuations. A significant transverse momentum dependence of the ratio $v_2\{\Psi_\mathrm{SP}\}/v_2\{4\}$ is observed in all but the most central collisions, which may help to understand whether momentum anisotropies at low and intermediate transverse momentum have a common origin in initial state fluctuations. The ratios of $v_2\{\Psi_\mathrm{SP}\}$ and $v_2\{4\}$ to the corresponding initial state eccentricities for Xe--Xe and Pb--Pb collisions at similar initial entropy density show a difference of $(7.0\pm0.9)\%$ with an additional variation of $+1.8\%$ when including RHIC data in the TRENTo parameter extraction. These observations provide new experimental constraints for viscous effects in the hydrodynamic modeling of the expanding quark--gluon plasma produced in heavy-ion collisions at the LHC.
DOI: 10.17182/hepdata.135830.v1/t3
title: "Psi(2S) vs mult., pPb, -4.46 &lt; y &lt; -2.96" of "Measurement of $\psi$(2S) production as a function of charged-particle pseudorapidity density in pp collisions at $\sqrt{s}$ = 13 TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV with ALICE at the LHC"

description: Ratio of measured PSI(2S) cross section in charged-particle multiplicity intervals and integrated in multiplicity.
description: CERN-LHC. Measurement of J/psi and Psi(2S) yields and their ratio as a function of charged-particle multiplicity in pp collisions at 13 TeV and p-Pb collisions at 8.16 TeV.

Quarkonia:
- in their dimuon decay
- pT&gt;0

Charged-particle multiplicity in |eta|&lt;1.0, pT&gt;0

Measurements reported in the INEL&gt;0 event class.
DOI: 10.17182/hepdata.135830.v1/t4
title: "Psi(2S)/J/psi vs mult., pp" of "Measurement of $\psi$(2S) production as a function of charged-particle pseudorapidity density in pp collisions at $\sqrt{s}$ = 13 TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV with ALICE at the LHC"

description: Ratio of measured PSI(2S) over J/PSI(1S) cross section in charged-particle multiplicity intervals and integrated in multiplicity.
description: CERN-LHC. Measurement of J/psi and Psi(2S) yields and their ratio as a function of charged-particle multiplicity in pp collisions at 13 TeV and p-Pb collisions at 8.16 TeV.

Quarkonia:
- in their dimuon decay
- pT&gt;0

Charged-particle multiplicity in |eta|&lt;1.0, pT&gt;0

Measurements reported in the INEL&gt;0 event class.
DOI: 10.17182/hepdata.135830.v1/t5
title: "Psi(2S)/J/psi vs mult., pPb, 2.03 &lt; y &lt; 3.53" of "Measurement of $\psi$(2S) production as a function of charged-particle pseudorapidity density in pp collisions at $\sqrt{s}$ = 13 TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV with ALICE at the LHC"

description: Ratio of measured PSI(2S) over J/PSI(1S) cross section in charged-particle multiplicity intervals and integrated in multiplicity.
description: CERN-LHC. Measurement of J/psi and Psi(2S) yields and their ratio as a function of charged-particle multiplicity in pp collisions at 13 TeV and p-Pb collisions at 8.16 TeV.

Quarkonia:
- in their dimuon decay
- pT&gt;0

Charged-particle multiplicity in |eta|&lt;1.0, pT&gt;0

Measurements reported in the INEL&gt;0 event class.
DOI: 10.17182/hepdata.135830.v1/t6
title: "Psi(2S)/J/psi vs mult., pPb, -4.46 &lt; y &lt; -2.96" of "Measurement of $\psi$(2S) production as a function of charged-particle pseudorapidity density in pp collisions at $\sqrt{s}$ = 13 TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV with ALICE at the LHC"

description: Ratio of measured PSI(2S) over J/PSI(1S) cross section in charged-particle multiplicity intervals and integrated in multiplicity.
description: CERN-LHC. Measurement of J/psi and Psi(2S) yields and their ratio as a function of charged-particle multiplicity in pp collisions at 13 TeV and p-Pb collisions at 8.16 TeV.

Quarkonia:
- in their dimuon decay
- pT&gt;0

Charged-particle multiplicity in |eta|&lt;1.0, pT&gt;0

Measurements reported in the INEL&gt;0 event class.
DOI: 10.17182/hepdata.133562.v1/t2
title: "Table 2" of "Measurement of inclusive and leading subjet fragmentation in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Inclusive subjet $z_r$ in pp collisions for $r=0.2$
$80
description: No data abstract available.
DOI: 10.17182/hepdata.133562.v1/t3
title: "Table 3" of "Measurement of inclusive and leading subjet fragmentation in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Leading subjet $z_r$ in pp collisions for $r=0.1$
$80
description: No data abstract available.
DOI: 10.17182/hepdata.133562.v1/t4
title: "Table 4" of "Measurement of inclusive and leading subjet fragmentation in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Leading subjet $z_r$ in pp collisions for $r=0.2$
$80
description: No data abstract available.
DOI: 10.17182/hepdata.133562.v1/t5
title: "Table 5" of "Measurement of inclusive and leading subjet fragmentation in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Leading subjet $z_r$ for $r=0.1$ in pp collisions.
$80
description: No data abstract available.
DOI: 10.17182/hepdata.134258.v1/t3
title: "Figure 2.3" of "Elliptic flow of charged particles at midrapidity relative to the spectator plane in Pb-Pb and Xe-Xe collisions"

description: Centrality dependence of $v_2\{\Psi_{\mathrm{SP}}\}/v_2\{4\}$ and $v_2\{2,|\Delta\eta|&gt;1\}/v_2\{4\}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76~\mathrm{TeV}$.
description: Measurements of the elliptic flow coefficient relative to the collision plane defined by the spectator neutrons $v_2\{\Psi_\mathrm{SP}\}$ in collisions of Pb ions at center-of-mass energy per nucleon-nucleon pair $\sqrt{s_\mathrm{NN}}=2.76$ TeV and Xe ions at $\sqrt{s_\mathrm{NN}}=5.44$ TeV are reported. The results are presented for charged particles produced at midrapidity as a function of centrality and transverse momentum for the $5-70\%$ and $0.2-6\ \mathrm{GeV}/c$ ranges, respectively. The ratio between $v_2\{\Psi_\mathrm{SP}\}$ and the elliptic flow coefficient relative to the participant plane $v_2\{4\}$, estimated using four-particle correlations, deviates by up to $20\%$ from unity depending on centrality. This observation differs strongly from the magnitude of the corresponding eccentricity ratios predicted by the TRENTo and the elliptic power models of initial state fluctuations that are tuned to describe the participant plane anisotropies. The differences can be interpreted as a decorrelation of the neutron spectator plane and the reaction plane because of fragmentation of the remnants from the colliding nuclei, which points to an incompleteness of current models describing the initial state fluctuations. A significant transverse momentum dependence of the ratio $v_2\{\Psi_\mathrm{SP}\}/v_2\{4\}$ is observed in all but the most central collisions, which may help to understand whether momentum anisotropies at low and intermediate transverse momentum have a common origin in initial state fluctuations. The ratios of $v_2\{\Psi_\mathrm{SP}\}$ and $v_2\{4\}$ to the corresponding initial state eccentricities for Xe--Xe and Pb--Pb collisions at similar initial entropy density show a difference of $(7.0\pm0.9)\%$ with an additional variation of $+1.8\%$ when including RHIC data in the TRENTo parameter extraction. These observations provide new experimental constraints for viscous effects in the hydrodynamic modeling of the expanding quark--gluon plasma produced in heavy-ion collisions at the LHC.
DOI: 10.17182/hepdata.134258.v1/t4
title: "Figure 2.4" of "Elliptic flow of charged particles at midrapidity relative to the spectator plane in Pb-Pb and Xe-Xe collisions"

description: Centrality dependence of $v_2\{\Psi_{\mathrm{SP}}\}/v_2\{4\}$ and $v_2\{2,|\Delta\eta|&gt;1\}/v_2\{4\}$ in Xe-Xe collisions at $\sqrt{s_{\mathrm{NN}}}=5.44~\mathrm{TeV}$.
description: Measurements of the elliptic flow coefficient relative to the collision plane defined by the spectator neutrons $v_2\{\Psi_\mathrm{SP}\}$ in collisions of Pb ions at center-of-mass energy per nucleon-nucleon pair $\sqrt{s_\mathrm{NN}}=2.76$ TeV and Xe ions at $\sqrt{s_\mathrm{NN}}=5.44$ TeV are reported. The results are presented for charged particles produced at midrapidity as a function of centrality and transverse momentum for the $5-70\%$ and $0.2-6\ \mathrm{GeV}/c$ ranges, respectively. The ratio between $v_2\{\Psi_\mathrm{SP}\}$ and the elliptic flow coefficient relative to the participant plane $v_2\{4\}$, estimated using four-particle correlations, deviates by up to $20\%$ from unity depending on centrality. This observation differs strongly from the magnitude of the corresponding eccentricity ratios predicted by the TRENTo and the elliptic power models of initial state fluctuations that are tuned to describe the participant plane anisotropies. The differences can be interpreted as a decorrelation of the neutron spectator plane and the reaction plane because of fragmentation of the remnants from the colliding nuclei, which points to an incompleteness of current models describing the initial state fluctuations. A significant transverse momentum dependence of the ratio $v_2\{\Psi_\mathrm{SP}\}/v_2\{4\}$ is observed in all but the most central collisions, which may help to understand whether momentum anisotropies at low and intermediate transverse momentum have a common origin in initial state fluctuations. The ratios of $v_2\{\Psi_\mathrm{SP}\}$ and $v_2\{4\}$ to the corresponding initial state eccentricities for Xe--Xe and Pb--Pb collisions at similar initial entropy density show a difference of $(7.0\pm0.9)\%$ with an additional variation of $+1.8\%$ when including RHIC data in the TRENTo parameter extraction. These observations provide new experimental constraints for viscous effects in the hydrodynamic modeling of the expanding quark--gluon plasma produced in heavy-ion collisions at the LHC.