cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.113759.v1/t4
title: "Figure 2 (bottom right)" of "Measurements of the pp $\to$ W$^\pm\gamma\gamma$ and pp $\to$ Z$\gamma\gamma$ cross sections at $\sqrt{s} =$ 13 TeV and limits on anomalous quartic gauge couplings"

description: Distribution of the transverse momentum of the diphoton system for the $\mathrm{Z}\gamma\gamma$ muon channel. The predicted yields are shown with their pre-fit normalisations. The observed data, the expected signal contribution and the background estimates are presented with error bars showing the corresponding statistical uncertainties.
description: The cross section for $\mathrm{W}$ or $\mathrm{Z}$ boson production in association with two photons is measured in proton-proton collisions at a centre-of-mass energy of $13\,\mathrm{TeV}$. The data set corresponds to an integrated luminosity of $137\,\mathrm{fb}^{-1}$ collected by the CMS experiment at the LHC. The $\mathrm{W}\to\ell\nu$ and $\mathrm{Z}\to\ell\ell$ decay modes (where $\ell=\mathrm{e},\mu$) are used to extract the $\mathrm{W}\gamma\gamma$ and $\mathrm{Z}\gamma\gamma$ cross sections in a phase space defined by electron (muon) with transverse momentum larger than $35\,(30)\,\mathrm{GeV}$ and photon transverse momentum larger than $20\,\mathrm{GeV}$. The measured cross sections in this phase space are $\sigma(\mathrm{W}\gamma\gamma)=13.6^{+1.9}_{-1.9}\,\mathrm{(stat)}^{+4.0}_{-4.0}\,\mathrm{(syst)}\pm 0.08\,\mathrm{(PDF + scale)}\,\mathrm{fb}$ and $\sigma(\mathrm{Z}\gamma\gamma)=5.41^{+0.58}_{-0.55}\,\mathrm{(stat)}^{+0.64}_{-0.70}\,\mathrm{(syst)}\pm 0.06\,\mathrm{(PDF + scale)}\,\mathrm{fb}$. Limits on anomalous quartic gauge couplings are set in the framework of an effective field theory with dimension-8 operators.
DOI: 10.17182/hepdata.113759.v1/t5
title: "Figure 3 (left)" of "Measurements of the pp $\to$ W$^\pm\gamma\gamma$ and pp $\to$ Z$\gamma\gamma$ cross sections at $\sqrt{s} =$ 13 TeV and limits on anomalous quartic gauge couplings"

description: Distribution of the transverse momentum of the diphoton system, obtained in the control region enriched in misidentified photons for the $\mathrm{W}\gamma\gamma$ electron channel. The predicted yields are shown with their pre-fit normalisations. The observed data, the expected signal contribution and the background estimates are presented with error bars showing the corresponding statistical uncertainties.
description: The cross section for $\mathrm{W}$ or $\mathrm{Z}$ boson production in association with two photons is measured in proton-proton collisions at a centre-of-mass energy of $13\,\mathrm{TeV}$. The data set corresponds to an integrated luminosity of $137\,\mathrm{fb}^{-1}$ collected by the CMS experiment at the LHC. The $\mathrm{W}\to\ell\nu$ and $\mathrm{Z}\to\ell\ell$ decay modes (where $\ell=\mathrm{e},\mu$) are used to extract the $\mathrm{W}\gamma\gamma$ and $\mathrm{Z}\gamma\gamma$ cross sections in a phase space defined by electron (muon) with transverse momentum larger than $35\,(30)\,\mathrm{GeV}$ and photon transverse momentum larger than $20\,\mathrm{GeV}$. The measured cross sections in this phase space are $\sigma(\mathrm{W}\gamma\gamma)=13.6^{+1.9}_{-1.9}\,\mathrm{(stat)}^{+4.0}_{-4.0}\,\mathrm{(syst)}\pm 0.08\,\mathrm{(PDF + scale)}\,\mathrm{fb}$ and $\sigma(\mathrm{Z}\gamma\gamma)=5.41^{+0.58}_{-0.55}\,\mathrm{(stat)}^{+0.64}_{-0.70}\,\mathrm{(syst)}\pm 0.06\,\mathrm{(PDF + scale)}\,\mathrm{fb}$. Limits on anomalous quartic gauge couplings are set in the framework of an effective field theory with dimension-8 operators.
DOI: 10.17182/hepdata.113759.v1/t6
title: "Figure 3 (right)" of "Measurements of the pp $\to$ W$^\pm\gamma\gamma$ and pp $\to$ Z$\gamma\gamma$ cross sections at $\sqrt{s} =$ 13 TeV and limits on anomalous quartic gauge couplings"

description: Distribution of the transverse momentum of the diphoton system, obtained in the control region enriched in misidentified photons for the $\mathrm{Z}\gamma\gamma$ electron channel. The predicted yields are shown with their pre-fit normalisations. The observed data, the expected signal contribution and the background estimates are presented with error bars showing the corresponding statistical uncertainties.
description: The cross section for $\mathrm{W}$ or $\mathrm{Z}$ boson production in association with two photons is measured in proton-proton collisions at a centre-of-mass energy of $13\,\mathrm{TeV}$. The data set corresponds to an integrated luminosity of $137\,\mathrm{fb}^{-1}$ collected by the CMS experiment at the LHC. The $\mathrm{W}\to\ell\nu$ and $\mathrm{Z}\to\ell\ell$ decay modes (where $\ell=\mathrm{e},\mu$) are used to extract the $\mathrm{W}\gamma\gamma$ and $\mathrm{Z}\gamma\gamma$ cross sections in a phase space defined by electron (muon) with transverse momentum larger than $35\,(30)\,\mathrm{GeV}$ and photon transverse momentum larger than $20\,\mathrm{GeV}$. The measured cross sections in this phase space are $\sigma(\mathrm{W}\gamma\gamma)=13.6^{+1.9}_{-1.9}\,\mathrm{(stat)}^{+4.0}_{-4.0}\,\mathrm{(syst)}\pm 0.08\,\mathrm{(PDF + scale)}\,\mathrm{fb}$ and $\sigma(\mathrm{Z}\gamma\gamma)=5.41^{+0.58}_{-0.55}\,\mathrm{(stat)}^{+0.64}_{-0.70}\,\mathrm{(syst)}\pm 0.06\,\mathrm{(PDF + scale)}\,\mathrm{fb}$. Limits on anomalous quartic gauge couplings are set in the framework of an effective field theory with dimension-8 operators.
DOI: 10.17182/hepdata.113759.v1/t7
title: "Table 1" of "Measurements of the pp $\to$ W$^\pm\gamma\gamma$ and pp $\to$ Z$\gamma\gamma$ cross sections at $\sqrt{s} =$ 13 TeV and limits on anomalous quartic gauge couplings"

description: The measured $\mathrm{W}\gamma\gamma$ and $\mathrm{Z}\gamma\gamma$ fiducial cross sections and corresponding theoretical predictions from MadGraph5_aMC@NLO. The measured yields in the electron and muon channels are extrapolated to a common fiducial phase space determined from simulated signal events at the generated particle level. Generated particles are considered stable if their mean decay length is larger than $1\,\mathrm{cm}$. Generated leptons are required to have a $\mathrm{p}_\mathrm{t}&gt;15\,\mathrm{GeV}$ and $|\eta|&lt;2.5$. The momenta of photons in a cone of $\Delta R=0.1$, the same cone size as the one applied to reconstructed data, are added to the charged lepton momentum to correct for final-state radiation. Generated photons are required to have $\mathrm{p}_\mathrm{t}&gt;15\,\mathrm{GeV}$ and $|\eta|&lt;2.5$. Additionally, the candidate photons are required to have no selected leptons or photons in a cone of radius $\Delta R=0.4$ and no other stable particles, apart from photons and neutrinos, in a cone of radius $\Delta R=0.1$. Events are then selected in the $\mathrm{W}\gamma\gamma$ channel by requiring exactly one electron (muon) with $\mathrm{p}_\mathrm{t}&gt;30\,\mathrm{GeV}$ and at least two photons with $\mathrm{p}_\mathrm{t}&gt;20\,\mathrm{GeV}$. Events are selected in the $\mathrm{Z}\gamma\gamma$ channel by requiring two electrons (muons), at least one of them with $\mathrm{p}_\mathrm{t}&gt;30\,\mathrm{GeV}$, and not less than two photons, each of them with $\mathrm{p}_\mathrm{t}&gt;20\,\mathrm{GeV}$. Additionally, the invariant mass of the dilepton system is required to be $m_{\ell\ell}&gt;55\,\mathrm{GeV}$.
description: The cross section for $\mathrm{W}$ or $\mathrm{Z}$ boson production in association with two photons is measured in proton-proton collisions at a centre-of-mass energy of $13\,\mathrm{TeV}$. The data set corresponds to an integrated luminosity of $137\,\mathrm{fb}^{-1}$ collected by the CMS experiment at the LHC. The $\mathrm{W}\to\ell\nu$ and $\mathrm{Z}\to\ell\ell$ decay modes (where $\ell=\mathrm{e},\mu$) are used to extract the $\mathrm{W}\gamma\gamma$ and $\mathrm{Z}\gamma\gamma$ cross sections in a phase space defined by electron (muon) with transverse momentum larger than $35\,(30)\,\mathrm{GeV}$ and photon transverse momentum larger than $20\,\mathrm{GeV}$. The measured cross sections in this phase space are $\sigma(\mathrm{W}\gamma\gamma)=13.6^{+1.9}_{-1.9}\,\mathrm{(stat)}^{+4.0}_{-4.0}\,\mathrm{(syst)}\pm 0.08\,\mathrm{(PDF + scale)}\,\mathrm{fb}$ and $\sigma(\mathrm{Z}\gamma\gamma)=5.41^{+0.58}_{-0.55}\,\mathrm{(stat)}^{+0.64}_{-0.70}\,\mathrm{(syst)}\pm 0.06\,\mathrm{(PDF + scale)}\,\mathrm{fb}$. Limits on anomalous quartic gauge couplings are set in the framework of an effective field theory with dimension-8 operators.
DOI: 10.17182/hepdata.113759.v1/t8
title: "Table 2" of "Measurements of the pp $\to$ W$^\pm\gamma\gamma$ and pp $\to$ Z$\gamma\gamma$ cross sections at $\sqrt{s} =$ 13 TeV and limits on anomalous quartic gauge couplings"

description: Expected and observed 95% confidence level intervals for the different anomalous couplings parameters in both the $\ell\nu\gamma\gamma$ and $\ell\ell\gamma\gamma$ channels. All parameters are fixed to their SM values except the one that is fitted. No unitarity regularisation scheme is applied. Intervals with a NAN value are not measured in the corresponding channels.
description: The cross section for $\mathrm{W}$ or $\mathrm{Z}$ boson production in association with two photons is measured in proton-proton collisions at a centre-of-mass energy of $13\,\mathrm{TeV}$. The data set corresponds to an integrated luminosity of $137\,\mathrm{fb}^{-1}$ collected by the CMS experiment at the LHC. The $\mathrm{W}\to\ell\nu$ and $\mathrm{Z}\to\ell\ell$ decay modes (where $\ell=\mathrm{e},\mu$) are used to extract the $\mathrm{W}\gamma\gamma$ and $\mathrm{Z}\gamma\gamma$ cross sections in a phase space defined by electron (muon) with transverse momentum larger than $35\,(30)\,\mathrm{GeV}$ and photon transverse momentum larger than $20\,\mathrm{GeV}$. The measured cross sections in this phase space are $\sigma(\mathrm{W}\gamma\gamma)=13.6^{+1.9}_{-1.9}\,\mathrm{(stat)}^{+4.0}_{-4.0}\,\mathrm{(syst)}\pm 0.08\,\mathrm{(PDF + scale)}\,\mathrm{fb}$ and $\sigma(\mathrm{Z}\gamma\gamma)=5.41^{+0.58}_{-0.55}\,\mathrm{(stat)}^{+0.64}_{-0.70}\,\mathrm{(syst)}\pm 0.06\,\mathrm{(PDF + scale)}\,\mathrm{fb}$. Limits on anomalous quartic gauge couplings are set in the framework of an effective field theory with dimension-8 operators.
DOI: 10.17182/hepdata.113760.v1/t1
title: "Table 1" of "Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: $j_\mathrm{T}$ distribution in pp collisions at $\sqrt{s}$ = 5.02 TeV in $40 &lt; p_\mathrm{T, jet}$ &lt; 60 GeV/$c$.
description: CERN-LHC. Jet fragmentation transverse momentum ($j_\mathrm{T}$) distributions are measured in proton-proton (pp) and proton-lead (p--Pb) collisions at $\sqrt{s_\mathrm{NN}}$ with the ALICE experiment at the LHC. Jets are reconstructed with the ALICE tracking detectors and electromagnetic calorimeter using the anti-$k_\mathrm{T}$ algorithm with resolution parameter $R = 0.4$ in the pseudorapidity range $|\eta|&lt;0.25$. The $j_\mathrm{T}$ values are calculated for charged particles inside a fixed cone with a radius $R = 0.4$ around the reconstructed jet axis. The $j_\mathrm{T}$ distributions are further characterised by fitting them with a function composed of an inverse gamma function for higher $j_\mathrm{T}$ values (called the wide component), related to the perturbative component of the fragmentation process, and with a Gaussian for lower $j_\mathrm{T}$ values (called the narrow component), predominantly connected to the hadronisation process.
DOI: 10.17182/hepdata.113760.v1/t2
title: "Table 2" of "Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: $j_\mathrm{T}$ distributions in p--Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV in $40 &lt; p_\mathrm{T, jet}$ &lt; 150 GeV/$c$.
description: CERN-LHC. Jet fragmentation transverse momentum ($j_\mathrm{T}$) distributions are measured in proton-proton (pp) and proton-lead (p--Pb) collisions at $\sqrt{s_\mathrm{NN}}$ with the ALICE experiment at the LHC. Jets are reconstructed with the ALICE tracking detectors and electromagnetic calorimeter using the anti-$k_\mathrm{T}$ algorithm with resolution parameter $R = 0.4$ in the pseudorapidity range $|\eta|&lt;0.25$. The $j_\mathrm{T}$ values are calculated for charged particles inside a fixed cone with a radius $R = 0.4$ around the reconstructed jet axis. The $j_\mathrm{T}$ distributions are further characterised by fitting them with a function composed of an inverse gamma function for higher $j_\mathrm{T}$ values (called the wide component), related to the perturbative component of the fragmentation process, and with a Gaussian for lower $j_\mathrm{T}$ values (called the narrow component), predominantly connected to the hadronisation process.
DOI: 10.25549/vercoutere-ouc110610416
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: 10.17182/hepdata.113760.v1/t4
title: "Table 4" of "Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: $\sqrt{\langle j_\mathrm{T}^2 \rangle }$ values for the narrow and wide components in p--Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV in $40 &lt; p_\mathrm{T, jet}$ &lt; 150 GeV/$c$.
description: CERN-LHC. Jet fragmentation transverse momentum ($j_\mathrm{T}$) distributions are measured in proton-proton (pp) and proton-lead (p--Pb) collisions at $\sqrt{s_\mathrm{NN}}$ with the ALICE experiment at the LHC. Jets are reconstructed with the ALICE tracking detectors and electromagnetic calorimeter using the anti-$k_\mathrm{T}$ algorithm with resolution parameter $R = 0.4$ in the pseudorapidity range $|\eta|&lt;0.25$. The $j_\mathrm{T}$ values are calculated for charged particles inside a fixed cone with a radius $R = 0.4$ around the reconstructed jet axis. The $j_\mathrm{T}$ distributions are further characterised by fitting them with a function composed of an inverse gamma function for higher $j_\mathrm{T}$ values (called the wide component), related to the perturbative component of the fragmentation process, and with a Gaussian for lower $j_\mathrm{T}$ values (called the narrow component), predominantly connected to the hadronisation process.
DOI: 10.17182/hepdata.113834.v1/t1
title: "Sensitivity and upper limits" of "A Search for electron neutrino appearance at the Delta m**2 ~ 1- eV**2 scale"

description: $\sin^2(2\theta)$ sensitivity and upper limit as a function of $\Delta m^2$ for a 2-neutrino muon-to-electron oscillation fit. The $90\%$ and $3\sigma$ levels are shown for both the upper limit and sensitivity in the range $10^{-2} \text{eV}^2 &lt; \Delta m^2 &lt; 10^2 \text{eV}^2$.
description: The MiniBooNE Collaboration reports first results of a search for $\nu_e$ appearance in a $\nu_\mu$ beam. With two largely independent analyses, we observe no significant excess of events above background for reconstructed neutrino energies above 475 MeV. The data are consistent with no oscillations within a two-neutrino appearance-only oscillation model.

The data release is intended to enable the oscillation fit in two different energy ranges: the default energy range (475 MeV - 3000 MeV), and the low energy threshold range (300 MeV - 3000 MeV).
Instructions on how to use the data release and an example FORTRAN program are provided in the additional resources.

Files and numbers are taken from the MiniBooNE Data Release (http://www-boone.fnal.gov/for_physicists/data_release/nue/). Original data release files are available in the additional resources.
DOI: 10.17182/hepdata.113834.v1/t2
title: "$\chi^2$" of "A Search for electron neutrino appearance at the Delta m**2 ~ 1- eV**2 scale"

description: The $\chi^2$ as a function of $\Delta m^2$ and $\sin^2(2\theta)$ for a 2-neutrino muon-to-electron oscillation fit. Note the value quoted in the third column is the total, and not the reduced, $\chi^2$ value (i.e. it has not been divided by the number of degrees of freedom).
description: The MiniBooNE Collaboration reports first results of a search for $\nu_e$ appearance in a $\nu_\mu$ beam. With two largely independent analyses, we observe no significant excess of events above background for reconstructed neutrino energies above 475 MeV. The data are consistent with no oscillations within a two-neutrino appearance-only oscillation model.

The data release is intended to enable the oscillation fit in two different energy ranges: the default energy range (475 MeV - 3000 MeV), and the low energy threshold range (300 MeV - 3000 MeV).
Instructions on how to use the data release and an example FORTRAN program are provided in the additional resources.

Files and numbers are taken from the MiniBooNE Data Release (http://www-boone.fnal.gov/for_physicists/data_release/nue/). Original data release files are available in the additional resources.
DOI: 10.17182/hepdata.113760.v1/t3
title: "Table 3" of "Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: $\sqrt{\langle j_\mathrm{T}^2 \rangle }$ values for the narrow and wide components in pp collisions at $\sqrt{s}$ = 5.02 TeV in $40 &lt; p_\mathrm{T, jet}$ &lt; 60 GeV/$c$.
description: CERN-LHC. Jet fragmentation transverse momentum ($j_\mathrm{T}$) distributions are measured in proton-proton (pp) and proton-lead (p--Pb) collisions at $\sqrt{s_\mathrm{NN}}$ with the ALICE experiment at the LHC. Jets are reconstructed with the ALICE tracking detectors and electromagnetic calorimeter using the anti-$k_\mathrm{T}$ algorithm with resolution parameter $R = 0.4$ in the pseudorapidity range $|\eta|&lt;0.25$. The $j_\mathrm{T}$ values are calculated for charged particles inside a fixed cone with a radius $R = 0.4$ around the reconstructed jet axis. The $j_\mathrm{T}$ distributions are further characterised by fitting them with a function composed of an inverse gamma function for higher $j_\mathrm{T}$ values (called the wide component), related to the perturbative component of the fragmentation process, and with a Gaussian for lower $j_\mathrm{T}$ values (called the narrow component), predominantly connected to the hadronisation process.
DOI: 10.17182/hepdata.113834.v1/t3
title: "NuE data and background" of "A Search for electron neutrino appearance at the Delta m**2 ~ 1- eV**2 scale"

description: Observed NuE data and background prediction for arXiv:0704.1500
description: The MiniBooNE Collaboration reports first results of a search for $\nu_e$ appearance in a $\nu_\mu$ beam. With two largely independent analyses, we observe no significant excess of events above background for reconstructed neutrino energies above 475 MeV. The data are consistent with no oscillations within a two-neutrino appearance-only oscillation model.

The data release is intended to enable the oscillation fit in two different energy ranges: the default energy range (475 MeV - 3000 MeV), and the low energy threshold range (300 MeV - 3000 MeV).
Instructions on how to use the data release and an example FORTRAN program are provided in the additional resources.

Files and numbers are taken from the MiniBooNE Data Release (http://www-boone.fnal.gov/for_physicists/data_release/nue/). Original data release files are available in the additional resources.
DOI: 10.17182/hepdata.113834.v1/t4
title: "NuE background fractional covariance matrix" of "A Search for electron neutrino appearance at the Delta m**2 ~ 1- eV**2 scale"

description: NuE background fractional covariance matrix for arXiv:0704.1500
description: The MiniBooNE Collaboration reports first results of a search for $\nu_e$ appearance in a $\nu_\mu$ beam. With two largely independent analyses, we observe no significant excess of events above background for reconstructed neutrino energies above 475 MeV. The data are consistent with no oscillations within a two-neutrino appearance-only oscillation model.

The data release is intended to enable the oscillation fit in two different energy ranges: the default energy range (475 MeV - 3000 MeV), and the low energy threshold range (300 MeV - 3000 MeV).
Instructions on how to use the data release and an example FORTRAN program are provided in the additional resources.

Files and numbers are taken from the MiniBooNE Data Release (http://www-boone.fnal.gov/for_physicists/data_release/nue/). Original data release files are available in the additional resources.
DOI: 10.17182/hepdata.113834.v1/t5
title: "NuMu to NuE simulation" of "A Search for electron neutrino appearance at the Delta m**2 ~ 1- eV**2 scale"

description: NuMu to NuE oscillation simulation for arXiv:0704.1500. ntuple file of 9,934 predicted muon-to-electron full transmutation events, containing information on reconstructed neutrino energy ($E_\text{vis}$), true neutrino energy, neutrino baseline, and event weight for each event.
description: The MiniBooNE Collaboration reports first results of a search for $\nu_e$ appearance in a $\nu_\mu$ beam. With two largely independent analyses, we observe no significant excess of events above background for reconstructed neutrino energies above 475 MeV. The data are consistent with no oscillations within a two-neutrino appearance-only oscillation model.

The data release is intended to enable the oscillation fit in two different energy ranges: the default energy range (475 MeV - 3000 MeV), and the low energy threshold range (300 MeV - 3000 MeV).
Instructions on how to use the data release and an example FORTRAN program are provided in the additional resources.

Files and numbers are taken from the MiniBooNE Data Release (http://www-boone.fnal.gov/for_physicists/data_release/nue/). Original data release files are available in the additional resources.
DOI: 10.17182/hepdata.113834.v1/t6
title: "NuMu to NuE fractional covariance matrix" of "A Search for electron neutrino appearance at the Delta m**2 ~ 1- eV**2 scale"

description: NuMu to NuE oscillation fractional covariance matrix for arXiv:0704.1500
description: The MiniBooNE Collaboration reports first results of a search for $\nu_e$ appearance in a $\nu_\mu$ beam. With two largely independent analyses, we observe no significant excess of events above background for reconstructed neutrino energies above 475 MeV. The data are consistent with no oscillations within a two-neutrino appearance-only oscillation model.

The data release is intended to enable the oscillation fit in two different energy ranges: the default energy range (475 MeV - 3000 MeV), and the low energy threshold range (300 MeV - 3000 MeV).
Instructions on how to use the data release and an example FORTRAN program are provided in the additional resources.

Files and numbers are taken from the MiniBooNE Data Release (http://www-boone.fnal.gov/for_physicists/data_release/nue/). Original data release files are available in the additional resources.
DOI: 10.25549/vercoutere-ouc110610413
title: Giraffe, dog, and duck plus word salad

description: One orange giraffe with brown spots standing beside a palm tree drawn in pencil; one brown dog; one duck drawn in pencil; remainder of the page is blank and unpainted except a brief word salad: DR.ST QUEEN ELIZABIETH OLGAS WBJ WIITAS at the bottom of the page. See description of 347 for OT notes.