cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.15468/dl.986g43
title: Occurrence Download

description: A dataset containing 145148 species occurrences available in GBIF matching the query:
{
 "and" : [
 "TaxonKey is one of (Macropsidius insignis (Van Duzee, 1889), Balcanocerus myroxyli (Ishihara, 1956), Agrilus paradiseus Obenberger, 1924, Platypolia mactata (Guenée, 1852), Anoplognathus olivieri (Schönherr & Dalman, 1817), Cerace xanthocosma Diakonoff, 1950, Cantharis decipiens Baudi, 1871, Gaurotes cyanipennis (Say, 1824), Kalotermes flavicollis (Fabricius, 1793), Mimas tiliae Linnaeus, 1758, Malacosoma constricta Edwards, 1874, Xystopeplus rufago Hübner, 1818, Dasychira obliquata Grote & Robinson, 1866, Eugonobapta nivosaria (Guenée, 1857), Asaphes umbilicalis Xiao & Huang, 2000, Torymus prunicola (Huber, 1927), Notanisus oulmesiensis (Delucchi, 1962), Theocolax ingens Xiao & Huang, 2001, Sympiesis tschulensis Myartseva & Kurashev, 1991, Eurytoma maslovskii Nikol'skaya, 1945, Ophioneurus longiclavatus Viggiani, 1974, Pnigalio monilicornis (Zetterstedt, 1838), Aprostocetus grandii (Domenichini, 1965), Signiphora pulchra Girault, 1913, Torymus thompsoni Fyles, 1904, Elasmus albicoxa Howard, 1885, Lathromeris scutellaris Forster, 1856, Acerophagus citrinus (Howard, 1898), Encarsia clariscutellum (Girault, 1915), Phyllocoptes eupadi (Newkirk, 1984), Ditangium cerasi (Schumach.) Costantin & L.M.Dufour, Agromyzaphagus detrimentosus Gahan, 1912, Balcha indica (Mani & Kaul, 1973), Achrysocharoides maieri Shevtsova & Hansson, 2011, Argyresthia pruniella (Clerck, 1759), Pristiphora biscalis (Foerster, 1854), Foveostroma drupacearum (Lév.) DiCosmo, Panellus ringens (Fr.) Romagn., Pristiphora monogyniae (Hartig, 1840), Sterictiphora angelicae (Panzer, 1799), Chrysocharis assis (Walker, 1839), Cosmocomoidea inexpectata (Huber, 1988), Eurytoma armenica Zerova & Fursov, 1991, Microterys iranicus Fallahzadeh & Japoshvili, 2010, Chrysozephyrus lingi Okano & Okura, 1969, Thecla martialis Herrich-Schäffer, 1864, Pionus tumultuosus (Tschudi, 1844), Geothlypis aequinoctialis (J.F.Gmelin, 1789), Arremon taciturnus (Hermann, 1783), Scaphytopius triangularis (DeLong, 1945))",
 "HasCoordinate is true",
 "HasGeospatialIssue is false"
 ]
}

 The dataset includes 145148 records from 1006 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0017080-250515123054153/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.15468/dl.kjv3an
title: Occurrence Download

description: A dataset containing 2300 species occurrences available in GBIF matching the query:
{
 "and" : [
 "Country is Colombia",
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "TaxonKey is Thunbergia alata Bojer ex Sims"
 ]
}

 The dataset includes 2300 records from 46 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0017084-250515123054153/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.15468/dl.js5sea
title: Occurrence Download

description: A dataset containing 769259 species occurrences available in GBIF matching the query:
{
 "and" : [
 "TaxonKey is one of (Ribautodelphax imitans (Ribaut, 1953), Forcipata loca (DeLong & Caldwell, 1936), Anusia nasicornis Forster, 1860, Tetramesa motschulskyi Narendran, 1994, Mesopolobus pseudolaticornis Rosen, 1966, Euplectrus comstockii Howard, 1880, Physothorax bidentulus Burks, 1969, Conidarnes sulcata Farache & Rasplus, 2015, Micranisa ralianga Mathew & Balakrishnan, 1981, Eupristina altissima Balakrishnan & Abdurahiman, 1981, Heterandrium brevicaude (Mayr, 1885), Megalaima henricii (Temminck, 1831), Rattus andamanensis (Blyth, 1860), Megalaima faiostricta (Temminck, 1832), Cerasophila thompsoni Bingham, 1900, Pycnonotus aurigaster (Vieillot, 1818), Pycnonotus flavescens Blyth, 1845, Aethopyga siparaja (Raffles, 1822), Megalaima virens (Boddaert, 1783), Rattus sikkimensis Hinton, 1919, Pycnonotus flaviventris (Tickell, 1833), Dicaeum chrysorrheum Temminck, 1829, Pycnonotus finlaysoni Strickland, 1844, Ampeliceps coronatus Blyth, 1842, Coracina melaschistos (Hodgson, 1836), Hemixos flavala Blyth, 1845, Megalaima incognita Hume, 1874, Anorrhinus austeni Jerdon, 1872, Eumyias thalassinus (Swainson, 1838), Iole propinqua (Oustalet, 1903), Megalaima australis (Horsfield, 1821), Alophoixus pallidus (Swinhoe, 1870), Anthracoceros albirostris (Shaw, 1808), Pycnonotus xanthorrhous Anderson, 1869, Rhyticeros undulatus (Shaw, 1812), Dicaeum cruentatum (Linnaeus, 1758), Dicaeum minullum Swinhoe, 1870, Ratufa bicolor (Sparrman, 1778), Arctictis binturong (Raffles, 1821), Callosciurus finlaysonii (Horsfield, 1823), Tamiops mcclellandii (Horsfield, 1840), Menetes berdmorei (Blyth, 1849), Tupaia belangeri (Wagner, 1841), Gracula religiosa Linnaeus, 1758, Nomascus gabriellae (Thomas, 1909), Leopoldamys sabanus (Thomas, 1887), Irena puella (Latham, 1790), Azochis rufidiscalis Hampson, 1904, Philiris innotatus (Miskin, 1874), Corvus macrorhynchos culminatus)",
 "HasCoordinate is true",
 "HasGeospatialIssue is false"
 ]
}

 The dataset includes 769259 records from 192 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0017082-250515123054153/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.99047.v1/t24
title: "Figure 8, (bottom, pp 200GeV exp)" of "Measurements of $\phi$ meson production in relativistic heavy-ion collisions at RHIC"

description: Masses and widths (FWHMs) of $\phi$ as a function of $p_{T}$ in p + p 200 GeV (NSD), d + Au 200 GeV (0–20$\%$), Au + Au 62.4 GeV (0–20$\%$), and Au + Au 200 GeV (0–5$\%$) collisions, with the corresponding $PDG$ values.
description: BNL-RHIC. We present results for the measurement of $\phi$ meson production via its charged kaon decay channel $\phi$ → $K^{+}K^{-}$ in Au + Au collisions at $\sqrt{s_{NN}} = 62.4, 130,$ and $200 GeV$, and in p + p and d + Au collisions at $\sqrt{s_{NN}} = 200 GeV$ from the STAR experiment at the BNL Relativistic Heavy Ion Collider (RHIC). The midrapidity (|y| &lt; 0.5) $\phi$ meson transverse momentum ($p_{T}$) spectra in central Au + Au collisions are found to be well described by a single exponential distribution. On the other hand, the $p_{T}$ spectra from p + p, d + Au, and peripheral Au + Au collisions show power-law tails at intermediate and high pT and are described better by Levy distributions. The constant $\phi/K^{-}$ yield ratio vs beam species, collision centrality, and colliding energy is in contradiction with expectations from models having kaon coalescence as the dominant mechanism for $\phi$ production at RHIC. The $\Omega/\phi$ yield ratio as a function of $p_{T}$ is consistent with a model based on the recombination of thermal s quarks up to $p_{T}$ ∼ 4 GeV/c, but disagrees at higher transverse momenta. The measured nuclear modification factor, RdAu, for the $\phi$ meson increases above unity at intermediate $p_{T}$ , similar to that for pions and protons, while $R_{AA}$ is suppressed due to the energy loss effect in central Au + Au collisions. Number of constituent quark scaling of both $R_{cp}$ and $v_{2}$ for the $\phi$ meson with respect to other hadrons in Au + Au collisions at $\sqrt{s_{NN}} = 200 GeV$ at intermediate $p_{T}$ is observed. These observations support quark coalescence as being the dominant mechanism of hadronization in the intermediate $p_{T}$ region at RHIC.
DOI: 10.17182/hepdata.99047.v1/t25
title: "Figure 8, (bottom, pp 200GeV MC)" of "Measurements of $\phi$ meson production in relativistic heavy-ion collisions at RHIC"

description: Masses and widths (FWHMs) of $\phi$ as a function of $p_{T}$ in p + p 200 GeV (NSD), d + Au 200 GeV (0–20$\%$), Au + Au 62.4 GeV (0–20$\%$), and Au + Au 200 GeV (0–5$\%$) collisions, with the corresponding $PDG$ values.
description: BNL-RHIC. We present results for the measurement of $\phi$ meson production via its charged kaon decay channel $\phi$ → $K^{+}K^{-}$ in Au + Au collisions at $\sqrt{s_{NN}} = 62.4, 130,$ and $200 GeV$, and in p + p and d + Au collisions at $\sqrt{s_{NN}} = 200 GeV$ from the STAR experiment at the BNL Relativistic Heavy Ion Collider (RHIC). The midrapidity (|y| &lt; 0.5) $\phi$ meson transverse momentum ($p_{T}$) spectra in central Au + Au collisions are found to be well described by a single exponential distribution. On the other hand, the $p_{T}$ spectra from p + p, d + Au, and peripheral Au + Au collisions show power-law tails at intermediate and high pT and are described better by Levy distributions. The constant $\phi/K^{-}$ yield ratio vs beam species, collision centrality, and colliding energy is in contradiction with expectations from models having kaon coalescence as the dominant mechanism for $\phi$ production at RHIC. The $\Omega/\phi$ yield ratio as a function of $p_{T}$ is consistent with a model based on the recombination of thermal s quarks up to $p_{T}$ ∼ 4 GeV/c, but disagrees at higher transverse momenta. The measured nuclear modification factor, RdAu, for the $\phi$ meson increases above unity at intermediate $p_{T}$ , similar to that for pions and protons, while $R_{AA}$ is suppressed due to the energy loss effect in central Au + Au collisions. Number of constituent quark scaling of both $R_{cp}$ and $v_{2}$ for the $\phi$ meson with respect to other hadrons in Au + Au collisions at $\sqrt{s_{NN}} = 200 GeV$ at intermediate $p_{T}$ is observed. These observations support quark coalescence as being the dominant mechanism of hadronization in the intermediate $p_{T}$ region at RHIC.
DOI: 10.17182/hepdata.99047.v1/t26
title: "Figure 9, p+p 200GeV Exp.data" of "Measurements of $\phi$ meson production in relativistic heavy-ion collisions at RHIC"

description: Invariant mass distributions of $\phi$ meson at 0.6 &lt; $p_{T}$ &lt; 1.0 GeV/c in p + p 200 GeV (NSD) and Au + Au 200 GeV (0–5$\%$) collisions. Solid symbols: experimental data. Open symbols: MC simulation. Curves are the results of a Breit-Wigner function fit. Note: Two sets of MC data are shown for Au + Au 200 GeV, and see text for details.
description: BNL-RHIC. We present results for the measurement of $\phi$ meson production via its charged kaon decay channel $\phi$ → $K^{+}K^{-}$ in Au + Au collisions at $\sqrt{s_{NN}} = 62.4, 130,$ and $200 GeV$, and in p + p and d + Au collisions at $\sqrt{s_{NN}} = 200 GeV$ from the STAR experiment at the BNL Relativistic Heavy Ion Collider (RHIC). The midrapidity (|y| &lt; 0.5) $\phi$ meson transverse momentum ($p_{T}$) spectra in central Au + Au collisions are found to be well described by a single exponential distribution. On the other hand, the $p_{T}$ spectra from p + p, d + Au, and peripheral Au + Au collisions show power-law tails at intermediate and high pT and are described better by Levy distributions. The constant $\phi/K^{-}$ yield ratio vs beam species, collision centrality, and colliding energy is in contradiction with expectations from models having kaon coalescence as the dominant mechanism for $\phi$ production at RHIC. The $\Omega/\phi$ yield ratio as a function of $p_{T}$ is consistent with a model based on the recombination of thermal s quarks up to $p_{T}$ ∼ 4 GeV/c, but disagrees at higher transverse momenta. The measured nuclear modification factor, RdAu, for the $\phi$ meson increases above unity at intermediate $p_{T}$ , similar to that for pions and protons, while $R_{AA}$ is suppressed due to the energy loss effect in central Au + Au collisions. Number of constituent quark scaling of both $R_{cp}$ and $v_{2}$ for the $\phi$ meson with respect to other hadrons in Au + Au collisions at $\sqrt{s_{NN}} = 200 GeV$ at intermediate $p_{T}$ is observed. These observations support quark coalescence as being the dominant mechanism of hadronization in the intermediate $p_{T}$ region at RHIC.
DOI: 10.17182/hepdata.99047.v1/t27
title: "Figure 9, p+p 200GeV MC.data" of "Measurements of $\phi$ meson production in relativistic heavy-ion collisions at RHIC"

description: Invariant mass distributions of $\phi$ meson at 0.6 &lt; $p_{T}$ &lt; 1.0 GeV/c in p + p 200 GeV (NSD) and Au + Au 200 GeV (0–5$\%$) collisions. Solid symbols: experimental data. Open symbols: MC simulation. Curves are the results of a Breit-Wigner function fit. Note: Two sets of MC data are shown for Au + Au 200 GeV, and see text for details.
description: BNL-RHIC. We present results for the measurement of $\phi$ meson production via its charged kaon decay channel $\phi$ → $K^{+}K^{-}$ in Au + Au collisions at $\sqrt{s_{NN}} = 62.4, 130,$ and $200 GeV$, and in p + p and d + Au collisions at $\sqrt{s_{NN}} = 200 GeV$ from the STAR experiment at the BNL Relativistic Heavy Ion Collider (RHIC). The midrapidity (|y| &lt; 0.5) $\phi$ meson transverse momentum ($p_{T}$) spectra in central Au + Au collisions are found to be well described by a single exponential distribution. On the other hand, the $p_{T}$ spectra from p + p, d + Au, and peripheral Au + Au collisions show power-law tails at intermediate and high pT and are described better by Levy distributions. The constant $\phi/K^{-}$ yield ratio vs beam species, collision centrality, and colliding energy is in contradiction with expectations from models having kaon coalescence as the dominant mechanism for $\phi$ production at RHIC. The $\Omega/\phi$ yield ratio as a function of $p_{T}$ is consistent with a model based on the recombination of thermal s quarks up to $p_{T}$ ∼ 4 GeV/c, but disagrees at higher transverse momenta. The measured nuclear modification factor, RdAu, for the $\phi$ meson increases above unity at intermediate $p_{T}$ , similar to that for pions and protons, while $R_{AA}$ is suppressed due to the energy loss effect in central Au + Au collisions. Number of constituent quark scaling of both $R_{cp}$ and $v_{2}$ for the $\phi$ meson with respect to other hadrons in Au + Au collisions at $\sqrt{s_{NN}} = 200 GeV$ at intermediate $p_{T}$ is observed. These observations support quark coalescence as being the dominant mechanism of hadronization in the intermediate $p_{T}$ region at RHIC.
DOI: 10.17182/hepdata.99047.v1/t28
title: "Figure 9, Au+Au 200GeV Exp.data" of "Measurements of $\phi$ meson production in relativistic heavy-ion collisions at RHIC"

description: Invariant mass distributions of $\phi$ meson at 0.6 &lt; $p_{T}$ &lt; 1.0 GeV/c in p + p 200 GeV (NSD) and Au + Au 200 GeV (0–5$\%$) collisions. Solid symbols: experimental data. Open symbols: MC simulation. Curves are the results of a Breit-Wigner function fit. Note: Two sets of MC data are shown for Au + Au 200 GeV, and see text for details.
description: BNL-RHIC. We present results for the measurement of $\phi$ meson production via its charged kaon decay channel $\phi$ → $K^{+}K^{-}$ in Au + Au collisions at $\sqrt{s_{NN}} = 62.4, 130,$ and $200 GeV$, and in p + p and d + Au collisions at $\sqrt{s_{NN}} = 200 GeV$ from the STAR experiment at the BNL Relativistic Heavy Ion Collider (RHIC). The midrapidity (|y| &lt; 0.5) $\phi$ meson transverse momentum ($p_{T}$) spectra in central Au + Au collisions are found to be well described by a single exponential distribution. On the other hand, the $p_{T}$ spectra from p + p, d + Au, and peripheral Au + Au collisions show power-law tails at intermediate and high pT and are described better by Levy distributions. The constant $\phi/K^{-}$ yield ratio vs beam species, collision centrality, and colliding energy is in contradiction with expectations from models having kaon coalescence as the dominant mechanism for $\phi$ production at RHIC. The $\Omega/\phi$ yield ratio as a function of $p_{T}$ is consistent with a model based on the recombination of thermal s quarks up to $p_{T}$ ∼ 4 GeV/c, but disagrees at higher transverse momenta. The measured nuclear modification factor, RdAu, for the $\phi$ meson increases above unity at intermediate $p_{T}$ , similar to that for pions and protons, while $R_{AA}$ is suppressed due to the energy loss effect in central Au + Au collisions. Number of constituent quark scaling of both $R_{cp}$ and $v_{2}$ for the $\phi$ meson with respect to other hadrons in Au + Au collisions at $\sqrt{s_{NN}} = 200 GeV$ at intermediate $p_{T}$ is observed. These observations support quark coalescence as being the dominant mechanism of hadronization in the intermediate $p_{T}$ region at RHIC.
DOI: 10.17182/hepdata.99047.v1/t29
title: "Figure 9, Au+Au 200GeV MC(1).data" of "Measurements of $\phi$ meson production in relativistic heavy-ion collisions at RHIC"

description: Invariant mass distributions of $\phi$ meson at 0.6 &lt; $p_{T}$ &lt; 1.0 GeV/c in p + p 200 GeV (NSD) and Au + Au 200 GeV (0–5$\%$) collisions. Solid symbols: experimental data. Open symbols: MC simulation. Curves are the results of a Breit-Wigner function fit. Note: Two sets of MC data are shown for Au + Au 200 GeV, and see text for details.
description: BNL-RHIC. We present results for the measurement of $\phi$ meson production via its charged kaon decay channel $\phi$ → $K^{+}K^{-}$ in Au + Au collisions at $\sqrt{s_{NN}} = 62.4, 130,$ and $200 GeV$, and in p + p and d + Au collisions at $\sqrt{s_{NN}} = 200 GeV$ from the STAR experiment at the BNL Relativistic Heavy Ion Collider (RHIC). The midrapidity (|y| &lt; 0.5) $\phi$ meson transverse momentum ($p_{T}$) spectra in central Au + Au collisions are found to be well described by a single exponential distribution. On the other hand, the $p_{T}$ spectra from p + p, d + Au, and peripheral Au + Au collisions show power-law tails at intermediate and high pT and are described better by Levy distributions. The constant $\phi/K^{-}$ yield ratio vs beam species, collision centrality, and colliding energy is in contradiction with expectations from models having kaon coalescence as the dominant mechanism for $\phi$ production at RHIC. The $\Omega/\phi$ yield ratio as a function of $p_{T}$ is consistent with a model based on the recombination of thermal s quarks up to $p_{T}$ ∼ 4 GeV/c, but disagrees at higher transverse momenta. The measured nuclear modification factor, RdAu, for the $\phi$ meson increases above unity at intermediate $p_{T}$ , similar to that for pions and protons, while $R_{AA}$ is suppressed due to the energy loss effect in central Au + Au collisions. Number of constituent quark scaling of both $R_{cp}$ and $v_{2}$ for the $\phi$ meson with respect to other hadrons in Au + Au collisions at $\sqrt{s_{NN}} = 200 GeV$ at intermediate $p_{T}$ is observed. These observations support quark coalescence as being the dominant mechanism of hadronization in the intermediate $p_{T}$ region at RHIC.
DOI: 10.3535/a41-bxy-kgr
title: Dianella ensifolia (L.) Redouté

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/yx9-n2l-mrt
title: Hydrocotyle L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.99047.v1/t30
title: "Figure 9, Au+Au 200GeV MC(2).data" of "Measurements of $\phi$ meson production in relativistic heavy-ion collisions at RHIC"

description: Invariant mass distributions of $\phi$ meson at 0.6 &lt; $p_{T}$ &lt; 1.0 GeV/c in p + p 200 GeV (NSD) and Au + Au 200 GeV (0–5$\%$) collisions. Solid symbols: experimental data. Open symbols: MC simulation. Curves are the results of a Breit-Wigner function fit. Note: Two sets of MC data are shown for Au + Au 200 GeV, and see text for details.
description: BNL-RHIC. We present results for the measurement of $\phi$ meson production via its charged kaon decay channel $\phi$ → $K^{+}K^{-}$ in Au + Au collisions at $\sqrt{s_{NN}} = 62.4, 130,$ and $200 GeV$, and in p + p and d + Au collisions at $\sqrt{s_{NN}} = 200 GeV$ from the STAR experiment at the BNL Relativistic Heavy Ion Collider (RHIC). The midrapidity (|y| &lt; 0.5) $\phi$ meson transverse momentum ($p_{T}$) spectra in central Au + Au collisions are found to be well described by a single exponential distribution. On the other hand, the $p_{T}$ spectra from p + p, d + Au, and peripheral Au + Au collisions show power-law tails at intermediate and high pT and are described better by Levy distributions. The constant $\phi/K^{-}$ yield ratio vs beam species, collision centrality, and colliding energy is in contradiction with expectations from models having kaon coalescence as the dominant mechanism for $\phi$ production at RHIC. The $\Omega/\phi$ yield ratio as a function of $p_{T}$ is consistent with a model based on the recombination of thermal s quarks up to $p_{T}$ ∼ 4 GeV/c, but disagrees at higher transverse momenta. The measured nuclear modification factor, RdAu, for the $\phi$ meson increases above unity at intermediate $p_{T}$ , similar to that for pions and protons, while $R_{AA}$ is suppressed due to the energy loss effect in central Au + Au collisions. Number of constituent quark scaling of both $R_{cp}$ and $v_{2}$ for the $\phi$ meson with respect to other hadrons in Au + Au collisions at $\sqrt{s_{NN}} = 200 GeV$ at intermediate $p_{T}$ is observed. These observations support quark coalescence as being the dominant mechanism of hadronization in the intermediate $p_{T}$ region at RHIC.
DOI: 10.17182/hepdata.99047.v1/t31
title: "Figure 10, table (a)" of "Measurements of $\phi$ meson production in relativistic heavy-ion collisions at RHIC"

description: $\phi$ meson transverse mass distributions for different collision systems and different energies. For clarity, distributions for some centrality bins have been scaled by factors indicated in the figure. Curves represent the exponential (solid) and Levy (dashed) function fits to the distributions. Error bars are statistical only. Note that a scale factor of 1.09 is applied to the $\phi$ meson spectra for Au + Au collisions at 200 GeV in Ref. [50] to correct for the kaon identification efficiency effect missed previously.
description: BNL-RHIC. We present results for the measurement of $\phi$ meson production via its charged kaon decay channel $\phi$ → $K^{+}K^{-}$ in Au + Au collisions at $\sqrt{s_{NN}} = 62.4, 130,$ and $200 GeV$, and in p + p and d + Au collisions at $\sqrt{s_{NN}} = 200 GeV$ from the STAR experiment at the BNL Relativistic Heavy Ion Collider (RHIC). The midrapidity (|y| &lt; 0.5) $\phi$ meson transverse momentum ($p_{T}$) spectra in central Au + Au collisions are found to be well described by a single exponential distribution. On the other hand, the $p_{T}$ spectra from p + p, d + Au, and peripheral Au + Au collisions show power-law tails at intermediate and high pT and are described better by Levy distributions. The constant $\phi/K^{-}$ yield ratio vs beam species, collision centrality, and colliding energy is in contradiction with expectations from models having kaon coalescence as the dominant mechanism for $\phi$ production at RHIC. The $\Omega/\phi$ yield ratio as a function of $p_{T}$ is consistent with a model based on the recombination of thermal s quarks up to $p_{T}$ ∼ 4 GeV/c, but disagrees at higher transverse momenta. The measured nuclear modification factor, RdAu, for the $\phi$ meson increases above unity at intermediate $p_{T}$ , similar to that for pions and protons, while $R_{AA}$ is suppressed due to the energy loss effect in central Au + Au collisions. Number of constituent quark scaling of both $R_{cp}$ and $v_{2}$ for the $\phi$ meson with respect to other hadrons in Au + Au collisions at $\sqrt{s_{NN}} = 200 GeV$ at intermediate $p_{T}$ is observed. These observations support quark coalescence as being the dominant mechanism of hadronization in the intermediate $p_{T}$ region at RHIC.