cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.99752.v2/t2
title: "Figure 2" of "Single electron yields from semileptonic charm and bottom hadron decays in Au$+$Au collisions at $\sqrt{s_{NN}}=200$ GeV"

description: Bottom hadron election fraction with respect to heavy flavor electron as a function of $p_{T}$.
description: The PHENIX Collaboration at the Relativistic Heavy Ion Collider has measured open heavy-flavor production in minimum bias Au+Au collisions at $\sqrt{s_{NN}}=200$ GeV via the yields of electrons from semileptonic decays of charm and bottom hadrons. Previous heavy-flavor electron measurements indicated substantial modification in the momentum distribution of the parent heavy quarks due to the quark-gluon plasma created in these collisions. For the first time, using the PHENIX silicon vertex detector to measure precision displaced tracking, the relative contributions from charm and bottom hadrons to these electrons as a function of transverse momentum are measured in Au+Au collisions. We use the bottom electron fractions in Au+Au and p+p along with the previously measured heavy flavor electron $R_{AA}$ to calculate the $R_{AA}$ for electrons from charm and bottom hadron decays separately.
DOI: 10.17182/hepdata.99752.v2/t3
title: "Figure 3" of "Single electron yields from semileptonic charm and bottom hadron decays in Au$+$Au collisions at $\sqrt{s_{NN}}=200$ GeV"

description: Bottom and charm hadron $R_{AA}$ as a function of $p_{T}$.
description: The PHENIX Collaboration at the Relativistic Heavy Ion Collider has measured open heavy-flavor production in minimum bias Au+Au collisions at $\sqrt{s_{NN}}=200$ GeV via the yields of electrons from semileptonic decays of charm and bottom hadrons. Previous heavy-flavor electron measurements indicated substantial modification in the momentum distribution of the parent heavy quarks due to the quark-gluon plasma created in these collisions. For the first time, using the PHENIX silicon vertex detector to measure precision displaced tracking, the relative contributions from charm and bottom hadrons to these electrons as a function of transverse momentum are measured in Au+Au collisions. We use the bottom electron fractions in Au+Au and p+p along with the previously measured heavy flavor electron $R_{AA}$ to calculate the $R_{AA}$ for electrons from charm and bottom hadron decays separately.
DOI: 10.17182/hepdata.99752.v2/t4
title: "Figure 4" of "Single electron yields from semileptonic charm and bottom hadron decays in Au$+$Au collisions at $\sqrt{s_{NN}}=200$ GeV"

description: $(b\rightarrow e$ $R_{AA}) / (c\rightarrow e$ $R_{AA})$ as a function of $p_{T}$.
description: The PHENIX Collaboration at the Relativistic Heavy Ion Collider has measured open heavy-flavor production in minimum bias Au+Au collisions at $\sqrt{s_{NN}}=200$ GeV via the yields of electrons from semileptonic decays of charm and bottom hadrons. Previous heavy-flavor electron measurements indicated substantial modification in the momentum distribution of the parent heavy quarks due to the quark-gluon plasma created in these collisions. For the first time, using the PHENIX silicon vertex detector to measure precision displaced tracking, the relative contributions from charm and bottom hadrons to these electrons as a function of transverse momentum are measured in Au+Au collisions. We use the bottom electron fractions in Au+Au and p+p along with the previously measured heavy flavor electron $R_{AA}$ to calculate the $R_{AA}$ for electrons from charm and bottom hadron decays separately.
DOI: 10.17182/hepdata.99752.v3/t4
title: "Figure 4" of "Single electron yields from semileptonic charm and bottom hadron decays in Au$+$Au collisions at $\sqrt{s_{NN}}=200$ GeV"

description: $(b\rightarrow e$ $R_{AA}) / (c\rightarrow e$ $R_{AA})$ as a function of $p_{T}$.
description: The PHENIX Collaboration at the Relativistic Heavy Ion Collider has measured open heavy-flavor production in minimum bias Au+Au collisions at $\sqrt{s_{NN}}=200$ GeV via the yields of electrons from semileptonic decays of charm and bottom hadrons. Previous heavy-flavor electron measurements indicated substantial modification in the momentum distribution of the parent heavy quarks due to the quark-gluon plasma created in these collisions. For the first time, using the PHENIX silicon vertex detector to measure precision displaced tracking, the relative contributions from charm and bottom hadrons to these electrons as a function of transverse momentum are measured in Au+Au collisions. We use the bottom electron fractions in Au+Au and p+p along with the previously measured heavy flavor electron $R_{AA}$ to calculate the $R_{AA}$ for electrons from charm and bottom hadron decays separately.
DOI: 10.3535/cce-qlv-rlg
title: Dracaena bagamoyensis (N.E.Br.) Byng & Christenh.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/ttt-9gv-wpn
title: Syzygium Gaertn.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.99752.v1/t1
title: "Figure 1" of "Single electron yields from semileptonic charm and bottom hadron decays in Au$+$Au collisions at $\sqrt{s_{NN}}=200$ GeV"

description: Bottom and charm hadron invariant yields as a function of $p_{T}$.
description: The PHENIX Collaboration at the Relativistic Heavy Ion Collider has measured open heavy-flavor production in minimum bias Au+Au collisions at $\sqrt{s_{NN}}=200$ GeV via the yields of electrons from semileptonic decays of charm and bottom hadrons. Previous heavy-flavor electron measurements indicated substantial modification in the momentum distribution of the parent heavy quarks due to the quark-gluon plasma created in these collisions. For the first time, using the PHENIX silicon vertex detector to measure precision displaced tracking, the relative contributions from charm and bottom hadrons to these electrons as a function of transverse momentum are measured in Au+Au collisions. We use the bottom electron fractions in Au+Au and p+p along with the previously measured heavy flavor electron $R_{AA}$ to calculate the $R_{AA}$ for electrons from charm and bottom hadron decays separately.
DOI: 10.17182/hepdata.99752.v1/t2
title: "Figure 2" of "Single electron yields from semileptonic charm and bottom hadron decays in Au$+$Au collisions at $\sqrt{s_{NN}}=200$ GeV"

description: Bottom hadron election fraction with respect to heavy flavor electron as a function of $p_{T}$.
description: The PHENIX Collaboration at the Relativistic Heavy Ion Collider has measured open heavy-flavor production in minimum bias Au+Au collisions at $\sqrt{s_{NN}}=200$ GeV via the yields of electrons from semileptonic decays of charm and bottom hadrons. Previous heavy-flavor electron measurements indicated substantial modification in the momentum distribution of the parent heavy quarks due to the quark-gluon plasma created in these collisions. For the first time, using the PHENIX silicon vertex detector to measure precision displaced tracking, the relative contributions from charm and bottom hadrons to these electrons as a function of transverse momentum are measured in Au+Au collisions. We use the bottom electron fractions in Au+Au and p+p along with the previously measured heavy flavor electron $R_{AA}$ to calculate the $R_{AA}$ for electrons from charm and bottom hadron decays separately.
DOI: 10.17182/hepdata.99752.v1/t3
title: "Figure 3" of "Single electron yields from semileptonic charm and bottom hadron decays in Au$+$Au collisions at $\sqrt{s_{NN}}=200$ GeV"

description: Bottom and charm hadron $R_{AA}$ as a function of $p_{T}$.
description: The PHENIX Collaboration at the Relativistic Heavy Ion Collider has measured open heavy-flavor production in minimum bias Au+Au collisions at $\sqrt{s_{NN}}=200$ GeV via the yields of electrons from semileptonic decays of charm and bottom hadrons. Previous heavy-flavor electron measurements indicated substantial modification in the momentum distribution of the parent heavy quarks due to the quark-gluon plasma created in these collisions. For the first time, using the PHENIX silicon vertex detector to measure precision displaced tracking, the relative contributions from charm and bottom hadrons to these electrons as a function of transverse momentum are measured in Au+Au collisions. We use the bottom electron fractions in Au+Au and p+p along with the previously measured heavy flavor electron $R_{AA}$ to calculate the $R_{AA}$ for electrons from charm and bottom hadron decays separately.
DOI: 10.17182/hepdata.99752.v1/t4
title: "Figure 4" of "Single electron yields from semileptonic charm and bottom hadron decays in Au$+$Au collisions at $\sqrt{s_{NN}}=200$ GeV"

description: $(b\rightarrow e$ $R_{AA}) / (c\rightarrow e$ $R_{AA})$ as a function of $p_{T}$.
description: The PHENIX Collaboration at the Relativistic Heavy Ion Collider has measured open heavy-flavor production in minimum bias Au+Au collisions at $\sqrt{s_{NN}}=200$ GeV via the yields of electrons from semileptonic decays of charm and bottom hadrons. Previous heavy-flavor electron measurements indicated substantial modification in the momentum distribution of the parent heavy quarks due to the quark-gluon plasma created in these collisions. For the first time, using the PHENIX silicon vertex detector to measure precision displaced tracking, the relative contributions from charm and bottom hadrons to these electrons as a function of transverse momentum are measured in Au+Au collisions. We use the bottom electron fractions in Au+Au and p+p along with the previously measured heavy flavor electron $R_{AA}$ to calculate the $R_{AA}$ for electrons from charm and bottom hadron decays separately.
DOI: 10.3535/0ea-mq6-jc3
title: Illigera celebica Miq.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.25549/vercoutere-ouc1sto1770473
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: 10.3535/1l0-hxe-9dy
title: Melastoma L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/xt2-3lb-mlz
title: Praxelis clematidea (Griseb.) R. M. King & H. Rob.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.99788.v1/t2
title: "sbottom-tau obs" of "Search for bottom-squark pair production in $pp$ collision events at $\sqrt{s} = 13$ TeV with hadronically decaying $\tau$-leptons, $b$-jets and missing transverse momentum using the ATLAS detector"

description: The observed exclusion contour at $95\%$ CL as a function of the M(Sbottom) vs. M(N2) with the $\Delta M$(N2,N1) = 130 GeV. Masses within the contour are excluded.
description: CERN-LHC. ATLAS. What else belongs here?
DOI: 10.3535/50q-wc4-zpe
title: Ficus L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/d54-ze9-m5r
title: Cratoxylum formosum (Jack) Benth. & Hook. fil. ex Dyer

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.99788.v1/t1
title: "sbottom-tau exp" of "Search for bottom-squark pair production in $pp$ collision events at $\sqrt{s} = 13$ TeV with hadronically decaying $\tau$-leptons, $b$-jets and missing transverse momentum using the ATLAS detector"

description: The expected exclusion contour at $95\%$ CL as a function of the M(Sbottom) vs. M(N2) with the $\Delta M$(N2,N1) = 130 GeV. Masses within the contour are excluded.
description: CERN-LHC. ATLAS. What else belongs here?
DOI: 10.17182/hepdata.99788.v1/t3
title: "Acc_SingleBin" of "Search for bottom-squark pair production in $pp$ collision events at $\sqrt{s} = 13$ TeV with hadronically decaying $\tau$-leptons, $b$-jets and missing transverse momentum using the ATLAS detector"

description: Acceptance in the Single-bin SR as a function of the M(Sbottom) vs. M(N2) with the $\Delta M$(N2,N1) = 130 GeV. Keep in mind that the acceptance is given in units of $10^{-4}$.
description: CERN-LHC. ATLAS. What else belongs here?
DOI: 10.17182/hepdata.99788.v1/t4
title: "Eff_SingleBin" of "Search for bottom-squark pair production in $pp$ collision events at $\sqrt{s} = 13$ TeV with hadronically decaying $\tau$-leptons, $b$-jets and missing transverse momentum using the ATLAS detector"

description: Efficiency in the Single-bin SR as a function of the M(Sbottom) vs. M(N2) with the $\Delta$ M(N2,N1) $= 130$ GeV. Keep in mind that the efficiency is given in units of $10^{-2}$.
description: CERN-LHC. ATLAS. What else belongs here?
DOI: 10.17182/hepdata.99788.v1/t5
title: "Acc_MultiBin1" of "Search for bottom-squark pair production in $pp$ collision events at $\sqrt{s} = 13$ TeV with hadronically decaying $\tau$-leptons, $b$-jets and missing transverse momentum using the ATLAS detector"

description: Acceptance in the Multi-bin SR, $\min_{\Theta} &lt; 0.5$ bin as a function of the M(Sbottom) vs. M(N2) with the $\Delta M$(N2,N1) = 130 GeV. Keep in mind that the acceptance is given in units of $10^{-4}$.
description: CERN-LHC. ATLAS. What else belongs here?
DOI: 10.17182/hepdata.99788.v1/t6
title: "Eff_MultiBin1" of "Search for bottom-squark pair production in $pp$ collision events at $\sqrt{s} = 13$ TeV with hadronically decaying $\tau$-leptons, $b$-jets and missing transverse momentum using the ATLAS detector"

description: Efficiency in the Multi-bin SR, $\min_{\Theta} &lt; 0.5$ bin as a function of the M(Sbottom) vs. M(N2) with the $\Delta M$(N2,N1) = 130 GeV. Keep in mind that the efficiency is given in units of $10^{-2}$.
description: CERN-LHC. ATLAS. What else belongs here?
DOI: 10.17182/hepdata.99788.v1/t7
title: "Acc_MultiBin2" of "Search for bottom-squark pair production in $pp$ collision events at $\sqrt{s} = 13$ TeV with hadronically decaying $\tau$-leptons, $b$-jets and missing transverse momentum using the ATLAS detector"

description: Acceptance in the Multi-bin SR, $0.5 &lt; \min_{\Theta} &lt; 1.0$ bin as a function of the M(Sbottom) vs. M(N2) with the $\Delta M$(N2,N1) = 130 GeV. Keep in mind that the acceptance is given in units of $10^{-4}$.
description: CERN-LHC. ATLAS. What else belongs here?
DOI: 10.17182/hepdata.99788.v1/t8
title: "Eff_MultiBin2" of "Search for bottom-squark pair production in $pp$ collision events at $\sqrt{s} = 13$ TeV with hadronically decaying $\tau$-leptons, $b$-jets and missing transverse momentum using the ATLAS detector"

description: Efficiency in the Multi-bin SR, $0.5 &lt; \min_{\Theta} &lt; 1.0$ bin as a function of the M(Sbottom) vs. M(N2) with the $\Delta M$(N2,N1) = 130 GeV. Keep in mind that the efficiency is given in units of $10^{-2}$.
description: CERN-LHC. ATLAS. What else belongs here?
DOI: 10.25549/vercoutere-ouc110611135
title: 3 nude women standing and 1 partially dressed woman sitting

description: Three standing nude females (gray, red, white) and one sitting female (blue) with stockings and heels on a white and gray background. See description of 001 for OT notes.
DOI: 10.3535/ve4-eqs-jym
title: Schima Reinw. ex Blume

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.99788.v1/t10
title: "Eff_MultiBin3" of "Search for bottom-squark pair production in $pp$ collision events at $\sqrt{s} = 13$ TeV with hadronically decaying $\tau$-leptons, $b$-jets and missing transverse momentum using the ATLAS detector"

description: Efficiency in the Multi-bin SR, $\min_{\Theta} &gt; 1.0$ bin as a function of the M(Sbottom) vs. M(N2) with the $\Delta M$(N2,N1) = 130 GeV. Keep in mind that the efficiency is given in units of $10^{-2}$.
description: CERN-LHC. ATLAS. What else belongs here?
DOI: 10.17182/hepdata.99788.v1/t11
title: "UpperLimit" of "Search for bottom-squark pair production in $pp$ collision events at $\sqrt{s} = 13$ TeV with hadronically decaying $\tau$-leptons, $b$-jets and missing transverse momentum using the ATLAS detector"

description: Observed upper limits on the signal cross section as a function of the M(Sbottom) vs. M(N2) with the $\Delta M$(N2,N1) = 130 GeV.
description: CERN-LHC. ATLAS. What else belongs here?
DOI: 10.17182/hepdata.99788.v1/t12
title: "UpperLimitExp" of "Search for bottom-squark pair production in $pp$ collision events at $\sqrt{s} = 13$ TeV with hadronically decaying $\tau$-leptons, $b$-jets and missing transverse momentum using the ATLAS detector"

description: Expected upper limits on the signal cross section as a function of the M(Sbottom) vs. M(N2) with the $\Delta M$(N2,N1) = 130 GeV.
description: CERN-LHC. ATLAS. What else belongs here?
DOI: 10.17182/hepdata.99788.v1/t13
title: "Cutflow" of "Search for bottom-squark pair production in $pp$ collision events at $\sqrt{s} = 13$ TeV with hadronically decaying $\tau$-leptons, $b$-jets and missing transverse momentum using the ATLAS detector"

description: Cutflows for the bechmarl signal point M(Sbottom) = 800 GeV, M(N2) = 180 GeV. Weighted event yields are reported starting with the "Preselection" line, normalized to an integrated luminosity of $139$ fb$^{−1}$.
description: CERN-LHC. ATLAS. What else belongs here?
DOI: 10.17182/hepdata.99788.v1/t14
title: "PullPlots" of "Search for bottom-squark pair production in $pp$ collision events at $\sqrt{s} = 13$ TeV with hadronically decaying $\tau$-leptons, $b$-jets and missing transverse momentum using the ATLAS detector"

description: Comparison of the expected and observed event yields in the signal regions. The top-quark and Z(mumu) background contributions are scaled with the normalization factors obtained from the background-only fit. The other contribution includes all the backgrounds not explicitly listed in the legend (V+jets except Z(mumu)+jets, di-/triboson, multijet). The hatched band indicates the total statistical and systematic uncertainties in the SM background. The contributions from three signal models to the signal regions are also displayed, where the masses M(Sbottom) and M(N2) are given in GeV in the legend. The lower panel shows the significance of the deviation of the observed yield from the expected background yield.
description: CERN-LHC. ATLAS. What else belongs here?
DOI: 10.17182/hepdata.99788.v1/t9
title: "Acc_MultiBin3" of "Search for bottom-squark pair production in $pp$ collision events at $\sqrt{s} = 13$ TeV with hadronically decaying $\tau$-leptons, $b$-jets and missing transverse momentum using the ATLAS detector"

description: Acceptance in the Multi-bin SR, $\min_{\Theta} &gt; 1.0$ bin as a function of the M(Sbottom) vs. M(N2) with the $\Delta M$(N2,N1) = 130 GeV. Keep in mind that the acceptance is given in units of $10^{-4}$.
description: CERN-LHC. ATLAS. What else belongs here?
DOI: 10.3535/6gv-mcg-2l4
title: Breynia J.R.Forst. & G.Forst.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/s88-mty-st9
title: Callicarpa L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.99788.v1/t15
title: "SystTable" of "Search for bottom-squark pair production in $pp$ collision events at $\sqrt{s} = 13$ TeV with hadronically decaying $\tau$-leptons, $b$-jets and missing transverse momentum using the ATLAS detector"

description: Dominant systematic uncertainties in the background prediction for the signal regions after the fit to the control regions. “Other” includes the uncertainties arising from muons, jet-vertex tagging, modeling of pile-up, the $E_{T}^{miss}$ computation, multijet background, and luminosity. The individual uncertainties can be correlated and do not necessarily add up quadratically to the total uncertainty.
description: CERN-LHC. ATLAS. What else belongs here?
DOI: 10.17182/hepdata.99805.v1/t1
title: "Measured spectrum and normalized prediction for Phase-II" of "First antineutrino energy spectrum from $^{235}$U fissions with the STEREO detector at ILL"

description: Data from Figure 13 – Measured IBD yield spectrum and area-normalized HM-based prediction. Here, error bars inlude only uncorrelated uncertainties, namely statistics, time-evolution systematic, reactor background systematic. This uncorrelated uncertainty is $\sigma_j$ in eqn.(14). The full covariance matrix is provided in another entry.
description: These data support the measurement of the $^{235}$U-induced antineutrino spectrum shape by the STEREO experiment. 43 000 antineutrinos have been detected at about 10 m from the highly enriched core of the ILL reactor during 118 full days equivalent at nominal power. The measured inverse beta decay spectrum is unfolded to provide a pure $^{235}$U spectrum in antineutrino energy. A careful study of the unfolding procedure, including a cross-validation by an independent framework, has shown that no major biases are introduced by the method. A significant local distortion is found with respect to predictions around $E_\nu = 5.3$ MeV. A gaussian fit of this local excess leads to an amplitude of 12.1 $\pm$ 3.4% (3.5$\sigma$).
DOI: 10.17182/hepdata.99805.v1/t2
title: "Experimental covariance matrix" of "First antineutrino energy spectrum from $^{235}$U fissions with the STEREO detector at ILL"

description: Total covariance matrix of the measured spectrum, including statistics and all systematic uncertainties. It is denoted $V_\text{pr}$ in eqn.(18).
description: These data support the measurement of the $^{235}$U-induced antineutrino spectrum shape by the STEREO experiment. 43 000 antineutrinos have been detected at about 10 m from the highly enriched core of the ILL reactor during 118 full days equivalent at nominal power. The measured inverse beta decay spectrum is unfolded to provide a pure $^{235}$U spectrum in antineutrino energy. A careful study of the unfolding procedure, including a cross-validation by an independent framework, has shown that no major biases are introduced by the method. A significant local distortion is found with respect to predictions around $E_\nu = 5.3$ MeV. A gaussian fit of this local excess leads to an amplitude of 12.1 $\pm$ 3.4% (3.5$\sigma$).
DOI: 10.17182/hepdata.99805.v1/t3
title: "Response matrix" of "First antineutrino energy spectrum from $^{235}$U fissions with the STEREO detector at ILL"

description: STEREO Detector Response Matrix, sampled using STEREO's simulation using neutrinos with energy distributed according to HFR's IBD yield prediction. The matrix is given as a 200x22 matrix, with 200 50keV-wide $E_\nu$ bins (centers ranging from 0.05 to 10 MeV) and 22 250keV-wide measured-energy bins corresponding to measured data. The matrix is not normalized; desired normalization (e.g., $\sum_j R_{ij} = e_i$ where $e_i$ is the efficiency) has to be applied before the matrix can be used.
description: These data support the measurement of the $^{235}$U-induced antineutrino spectrum shape by the STEREO experiment. 43 000 antineutrinos have been detected at about 10 m from the highly enriched core of the ILL reactor during 118 full days equivalent at nominal power. The measured inverse beta decay spectrum is unfolded to provide a pure $^{235}$U spectrum in antineutrino energy. A careful study of the unfolding procedure, including a cross-validation by an independent framework, has shown that no major biases are introduced by the method. A significant local distortion is found with respect to predictions around $E_\nu = 5.3$ MeV. A gaussian fit of this local excess leads to an amplitude of 12.1 $\pm$ 3.4% (3.5$\sigma$).