cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.15468/dl.rsp2jh
title: Occurrence Download

description: A dataset containing 27613 species occurrences available in GBIF matching the query:
{
 "and" : [
 "TaxonKey is Centroptilum",
 "HasCoordinate is true",
 "HasGeospatialIssue is false"
 ]
}

 The dataset includes 27613 records from 161 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0033320-260208012135463/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.25549/uschist-ouc110761201
title: Daily Trojan, vol. 20, no. 28, Oct 23, 1928

description: Southern California Daily Trojan, vol. 20, no. 28, October 23, 1928.
DOI: 10.25549/uschist-ouc110761191
title: Daily Trojan, vol. 20, no. 47, Nov 20, 1928

description: Southern California Daily Trojan, vol. 20, no. 47, November 20, 1928.
DOI: 10.25549/uschist-ouc110755685
title: Daily Trojan, vol. 22, no. 114, Mar 25, 1931

description: Southern California Daily Trojan, vol. 22, no. 114, March 25, 1931.
DOI: 10.25549/uschist-ouc110755701
title: Daily Trojan, vol. 22, no. 128, Apr 23, 1931

description: Southern California Daily Trojan, vol. 22, no. 128, April 23, 1931.
DOI: 10.25549/uschist-ouc110755769
title: Daily Trojan, vol. 22, no. 137, May 6, 1931

description: Southern California Daily Trojan, vol. 22, no. 137, May 6, 1931.
DOI: 10.25549/uschist-ouc110755787
title: Daily Trojan, vol. 22, no. 140, May 11, 1931

description: Southern California Daily Trojan, vol. 22, no. 140, May 11, 1931
DOI: 10.25549/uschist-ouc110755723
title: Daily Trojan, vol. 22, no. 146, May 19, 1931

description: Southern California Daily Trojan, vol. 22, no. 146, May 19, 1931.
DOI: 10.25549/uschist-ouc110760829
title: The Southern California Trojan, vol. 6, no. 12, Aug 5, 1927

description: The Southern California Trojan, vol. 6, no. 12, August 5, 1927.
DOI: 10.17182/hepdata.167195.v1/t1
title: "Table 1" of "$\Sigma^{+}$ production in pp collisions at $\sqrt{s} = 13$ TeV"

description: $p_\mathrm{T}$-differential production yield of $\Sigma^+$ and $\bar{\Sigma}^-$ baryons in the high-multiplicity triggered pp collisions at $\sqrt{{s}}=13~\mathrm{{TeV}}$ in the rapidity interval $|y|&lt;0.8$.
description: The first measurement of $\Sigma^{+}$ production at the LHC is presented. The measurement is performed at midrapidity in both minimum-bias and high-multiplicity pp collisions at $\sqrt{{s}}=13~\mathrm{{TeV}}$. The $\Sigma^{+}$ is reconstructed via its weak-decay topology in the decay channel $\Sigma^{+} \rightarrow \rm{p} + \pi^{0}$ with $\pi^{0} \rightarrow \gamma + \gamma$. In a novel approach, the neutral pion is reconstructed by combining photons that convert in the detector material with photons measured in the calorimeters. The transverse-momentum ($p_{\rm T}$) distributions of the $\Sigma^{+}$ and its rapidity densities ${\rm d}N$/${\rm d}y$ in both event classes are reported. The $p_{\rm T}$ spectrum in minimum-bias collisions is compared to QCD-inspired event generators. The ratio of $\Sigma^{+}$ to previously measured $\Lambda$ baryons is in good agreement with calculations from the Statistical Hadronization Model. The high efficiency and purity of the novel reconstruction method for $\Sigma^{+}$ presented here will enable future studies of the interaction of $\Sigma^{+}$ with protons in the context of femtoscopic measurements, which could be crucial for understanding the equation of state of neutron stars.
DOI: 10.25549/uschist-ouc110760755
title: Daily Trojan, vol. 19, no. 1, Sep 13, 1927

description: Southern California Daily Trojan, vol. 19, no. 1, September 13, 1927.
DOI: 10.17182/hepdata.167195.v1/t2
title: "Table 2" of "$\Sigma^{+}$ production in pp collisions at $\sqrt{s} = 13$ TeV"

description: $p_\mathrm{T}$-differential production yield of $\Sigma^+$ and $\bar{\Sigma}^-$ baryons in the minimum-bias triggered pp collisions at $\sqrt{{s}}=13~\mathrm{{TeV}}$ in the rapidity interval $|y|&lt;0.8$.
description: The first measurement of $\Sigma^{+}$ production at the LHC is presented. The measurement is performed at midrapidity in both minimum-bias and high-multiplicity pp collisions at $\sqrt{{s}}=13~\mathrm{{TeV}}$. The $\Sigma^{+}$ is reconstructed via its weak-decay topology in the decay channel $\Sigma^{+} \rightarrow \rm{p} + \pi^{0}$ with $\pi^{0} \rightarrow \gamma + \gamma$. In a novel approach, the neutral pion is reconstructed by combining photons that convert in the detector material with photons measured in the calorimeters. The transverse-momentum ($p_{\rm T}$) distributions of the $\Sigma^{+}$ and its rapidity densities ${\rm d}N$/${\rm d}y$ in both event classes are reported. The $p_{\rm T}$ spectrum in minimum-bias collisions is compared to QCD-inspired event generators. The ratio of $\Sigma^{+}$ to previously measured $\Lambda$ baryons is in good agreement with calculations from the Statistical Hadronization Model. The high efficiency and purity of the novel reconstruction method for $\Sigma^{+}$ presented here will enable future studies of the interaction of $\Sigma^{+}$ with protons in the context of femtoscopic measurements, which could be crucial for understanding the equation of state of neutron stars.
DOI: 10.17182/hepdata.167265.v1/t1
title: "Cross sections. 12C+p, 12C+CH2, 12C+C at 13.5 GeV/c" of "Measurement of the mass-changing, charge-changing and production cross sections of $^{11}$C, $^{11}$B and $^{10}$B nuclei in $^{12}$C+p interactions at 13.5 GeV/c per nucleon"

description: Mass-changing, charge-changing and production cross sections of $^{11}\mathrm{C}$, $^{11}\mathrm{B}$ and $^{10}\mathrm{B}$ nuclei in $^{12}\mathrm{C}$ + p interactions at 13.5 GeV/c per nucleon. 
Graphite (C) and polyethylene (CH2) targets were used. The cross section on a proton target (p) was derived from the measurements on the CH2 and C targets according to the formula $\sigma_p = \frac{1}{2}\left( \sigma_{\mathrm{CH2}} - \sigma_{\mathrm{C}} \right).$ 
Notation for the type of cross section in the table: mc – mass-changing, cc – charge-changing, prod – production.
description: No data abstract available.
DOI: 10.25549/uschist-ouc110760741
title: Daily Trojan, vol. 19, no. 5, Sep 23, 1927

description: Southern California Daily Trojan, vol. 19, no. 5, September 23, 1927.
DOI: 10.15468/dl.gj78gd
title: Occurrence Download

description: A dataset containing 1379 species occurrences available in GBIF matching the query:
{
 "and" : [
 "TaxonKey is Cyanocorax heilprini",
 "Year is greater than or equal to 2000",
 "Year is less than or equal to 2026",
 "HasCoordinate is true"
 ]
}

 The dataset includes 1379 records from 8 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0033322-260208012135463/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.167421.v1/t1
title: "Table 1" of "Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV"

description: Transverse momentum spectra in different multiplicity classes. Each spectrum is corrected for the branching ratio of (46 $\pm$ 6)% based on [Phys. Rev. Lett. 111 no. 6, (2013) 062001].
description: The dependence of $\mathrm{f}_{0}$(980) production on the final-state charged-particle multiplicity is reported for proton--proton (pp) collisions at the centre-of-mass energy, $\sqrt{s}=$~13~TeV. The production of $\mathrm{f}_{0}$(980) is measured with the ALICE detector via the $\mathrm{f}_0 (980) \rightarrow \pi^{+}\pi^{-}$ decay channel in a midrapidity region of $|y|&lt;$~0.5. The evolution of the integrated yields and mean transverse momentum of f$_{0}$(980) as a function of charged-particle multiplicity measured in pp at $\sqrt{s}=$~13~TeV follows the trends observed in pp at $\sqrt{s}=$~5.02~TeV and in proton--lead (p--Pb) collisions at $\sqrt{s_{\mathrm{NN}}}=$~5.02~TeV. Particle yield ratios of $\mathrm{f}_{0}$(980) to $\pi^{\pm}$ and $\mathrm{K}^{*}$(892)$^{0}$ are found to decrease with increasing charged-particle multiplicity. These particle ratios are compared with calculations from the canonical statistical thermal model as a function of charged-particle multiplicity. The thermal model calculations provide a better description of the decreasing trend of particle ratios when no strange or antistrange quark composition for f$_{0}$(980) is assumed, which suggests that the tetraquark interpretation of the f$_{0}$(980) is disfavored.
DOI: 10.17182/hepdata.167421.v1/t2
title: "Table 2" of "Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV"

description: The ratio of transverse momentum spectrum to the INEL &gt; 0 spectrum
description: The dependence of $\mathrm{f}_{0}$(980) production on the final-state charged-particle multiplicity is reported for proton--proton (pp) collisions at the centre-of-mass energy, $\sqrt{s}=$~13~TeV. The production of $\mathrm{f}_{0}$(980) is measured with the ALICE detector via the $\mathrm{f}_0 (980) \rightarrow \pi^{+}\pi^{-}$ decay channel in a midrapidity region of $|y|&lt;$~0.5. The evolution of the integrated yields and mean transverse momentum of f$_{0}$(980) as a function of charged-particle multiplicity measured in pp at $\sqrt{s}=$~13~TeV follows the trends observed in pp at $\sqrt{s}=$~5.02~TeV and in proton--lead (p--Pb) collisions at $\sqrt{s_{\mathrm{NN}}}=$~5.02~TeV. Particle yield ratios of $\mathrm{f}_{0}$(980) to $\pi^{\pm}$ and $\mathrm{K}^{*}$(892)$^{0}$ are found to decrease with increasing charged-particle multiplicity. These particle ratios are compared with calculations from the canonical statistical thermal model as a function of charged-particle multiplicity. The thermal model calculations provide a better description of the decreasing trend of particle ratios when no strange or antistrange quark composition for f$_{0}$(980) is assumed, which suggests that the tetraquark interpretation of the f$_{0}$(980) is disfavored.
DOI: 10.17182/hepdata.167421.v1/t3
title: "Table 3" of "Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV"

description: Transverse momentum integrated f0(980) yield in pp collisions
description: The dependence of $\mathrm{f}_{0}$(980) production on the final-state charged-particle multiplicity is reported for proton--proton (pp) collisions at the centre-of-mass energy, $\sqrt{s}=$~13~TeV. The production of $\mathrm{f}_{0}$(980) is measured with the ALICE detector via the $\mathrm{f}_0 (980) \rightarrow \pi^{+}\pi^{-}$ decay channel in a midrapidity region of $|y|&lt;$~0.5. The evolution of the integrated yields and mean transverse momentum of f$_{0}$(980) as a function of charged-particle multiplicity measured in pp at $\sqrt{s}=$~13~TeV follows the trends observed in pp at $\sqrt{s}=$~5.02~TeV and in proton--lead (p--Pb) collisions at $\sqrt{s_{\mathrm{NN}}}=$~5.02~TeV. Particle yield ratios of $\mathrm{f}_{0}$(980) to $\pi^{\pm}$ and $\mathrm{K}^{*}$(892)$^{0}$ are found to decrease with increasing charged-particle multiplicity. These particle ratios are compared with calculations from the canonical statistical thermal model as a function of charged-particle multiplicity. The thermal model calculations provide a better description of the decreasing trend of particle ratios when no strange or antistrange quark composition for f$_{0}$(980) is assumed, which suggests that the tetraquark interpretation of the f$_{0}$(980) is disfavored.
DOI: 10.17182/hepdata.167421.v1/t5
title: "Table 5" of "Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV"

description: The particle yield ratio of f0((980) to charged pions
description: The dependence of $\mathrm{f}_{0}$(980) production on the final-state charged-particle multiplicity is reported for proton--proton (pp) collisions at the centre-of-mass energy, $\sqrt{s}=$~13~TeV. The production of $\mathrm{f}_{0}$(980) is measured with the ALICE detector via the $\mathrm{f}_0 (980) \rightarrow \pi^{+}\pi^{-}$ decay channel in a midrapidity region of $|y|&lt;$~0.5. The evolution of the integrated yields and mean transverse momentum of f$_{0}$(980) as a function of charged-particle multiplicity measured in pp at $\sqrt{s}=$~13~TeV follows the trends observed in pp at $\sqrt{s}=$~5.02~TeV and in proton--lead (p--Pb) collisions at $\sqrt{s_{\mathrm{NN}}}=$~5.02~TeV. Particle yield ratios of $\mathrm{f}_{0}$(980) to $\pi^{\pm}$ and $\mathrm{K}^{*}$(892)$^{0}$ are found to decrease with increasing charged-particle multiplicity. These particle ratios are compared with calculations from the canonical statistical thermal model as a function of charged-particle multiplicity. The thermal model calculations provide a better description of the decreasing trend of particle ratios when no strange or antistrange quark composition for f$_{0}$(980) is assumed, which suggests that the tetraquark interpretation of the f$_{0}$(980) is disfavored.
DOI: 10.17182/hepdata.167421.v1/t6
title: "Table 6" of "Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV"

description: The particle yield ratio of f0((980) to K*(892)0
description: The dependence of $\mathrm{f}_{0}$(980) production on the final-state charged-particle multiplicity is reported for proton--proton (pp) collisions at the centre-of-mass energy, $\sqrt{s}=$~13~TeV. The production of $\mathrm{f}_{0}$(980) is measured with the ALICE detector via the $\mathrm{f}_0 (980) \rightarrow \pi^{+}\pi^{-}$ decay channel in a midrapidity region of $|y|&lt;$~0.5. The evolution of the integrated yields and mean transverse momentum of f$_{0}$(980) as a function of charged-particle multiplicity measured in pp at $\sqrt{s}=$~13~TeV follows the trends observed in pp at $\sqrt{s}=$~5.02~TeV and in proton--lead (p--Pb) collisions at $\sqrt{s_{\mathrm{NN}}}=$~5.02~TeV. Particle yield ratios of $\mathrm{f}_{0}$(980) to $\pi^{\pm}$ and $\mathrm{K}^{*}$(892)$^{0}$ are found to decrease with increasing charged-particle multiplicity. These particle ratios are compared with calculations from the canonical statistical thermal model as a function of charged-particle multiplicity. The thermal model calculations provide a better description of the decreasing trend of particle ratios when no strange or antistrange quark composition for f$_{0}$(980) is assumed, which suggests that the tetraquark interpretation of the f$_{0}$(980) is disfavored.
DOI: 10.17182/hepdata.167421.v1/t7
title: "Table 7" of "Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV"

description: The double ratio of particle yield of f0(980) to charged pions
description: The dependence of $\mathrm{f}_{0}$(980) production on the final-state charged-particle multiplicity is reported for proton--proton (pp) collisions at the centre-of-mass energy, $\sqrt{s}=$~13~TeV. The production of $\mathrm{f}_{0}$(980) is measured with the ALICE detector via the $\mathrm{f}_0 (980) \rightarrow \pi^{+}\pi^{-}$ decay channel in a midrapidity region of $|y|&lt;$~0.5. The evolution of the integrated yields and mean transverse momentum of f$_{0}$(980) as a function of charged-particle multiplicity measured in pp at $\sqrt{s}=$~13~TeV follows the trends observed in pp at $\sqrt{s}=$~5.02~TeV and in proton--lead (p--Pb) collisions at $\sqrt{s_{\mathrm{NN}}}=$~5.02~TeV. Particle yield ratios of $\mathrm{f}_{0}$(980) to $\pi^{\pm}$ and $\mathrm{K}^{*}$(892)$^{0}$ are found to decrease with increasing charged-particle multiplicity. These particle ratios are compared with calculations from the canonical statistical thermal model as a function of charged-particle multiplicity. The thermal model calculations provide a better description of the decreasing trend of particle ratios when no strange or antistrange quark composition for f$_{0}$(980) is assumed, which suggests that the tetraquark interpretation of the f$_{0}$(980) is disfavored.
DOI: 10.17182/hepdata.167421.v1/t10
title: "Table 10" of "Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV"

description: Transverse momentum differential particle yield ratio of f0(980) to K*(892)0
description: The dependence of $\mathrm{f}_{0}$(980) production on the final-state charged-particle multiplicity is reported for proton--proton (pp) collisions at the centre-of-mass energy, $\sqrt{s}=$~13~TeV. The production of $\mathrm{f}_{0}$(980) is measured with the ALICE detector via the $\mathrm{f}_0 (980) \rightarrow \pi^{+}\pi^{-}$ decay channel in a midrapidity region of $|y|&lt;$~0.5. The evolution of the integrated yields and mean transverse momentum of f$_{0}$(980) as a function of charged-particle multiplicity measured in pp at $\sqrt{s}=$~13~TeV follows the trends observed in pp at $\sqrt{s}=$~5.02~TeV and in proton--lead (p--Pb) collisions at $\sqrt{s_{\mathrm{NN}}}=$~5.02~TeV. Particle yield ratios of $\mathrm{f}_{0}$(980) to $\pi^{\pm}$ and $\mathrm{K}^{*}$(892)$^{0}$ are found to decrease with increasing charged-particle multiplicity. These particle ratios are compared with calculations from the canonical statistical thermal model as a function of charged-particle multiplicity. The thermal model calculations provide a better description of the decreasing trend of particle ratios when no strange or antistrange quark composition for f$_{0}$(980) is assumed, which suggests that the tetraquark interpretation of the f$_{0}$(980) is disfavored.
DOI: 10.17182/hepdata.167421.v1/t11
title: "Table 11" of "Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV"

description: Transverse momentum differential double ratio of particle yield of f0(980) to charged pions
description: The dependence of $\mathrm{f}_{0}$(980) production on the final-state charged-particle multiplicity is reported for proton--proton (pp) collisions at the centre-of-mass energy, $\sqrt{s}=$~13~TeV. The production of $\mathrm{f}_{0}$(980) is measured with the ALICE detector via the $\mathrm{f}_0 (980) \rightarrow \pi^{+}\pi^{-}$ decay channel in a midrapidity region of $|y|&lt;$~0.5. The evolution of the integrated yields and mean transverse momentum of f$_{0}$(980) as a function of charged-particle multiplicity measured in pp at $\sqrt{s}=$~13~TeV follows the trends observed in pp at $\sqrt{s}=$~5.02~TeV and in proton--lead (p--Pb) collisions at $\sqrt{s_{\mathrm{NN}}}=$~5.02~TeV. Particle yield ratios of $\mathrm{f}_{0}$(980) to $\pi^{\pm}$ and $\mathrm{K}^{*}$(892)$^{0}$ are found to decrease with increasing charged-particle multiplicity. These particle ratios are compared with calculations from the canonical statistical thermal model as a function of charged-particle multiplicity. The thermal model calculations provide a better description of the decreasing trend of particle ratios when no strange or antistrange quark composition for f$_{0}$(980) is assumed, which suggests that the tetraquark interpretation of the f$_{0}$(980) is disfavored.
DOI: 10.17182/hepdata.167421.v1/t12
title: "Table 12" of "Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV"

description: Transverse momentum differential double ratio of particle yield of f0(980) to K*0
description: The dependence of $\mathrm{f}_{0}$(980) production on the final-state charged-particle multiplicity is reported for proton--proton (pp) collisions at the centre-of-mass energy, $\sqrt{s}=$~13~TeV. The production of $\mathrm{f}_{0}$(980) is measured with the ALICE detector via the $\mathrm{f}_0 (980) \rightarrow \pi^{+}\pi^{-}$ decay channel in a midrapidity region of $|y|&lt;$~0.5. The evolution of the integrated yields and mean transverse momentum of f$_{0}$(980) as a function of charged-particle multiplicity measured in pp at $\sqrt{s}=$~13~TeV follows the trends observed in pp at $\sqrt{s}=$~5.02~TeV and in proton--lead (p--Pb) collisions at $\sqrt{s_{\mathrm{NN}}}=$~5.02~TeV. Particle yield ratios of $\mathrm{f}_{0}$(980) to $\pi^{\pm}$ and $\mathrm{K}^{*}$(892)$^{0}$ are found to decrease with increasing charged-particle multiplicity. These particle ratios are compared with calculations from the canonical statistical thermal model as a function of charged-particle multiplicity. The thermal model calculations provide a better description of the decreasing trend of particle ratios when no strange or antistrange quark composition for f$_{0}$(980) is assumed, which suggests that the tetraquark interpretation of the f$_{0}$(980) is disfavored.
DOI: 10.17182/hepdata.167421.v1/t4
title: "Table 4" of "Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV"

description: Mean transverse momentum of f0(980) in pp collisions
description: The dependence of $\mathrm{f}_{0}$(980) production on the final-state charged-particle multiplicity is reported for proton--proton (pp) collisions at the centre-of-mass energy, $\sqrt{s}=$~13~TeV. The production of $\mathrm{f}_{0}$(980) is measured with the ALICE detector via the $\mathrm{f}_0 (980) \rightarrow \pi^{+}\pi^{-}$ decay channel in a midrapidity region of $|y|&lt;$~0.5. The evolution of the integrated yields and mean transverse momentum of f$_{0}$(980) as a function of charged-particle multiplicity measured in pp at $\sqrt{s}=$~13~TeV follows the trends observed in pp at $\sqrt{s}=$~5.02~TeV and in proton--lead (p--Pb) collisions at $\sqrt{s_{\mathrm{NN}}}=$~5.02~TeV. Particle yield ratios of $\mathrm{f}_{0}$(980) to $\pi^{\pm}$ and $\mathrm{K}^{*}$(892)$^{0}$ are found to decrease with increasing charged-particle multiplicity. These particle ratios are compared with calculations from the canonical statistical thermal model as a function of charged-particle multiplicity. The thermal model calculations provide a better description of the decreasing trend of particle ratios when no strange or antistrange quark composition for f$_{0}$(980) is assumed, which suggests that the tetraquark interpretation of the f$_{0}$(980) is disfavored.
DOI: 10.17182/hepdata.167421.v1/t8
title: "Table 8" of "Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV"

description: The double ratio of particle yield of f0((980) to K*(892)0
description: The dependence of $\mathrm{f}_{0}$(980) production on the final-state charged-particle multiplicity is reported for proton--proton (pp) collisions at the centre-of-mass energy, $\sqrt{s}=$~13~TeV. The production of $\mathrm{f}_{0}$(980) is measured with the ALICE detector via the $\mathrm{f}_0 (980) \rightarrow \pi^{+}\pi^{-}$ decay channel in a midrapidity region of $|y|&lt;$~0.5. The evolution of the integrated yields and mean transverse momentum of f$_{0}$(980) as a function of charged-particle multiplicity measured in pp at $\sqrt{s}=$~13~TeV follows the trends observed in pp at $\sqrt{s}=$~5.02~TeV and in proton--lead (p--Pb) collisions at $\sqrt{s_{\mathrm{NN}}}=$~5.02~TeV. Particle yield ratios of $\mathrm{f}_{0}$(980) to $\pi^{\pm}$ and $\mathrm{K}^{*}$(892)$^{0}$ are found to decrease with increasing charged-particle multiplicity. These particle ratios are compared with calculations from the canonical statistical thermal model as a function of charged-particle multiplicity. The thermal model calculations provide a better description of the decreasing trend of particle ratios when no strange or antistrange quark composition for f$_{0}$(980) is assumed, which suggests that the tetraquark interpretation of the f$_{0}$(980) is disfavored.