cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.129959.v1/t5
title: "Figure 5 right" of "Search for flavour-changing neutral-current couplings between the top quark and the photon with the ATLAS detector at $\sqrt{s} = 13$ TeV"

description: The 95% CL limits on the branching fractions. The scale of new physics is set to $\Lambda = 1$ TeV.
description: Search for flavour-changing neutral-current couplings between the top-quark and the photon with the ATLAS detector at $\sqrt{s} = 13$ TeV

The analysis uses data collected in $pp$ collisions at $\sqrt{s} = 13$~TeV during the LHC Run 2 corresponding to an integrated luminosity of 139~fb$^{-1}$.
Both FCNC top-quark production and decay are considered.
The final state consists of a charged lepton, missing transverse momentum, a $b$-tagged jet, one high momentum photon and possibly additional jets.
A multiclass deep neural network is used to classify events as either one of the two signal categories, FCNC production or decay, or as background.
# hepdata_doi: 10.17182/hepdata.105039.v1
DOI: 10.17182/hepdata.129959.v1/t6
title: "Figure Aux 03a" of "Search for flavour-changing neutral-current couplings between the top quark and the photon with the ATLAS detector at $\sqrt{s} = 13$ TeV"

description: The pre-fit distribution of the NN discriminant for the FCNC $tu\gamma$ LH signal scaled to 10 times the observed limit and all SM backgrounds as well as measured data in the SR. The last bin of the distribution contains the overflow and the first bin also contains the underflow. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction.
description: Search for flavour-changing neutral-current couplings between the top-quark and the photon with the ATLAS detector at $\sqrt{s} = 13$ TeV

The analysis uses data collected in $pp$ collisions at $\sqrt{s} = 13$~TeV during the LHC Run 2 corresponding to an integrated luminosity of 139~fb$^{-1}$.
Both FCNC top-quark production and decay are considered.
The final state consists of a charged lepton, missing transverse momentum, a $b$-tagged jet, one high momentum photon and possibly additional jets.
A multiclass deep neural network is used to classify events as either one of the two signal categories, FCNC production or decay, or as background.
# hepdata_doi: 10.17182/hepdata.105039.v1
DOI: 10.17182/hepdata.129959.v1/t7
title: "Figure Aux 03b" of "Search for flavour-changing neutral-current couplings between the top quark and the photon with the ATLAS detector at $\sqrt{s} = 13$ TeV"

description: The pre-fit distribution of the photon transverse momentum for SM backgrounds as well as measured data in the $t\bar{t}\gamma$ CR. The last bin of the distribution contains the overflow. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction.
description: Search for flavour-changing neutral-current couplings between the top-quark and the photon with the ATLAS detector at $\sqrt{s} = 13$ TeV

The analysis uses data collected in $pp$ collisions at $\sqrt{s} = 13$~TeV during the LHC Run 2 corresponding to an integrated luminosity of 139~fb$^{-1}$.
Both FCNC top-quark production and decay are considered.
The final state consists of a charged lepton, missing transverse momentum, a $b$-tagged jet, one high momentum photon and possibly additional jets.
A multiclass deep neural network is used to classify events as either one of the two signal categories, FCNC production or decay, or as background.
# hepdata_doi: 10.17182/hepdata.105039.v1
DOI: 10.17182/hepdata.129959.v1/t8
title: "Figure Aux 03c" of "Search for flavour-changing neutral-current couplings between the top quark and the photon with the ATLAS detector at $\sqrt{s} = 13$ TeV"

description: The pre-fit distribution of the photon transverse momentum for the all SM backgrounds as well as measured data in the $W\gamma$+jets CR. The last bin of the distribution contains the overflow. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction.
description: Search for flavour-changing neutral-current couplings between the top-quark and the photon with the ATLAS detector at $\sqrt{s} = 13$ TeV

The analysis uses data collected in $pp$ collisions at $\sqrt{s} = 13$~TeV during the LHC Run 2 corresponding to an integrated luminosity of 139~fb$^{-1}$.
Both FCNC top-quark production and decay are considered.
The final state consists of a charged lepton, missing transverse momentum, a $b$-tagged jet, one high momentum photon and possibly additional jets.
A multiclass deep neural network is used to classify events as either one of the two signal categories, FCNC production or decay, or as background.
# hepdata_doi: 10.17182/hepdata.105039.v1
DOI: 10.17182/hepdata.130198.v1/t1
title: "tcs" of "Photoproduction of the omega meson off the proton near threshold"

description: Total cross section as a function of c.m. energy W.
description: A2 Collaboration at MAMI.
An experimental study of $\omega$ photoproduction on the proton was
conducted by using the Crystal Ball and TAPS multiphoton
spectrometers together with the photon tagging facility at the Mainz
Microtron MAMI.
The $\gamma p \to \omega p$ differential cross sections are measured from
threshold to the incident-photon energy $E_{\gamma}$=1.4 GeV (W=1.87 GeV
for the center-of-mass energy) with 15-MeV binning in $E_{\gamma}$ and
full production-angle coverage. One contribution to the systematic
uncertainty comes from the uncertainty in the shape of the
background. It is not larger than 6%. Another contribution comes from
the determination of the detector acceptance and the photon-beam flux.
It was estimated as 5%.
The quality of the present data near threshold gives access to a 
variety of interesting physics aspects. As an example, an estimation 
of the $\omega$N scattering length is provided.
DOI: 10.17182/hepdata.130198.v1/t2
title: "dcs01" of "Photoproduction of the omega meson off the proton near threshold"

description: Differential cross section at W= 1.7245 GeV
description: A2 Collaboration at MAMI.
An experimental study of $\omega$ photoproduction on the proton was
conducted by using the Crystal Ball and TAPS multiphoton
spectrometers together with the photon tagging facility at the Mainz
Microtron MAMI.
The $\gamma p \to \omega p$ differential cross sections are measured from
threshold to the incident-photon energy $E_{\gamma}$=1.4 GeV (W=1.87 GeV
for the center-of-mass energy) with 15-MeV binning in $E_{\gamma}$ and
full production-angle coverage. One contribution to the systematic
uncertainty comes from the uncertainty in the shape of the
background. It is not larger than 6%. Another contribution comes from
the determination of the detector acceptance and the photon-beam flux.
It was estimated as 5%.
The quality of the present data near threshold gives access to a 
variety of interesting physics aspects. As an example, an estimation 
of the $\omega$N scattering length is provided.
DOI: 10.25549/vercoutere-ouc110611294
title: Nude woman sitting next to a brown man

description: One nude dark green female outlined in black sits on a red platform. She has one leg raised and bent at the knee and is depicted from breasts to ankle. She sits beside a brown male outlined in black and is depicted from head to waist. Behind the male is a face outlined in brown on the orange wall. See description of 001 for OT notes.
DOI: 10.17182/hepdata.130198.v1/t3
title: "dcs02" of "Photoproduction of the omega meson off the proton near threshold"

description: Differential cross section at W= 1.7319 GeV
description: A2 Collaboration at MAMI.
An experimental study of $\omega$ photoproduction on the proton was
conducted by using the Crystal Ball and TAPS multiphoton
spectrometers together with the photon tagging facility at the Mainz
Microtron MAMI.
The $\gamma p \to \omega p$ differential cross sections are measured from
threshold to the incident-photon energy $E_{\gamma}$=1.4 GeV (W=1.87 GeV
for the center-of-mass energy) with 15-MeV binning in $E_{\gamma}$ and
full production-angle coverage. One contribution to the systematic
uncertainty comes from the uncertainty in the shape of the
background. It is not larger than 6%. Another contribution comes from
the determination of the detector acceptance and the photon-beam flux.
It was estimated as 5%.
The quality of the present data near threshold gives access to a 
variety of interesting physics aspects. As an example, an estimation 
of the $\omega$N scattering length is provided.
DOI: 10.17182/hepdata.130198.v1/t4
title: "dcs03" of "Photoproduction of the omega meson off the proton near threshold"

description: Differential cross section at W= 1.7401 GeV
description: A2 Collaboration at MAMI.
An experimental study of $\omega$ photoproduction on the proton was
conducted by using the Crystal Ball and TAPS multiphoton
spectrometers together with the photon tagging facility at the Mainz
Microtron MAMI.
The $\gamma p \to \omega p$ differential cross sections are measured from
threshold to the incident-photon energy $E_{\gamma}$=1.4 GeV (W=1.87 GeV
for the center-of-mass energy) with 15-MeV binning in $E_{\gamma}$ and
full production-angle coverage. One contribution to the systematic
uncertainty comes from the uncertainty in the shape of the
background. It is not larger than 6%. Another contribution comes from
the determination of the detector acceptance and the photon-beam flux.
It was estimated as 5%.
The quality of the present data near threshold gives access to a 
variety of interesting physics aspects. As an example, an estimation 
of the $\omega$N scattering length is provided.
DOI: 10.17182/hepdata.130198.v1/t6
title: "dcs05" of "Photoproduction of the omega meson off the proton near threshold"

description: Differential cross section at W= 1.7568 GeV
description: A2 Collaboration at MAMI.
An experimental study of $\omega$ photoproduction on the proton was
conducted by using the Crystal Ball and TAPS multiphoton
spectrometers together with the photon tagging facility at the Mainz
Microtron MAMI.
The $\gamma p \to \omega p$ differential cross sections are measured from
threshold to the incident-photon energy $E_{\gamma}$=1.4 GeV (W=1.87 GeV
for the center-of-mass energy) with 15-MeV binning in $E_{\gamma}$ and
full production-angle coverage. One contribution to the systematic
uncertainty comes from the uncertainty in the shape of the
background. It is not larger than 6%. Another contribution comes from
the determination of the detector acceptance and the photon-beam flux.
It was estimated as 5%.
The quality of the present data near threshold gives access to a 
variety of interesting physics aspects. As an example, an estimation 
of the $\omega$N scattering length is provided.
DOI: 10.17182/hepdata.130198.v1/t7
title: "dcs06" of "Photoproduction of the omega meson off the proton near threshold"

description: Differential cross section at W= 1.7645 GeV
description: A2 Collaboration at MAMI.
An experimental study of $\omega$ photoproduction on the proton was
conducted by using the Crystal Ball and TAPS multiphoton
spectrometers together with the photon tagging facility at the Mainz
Microtron MAMI.
The $\gamma p \to \omega p$ differential cross sections are measured from
threshold to the incident-photon energy $E_{\gamma}$=1.4 GeV (W=1.87 GeV
for the center-of-mass energy) with 15-MeV binning in $E_{\gamma}$ and
full production-angle coverage. One contribution to the systematic
uncertainty comes from the uncertainty in the shape of the
background. It is not larger than 6%. Another contribution comes from
the determination of the detector acceptance and the photon-beam flux.
It was estimated as 5%.
The quality of the present data near threshold gives access to a 
variety of interesting physics aspects. As an example, an estimation 
of the $\omega$N scattering length is provided.
DOI: 10.17182/hepdata.130198.v1/t10
title: "dcs09" of "Photoproduction of the omega meson off the proton near threshold"

description: Differential cross section at W= 1.7891 GeV
description: A2 Collaboration at MAMI.
An experimental study of $\omega$ photoproduction on the proton was
conducted by using the Crystal Ball and TAPS multiphoton
spectrometers together with the photon tagging facility at the Mainz
Microtron MAMI.
The $\gamma p \to \omega p$ differential cross sections are measured from
threshold to the incident-photon energy $E_{\gamma}$=1.4 GeV (W=1.87 GeV
for the center-of-mass energy) with 15-MeV binning in $E_{\gamma}$ and
full production-angle coverage. One contribution to the systematic
uncertainty comes from the uncertainty in the shape of the
background. It is not larger than 6%. Another contribution comes from
the determination of the detector acceptance and the photon-beam flux.
It was estimated as 5%.
The quality of the present data near threshold gives access to a 
variety of interesting physics aspects. As an example, an estimation 
of the $\omega$N scattering length is provided.
DOI: 10.17182/hepdata.130198.v1/t11
title: "dcs10" of "Photoproduction of the omega meson off the proton near threshold"

description: Differential cross section at W= 1.7968 GeV
description: A2 Collaboration at MAMI.
An experimental study of $\omega$ photoproduction on the proton was
conducted by using the Crystal Ball and TAPS multiphoton
spectrometers together with the photon tagging facility at the Mainz
Microtron MAMI.
The $\gamma p \to \omega p$ differential cross sections are measured from
threshold to the incident-photon energy $E_{\gamma}$=1.4 GeV (W=1.87 GeV
for the center-of-mass energy) with 15-MeV binning in $E_{\gamma}$ and
full production-angle coverage. One contribution to the systematic
uncertainty comes from the uncertainty in the shape of the
background. It is not larger than 6%. Another contribution comes from
the determination of the detector acceptance and the photon-beam flux.
It was estimated as 5%.
The quality of the present data near threshold gives access to a 
variety of interesting physics aspects. As an example, an estimation 
of the $\omega$N scattering length is provided.
DOI: 10.17182/hepdata.130198.v1/t12
title: "dcs11" of "Photoproduction of the omega meson off the proton near threshold"

description: Differential cross section at W= 1.8045 GeV
description: A2 Collaboration at MAMI.
An experimental study of $\omega$ photoproduction on the proton was
conducted by using the Crystal Ball and TAPS multiphoton
spectrometers together with the photon tagging facility at the Mainz
Microtron MAMI.
The $\gamma p \to \omega p$ differential cross sections are measured from
threshold to the incident-photon energy $E_{\gamma}$=1.4 GeV (W=1.87 GeV
for the center-of-mass energy) with 15-MeV binning in $E_{\gamma}$ and
full production-angle coverage. One contribution to the systematic
uncertainty comes from the uncertainty in the shape of the
background. It is not larger than 6%. Another contribution comes from
the determination of the detector acceptance and the photon-beam flux.
It was estimated as 5%.
The quality of the present data near threshold gives access to a 
variety of interesting physics aspects. As an example, an estimation 
of the $\omega$N scattering length is provided.
DOI: 10.17182/hepdata.130198.v1/t13
title: "dcs12" of "Photoproduction of the omega meson off the proton near threshold"

description: Differential cross section at W= 1.8119 GeV
description: A2 Collaboration at MAMI.
An experimental study of $\omega$ photoproduction on the proton was
conducted by using the Crystal Ball and TAPS multiphoton
spectrometers together with the photon tagging facility at the Mainz
Microtron MAMI.
The $\gamma p \to \omega p$ differential cross sections are measured from
threshold to the incident-photon energy $E_{\gamma}$=1.4 GeV (W=1.87 GeV
for the center-of-mass energy) with 15-MeV binning in $E_{\gamma}$ and
full production-angle coverage. One contribution to the systematic
uncertainty comes from the uncertainty in the shape of the
background. It is not larger than 6%. Another contribution comes from
the determination of the detector acceptance and the photon-beam flux.
It was estimated as 5%.
The quality of the present data near threshold gives access to a 
variety of interesting physics aspects. As an example, an estimation 
of the $\omega$N scattering length is provided.
DOI: 10.17182/hepdata.130198.v1/t5
title: "dcs04" of "Photoproduction of the omega meson off the proton near threshold"

description: Differential cross section at W= 1.7490 GeV
description: A2 Collaboration at MAMI.
An experimental study of $\omega$ photoproduction on the proton was
conducted by using the Crystal Ball and TAPS multiphoton
spectrometers together with the photon tagging facility at the Mainz
Microtron MAMI.
The $\gamma p \to \omega p$ differential cross sections are measured from
threshold to the incident-photon energy $E_{\gamma}$=1.4 GeV (W=1.87 GeV
for the center-of-mass energy) with 15-MeV binning in $E_{\gamma}$ and
full production-angle coverage. One contribution to the systematic
uncertainty comes from the uncertainty in the shape of the
background. It is not larger than 6%. Another contribution comes from
the determination of the detector acceptance and the photon-beam flux.
It was estimated as 5%.
The quality of the present data near threshold gives access to a 
variety of interesting physics aspects. As an example, an estimation 
of the $\omega$N scattering length is provided.
DOI: 10.17182/hepdata.130198.v1/t8
title: "dcs07" of "Photoproduction of the omega meson off the proton near threshold"

description: Differential cross section at W= 1.7729 GeV
description: A2 Collaboration at MAMI.
An experimental study of $\omega$ photoproduction on the proton was
conducted by using the Crystal Ball and TAPS multiphoton
spectrometers together with the photon tagging facility at the Mainz
Microtron MAMI.
The $\gamma p \to \omega p$ differential cross sections are measured from
threshold to the incident-photon energy $E_{\gamma}$=1.4 GeV (W=1.87 GeV
for the center-of-mass energy) with 15-MeV binning in $E_{\gamma}$ and
full production-angle coverage. One contribution to the systematic
uncertainty comes from the uncertainty in the shape of the
background. It is not larger than 6%. Another contribution comes from
the determination of the detector acceptance and the photon-beam flux.
It was estimated as 5%.
The quality of the present data near threshold gives access to a 
variety of interesting physics aspects. As an example, an estimation 
of the $\omega$N scattering length is provided.
DOI: 10.17182/hepdata.130198.v1/t9
title: "dcs08" of "Photoproduction of the omega meson off the proton near threshold"

description: Differential cross section at W= 1.7811 GeV
description: A2 Collaboration at MAMI.
An experimental study of $\omega$ photoproduction on the proton was
conducted by using the Crystal Ball and TAPS multiphoton
spectrometers together with the photon tagging facility at the Mainz
Microtron MAMI.
The $\gamma p \to \omega p$ differential cross sections are measured from
threshold to the incident-photon energy $E_{\gamma}$=1.4 GeV (W=1.87 GeV
for the center-of-mass energy) with 15-MeV binning in $E_{\gamma}$ and
full production-angle coverage. One contribution to the systematic
uncertainty comes from the uncertainty in the shape of the
background. It is not larger than 6%. Another contribution comes from
the determination of the detector acceptance and the photon-beam flux.
It was estimated as 5%.
The quality of the present data near threshold gives access to a 
variety of interesting physics aspects. As an example, an estimation 
of the $\omega$N scattering length is provided.
DOI: 10.17182/hepdata.130198.v1/t14
title: "dcs13" of "Photoproduction of the omega meson off the proton near threshold"

description: Differential cross section at W= 1.8192 GeV
description: A2 Collaboration at MAMI.
An experimental study of $\omega$ photoproduction on the proton was
conducted by using the Crystal Ball and TAPS multiphoton
spectrometers together with the photon tagging facility at the Mainz
Microtron MAMI.
The $\gamma p \to \omega p$ differential cross sections are measured from
threshold to the incident-photon energy $E_{\gamma}$=1.4 GeV (W=1.87 GeV
for the center-of-mass energy) with 15-MeV binning in $E_{\gamma}$ and
full production-angle coverage. One contribution to the systematic
uncertainty comes from the uncertainty in the shape of the
background. It is not larger than 6%. Another contribution comes from
the determination of the detector acceptance and the photon-beam flux.
It was estimated as 5%.
The quality of the present data near threshold gives access to a 
variety of interesting physics aspects. As an example, an estimation 
of the $\omega$N scattering length is provided.
DOI: 10.17182/hepdata.130198.v1/t15
title: "dcs14" of "Photoproduction of the omega meson off the proton near threshold"

description: Differential cross section at W= 1.8269 GeV
description: A2 Collaboration at MAMI.
An experimental study of $\omega$ photoproduction on the proton was
conducted by using the Crystal Ball and TAPS multiphoton
spectrometers together with the photon tagging facility at the Mainz
Microtron MAMI.
The $\gamma p \to \omega p$ differential cross sections are measured from
threshold to the incident-photon energy $E_{\gamma}$=1.4 GeV (W=1.87 GeV
for the center-of-mass energy) with 15-MeV binning in $E_{\gamma}$ and
full production-angle coverage. One contribution to the systematic
uncertainty comes from the uncertainty in the shape of the
background. It is not larger than 6%. Another contribution comes from
the determination of the detector acceptance and the photon-beam flux.
It was estimated as 5%.
The quality of the present data near threshold gives access to a 
variety of interesting physics aspects. As an example, an estimation 
of the $\omega$N scattering length is provided.
DOI: 10.17182/hepdata.130198.v1/t16
title: "dcs15" of "Photoproduction of the omega meson off the proton near threshold"

description: Differential cross section at W= 1.8348 GeV
description: A2 Collaboration at MAMI.
An experimental study of $\omega$ photoproduction on the proton was
conducted by using the Crystal Ball and TAPS multiphoton
spectrometers together with the photon tagging facility at the Mainz
Microtron MAMI.
The $\gamma p \to \omega p$ differential cross sections are measured from
threshold to the incident-photon energy $E_{\gamma}$=1.4 GeV (W=1.87 GeV
for the center-of-mass energy) with 15-MeV binning in $E_{\gamma}$ and
full production-angle coverage. One contribution to the systematic
uncertainty comes from the uncertainty in the shape of the
background. It is not larger than 6%. Another contribution comes from
the determination of the detector acceptance and the photon-beam flux.
It was estimated as 5%.
The quality of the present data near threshold gives access to a 
variety of interesting physics aspects. As an example, an estimation 
of the $\omega$N scattering length is provided.
DOI: 10.17182/hepdata.130198.v1/t17
title: "dcs16" of "Photoproduction of the omega meson off the proton near threshold"

description: Differential cross section at W= 1.8424 GeV
description: A2 Collaboration at MAMI.
An experimental study of $\omega$ photoproduction on the proton was
conducted by using the Crystal Ball and TAPS multiphoton
spectrometers together with the photon tagging facility at the Mainz
Microtron MAMI.
The $\gamma p \to \omega p$ differential cross sections are measured from
threshold to the incident-photon energy $E_{\gamma}$=1.4 GeV (W=1.87 GeV
for the center-of-mass energy) with 15-MeV binning in $E_{\gamma}$ and
full production-angle coverage. One contribution to the systematic
uncertainty comes from the uncertainty in the shape of the
background. It is not larger than 6%. Another contribution comes from
the determination of the detector acceptance and the photon-beam flux.
It was estimated as 5%.
The quality of the present data near threshold gives access to a 
variety of interesting physics aspects. As an example, an estimation 
of the $\omega$N scattering length is provided.