cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.76740.v1/t5
title: "Table 5" of "Measurement of the decay $B\to D\ell\nu_\ell$ in fully reconstructed events and determination of the Cabibbo-Kobayashi-Maskawa matrix element $|V_{cb}|$"

description: Branching fractions of the decays ${B^+ \to \bar{D}^0 e^+ \nu_{e}}, {B^+ \to \bar{D}^0 \mu^+ \nu_{\mu}}, {B^0 \to D^- e^+ \nu_{e}},$ and ${B^0 \to D^- \mu^+ \nu_{\mu}}$. The branching fractions of ${B^+ \to \bar{D}^0 \ell^+ \nu_{\ell}}$ (${B^0 \to D^- \ell^+ \nu_{\ell}}$) are the weighted averages of the ${B^+ \to \bar{D}^0 e^+ \nu_{e}}$ and ${B^+ \to \bar{D}^0 \mu^+ \nu_{\mu}}$ (${B^0 \to D^- e^+ \nu_{e}}$ and ${B^0 \to D^- \mu^+ \nu_{\mu}}$) branching fraction results. The last row of the table corresponds to the branching fraction of all four sub-samples combined, expressed in terms of the neutral mode ${B^0 \to D^- \ell^+ \nu_{\ell}}$ assuming the lifetime $\tau_{B^0}$ = 1.519 (PDG 2014). The first error on the yields and on the branching fractions is statistical. The second uncertainty is systematic.
description: KEK-BF. We present a determination of the magnitude of the Cabibbo-Kobayashi-Maskawa matrix element $|V_{cb}|$ using the decay $B\to D\ell\nu_\ell$ ($\ell=e,\mu$) based on 711 fb$^{-1}$ of $e^+e^-\to \Upsilon(4S)$ data recorded by the Belle detector and containing $772 \times 10^6$ $B\bar{B}$ pairs. One $B$ meson in the event is fully reconstructed in a hadronic decay mode while the other, on the signal side, is partially reconstructed from a charged lepton and either a $D^+$ or $D^0$ meson in a total of 23 hadronic decay modes. The isospin-averaged branching fraction of the decay $B\to D\ell\nu_\ell$ is found to be $\mathcal{B}(B^0 \to D^- \ell^+ \nu_{\ell})=(2.31\pm 0.03(\mathrm{stat})\pm 0.11(\mathrm{syst}))\%$.

UPDATE (23 FEB 2017): split Table 1 from paper into two data tables so that $w_\rm{max}$ can be replaced by the numerical value (different for charged and neutral $B$ mesons).
DOI: 10.17182/hepdata.76745.v1/t2
title: "Table 2" of "Measurement of the beam asymmetry $\Sigma$ for $\pi^0$ and $\eta$ photoproduction on the proton at $E_\gamma = 9$ GeV"

description: Measurement of the beam asymmetry $\Sigma$ for $\eta$ photoproduction on the proton at $E_\gamma = 9$ GeV. The uncorrelated systematic errors (syst) are given in the table below along with a correlated normalization uncertainty (norm) of 3.6% due to the beam polarization.
description: No data abstract available.
DOI: 10.17182/hepdata.76790.v1/t3
title: "Table 3" of "J/$\psi$ suppression at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV"

description: Centrality dependence (with 10% width centrality classes) of the inclusive J/$\psi$ $R_{\rm AA}$ for $0.3
description: CERN-LHC. The inclusive J/$\psi$ production has been studied in Pb-Pb and pp collisions at the centre-of-mass energy per nucleon pair $\sqrt{s_{\rm NN}}=5.02$ TeV, using the ALICE detector at the CERN LHC. The J/$\psi$ meson is reconstructed, in the centre-of-mass rapidity interval $2.5
DOI: 10.17182/hepdata.76790.v1/t4
title: "Table 4" of "J/$\psi$ suppression at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV"

description: Centrality dependence (with 10% width centrality classes) of the ratio of the inclusive J/$\psi$ $R_{\rm AA}$ for $0.3
description: CERN-LHC. The inclusive J/$\psi$ production has been studied in Pb-Pb and pp collisions at the centre-of-mass energy per nucleon pair $\sqrt{s_{\rm NN}}=5.02$ TeV, using the ALICE detector at the CERN LHC. The J/$\psi$ meson is reconstructed, in the centre-of-mass rapidity interval $2.5
DOI: 10.17182/hepdata.76790.v1/t5
title: "Table 5" of "J/$\psi$ suppression at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV"

description: Transverse momentum dependence (in 0-20% centrality class) of the inclusive J/$\psi$ $R_{\rm AA}$. 
The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a $p_{\rm T}$-correlated systematic uncertainty.
description: CERN-LHC. The inclusive J/$\psi$ production has been studied in Pb-Pb and pp collisions at the centre-of-mass energy per nucleon pair $\sqrt{s_{\rm NN}}=5.02$ TeV, using the ALICE detector at the CERN LHC. The J/$\psi$ meson is reconstructed, in the centre-of-mass rapidity interval $2.5
DOI: 10.17182/hepdata.76790.v1/t6
title: "Table 6" of "J/$\psi$ suppression at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV"

description: Transverse momentum dependence (in 0-20% centrality class) of the double ratio of the inclusive J/$\psi$ $R_{\rm AA}$ at $\sqrt{s_{NN}}$= 5.02 and 2.76 TeV. 
The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a $p_{\rm T}$-correlated systematic uncertainty.
description: CERN-LHC. The inclusive J/$\psi$ production has been studied in Pb-Pb and pp collisions at the centre-of-mass energy per nucleon pair $\sqrt{s_{\rm NN}}=5.02$ TeV, using the ALICE detector at the CERN LHC. The J/$\psi$ meson is reconstructed, in the centre-of-mass rapidity interval $2.5
DOI: 10.17182/hepdata.76800.v1/t1
title: "Table 1" of "Multiplicities of charged pions and unidentified charged hadrons from deep-inelastic scattering of muons off an isoscalar target"

description: Multiplicities of positively charged pions from semi-inclusive deep-inelastic scattering of muons off an isoscalar target, $M^{\pi^{+}}$, in bins of $x$, $y$, and $z$. Also given are the diffractive vector meson correction to the pion count, $DVM^{\pi^{+}}$, and DIS count, $DVM^{DIS}$, as well as the radiative correction factors to the pion count, $\eta^{\pi^{+}}$, and DIS count, $\eta^{DIS}$. The correction factors were applied to the raw multiplicity to arrive at the final multiplicity given in the table, $M^{\pi^{+}}$, as follows:

$M^{\pi^{+}}$ = $M_{raw}^{\pi^{+}}$ * $\frac{\eta^{\pi^{+}}} {\eta^{DIS}}$ * $\frac{ DVM^{\pi^{+}} } {DVM^{DIS} }$.
description: Multiplicities of charged pions and unidentified hadrons produced in semi-inclusive deep-inelastic scattering were measured in bins of the Bjorken scaling variable $x$, the relative virtual-photon energy $y$ and the relative hadron energy $z$. Data were obtained by the COMPASS Collaboration using a $160$ GeV muon beam and an isoscalar target ($^{6}$LiD). They cover the kinematic domain in the photon virtuality $Q^{2}$ $&gt;$ $1$ (GeV/$c$)$^{2}$, $0.004 &lt; x &lt; 0.4$, $0.2 &lt; z &lt; 0.85$ and $0.1 &lt; y &lt; 0.7$.
DOI: 10.17182/hepdata.76800.v1/t2
title: "Table 2" of "Multiplicities of charged pions and unidentified charged hadrons from deep-inelastic scattering of muons off an isoscalar target"

description: Multiplicities of negatively charged pions from semi-inclusive deep-inelastic scattering of muons off an isoscalar target, $M^{\pi^{-}}$, in bins of $x$, $y$, and $z$. Also given are the diffractive vector meson correction to the pion count, $DVM^{\pi^{-}}$, and DIS count, $DVM^{DIS}$, as well as the radiative correction factors to the pion count, $\eta^{\pi^{-}}$, and DIS count, $\eta^{DIS}$. The correction factors were applied to the raw multiplicity to arrive at the final multiplicity given in the table, $M^{\pi^{-}}$, as follows:

$M^{\pi^{-}}$ = $M_{raw}^{\pi^{-}}$ * $\frac{\eta^{\pi^{-}}} {\eta^{DIS}}$ * $\frac{ DVM^{\pi^{-}} } {DVM^{DIS} }$.
description: Multiplicities of charged pions and unidentified hadrons produced in semi-inclusive deep-inelastic scattering were measured in bins of the Bjorken scaling variable $x$, the relative virtual-photon energy $y$ and the relative hadron energy $z$. Data were obtained by the COMPASS Collaboration using a $160$ GeV muon beam and an isoscalar target ($^{6}$LiD). They cover the kinematic domain in the photon virtuality $Q^{2}$ $&gt;$ $1$ (GeV/$c$)$^{2}$, $0.004 &lt; x &lt; 0.4$, $0.2 &lt; z &lt; 0.85$ and $0.1 &lt; y &lt; 0.7$.
DOI: 10.17182/hepdata.76800.v1/t3
title: "Table 3" of "Multiplicities of charged pions and unidentified charged hadrons from deep-inelastic scattering of muons off an isoscalar target"

description: Multiplicities of unidentified positively charged hadrons from semi-inclusive deep-inelastic scattering of muons off an isoscalar target, $M^{h^{+}}$, in bins of $x$, $y$, and $z$. Also given are the diffractive vector meson correction to the hadron count, $DVM^{h^{+}}$, and DIS count, $DVM^{DIS}$, as well as the radiative correction factors to the hadron count, $\eta^{h^{+}}$, and DIS count, $\eta^{DIS}$. The correction factors were applied to the raw multiplicity to arrive at the final multiplicity given in the table, $M^{h^{+}}$, as follows:

$M^{h^{+}}$ = $M_{raw}^{h^{+}}$ * $\frac{\eta^{h^{+}}} {\eta^{DIS}}$ * $\frac{ DVM^{h^{+}} } {DVM^{DIS} }$.
description: Multiplicities of charged pions and unidentified hadrons produced in semi-inclusive deep-inelastic scattering were measured in bins of the Bjorken scaling variable $x$, the relative virtual-photon energy $y$ and the relative hadron energy $z$. Data were obtained by the COMPASS Collaboration using a $160$ GeV muon beam and an isoscalar target ($^{6}$LiD). They cover the kinematic domain in the photon virtuality $Q^{2}$ $&gt;$ $1$ (GeV/$c$)$^{2}$, $0.004 &lt; x &lt; 0.4$, $0.2 &lt; z &lt; 0.85$ and $0.1 &lt; y &lt; 0.7$.
DOI: 10.17182/hepdata.76739.v1/t2
title: "Total cross section" of "Measurement of the WZ production cross section in pp collisions at sqrt(s) = 13 TeV"

description: The total pp to WZ cross section. The first systematic uncertainty is detector systematics and the second is luminosity uncertainty. The first theoretical prediction is calculated with MCFM at NLO with NNPDF3.0 PDFs, with dynamic renormalization and factorization scales set to muR = muF = m[WZ]. The second theoretical prediction is calculated with MATRIX at NNLO with fixed QCD scales set to muR = muF = 1/2 (m[Z] + m[W]) and with NNPDF3.0 PDFs. The uncertainty is obtained by varying the factorization and renormalization scales independently up and down by a factor of two with the condition that 0.5 &lt; muR/muF &lt; 2.
description: CERN-LHC. The WZ production cross section in proton-proton collisions at sqrt(s) = 13 TeV is measured with the CMS experiment at the LHC using a data sample corresponding to an integrated luminosity of 2.3 inverse fb. The measurement is performed in the leptonic decay modes WZ to l nu l' l', where l, l' = e, mu. The measured cross section for the range 60 &lt; m[l'l'] &lt; 120 GeV is 39.9 +/- 3.2 (stat) +2.9/-3.1 (syst) +/- 0.4 (theo) +/- 1.3 (lumi) pb, consistent with the standard model prediction.

Fiducial region definition
- leading Z lepton pt &gt; 20 GeV
- subleading Z lepton pt &gt; 10 GeV
- W lepton pt &gt; 20 GeV
- lepton |eta| &lt; 2.5
- Z invariant mass between 60 and 120 GeV
- any same-flavor opposite-sign lepton pair invariant mass &gt; 4 GeV

Total cross section region definition
- Z invariant mass between 60 and 120 GeV
- any same-flavor opposite-sign lepton pair invariant mass &gt; 4 GeV
DOI: 10.17182/hepdata.76808.v1/t1
title: "Table 1" of "Measurement of total and differential $W^+W^-$ production cross sections in proton-proton collisions at $\sqrt{s}=$ 8 TeV with the ATLAS detector and limits on anomalous triple-gauge-boson couplings"

description: Measured production cross sections of WW production in the fiducial region for different final states corresponding to different W decay channels: both W's decaying into electrons or both decaying to muon. The cross sections are defined for direct decays of the W bosons into prompt electrons or muons, intermediate decays into tau leptons are disregarded. The electrons are required to be contained within abs(eta)&lt;2.47 and to lie outside of 1.37 &lt; abs(eta) &lt; 1.53, muons are required to lie within abs(eta)&lt;2.4. The leading and subleading leptons in the events are required to have a transverse momentum above 25 and 20 GeV respectively. 
The transverse momentum of the vectorial sum of the neutrinos in the event should be larger than 45 GeV (PT(C=SUM(NU))). The transverse momentum of the vectorial sum of the neutrinos multiplied by the sine of azimuthal difference between lepton and the vectorial sum of the neutrinos in the event should be larger than 45 GeV if the azimuthal difference between lepton and the vectorial sum of the neutrinos is smaller than PI/2. 
The invariant mass of the leptons should exceed 15 GeV. The absolute difference between the invariant mass of the leptons and the mass of the Z boson should be larger than 15 GeV. 
Particle-level jets are defined using the anti-kT algorithm with radius of 0.4. No jets above 25 GeV and within abs(eta)&lt;4.5 are allowed in the event. Both, resonant and non-resonant WW production processes, are included in the cross sections.
description: No description provided.
DOI: 10.17182/hepdata.76808.v1/t2
title: "Table 2" of "Measurement of total and differential $W^+W^-$ production cross sections in proton-proton collisions at $\sqrt{s}=$ 8 TeV with the ATLAS detector and limits on anomalous triple-gauge-boson couplings"

description: Measured production cross section of WW production in the fiducial region in case one W boson decays into a prompt electron and the other one into a prompt muon. The cross section is defined for direct decays of the W bosons into prompt electrons or muons, intermediate decays into tau leptons are disregarded. The electrons are required to be contained within abs(eta)&lt;2.47 and to lie outside of 1.37 &lt; abs(eta) &lt; 1.53, muons are required to lie within abs(eta)&lt;2.4. The leading and subleading leptons in the events are required to have a transverse momentum above 25 and 20 GeV respectively. 
The transverse momentum of the vectorial sum of the neutrinos in the event should be larger than 20 GeV (PT(C=SUM(NU))). 
The transverse momentum of the vectorial sum of the neutrinos is multiplied by the sine of the azimuthal difference between lepton and the vectorial sum of the neutrinos if their azimuthal difference is smaller than PI/2. It is required to be larger than 15 GeV. 
The invariant mass of the leptons should exceed 10 GeV. Particle-level jets are defined using the anti-kT algorithm with radius of 0.4. No jets above 25 GeV and within abs(eta)&lt;4.5 are allowed in the event. Both, resonant and non-resonant WW production processes, are included in the cross sections.
description: No description provided.
DOI: 10.17182/hepdata.76808.v1/t3
title: "Table 3" of "Measurement of total and differential $W^+W^-$ production cross sections in proton-proton collisions at $\sqrt{s}=$ 8 TeV with the ATLAS detector and limits on anomalous triple-gauge-boson couplings"

description: Measured total production cross sections of WW production in the total phase space. Both, resonant and non-resonant WW, production are considered as signal.
description: No description provided.
DOI: 10.17182/hepdata.76808.v1/t4
title: "Table 4" of "Measurement of total and differential $W^+W^-$ production cross sections in proton-proton collisions at $\sqrt{s}=$ 8 TeV with the ATLAS detector and limits on anomalous triple-gauge-boson couplings"

description: Extrapolation factors AWW and CWW for emu channel.
description: No description provided.
DOI: 10.5517/ccdc.csd.cc2lzs9p
title: CCDC 2412863: Experimental Crystal Structure Determination

description: Related Article: Cai-Ming Liu, Hua-Hong Zou, Yi-Quan Zhang, Xiang Hao, Xiao-Ming Ren|2025|Chin.J.Chem.|43|1051|doi:10.1002/cjoc.202401318
description: An entry from the Cambridge Structural Database, the world’s repository for small molecule crystal structures. The entry contains experimental data from a crystal diffraction study. The deposited dataset for this entry is freely available from the CCDC and typically includes 3D coordinates, cell parameters, space group, experimental conditions and quality measures.
DOI: 10.5517/ccdc.csd.cc2lzsbq
title: CCDC 2412864: Experimental Crystal Structure Determination

description: Related Article: Cai-Ming Liu, Hua-Hong Zou, Yi-Quan Zhang, Xiang Hao, Xiao-Ming Ren|2025|Chin.J.Chem.|43|1051|doi:10.1002/cjoc.202401318
description: An entry from the Cambridge Structural Database, the world’s repository for small molecule crystal structures. The entry contains experimental data from a crystal diffraction study. The deposited dataset for this entry is freely available from the CCDC and typically includes 3D coordinates, cell parameters, space group, experimental conditions and quality measures.
DOI: 10.17182/hepdata.76745.v1/t1
title: "Table 1" of "Measurement of the beam asymmetry $\Sigma$ for $\pi^0$ and $\eta$ photoproduction on the proton at $E_\gamma = 9$ GeV"

description: Measurement of the beam asymmetry $\Sigma$ for $\pi^0$ photoproduction on the proton at $E_\gamma = 9$ GeV. The uncorrelated systematic errors (syst) are given in the table below along with a correlated normalization uncertainty (norm) of 3.6% due to the beam polarization.
description: No data abstract available.
DOI: 10.17182/hepdata.76790.v1/t1
title: "Table 1" of "J/$\psi$ suppression at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV"

description: Differential cross section ${\rm d}^2\sigma^{\rm pp}_{{\rm J}/\psi}/{\rm d}y{\rm d}p_{\rm T}$ for inclusive J/$\psi$ cross section in pp collisions at $\sqrt{s}=5.02$ TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a $p_{\rm T}$-correlated systematic uncertainty.
description: CERN-LHC. The inclusive J/$\psi$ production has been studied in Pb-Pb and pp collisions at the centre-of-mass energy per nucleon pair $\sqrt{s_{\rm NN}}=5.02$ TeV, using the ALICE detector at the CERN LHC. The J/$\psi$ meson is reconstructed, in the centre-of-mass rapidity interval $2.5
DOI: 10.17182/hepdata.76808.v1/t7
title: "Table 7" of "Measurement of total and differential $W^+W^-$ production cross sections in proton-proton collisions at $\sqrt{s}=$ 8 TeV with the ATLAS detector and limits on anomalous triple-gauge-boson couplings"

description: Uncertainty on extrapolation factors AWW and CWW for emu channel.
description: No description provided.
DOI: 10.17182/hepdata.76808.v1/t8
title: "Table 8" of "Measurement of total and differential $W^+W^-$ production cross sections in proton-proton collisions at $\sqrt{s}=$ 8 TeV with the ATLAS detector and limits on anomalous triple-gauge-boson couplings"

description: Uncertainty on extrapolation factors AWW and CWW for ee channel.
description: No description provided.
DOI: 10.17182/hepdata.76808.v1/t10
title: "Table 10" of "Measurement of total and differential $W^+W^-$ production cross sections in proton-proton collisions at $\sqrt{s}=$ 8 TeV with the ATLAS detector and limits on anomalous triple-gauge-boson couplings"

description: Measured differential cross sections as function of the leading lepton transverse momentum of WW production in the fiducial region for same different final states corresponding to different W decay channels: both W's decaying into electrons, both decaying to muon, and final states with one prompt electron and one prompt muon. The cross sections are defined for direct decays of the W bosons into prompt electrons or muons, intermediate decays into tau leptons are disregarded. The electrons are required to be contained within abs(eta)&lt;2.47 and to lie outside of 1.37 &lt; abs(eta) &lt; 1.53, muons are required to lie within abs(eta)&lt;2.4. The leading and subleading leptons in the events are required to have a transverse momentum above 25 and 20 GeV respectively. 
The transverse momentum of the vectorial sum of the neutrinos in the event should be larger than 20 GeV (PT(C=SUM(NU))). 
The transverse momentum of the vectorial sum of the neutrinos multiplied by the sin of azimuthal difference between lepton and the vectorial sum of the neutrinos in the event should be larger than 15 GeV. 
The invariant mass of the leptons should exceed 10 GeV. Particle-level jets are defined using the anti-kT algorithm with radius of 0.4. No jets above 25 GeV and within abs(eta)&lt;4.5 are allowed in the event. Both, resonant and non-resonant WW production processes, are included in the cross sections. 
All differential distributions are obtained using this selections.
description: No description provided.
DOI: 10.7914/rb8x-e739
title: CROSSNET OBS Deployment in Adriatic

description: Deployment of 10 OBS Nammu instruments in the Adriatic. Test deployment of three instrument for half a year in shallow water, 7 deployment in mid to deep waters (Adriatic is a shallow sea).
DOI: 10.17182/hepdata.76808.v1/t11
title: "Table 11" of "Measurement of total and differential $W^+W^-$ production cross sections in proton-proton collisions at $\sqrt{s}=$ 8 TeV with the ATLAS detector and limits on anomalous triple-gauge-boson couplings"

description: All differential distributions are obtained using the selection described for the transverse momentum distribution of leading lepton (PT(C=LEADING LEPTON)).
description: No description provided.
DOI: 10.17182/hepdata.76790.v1/t2
title: "Table 2" of "J/$\psi$ suppression at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV"

description: The nuclear modification factor for inclusive J/$\psi$ production, as a function of centrality, at $\sqrt{s_{\rm NN}}=5.02$ TeV. The widths of the centrality classes used are 2% from 0 to 12%, then 3% up to 30% and 5% for more peripheral collisions. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a centrality-correlated systematic uncertainty.
description: CERN-LHC. The inclusive J/$\psi$ production has been studied in Pb-Pb and pp collisions at the centre-of-mass energy per nucleon pair $\sqrt{s_{\rm NN}}=5.02$ TeV, using the ALICE detector at the CERN LHC. The J/$\psi$ meson is reconstructed, in the centre-of-mass rapidity interval $2.5
DOI: 10.17182/hepdata.76808.v1/t13
title: "Table 13" of "Measurement of total and differential $W^+W^-$ production cross sections in proton-proton collisions at $\sqrt{s}=$ 8 TeV with the ATLAS detector and limits on anomalous triple-gauge-boson couplings"

description: All differential distributions are obtained using the selection described for the transverse momentum distribution of leading lepton (PT(C=LEADING LEPTON)).
description: No description provided.