cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.5281/zenodo.15280749
title: Dataset for Engineering MXene/metal composites from MAX phase/metal-Al precursors for high-performance energy conversion and storage

description: Two-dimensional (2D) transition metal carbides, MXenes, have garnered significant interest for their potential applications in various energy storage and conversion systems. This work presents a novel approach to synthesizing MXene/metal composites via direct etching of MAX phase/metal-Al alloy precursor materials. 

By combining the Ti3AlC2 MAX phase with metal alloys and optimizing the processing conditions, we demonstrate a scalable method for producing MXene/metal composites with a 3D porous architecture and good mechanical integrity. Electrochemical tests have revealed that these composites exhibit high electrochemical activity towards the hydrogen evolution reaction (HER) and possess substantial areal capacitance, making them promising candidates for energy storage applications. Additionally, this synthesis strategy is adaptable to other MAX phases and metal-Al alloys, enabling the fabrication of customizable MXene/metal composites with tailored nanostructures for a broad range of electrochemical applications.
DOI: 10.6084/m9.figshare.28868882
title: Supplemental material.docx

description: Supplemental material for the Research paper titled "An investigation on the application of rice husk ash in concrete"
DOI: 10.57783/bpnh-v406
title: LibreChat
DOI: 10.17182/hepdata.113758.v1/t1
title: "Table 1" of "Experimental evidence for an attractive p-$\phi$ interaction"

description: Measured $\mathrm{p}-\phi$ $\oplus$ $\overline{\mathrm{p}}-\phi$ correlation function.
description: This represents the first experimental evidence of the attractive strong interaction between a proton and a $\phi$ meson. The result is obtained from two-particle correlations of combined $\mathrm{p}-\phi\oplus\mathrm{\overline{p}}-\phi$ pairs measured in high-multiplicity pp collisions at $\sqrt{s} = 13$ TeV by the ALICE collaboration. The spin-averaged scattering length and effective range of the $\mathrm{p}-\phi$ interaction are extracted from the fully corrected correlation function employing the Lednick'y-Lyuboshits approach. In particular, the imaginary part of the scattering length vanishes within uncertainties, indicating that inelastic processes do not play a prominent role for the $\mathrm{p}-\phi$ interaction. These data demonstrate that the interaction is dominated by elastic $\mathrm{p}-\phi$ scattering. Furthermore, an analysis employing phenomenological Gaussian- and Yukawa-type potentials is conducted. This work provides valuable experimental input to accomplish a self-consistent description of the N-$\phi$ interaction, which is particularly relevant for the more fundamental studies on partial restoration of chiral symmetry in nuclear medium.
DOI: 10.17182/hepdata.113758.v1/t2
title: "Table 2" of "Experimental evidence for an attractive p-$\phi$ interaction"

description: Genuine $\mathrm{p}-\phi$ $\oplus$ $\overline{\mathrm{p}}-\phi$ correlation function.
description: This represents the first experimental evidence of the attractive strong interaction between a proton and a $\phi$ meson. The result is obtained from two-particle correlations of combined $\mathrm{p}-\phi\oplus\mathrm{\overline{p}}-\phi$ pairs measured in high-multiplicity pp collisions at $\sqrt{s} = 13$ TeV by the ALICE collaboration. The spin-averaged scattering length and effective range of the $\mathrm{p}-\phi$ interaction are extracted from the fully corrected correlation function employing the Lednick'y-Lyuboshits approach. In particular, the imaginary part of the scattering length vanishes within uncertainties, indicating that inelastic processes do not play a prominent role for the $\mathrm{p}-\phi$ interaction. These data demonstrate that the interaction is dominated by elastic $\mathrm{p}-\phi$ scattering. Furthermore, an analysis employing phenomenological Gaussian- and Yukawa-type potentials is conducted. This work provides valuable experimental input to accomplish a self-consistent description of the N-$\phi$ interaction, which is particularly relevant for the more fundamental studies on partial restoration of chiral symmetry in nuclear medium.
DOI: 10.17182/hepdata.144336.v1/t1
title: "Table 1" of "Measurement of electrons from beauty-hadron decays in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: $p_{T}$-differential cross section of electrons from beauty-hadron decays in pp collisions at $\sqrt{s}=5.02$ TeV. The rapidity of electrons is |y| &lt; 0.8.
description: The production of electrons from beauty-hadron decays was measured at midrapidity in proton--proton (pp) and central Pb--Pb collisions at center-of-mass energy per nucleon--nucleon pair $\sqrt{s_{\rm{NN}}} = 5.02~{\rm TeV}$, using the ALICE detector at the LHC. The cross section measured in pp collisions in the transverse momentum interval $2&lt; p_{T} &lt; 8$ GeV/c was compared with models based on perturbative quantum chromodynamics calculations. The yield in the 10% most central Pb--Pb collisions, measured in the interval $2&lt; p_{T} &lt; 26$ GeV/c, was used to compute the nuclear modification factor $R_{AA}$, extrapolating the pp reference cross section to $p_{T}$ larger than 8 GeV/c. The measured $R_{AA}$ shows significant suppression of the yield of electrons from beauty-hadron decays at high $p_{T}$ and does not show a significant dependence on $p_{T}$ above 8 GeV/c within uncertainties. The results are described by several theoretical models based on different implementations of the interaction of heavy quarks with a quark--gluon plasma, which predict a smaller energy loss for beauty quarks compared to light and charm quarks.
DOI: 10.17182/hepdata.144336.v1/t2
title: "Table 2" of "Measurement of electrons from beauty-hadron decays in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Yield of beauty-hadron decay electrons in 0--10% central Pb--Pb collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV. The rapidity of electrons for $p_{T} &lt; 8$ GeV/c is |y| &lt; 0.8 and |y| &lt; 0.6 for $p_{T} &gt; 8$ GeV/c.
description: The production of electrons from beauty-hadron decays was measured at midrapidity in proton--proton (pp) and central Pb--Pb collisions at center-of-mass energy per nucleon--nucleon pair $\sqrt{s_{\rm{NN}}} = 5.02~{\rm TeV}$, using the ALICE detector at the LHC. The cross section measured in pp collisions in the transverse momentum interval $2&lt; p_{T} &lt; 8$ GeV/c was compared with models based on perturbative quantum chromodynamics calculations. The yield in the 10% most central Pb--Pb collisions, measured in the interval $2&lt; p_{T} &lt; 26$ GeV/c, was used to compute the nuclear modification factor $R_{AA}$, extrapolating the pp reference cross section to $p_{T}$ larger than 8 GeV/c. The measured $R_{AA}$ shows significant suppression of the yield of electrons from beauty-hadron decays at high $p_{T}$ and does not show a significant dependence on $p_{T}$ above 8 GeV/c within uncertainties. The results are described by several theoretical models based on different implementations of the interaction of heavy quarks with a quark--gluon plasma, which predict a smaller energy loss for beauty quarks compared to light and charm quarks.
DOI: 10.17182/hepdata.144336.v1/t3
title: "Table 3" of "Measurement of electrons from beauty-hadron decays in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: The nuclear modification factor for beauty-hadron decay electrons in 0--10% central Pb--Pb collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV. The rapidity of electrons for $p_{T} &lt; 8$ GeV/c is |y| &lt; 0.8 and |y| &lt; 0.6 for $p_{T} &gt; 8$ GeV/c.
description: The production of electrons from beauty-hadron decays was measured at midrapidity in proton--proton (pp) and central Pb--Pb collisions at center-of-mass energy per nucleon--nucleon pair $\sqrt{s_{\rm{NN}}} = 5.02~{\rm TeV}$, using the ALICE detector at the LHC. The cross section measured in pp collisions in the transverse momentum interval $2&lt; p_{T} &lt; 8$ GeV/c was compared with models based on perturbative quantum chromodynamics calculations. The yield in the 10% most central Pb--Pb collisions, measured in the interval $2&lt; p_{T} &lt; 26$ GeV/c, was used to compute the nuclear modification factor $R_{AA}$, extrapolating the pp reference cross section to $p_{T}$ larger than 8 GeV/c. The measured $R_{AA}$ shows significant suppression of the yield of electrons from beauty-hadron decays at high $p_{T}$ and does not show a significant dependence on $p_{T}$ above 8 GeV/c within uncertainties. The results are described by several theoretical models based on different implementations of the interaction of heavy quarks with a quark--gluon plasma, which predict a smaller energy loss for beauty quarks compared to light and charm quarks.
DOI: 10.17182/hepdata.142624.v1/t1
title: "Table 1" of "Inclusive and multiplicity dependent production of electrons from heavy-flavour hadron decays in pp and p$-$Pb collisions"

description: pT-differential cross section of electrons from heavy-flavour hadron decays in pp collisions at $\sqrt{s}$ = 13 TeV measured at midrapidity
description: No data abstract available.
DOI: 10.17182/hepdata.142624.v1/t2
title: "Table 2" of "Inclusive and multiplicity dependent production of electrons from heavy-flavour hadron decays in pp and p$-$Pb collisions"

description: pT-differential cross section of electrons from heavy-flavour hadron decays in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV measured at midrapidity
description: No data abstract available.
DOI: 10.17182/hepdata.142624.v1/t3
title: "Table 3" of "Inclusive and multiplicity dependent production of electrons from heavy-flavour hadron decays in pp and p$-$Pb collisions"

description: The Nuclear modification factor RpPb of electrons from heavy-flavour hadron decays in p--Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV
description: No data abstract available.
DOI: 10.17182/hepdata.142624.v1/t5
title: "Table 5" of "Inclusive and multiplicity dependent production of electrons from heavy-flavour hadron decays in pp and p$-$Pb collisions"

description: Self-normalised yield of electrons from heavy-flavour hadron decays as a function of normalised charged-particle pseudorapidity density at midrapidity computed in p--pPb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV in different $p_{\rm T}$ intervals
description: No data abstract available.
DOI: 10.17182/hepdata.142624.v1/t4
title: "Table 4" of "Inclusive and multiplicity dependent production of electrons from heavy-flavour hadron decays in pp and p$-$Pb collisions"

description: Self-normalised yield of electrons from heavy-flavour hadron decays as a function of normalised charged-particle pseudorapidity density at midrapidity computed in pp collisions at $\sqrt{s}$ = 13 TeV in different $p_{\rm T}$ intervals
description: No data abstract available.
DOI: 10.17182/hepdata.32488.v1/t1
title: "Table 1" of "A comparison of pi+ and pi- total cross-sections of light nuclei near the 3-3 resonance"

description: No description provided.
description: CERN-SC. A comparison of PI+ and PI- total cross sections of light nuclei.
DOI: 10.17182/hepdata.32488.v1/t3
title: "Table 3" of "A comparison of pi+ and pi- total cross-sections of light nuclei near the 3-3 resonance"

description: No description provided.
description: CERN-SC. A comparison of PI+ and PI- total cross sections of light nuclei.
DOI: 10.17182/hepdata.32488.v1/t4
title: "Table 4" of "A comparison of pi+ and pi- total cross-sections of light nuclei near the 3-3 resonance"

description: No description provided.
description: CERN-SC. A comparison of PI+ and PI- total cross sections of light nuclei.
DOI: 10.17182/hepdata.111055.v1/t1
title: "$\Delta R$ with $k_{T}$ reclustering in pp" of "First measurements of N-subjettiness in central Pb-Pb collisions at $ \sqrt{s_{\mathrm{NN}}} $ = 2.76 TeV"

description: The $\Delta R$ (with $k_{T}$) fully corrected data distributions for jetsin the jet transverse momentum range 40-60 GeV/c in pp collisions
description: The ALICE Collaboration reports the first fully-corrected measurements of the $N$-subjettiness observable for track-based jets in heavy-ion collisions. This study is performed using data recorded in pp and Pb--Pb collisions at centre-of-mass energies of $\sqrt{s}= 7$ TeV and $\sqrt{s_{\rm NN}} = 2.76$ TeV, respectively. In particular the ratio of 2-subjettiness to 1-subjettiness, $\tau_{2}/\tau_{1}$, which is sensitive to the rate of two-pronged jet substructure, is presented. Energy loss of jets traversing the strongly interacting medium in heavy-ion collisions is expected to change the rate of two-pronged substructure relative to vacuum. The results are presented for jets with a resolution parameter of $R = 0.4$ and charged jet transverse momentum of $40 \leq p_{\rm T,\rm jet} \leq 60$ GeV/$c$, which constitute a larger jet resolution and lower jet transverse momentum interval than previous measurements in heavy-ion collisions. This has been achieved by utilising a semi-inclusive hadron-jet coincidence technique to suppress the larger jet combinatorial background in this kinematic region. No significant modification of the $\tau_{2}/\tau_{1}$ observable for track-based jets in Pb--Pb collisions is observed relative to vacuum PYTHIA6 and PYTHIA8 references at the same collision energy. The measurements of $\tau_{2}/\tau_{1}$, together with the splitting aperture angle $\Delta R$, are also performed in pp collisions at $\sqrt{s}=7$ TeV for inclusive jets. These results are compared with PYTHIA calculations at $\sqrt{s}=7$ TeV, in order to validate the model as a vacuum reference for the Pb--Pb centre-of-mass energy. The PYTHIA references for $\tau_{2}/\tau_{1}$ are shifted to larger values compared to the measurement in pp collisions. This hints at a reduction in the rate of two-pronged jets in Pb--Pb collisions compared to pp collisions.
DOI: 10.17182/hepdata.111055.v1/t2
title: "$\Delta R$ with CA reclustering in pp" of "First measurements of N-subjettiness in central Pb-Pb collisions at $ \sqrt{s_{\mathrm{NN}}} $ = 2.76 TeV"

description: The $\Delta R$ (with C/A) fully corrected data distributions for jetsin the jet transverse momentum range 40-60 GeV/c in pp collisions
description: The ALICE Collaboration reports the first fully-corrected measurements of the $N$-subjettiness observable for track-based jets in heavy-ion collisions. This study is performed using data recorded in pp and Pb--Pb collisions at centre-of-mass energies of $\sqrt{s}= 7$ TeV and $\sqrt{s_{\rm NN}} = 2.76$ TeV, respectively. In particular the ratio of 2-subjettiness to 1-subjettiness, $\tau_{2}/\tau_{1}$, which is sensitive to the rate of two-pronged jet substructure, is presented. Energy loss of jets traversing the strongly interacting medium in heavy-ion collisions is expected to change the rate of two-pronged substructure relative to vacuum. The results are presented for jets with a resolution parameter of $R = 0.4$ and charged jet transverse momentum of $40 \leq p_{\rm T,\rm jet} \leq 60$ GeV/$c$, which constitute a larger jet resolution and lower jet transverse momentum interval than previous measurements in heavy-ion collisions. This has been achieved by utilising a semi-inclusive hadron-jet coincidence technique to suppress the larger jet combinatorial background in this kinematic region. No significant modification of the $\tau_{2}/\tau_{1}$ observable for track-based jets in Pb--Pb collisions is observed relative to vacuum PYTHIA6 and PYTHIA8 references at the same collision energy. The measurements of $\tau_{2}/\tau_{1}$, together with the splitting aperture angle $\Delta R$, are also performed in pp collisions at $\sqrt{s}=7$ TeV for inclusive jets. These results are compared with PYTHIA calculations at $\sqrt{s}=7$ TeV, in order to validate the model as a vacuum reference for the Pb--Pb centre-of-mass energy. The PYTHIA references for $\tau_{2}/\tau_{1}$ are shifted to larger values compared to the measurement in pp collisions. This hints at a reduction in the rate of two-pronged jets in Pb--Pb collisions compared to pp collisions.
DOI: 10.17182/hepdata.32488.v1/t2
title: "Table 2" of "A comparison of pi+ and pi- total cross-sections of light nuclei near the 3-3 resonance"

description: No description provided.
description: CERN-SC. A comparison of PI+ and PI- total cross sections of light nuclei.
DOI: 10.17182/hepdata.32488.v1/t5
title: "Table 5" of "A comparison of pi+ and pi- total cross-sections of light nuclei near the 3-3 resonance"

description: No description provided.
description: CERN-SC. A comparison of PI+ and PI- total cross sections of light nuclei.
DOI: 10.17182/hepdata.32488.v1/t6
title: "Table 6" of "A comparison of pi+ and pi- total cross-sections of light nuclei near the 3-3 resonance"

description: No description provided.
description: CERN-SC. A comparison of PI+ and PI- total cross sections of light nuclei.
DOI: 10.17182/hepdata.111055.v1/t3
title: "$\Delta R$ with Soft Drop in pp" of "First measurements of N-subjettiness in central Pb-Pb collisions at $ \sqrt{s_{\mathrm{NN}}} $ = 2.76 TeV"

description: The $\Delta R$ (with Soft Drop) fully corrected data distributions for jetsin the jet transverse momentum range 40-60 GeV/c in pp collisions
description: The ALICE Collaboration reports the first fully-corrected measurements of the $N$-subjettiness observable for track-based jets in heavy-ion collisions. This study is performed using data recorded in pp and Pb--Pb collisions at centre-of-mass energies of $\sqrt{s}= 7$ TeV and $\sqrt{s_{\rm NN}} = 2.76$ TeV, respectively. In particular the ratio of 2-subjettiness to 1-subjettiness, $\tau_{2}/\tau_{1}$, which is sensitive to the rate of two-pronged jet substructure, is presented. Energy loss of jets traversing the strongly interacting medium in heavy-ion collisions is expected to change the rate of two-pronged substructure relative to vacuum. The results are presented for jets with a resolution parameter of $R = 0.4$ and charged jet transverse momentum of $40 \leq p_{\rm T,\rm jet} \leq 60$ GeV/$c$, which constitute a larger jet resolution and lower jet transverse momentum interval than previous measurements in heavy-ion collisions. This has been achieved by utilising a semi-inclusive hadron-jet coincidence technique to suppress the larger jet combinatorial background in this kinematic region. No significant modification of the $\tau_{2}/\tau_{1}$ observable for track-based jets in Pb--Pb collisions is observed relative to vacuum PYTHIA6 and PYTHIA8 references at the same collision energy. The measurements of $\tau_{2}/\tau_{1}$, together with the splitting aperture angle $\Delta R$, are also performed in pp collisions at $\sqrt{s}=7$ TeV for inclusive jets. These results are compared with PYTHIA calculations at $\sqrt{s}=7$ TeV, in order to validate the model as a vacuum reference for the Pb--Pb centre-of-mass energy. The PYTHIA references for $\tau_{2}/\tau_{1}$ are shifted to larger values compared to the measurement in pp collisions. This hints at a reduction in the rate of two-pronged jets in Pb--Pb collisions compared to pp collisions.
DOI: 10.17182/hepdata.111055.v1/t4
title: "$\frac{\tau_{2}}{\tau_{1}}$ with $k_{T}$ reclustering in pp" of "First measurements of N-subjettiness in central Pb-Pb collisions at $ \sqrt{s_{\mathrm{NN}}} $ = 2.76 TeV"

description: The $\tau_{2}/\tau_{1}$ (with $k_{T}$) fully corrected data distributions for jetsin the jet transverse momentum range 40-60 GeV/c in pp collisions
description: The ALICE Collaboration reports the first fully-corrected measurements of the $N$-subjettiness observable for track-based jets in heavy-ion collisions. This study is performed using data recorded in pp and Pb--Pb collisions at centre-of-mass energies of $\sqrt{s}= 7$ TeV and $\sqrt{s_{\rm NN}} = 2.76$ TeV, respectively. In particular the ratio of 2-subjettiness to 1-subjettiness, $\tau_{2}/\tau_{1}$, which is sensitive to the rate of two-pronged jet substructure, is presented. Energy loss of jets traversing the strongly interacting medium in heavy-ion collisions is expected to change the rate of two-pronged substructure relative to vacuum. The results are presented for jets with a resolution parameter of $R = 0.4$ and charged jet transverse momentum of $40 \leq p_{\rm T,\rm jet} \leq 60$ GeV/$c$, which constitute a larger jet resolution and lower jet transverse momentum interval than previous measurements in heavy-ion collisions. This has been achieved by utilising a semi-inclusive hadron-jet coincidence technique to suppress the larger jet combinatorial background in this kinematic region. No significant modification of the $\tau_{2}/\tau_{1}$ observable for track-based jets in Pb--Pb collisions is observed relative to vacuum PYTHIA6 and PYTHIA8 references at the same collision energy. The measurements of $\tau_{2}/\tau_{1}$, together with the splitting aperture angle $\Delta R$, are also performed in pp collisions at $\sqrt{s}=7$ TeV for inclusive jets. These results are compared with PYTHIA calculations at $\sqrt{s}=7$ TeV, in order to validate the model as a vacuum reference for the Pb--Pb centre-of-mass energy. The PYTHIA references for $\tau_{2}/\tau_{1}$ are shifted to larger values compared to the measurement in pp collisions. This hints at a reduction in the rate of two-pronged jets in Pb--Pb collisions compared to pp collisions.
DOI: 10.17182/hepdata.111055.v1/t5
title: "$\frac{\tau_{2}}{\tau_{1}}$ with CA reclustering in pp" of "First measurements of N-subjettiness in central Pb-Pb collisions at $ \sqrt{s_{\mathrm{NN}}} $ = 2.76 TeV"

description: The $\tau_{2}/\tau_{1}$ (with C/A) fully corrected data distributions for jetsin the jet transverse momentum range 40-60 GeV/c in pp collisions
description: The ALICE Collaboration reports the first fully-corrected measurements of the $N$-subjettiness observable for track-based jets in heavy-ion collisions. This study is performed using data recorded in pp and Pb--Pb collisions at centre-of-mass energies of $\sqrt{s}= 7$ TeV and $\sqrt{s_{\rm NN}} = 2.76$ TeV, respectively. In particular the ratio of 2-subjettiness to 1-subjettiness, $\tau_{2}/\tau_{1}$, which is sensitive to the rate of two-pronged jet substructure, is presented. Energy loss of jets traversing the strongly interacting medium in heavy-ion collisions is expected to change the rate of two-pronged substructure relative to vacuum. The results are presented for jets with a resolution parameter of $R = 0.4$ and charged jet transverse momentum of $40 \leq p_{\rm T,\rm jet} \leq 60$ GeV/$c$, which constitute a larger jet resolution and lower jet transverse momentum interval than previous measurements in heavy-ion collisions. This has been achieved by utilising a semi-inclusive hadron-jet coincidence technique to suppress the larger jet combinatorial background in this kinematic region. No significant modification of the $\tau_{2}/\tau_{1}$ observable for track-based jets in Pb--Pb collisions is observed relative to vacuum PYTHIA6 and PYTHIA8 references at the same collision energy. The measurements of $\tau_{2}/\tau_{1}$, together with the splitting aperture angle $\Delta R$, are also performed in pp collisions at $\sqrt{s}=7$ TeV for inclusive jets. These results are compared with PYTHIA calculations at $\sqrt{s}=7$ TeV, in order to validate the model as a vacuum reference for the Pb--Pb centre-of-mass energy. The PYTHIA references for $\tau_{2}/\tau_{1}$ are shifted to larger values compared to the measurement in pp collisions. This hints at a reduction in the rate of two-pronged jets in Pb--Pb collisions compared to pp collisions.