cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.157267.v1/t27
title: "Table 21" of "First observation of strange baryon enhancement with effective energy in pp collisions at the LHC"

description: Self-normalised yield ratios of $K^{0}_{S}$, $\Lambda+\overline{\Lambda}$, and $\Xi^{-}+\overline{\Xi}^{+}$ as a function of the self-normalised $ZN$ signal in pp collisions at $\sqrt{s}$ = 13 TeV in the low-ZN-energy classification (V0M+SPDClusters event classes).
description: The production of (multi-)strange hadrons is measured at midrapidity in proton-proton (pp) collisions at $\sqrt{s} = 13$ TeV as a function of the local charged-particle multiplicity in the pseudorapidity interval $|\eta|&lt;0.5$ and of the very-forward energy measured by the ALICE Zero-Degree Calorimeters (ZDC). The latter provides information on the effective energy available for particle production in the collision once subtracted from the centre-of-mass energy. The yields of $K^{0}_{S}$, $\Lambda + \overline{\Lambda}$, and $\Xi^{-} + \overline{\Xi}^{+}$ per charged-particle increase with the effective energy. In addition, this work exploits a multi-differential approach to decouple the roles of local multiplicity and effective energy in such an enhancement. The results presented in this article provide new insights into the interplay between global properties of the collision, such as the initial available energy in the event, and the locally produced final hadronic state, connected to the charged-particle multiplicity at midrapidity. Notably, a strong increase of strange baryon production with effective energy is observed for fixed charged-particle multiplicity at midrapidity. These results are discussed within the context of existing phenomenological models of hadronisation implemented in different tunes of the PYTHIA 8 event generator.
DOI: 10.17182/hepdata.150695.v1/t1
title: "ridgeYield" of "Emergence of long-range angular correlations in low-multiplicity proton-proton collisions"

description: Ridge yield $Y_\mathrm{ridge}$ extracted at $1.4&lt;|\Delta\eta|&lt;1.8$ with $1.0
description: Multiplicity dependence of the ridge yield in low-multiplicity proton-proton collisions.
DOI: 10.17182/hepdata.156992.v1/t1
title: "Table 1" of "CIRCUS: an autonomous control system for antimatter, atomic and quantum physics experiments"

description: Synchronous voltage ramp-up to 20 V on three high-voltage amplifier channels 10 μs subsequent to the arrival of a common trigger pulse at zero time in the figure. The inset shows a zoom to the shoulder region for a better visualisation of the synchronicity.
description: Data related to the article describing the CIRCUS (Computer Interface for Reliably Controlling, in an Unsupervised manner, Scientific experiments), an autonomous control system for antimatter, atomic and quantum physics experiments. https://doi.org/10.1140/epjqt/s40507-024-00220-6
DOI: 10.17182/hepdata.156992.v1/t2
title: "Table 2" of "CIRCUS: an autonomous control system for antimatter, atomic and quantum physics experiments"

description: A feedback loop uses the uncorrected laser pulse timings (red squares) to calculate the deviation from the user setting (solid black line) over the course of an hour, and corrects the timing of the subsequent desired laser pulse that is used for the actual experiment (blue circles). Independent of short-term to long-term drifts or even sudden jumps, the resulting timing is always close to the desired value.
description: Data related to the article describing the CIRCUS (Computer Interface for Reliably Controlling, in an Unsupervised manner, Scientific experiments), an autonomous control system for antimatter, atomic and quantum physics experiments. https://doi.org/10.1140/epjqt/s40507-024-00220-6
DOI: 10.17182/hepdata.156992.v1/t3
title: "Table 3" of "CIRCUS: an autonomous control system for antimatter, atomic and quantum physics experiments"

description: A feedback loop uses the uncorrected laser pulse timings (red squares) to calculate the deviation from the user setting (solid black line) over the course of an hour, and corrects the timing of the subsequent desired laser pulse that is used for the actual experiment (blue circles). Independent of short-term to long-term drifts or even sudden jumps, the resulting timing is always close to the desired value.
description: Data related to the article describing the CIRCUS (Computer Interface for Reliably Controlling, in an Unsupervised manner, Scientific experiments), an autonomous control system for antimatter, atomic and quantum physics experiments. https://doi.org/10.1140/epjqt/s40507-024-00220-6
DOI: 10.17182/hepdata.156992.v1/t4
title: "Table 4" of "CIRCUS: an autonomous control system for antimatter, atomic and quantum physics experiments"

description: Scintillator counts of the annihilation of antiprotons inside the Penning trap. The two deltoid-like structures at ≈10 s and ≈25 s are emissions from the accelerators in the AD complex and are present independently of the ongoing trapping.
description: Data related to the article describing the CIRCUS (Computer Interface for Reliably Controlling, in an Unsupervised manner, Scientific experiments), an autonomous control system for antimatter, atomic and quantum physics experiments. https://doi.org/10.1140/epjqt/s40507-024-00220-6
DOI: 10.17182/hepdata.153245.v1/t1
title: "Table 1" of "Studying the interaction between charm and light-flavor mesons"

description: Genuine correlation function for $D^{+}\uppi^{-}$ in high-multiplicity pp collisions at $\sqrt{s}=13$ TeV.
description: The two-particle momentum correlation functions between charm mesons (D$^{*\pm}$ and D$^{\pm}$) and charged light-flavor mesons ($\uppi^{\pm}$ and K$^{\pm}$) in all charge-combinations are measured for the first time by the ALICE Collaboration in high-multiplicity proton--proton collisions at a center-of-mass energy of $\sqrt(s)=13$ TeV. For DK and D$^*$K pairs, the experimental results are in agreement with theoretical predictions of the residual strong interaction based on quantum chromodynamics calculations on the lattice and chiral effective field theory. In the case of D$\uppi$ and D$^*\uppi$ pairs, tension between the calculations including strong interactions and the measurement is observed. For all particle pairs, the data can be adequately described by Coulomb interaction only, indicating a shallow interaction between charm and light-flavor mesons. Finally, the scattering lengths governing the residual strong interaction of the D$\uppi$ and D$^*\uppi$ systems are determined by fitting the experimental correlation functions with a model that employs a Gaussian potential. The extracted values are small and compatible with zero.
DOI: 10.17182/hepdata.153245.v1/t2
title: "Table 2" of "Studying the interaction between charm and light-flavor mesons"

description: Genuine correlation function for $D^{+}\uppi^{+}$ in high-multiplicity pp collisions at $\sqrt{s}=13$ TeV.
description: The two-particle momentum correlation functions between charm mesons (D$^{*\pm}$ and D$^{\pm}$) and charged light-flavor mesons ($\uppi^{\pm}$ and K$^{\pm}$) in all charge-combinations are measured for the first time by the ALICE Collaboration in high-multiplicity proton--proton collisions at a center-of-mass energy of $\sqrt(s)=13$ TeV. For DK and D$^*$K pairs, the experimental results are in agreement with theoretical predictions of the residual strong interaction based on quantum chromodynamics calculations on the lattice and chiral effective field theory. In the case of D$\uppi$ and D$^*\uppi$ pairs, tension between the calculations including strong interactions and the measurement is observed. For all particle pairs, the data can be adequately described by Coulomb interaction only, indicating a shallow interaction between charm and light-flavor mesons. Finally, the scattering lengths governing the residual strong interaction of the D$\uppi$ and D$^*\uppi$ systems are determined by fitting the experimental correlation functions with a model that employs a Gaussian potential. The extracted values are small and compatible with zero.
DOI: 10.17182/hepdata.156992.v1/t5
title: "Table 5" of "CIRCUS: an autonomous control system for antimatter, atomic and quantum physics experiments"

description: Difference between the desired voltage on the amplifier channels and the measured output voltage versus the expected voltage before (top) and after (bottom) the amplifier calibration for all eight amplifier channels of one example board. The shown legend identifies the channel numbers of the given board.
description: Data related to the article describing the CIRCUS (Computer Interface for Reliably Controlling, in an Unsupervised manner, Scientific experiments), an autonomous control system for antimatter, atomic and quantum physics experiments. https://doi.org/10.1140/epjqt/s40507-024-00220-6
DOI: 10.17182/hepdata.156992.v1/t6
title: "Table 6" of "CIRCUS: an autonomous control system for antimatter, atomic and quantum physics experiments"

description: Difference between the desired voltage on the amplifier channels and the measured output voltage versus the expected voltage before (top) and after (bottom) the amplifier calibration for all eight amplifier channels of one example board. The shown legend identifies the channel numbers of the given board.
description: Data related to the article describing the CIRCUS (Computer Interface for Reliably Controlling, in an Unsupervised manner, Scientific experiments), an autonomous control system for antimatter, atomic and quantum physics experiments. https://doi.org/10.1140/epjqt/s40507-024-00220-6
DOI: 10.17182/hepdata.153245.v1/t3
title: "Table 3" of "Studying the interaction between charm and light-flavor mesons"

description: Genuine correlation function for $D^{+}K^{-}$ in high-multiplicity pp collisions at $\sqrt{s}=13$ TeV.
description: The two-particle momentum correlation functions between charm mesons (D$^{*\pm}$ and D$^{\pm}$) and charged light-flavor mesons ($\uppi^{\pm}$ and K$^{\pm}$) in all charge-combinations are measured for the first time by the ALICE Collaboration in high-multiplicity proton--proton collisions at a center-of-mass energy of $\sqrt(s)=13$ TeV. For DK and D$^*$K pairs, the experimental results are in agreement with theoretical predictions of the residual strong interaction based on quantum chromodynamics calculations on the lattice and chiral effective field theory. In the case of D$\uppi$ and D$^*\uppi$ pairs, tension between the calculations including strong interactions and the measurement is observed. For all particle pairs, the data can be adequately described by Coulomb interaction only, indicating a shallow interaction between charm and light-flavor mesons. Finally, the scattering lengths governing the residual strong interaction of the D$\uppi$ and D$^*\uppi$ systems are determined by fitting the experimental correlation functions with a model that employs a Gaussian potential. The extracted values are small and compatible with zero.
DOI: 10.17182/hepdata.153245.v1/t4
title: "Table 4" of "Studying the interaction between charm and light-flavor mesons"

description: Genuine correlation function for $D^{+}K^{+}$ in high-multiplicity pp collisions at $\sqrt{s}=13$ TeV.
description: The two-particle momentum correlation functions between charm mesons (D$^{*\pm}$ and D$^{\pm}$) and charged light-flavor mesons ($\uppi^{\pm}$ and K$^{\pm}$) in all charge-combinations are measured for the first time by the ALICE Collaboration in high-multiplicity proton--proton collisions at a center-of-mass energy of $\sqrt(s)=13$ TeV. For DK and D$^*$K pairs, the experimental results are in agreement with theoretical predictions of the residual strong interaction based on quantum chromodynamics calculations on the lattice and chiral effective field theory. In the case of D$\uppi$ and D$^*\uppi$ pairs, tension between the calculations including strong interactions and the measurement is observed. For all particle pairs, the data can be adequately described by Coulomb interaction only, indicating a shallow interaction between charm and light-flavor mesons. Finally, the scattering lengths governing the residual strong interaction of the D$\uppi$ and D$^*\uppi$ systems are determined by fitting the experimental correlation functions with a model that employs a Gaussian potential. The extracted values are small and compatible with zero.
DOI: 10.17182/hepdata.153245.v1/t5
title: "Table 5" of "Studying the interaction between charm and light-flavor mesons"

description: Genuine correlation function for $D^{*+}\uppi^{-}$ in high-multiplicity pp collisions at $\sqrt{s}=13$ TeV.
description: The two-particle momentum correlation functions between charm mesons (D$^{*\pm}$ and D$^{\pm}$) and charged light-flavor mesons ($\uppi^{\pm}$ and K$^{\pm}$) in all charge-combinations are measured for the first time by the ALICE Collaboration in high-multiplicity proton--proton collisions at a center-of-mass energy of $\sqrt(s)=13$ TeV. For DK and D$^*$K pairs, the experimental results are in agreement with theoretical predictions of the residual strong interaction based on quantum chromodynamics calculations on the lattice and chiral effective field theory. In the case of D$\uppi$ and D$^*\uppi$ pairs, tension between the calculations including strong interactions and the measurement is observed. For all particle pairs, the data can be adequately described by Coulomb interaction only, indicating a shallow interaction between charm and light-flavor mesons. Finally, the scattering lengths governing the residual strong interaction of the D$\uppi$ and D$^*\uppi$ systems are determined by fitting the experimental correlation functions with a model that employs a Gaussian potential. The extracted values are small and compatible with zero.
DOI: 10.17182/hepdata.153245.v1/t6
title: "Table 6" of "Studying the interaction between charm and light-flavor mesons"

description: Genuine correlation function for $D^{*+}\uppi^{+}$ in high-multiplicity pp collisions at $\sqrt{s}=13$ TeV.
description: The two-particle momentum correlation functions between charm mesons (D$^{*\pm}$ and D$^{\pm}$) and charged light-flavor mesons ($\uppi^{\pm}$ and K$^{\pm}$) in all charge-combinations are measured for the first time by the ALICE Collaboration in high-multiplicity proton--proton collisions at a center-of-mass energy of $\sqrt(s)=13$ TeV. For DK and D$^*$K pairs, the experimental results are in agreement with theoretical predictions of the residual strong interaction based on quantum chromodynamics calculations on the lattice and chiral effective field theory. In the case of D$\uppi$ and D$^*\uppi$ pairs, tension between the calculations including strong interactions and the measurement is observed. For all particle pairs, the data can be adequately described by Coulomb interaction only, indicating a shallow interaction between charm and light-flavor mesons. Finally, the scattering lengths governing the residual strong interaction of the D$\uppi$ and D$^*\uppi$ systems are determined by fitting the experimental correlation functions with a model that employs a Gaussian potential. The extracted values are small and compatible with zero.
DOI: 10.17182/hepdata.153245.v1/t7
title: "Table 7" of "Studying the interaction between charm and light-flavor mesons"

description: Genuine correlation function for $D^{*+}K^{-}$ in high-multiplicity pp collisions at $\sqrt{s}=13$ TeV.
description: The two-particle momentum correlation functions between charm mesons (D$^{*\pm}$ and D$^{\pm}$) and charged light-flavor mesons ($\uppi^{\pm}$ and K$^{\pm}$) in all charge-combinations are measured for the first time by the ALICE Collaboration in high-multiplicity proton--proton collisions at a center-of-mass energy of $\sqrt(s)=13$ TeV. For DK and D$^*$K pairs, the experimental results are in agreement with theoretical predictions of the residual strong interaction based on quantum chromodynamics calculations on the lattice and chiral effective field theory. In the case of D$\uppi$ and D$^*\uppi$ pairs, tension between the calculations including strong interactions and the measurement is observed. For all particle pairs, the data can be adequately described by Coulomb interaction only, indicating a shallow interaction between charm and light-flavor mesons. Finally, the scattering lengths governing the residual strong interaction of the D$\uppi$ and D$^*\uppi$ systems are determined by fitting the experimental correlation functions with a model that employs a Gaussian potential. The extracted values are small and compatible with zero.
DOI: 10.17182/hepdata.153245.v1/t8
title: "Table 8" of "Studying the interaction between charm and light-flavor mesons"

description: Genuine correlation function for $D^{*+}K^{+}$ in high-multiplicity pp collisions at $\sqrt{s}=13$ TeV.
description: The two-particle momentum correlation functions between charm mesons (D$^{*\pm}$ and D$^{\pm}$) and charged light-flavor mesons ($\uppi^{\pm}$ and K$^{\pm}$) in all charge-combinations are measured for the first time by the ALICE Collaboration in high-multiplicity proton--proton collisions at a center-of-mass energy of $\sqrt(s)=13$ TeV. For DK and D$^*$K pairs, the experimental results are in agreement with theoretical predictions of the residual strong interaction based on quantum chromodynamics calculations on the lattice and chiral effective field theory. In the case of D$\uppi$ and D$^*\uppi$ pairs, tension between the calculations including strong interactions and the measurement is observed. For all particle pairs, the data can be adequately described by Coulomb interaction only, indicating a shallow interaction between charm and light-flavor mesons. Finally, the scattering lengths governing the residual strong interaction of the D$\uppi$ and D$^*\uppi$ systems are determined by fitting the experimental correlation functions with a model that employs a Gaussian potential. The extracted values are small and compatible with zero.
DOI: 10.17182/hepdata.156190.v1/t1
title: "Table 1 - Antideuteron PT spectrum rapidity 0 to 0.1" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: Transverse momentum spectra of antideuterons measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as shown in Fig. 1 (right panel). Rapidity interval 0 to 0.1.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t2
title: "Table 2 - Antideuteron PT spectrum rapidity 0.1 to 0.2" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: Transverse momentum spectra of antideuterons measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as shown in Fig. 1 (right panel). Rapidity interval 0.1 to 0.2.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t3
title: "Table 3 - Antideuteron PT spectrum rapidity 0.2 to 0.3" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: Transverse momentum spectra of antideuterons measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as shown in Fig. 1 (right panel). Rapidity interval 0.2 to 0.3.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t4
title: "Table 4 - Antideuteron PT spectrum rapidity 0.3 to 0.4" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: Transverse momentum spectra of antideuterons measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as shown in Fig. 1 (right panel). Rapidity interval 0.3 to 0.4.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t5
title: "Table 5 - Antideuteron PT spectrum rapidity 0.4 to 0.5" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: Transverse momentum spectra of antideuterons measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as shown in Fig. 1 (right panel). Rapidity interval 0.4 to 0.5.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t6
title: "Table 6 - Antideuteron PT spectrum rapidity 0.5 to 0.6" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: Transverse momentum spectra of antideuterons measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as shown in Fig. 1 (right panel). Rapidity interval 0.5 to 0.6.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t10
title: "Table 10 - Antiproton PT spectrum rapidity 0.2 to 0.3" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: Transverse momentum spectra of antiprotons measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as shown in Fig. 1 (left panel). Rapidity interval 0.2 to 0.3.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t7
title: "Table 7 - Antideuteron PT spectrum rapidity 0.6 to 0.7" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: Transverse momentum spectra of antideuterons measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as shown in Fig. 1 (right panel). Rapidity interval 0.6 to 0.7.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t8
title: "Table 8 - Antiproton PT spectrum rapidity 0 to 0.1" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: Transverse momentum spectra of antiprotons measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as shown in Fig. 1 (left panel). Rapidity interval 0 to 0.1.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.