cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.98621.v1/t4
title: "Figure 3 down" of "Measurements of transverse energy distributions in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Upper plot: points are measured $p/E_{tower}$ electron peak position as a function of the distance to the center of the tower. The solid line is from a calculation based on a full GEANT simulation of the detector response to electrons. Lower plot: points show measured energy deposited by electrons in the tower as a function of the momentum for distances to the center of the tower smaller than 2.0 cm. The first point is the electron equivalent energy of the minimum ionizing particles. The solid line is a second order polynomial fit of the data.
description: Transverse energy ($E_{T}$) distributions have been measured for Au+Au collisions at $sqrt{s_{NN}}$=200 GeV by the STAR collaboration at RHIC. $E_{T}$ is constructed from its hadronic and electromagnetic components, which have been measured separately. $E_{T}$ production for the most central collisions is well described by several theoretical models whose common feature is large energy density achieved early in the fireball evolution. The magnitude and centrality dependence of $E_{T}$ per charged particle agrees well with measurements at lower collision energy, indicating that the growth in $E_{T}$ for larger collision energy results from the growth in particle production. The electromagnetic fraction of the total $E_{T}$ is consistent with a final state dominated by mesons and independent of centrality.
DOI: 10.17182/hepdata.98621.v1/t5
title: "Figure 4" of "Measurements of transverse energy distributions in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Mean values from GEANT simulations of the energy deposited in the EMC by various hadronic species as a function of momentum.
description: Transverse energy ($E_{T}$) distributions have been measured for Au+Au collisions at $sqrt{s_{NN}}$=200 GeV by the STAR collaboration at RHIC. $E_{T}$ is constructed from its hadronic and electromagnetic components, which have been measured separately. $E_{T}$ production for the most central collisions is well described by several theoretical models whose common feature is large energy density achieved early in the fireball evolution. The magnitude and centrality dependence of $E_{T}$ per charged particle agrees well with measurements at lower collision energy, indicating that the growth in $E_{T}$ for larger collision energy results from the growth in particle production. The electromagnetic fraction of the total $E_{T}$ is consistent with a final state dominated by mesons and independent of centrality.
DOI: 10.17182/hepdata.98621.v1/t6
title: "Figure 5" of "Measurements of transverse energy distributions in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Spatial profiles of energy deposition in the EMC as a function of distance ($d$) from the hit point to the center of the tower for $\pi^{+}$ and $\pi^{-}$ from simulations and for positive and negative hadrons from data. The arrow indicates the distance corresponding to the border of a tower in 0 &lt; $\eta$ &lt; 0.2. An overall agreement between the shapes of the profiles is observed, with a small normalization difference.
description: Transverse energy ($E_{T}$) distributions have been measured for Au+Au collisions at $sqrt{s_{NN}}$=200 GeV by the STAR collaboration at RHIC. $E_{T}$ is constructed from its hadronic and electromagnetic components, which have been measured separately. $E_{T}$ production for the most central collisions is well described by several theoretical models whose common feature is large energy density achieved early in the fireball evolution. The magnitude and centrality dependence of $E_{T}$ per charged particle agrees well with measurements at lower collision energy, indicating that the growth in $E_{T}$ for larger collision energy results from the growth in particle production. The electromagnetic fraction of the total $E_{T}$ is consistent with a final state dominated by mesons and independent of centrality.
DOI: 10.3535/v5d-jhf-rl5
title: Syzygium Gaertn.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.15468/dl.88hvrr
title: Occurrence Download

description: A dataset containing 1722 species occurrences available in GBIF matching the query:
{
 "and" : [
 "Geometry POLYGON((-70.9492 42.23059,-70.9492 42.3026,-71.04698 42.3026,-71.04698 42.23059,-70.9492 42.23059))",
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "OccurrenceStatus is Present",
 "TaxonKey is Magnoliopsida"
 ]
}

 The dataset includes 1722 records from 19 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015844-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.98621.v1/t10
title: "Figure 8 down" of "Measurements of transverse energy distributions in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: ⟨$dE_{T}/d\eta|_{\eta=0.5}$⟩ per $N_{part}$ pair vs. $N_{part}$. Upper panel: $N_{part}$ is obtained from Monte Carlo Glauber calculations. The lines show calculations using the HIJING model [27](solid), the EKRT saturation model [7] (dotted, Eq. 8) and the two component fit (dashed, see text). Results from WA98 [14] and PHENIX [15] are also shown. The grey bands correspond to overall systematic uncertainties, independent of $N_{part}$. Error bars are the quadrature sum of the errors on the measurements and the uncertainties on $N_{part}$ calculation. Lower panel: the same data are shown as in the upper panel but using and Optical Glauber model calculation for $N_{part}$. The line shows the same result from EKRT model calculation.
description: Transverse energy ($E_{T}$) distributions have been measured for Au+Au collisions at $sqrt{s_{NN}}$=200 GeV by the STAR collaboration at RHIC. $E_{T}$ is constructed from its hadronic and electromagnetic components, which have been measured separately. $E_{T}$ production for the most central collisions is well described by several theoretical models whose common feature is large energy density achieved early in the fireball evolution. The magnitude and centrality dependence of $E_{T}$ per charged particle agrees well with measurements at lower collision energy, indicating that the growth in $E_{T}$ for larger collision energy results from the growth in particle production. The electromagnetic fraction of the total $E_{T}$ is consistent with a final state dominated by mesons and independent of centrality.
DOI: 10.17182/hepdata.98621.v1/t11
title: "Figure 9" of "Measurements of transverse energy distributions in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: $dE_{T}/dy$ (see text for details) per $N_{part}$ pair vs $sqrt{s_{NN}}$ for central events. In this figure $dE_{T}/dy/(0.5N_{part})$ is seen to grow logarithmicaly with $sqrt{s_{NN}}$. The error bar in the STAR point represents the total systematic uncertainty. The solid line is a EKRT model prediction [7], corrected for $d\eta/dy$, for central Au+Au collisions.
description: Transverse energy ($E_{T}$) distributions have been measured for Au+Au collisions at $sqrt{s_{NN}}$=200 GeV by the STAR collaboration at RHIC. $E_{T}$ is constructed from its hadronic and electromagnetic components, which have been measured separately. $E_{T}$ production for the most central collisions is well described by several theoretical models whose common feature is large energy density achieved early in the fireball evolution. The magnitude and centrality dependence of $E_{T}$ per charged particle agrees well with measurements at lower collision energy, indicating that the growth in $E_{T}$ for larger collision energy results from the growth in particle production. The electromagnetic fraction of the total $E_{T}$ is consistent with a final state dominated by mesons and independent of centrality.
DOI: 10.17182/hepdata.98621.v1/t12
title: "Figure 10 up" of "Measurements of transverse energy distributions in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Upper panel - ⟨$dE_{T}/d\eta⟩/⟨dN_{ch}/d\eta$⟩ vs $N_{part}$. Predictions from HIJING simulations for Au+Au at 200 GeV are presented. Results from WA98 [14] and PHENIX [15] are also shown. The grey band corresponds to an overall normalization uncertainty for the STAR measurement. Bottom panel - Charged hadrons mean transverse momentum as a function of $N_{part}$ [37].
description: Transverse energy ($E_{T}$) distributions have been measured for Au+Au collisions at $sqrt{s_{NN}}$=200 GeV by the STAR collaboration at RHIC. $E_{T}$ is constructed from its hadronic and electromagnetic components, which have been measured separately. $E_{T}$ production for the most central collisions is well described by several theoretical models whose common feature is large energy density achieved early in the fireball evolution. The magnitude and centrality dependence of $E_{T}$ per charged particle agrees well with measurements at lower collision energy, indicating that the growth in $E_{T}$ for larger collision energy results from the growth in particle production. The electromagnetic fraction of the total $E_{T}$ is consistent with a final state dominated by mesons and independent of centrality.
DOI: 10.17182/hepdata.98621.v1/t14
title: "Figure 11" of "Measurements of transverse energy distributions in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: ⟨$dE_{T}/d\eta⟩/⟨dN_{ch}/d\eta$⟩ vs $sqrt{s_{NN}}$ for central events. The error bar in the STAR point corresponds to the systematic uncertaintiy. A constant value of ∼ 800 MeV per charged particle, within errors, characterizes transverse energy production over this full energy range.
description: Transverse energy ($E_{T}$) distributions have been measured for Au+Au collisions at $sqrt{s_{NN}}$=200 GeV by the STAR collaboration at RHIC. $E_{T}$ is constructed from its hadronic and electromagnetic components, which have been measured separately. $E_{T}$ production for the most central collisions is well described by several theoretical models whose common feature is large energy density achieved early in the fireball evolution. The magnitude and centrality dependence of $E_{T}$ per charged particle agrees well with measurements at lower collision energy, indicating that the growth in $E_{T}$ for larger collision energy results from the growth in particle production. The electromagnetic fraction of the total $E_{T}$ is consistent with a final state dominated by mesons and independent of centrality.
DOI: 10.17182/hepdata.98621.v1/t7
title: "Figure 6" of "Measurements of transverse energy distributions in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Event-by-event ratio of the reconstructed electromagnetic energy for the most central events. The solid line is a gaussian fit.
description: Transverse energy ($E_{T}$) distributions have been measured for Au+Au collisions at $sqrt{s_{NN}}$=200 GeV by the STAR collaboration at RHIC. $E_{T}$ is constructed from its hadronic and electromagnetic components, which have been measured separately. $E_{T}$ production for the most central collisions is well described by several theoretical models whose common feature is large energy density achieved early in the fireball evolution. The magnitude and centrality dependence of $E_{T}$ per charged particle agrees well with measurements at lower collision energy, indicating that the growth in $E_{T}$ for larger collision energy results from the growth in particle production. The electromagnetic fraction of the total $E_{T}$ is consistent with a final state dominated by mesons and independent of centrality.
DOI: 10.17182/hepdata.98621.v1/t8
title: "Figure 7" of "Measurements of transverse energy distributions in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Total Transverse Energy for 0 &lt; $\eta$ &lt; 1. The minimum bias distribution is presented as well as the distributions for the different centrality bins (see table III). The shaded area corresponds to the 5% most central bin. The main axis scale corresponds to the $E_{T}$ measured in the detector acceptance and the bottom axis is corrected to represent the extrapolation to full azimuthal acceptance.
description: Transverse energy ($E_{T}$) distributions have been measured for Au+Au collisions at $sqrt{s_{NN}}$=200 GeV by the STAR collaboration at RHIC. $E_{T}$ is constructed from its hadronic and electromagnetic components, which have been measured separately. $E_{T}$ production for the most central collisions is well described by several theoretical models whose common feature is large energy density achieved early in the fireball evolution. The magnitude and centrality dependence of $E_{T}$ per charged particle agrees well with measurements at lower collision energy, indicating that the growth in $E_{T}$ for larger collision energy results from the growth in particle production. The electromagnetic fraction of the total $E_{T}$ is consistent with a final state dominated by mesons and independent of centrality.
DOI: 10.17182/hepdata.98621.v1/t9
title: "Figure 8 up" of "Measurements of transverse energy distributions in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: ⟨$dE_{T}/d\eta|_{\eta=0.5}$⟩ per $N_{part}$ pair vs. $N_{part}$. Upper panel: $N_{part}$ is obtained from Monte Carlo Glauber calculations. The lines show calculations using the HIJING model [27](solid), the EKRT saturation model [7] (dotted, Eq. 8) and the two component fit (dashed, see text). Results from WA98 [14] and PHENIX [15] are also shown. The grey bands correspond to overall systematic uncertainties, independent of $N_{part}$. Error bars are the quadrature sum of the errors on the measurements and the uncertainties on $N_{part}$ calculation. Lower panel: the same data are shown as in the upper panel but using and Optical Glauber model calculation for $N_{part}$. The line shows the same result from EKRT model calculation.
description: Transverse energy ($E_{T}$) distributions have been measured for Au+Au collisions at $sqrt{s_{NN}}$=200 GeV by the STAR collaboration at RHIC. $E_{T}$ is constructed from its hadronic and electromagnetic components, which have been measured separately. $E_{T}$ production for the most central collisions is well described by several theoretical models whose common feature is large energy density achieved early in the fireball evolution. The magnitude and centrality dependence of $E_{T}$ per charged particle agrees well with measurements at lower collision energy, indicating that the growth in $E_{T}$ for larger collision energy results from the growth in particle production. The electromagnetic fraction of the total $E_{T}$ is consistent with a final state dominated by mesons and independent of centrality.
DOI: 10.3535/jaw-hj8-kyx
title: Callicarpa L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/rkq-1b1-54y
title: Gladiolus palustris Gaudin

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.98621.v1/t13
title: "Figure 10 down" of "Measurements of transverse energy distributions in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Upper panel - ⟨$dE_{T}/d\eta⟩/⟨dN_{ch}/d\eta$⟩ vs $N_{part}$. Predictions from HIJING simulations for Au+Au at 200 GeV are presented. Results from WA98 [14] and PHENIX [15] are also shown. The grey band corresponds to an overall normalization uncertainty for the STAR measurement. Bottom panel - Charged hadrons mean transverse momentum as a function of $N_{part}$ [37].
description: Transverse energy ($E_{T}$) distributions have been measured for Au+Au collisions at $sqrt{s_{NN}}$=200 GeV by the STAR collaboration at RHIC. $E_{T}$ is constructed from its hadronic and electromagnetic components, which have been measured separately. $E_{T}$ production for the most central collisions is well described by several theoretical models whose common feature is large energy density achieved early in the fireball evolution. The magnitude and centrality dependence of $E_{T}$ per charged particle agrees well with measurements at lower collision energy, indicating that the growth in $E_{T}$ for larger collision energy results from the growth in particle production. The electromagnetic fraction of the total $E_{T}$ is consistent with a final state dominated by mesons and independent of centrality.
DOI: 10.17182/hepdata.98621.v1/t15
title: "Figure 12" of "Measurements of transverse energy distributions in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Energy dependence of the electromagnetic fraction of the transverse energy for a number of systems spanning SPS to RHIC energy for central events.
description: Transverse energy ($E_{T}$) distributions have been measured for Au+Au collisions at $sqrt{s_{NN}}$=200 GeV by the STAR collaboration at RHIC. $E_{T}$ is constructed from its hadronic and electromagnetic components, which have been measured separately. $E_{T}$ production for the most central collisions is well described by several theoretical models whose common feature is large energy density achieved early in the fireball evolution. The magnitude and centrality dependence of $E_{T}$ per charged particle agrees well with measurements at lower collision energy, indicating that the growth in $E_{T}$ for larger collision energy results from the growth in particle production. The electromagnetic fraction of the total $E_{T}$ is consistent with a final state dominated by mesons and independent of centrality.
DOI: 10.17182/hepdata.98621.v1/t16
title: "Figure 13" of "Measurements of transverse energy distributions in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Participant number dependence of the electromagnetic fraction of the total transverse energy. The results are consistent with HIJING within errors over the full centrality range.
description: Transverse energy ($E_{T}$) distributions have been measured for Au+Au collisions at $sqrt{s_{NN}}$=200 GeV by the STAR collaboration at RHIC. $E_{T}$ is constructed from its hadronic and electromagnetic components, which have been measured separately. $E_{T}$ production for the most central collisions is well described by several theoretical models whose common feature is large energy density achieved early in the fireball evolution. The magnitude and centrality dependence of $E_{T}$ per charged particle agrees well with measurements at lower collision energy, indicating that the growth in $E_{T}$ for larger collision energy results from the growth in particle production. The electromagnetic fraction of the total $E_{T}$ is consistent with a final state dominated by mesons and independent of centrality.
DOI: 10.17182/hepdata.98622.v1/t1
title: "Figure 2" of "Directed and elliptic flow of charged particles in Cu+Cu collisions at $\sqrt{\bm {s_{NN}}} =$ 22.4 GeV"

description: The event plane resolution measured using the TPC (second order) and using the BBC (first order) are shown as a function of collision centrality for Cu+Cu collisions at $\sqrt{s_{NN}}$ = 22.4 GeV. Errors are statistical only.
description: This paper reports results for directed flow $v_{1}$ and elliptic flow $v_{2}$ of charged particles in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 22.4 GeV at the Relativistic Heavy Ion Collider. The measurements are for the 0-60% most central collisions, using charged particles observed in the STAR detector. Our measurements extend to 22.4 GeV Cu+Cu collisions the prior observation that $v_{1}$ is independent of the system size at 62.4 and 200 GeV, and also extend the scaling of $v_{1}$ with $\eta/y_{beam}$ to this system. The measured $v_{2}(p_{T})$ in Cu+Cu collisions is similar for $\sqrt{s_{NN}}$ = 22.4−200 GeV. We also report a comparison with results from transport model (UrQMD and AMPT) calculations. The model results do not agree quantitatively with the measured $v_{1}(\eta)$, $v_{2}(p_{T})$ and $v_{2}(\eta)$.
DOI: 10.17182/hepdata.98622.v1/t2
title: "Figure 3" of "Directed and elliptic flow of charged particles in Cu+Cu collisions at $\sqrt{\bm {s_{NN}}} =$ 22.4 GeV"

description: Charged hadron $v_{1}${BBC} vs. $\eta$ for 0-60% centrality Cu+Cu collisions at $\sqrt{s_{NN}}$ = 22.4 GeV. The errors shown are statistical. Systematic errors are discussed in Section III.C. Results are compared to $v_{1}$ from 0-40% centrality Au+Au collisions at $\sqrt{s_{NN}}$ = 19.6 GeV from the PHOBOS collaboration [10].
description: This paper reports results for directed flow $v_{1}$ and elliptic flow $v_{2}$ of charged particles in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 22.4 GeV at the Relativistic Heavy Ion Collider. The measurements are for the 0-60% most central collisions, using charged particles observed in the STAR detector. Our measurements extend to 22.4 GeV Cu+Cu collisions the prior observation that $v_{1}$ is independent of the system size at 62.4 and 200 GeV, and also extend the scaling of $v_{1}$ with $\eta/y_{beam}$ to this system. The measured $v_{2}(p_{T})$ in Cu+Cu collisions is similar for $\sqrt{s_{NN}}$ = 22.4−200 GeV. We also report a comparison with results from transport model (UrQMD and AMPT) calculations. The model results do not agree quantitatively with the measured $v_{1}(\eta)$, $v_{2}(p_{T})$ and $v_{2}(\eta)$.
DOI: 10.25549/vercoutere-ouc1sto1769229
title: Therapeutic Artworks

description: This collection includes over 900 pieces of art that were created by patients at the Atascadero State Hospital (ASH) in the mid-1950’s.  The artists were under the treatment of Albert R. Vercoutere who used the technique of providing photos from magazines for the patients to use as inspiration for their own artwork. Although not trained in the use of art therapy and during a time when art therapy was a new approach, Vercoutere often utilized art as a mechanism for working with his patients. The artwork was created during a time when psychotropic drugs were not yet available as treatment options for mental health patients.
DOI: 10.3535/1yt-8s7-2dg
title: Sida L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/kyq-awc-170
title: Scoparia dulcis L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.98622.v1/t3
title: "Figure 4" of "Directed and elliptic flow of charged particles in Cu+Cu collisions at $\sqrt{\bm {s_{NN}}} =$ 22.4 GeV"

description: Comparison of the measured $v_{1}${BBC} as a function of η in 0-60% Cu+Cu collisions at $\sqrt{s_{NN}}$ = 22.4 GeV with model predictions. The inset shows the central $\eta$ region in more detail. The errors are statistical only.
description: This paper reports results for directed flow $v_{1}$ and elliptic flow $v_{2}$ of charged particles in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 22.4 GeV at the Relativistic Heavy Ion Collider. The measurements are for the 0-60% most central collisions, using charged particles observed in the STAR detector. Our measurements extend to 22.4 GeV Cu+Cu collisions the prior observation that $v_{1}$ is independent of the system size at 62.4 and 200 GeV, and also extend the scaling of $v_{1}$ with $\eta/y_{beam}$ to this system. The measured $v_{2}(p_{T})$ in Cu+Cu collisions is similar for $\sqrt{s_{NN}}$ = 22.4−200 GeV. We also report a comparison with results from transport model (UrQMD and AMPT) calculations. The model results do not agree quantitatively with the measured $v_{1}(\eta)$, $v_{2}(p_{T})$ and $v_{2}(\eta)$.