cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.116552.v1/t9
title: "Table_T09" of "Measurement of the transverse target and beam-target asymmetries in $\eta$ meson photoproduction at MAMI"

description: Target asymmetry T for c.m. energy W= 1.7022 GeV
description: A2 at MAMI. We present new data for the transverse target asymmetry T and the very first data for the beam-target
asymmetry F in the $\gamma p \to \eta p$ reaction up to a center-of-mass energy of W = 1.9 GeV.
The systematic uncertainty is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%). By adding all
contributions in quadrature, a total systematic uncertainty of less than 6% is obtained.
The data were obtained with the Crystal Ball/TAPS detector setup at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.116552.v1/t12
title: "Table_T12" of "Measurement of the transverse target and beam-target asymmetries in $\eta$ meson photoproduction at MAMI"

description: Target asymmetry T for c.m. energy W= 1.8476 GeV
description: A2 at MAMI. We present new data for the transverse target asymmetry T and the very first data for the beam-target
asymmetry F in the $\gamma p \to \eta p$ reaction up to a center-of-mass energy of W = 1.9 GeV.
The systematic uncertainty is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%). By adding all
contributions in quadrature, a total systematic uncertainty of less than 6% is obtained.
The data were obtained with the Crystal Ball/TAPS detector setup at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.116552.v1/t13
title: "Table_F01" of "Measurement of the transverse target and beam-target asymmetries in $\eta$ meson photoproduction at MAMI"

description: Beam-target asymmetry F for c.m. energy W= 1.4969 GeV
description: A2 at MAMI. We present new data for the transverse target asymmetry T and the very first data for the beam-target
asymmetry F in the $\gamma p \to \eta p$ reaction up to a center-of-mass energy of W = 1.9 GeV.
The systematic uncertainty is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%). By adding all
contributions in quadrature, a total systematic uncertainty of less than 6% is obtained.
The data were obtained with the Crystal Ball/TAPS detector setup at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.116552.v1/t14
title: "Table_F02" of "Measurement of the transverse target and beam-target asymmetries in $\eta$ meson photoproduction at MAMI"

description: Beam-target asymmetry F for c.m. energy W= 1.5156 GeV
description: A2 at MAMI. We present new data for the transverse target asymmetry T and the very first data for the beam-target
asymmetry F in the $\gamma p \to \eta p$ reaction up to a center-of-mass energy of W = 1.9 GeV.
The systematic uncertainty is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%). By adding all
contributions in quadrature, a total systematic uncertainty of less than 6% is obtained.
The data were obtained with the Crystal Ball/TAPS detector setup at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.116552.v1/t15
title: "Table_F03" of "Measurement of the transverse target and beam-target asymmetries in $\eta$ meson photoproduction at MAMI"

description: Beam-target asymmetry F for c.m. energy W= 1.5341 GeV
description: A2 at MAMI. We present new data for the transverse target asymmetry T and the very first data for the beam-target
asymmetry F in the $\gamma p \to \eta p$ reaction up to a center-of-mass energy of W = 1.9 GeV.
The systematic uncertainty is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%). By adding all
contributions in quadrature, a total systematic uncertainty of less than 6% is obtained.
The data were obtained with the Crystal Ball/TAPS detector setup at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.116552.v1/t16
title: "Table_F04" of "Measurement of the transverse target and beam-target asymmetries in $\eta$ meson photoproduction at MAMI"

description: Beam-target asymmetry F for c.m. energy W= 1.5584 GeV
description: A2 at MAMI. We present new data for the transverse target asymmetry T and the very first data for the beam-target
asymmetry F in the $\gamma p \to \eta p$ reaction up to a center-of-mass energy of W = 1.9 GeV.
The systematic uncertainty is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%). By adding all
contributions in quadrature, a total systematic uncertainty of less than 6% is obtained.
The data were obtained with the Crystal Ball/TAPS detector setup at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.116552.v1/t17
title: "Table_F05" of "Measurement of the transverse target and beam-target asymmetries in $\eta$ meson photoproduction at MAMI"

description: Beam-target asymmetry F for c.m. energy W= 1.5882 GeV
description: A2 at MAMI. We present new data for the transverse target asymmetry T and the very first data for the beam-target
asymmetry F in the $\gamma p \to \eta p$ reaction up to a center-of-mass energy of W = 1.9 GeV.
The systematic uncertainty is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%). By adding all
contributions in quadrature, a total systematic uncertainty of less than 6% is obtained.
The data were obtained with the Crystal Ball/TAPS detector setup at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.116552.v1/t18
title: "Table_F06" of "Measurement of the transverse target and beam-target asymmetries in $\eta$ meson photoproduction at MAMI"

description: Beam-target asymmetry F for c.m. energy W= 1.6175 GeV
description: A2 at MAMI. We present new data for the transverse target asymmetry T and the very first data for the beam-target
asymmetry F in the $\gamma p \to \eta p$ reaction up to a center-of-mass energy of W = 1.9 GeV.
The systematic uncertainty is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%). By adding all
contributions in quadrature, a total systematic uncertainty of less than 6% is obtained.
The data were obtained with the Crystal Ball/TAPS detector setup at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.116552.v1/t19
title: "Table_F07" of "Measurement of the transverse target and beam-target asymmetries in $\eta$ meson photoproduction at MAMI"

description: Beam-target asymmetry F for c.m. energy W= 1.6462 GeV
description: A2 at MAMI. We present new data for the transverse target asymmetry T and the very first data for the beam-target
asymmetry F in the $\gamma p \to \eta p$ reaction up to a center-of-mass energy of W = 1.9 GeV.
The systematic uncertainty is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%). By adding all
contributions in quadrature, a total systematic uncertainty of less than 6% is obtained.
The data were obtained with the Crystal Ball/TAPS detector setup at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.116552.v1/t20
title: "Table_F08" of "Measurement of the transverse target and beam-target asymmetries in $\eta$ meson photoproduction at MAMI"

description: Beam-target asymmetry F for c.m. energy W= 1.6745 GeV
description: A2 at MAMI. We present new data for the transverse target asymmetry T and the very first data for the beam-target
asymmetry F in the $\gamma p \to \eta p$ reaction up to a center-of-mass energy of W = 1.9 GeV.
The systematic uncertainty is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%). By adding all
contributions in quadrature, a total systematic uncertainty of less than 6% is obtained.
The data were obtained with the Crystal Ball/TAPS detector setup at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.116552.v1/t21
title: "Table_F09" of "Measurement of the transverse target and beam-target asymmetries in $\eta$ meson photoproduction at MAMI"

description: Beam-target asymmetry F for c.m. energy W= 1.7022 GeV
description: A2 at MAMI. We present new data for the transverse target asymmetry T and the very first data for the beam-target
asymmetry F in the $\gamma p \to \eta p$ reaction up to a center-of-mass energy of W = 1.9 GeV.
The systematic uncertainty is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%). By adding all
contributions in quadrature, a total systematic uncertainty of less than 6% is obtained.
The data were obtained with the Crystal Ball/TAPS detector setup at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.116552.v1/t22
title: "Table_F10" of "Measurement of the transverse target and beam-target asymmetries in $\eta$ meson photoproduction at MAMI"

description: Beam-target asymmetry F for c.m. energy W= 1.7431 GeV
description: A2 at MAMI. We present new data for the transverse target asymmetry T and the very first data for the beam-target
asymmetry F in the $\gamma p \to \eta p$ reaction up to a center-of-mass energy of W = 1.9 GeV.
The systematic uncertainty is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%). By adding all
contributions in quadrature, a total systematic uncertainty of less than 6% is obtained.
The data were obtained with the Crystal Ball/TAPS detector setup at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.116552.v1/t23
title: "Table_F11" of "Measurement of the transverse target and beam-target asymmetries in $\eta$ meson photoproduction at MAMI"

description: Beam-target asymmetry F for c.m. energy W= 1.7961 GeV
description: A2 at MAMI. We present new data for the transverse target asymmetry T and the very first data for the beam-target
asymmetry F in the $\gamma p \to \eta p$ reaction up to a center-of-mass energy of W = 1.9 GeV.
The systematic uncertainty is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%). By adding all
contributions in quadrature, a total systematic uncertainty of less than 6% is obtained.
The data were obtained with the Crystal Ball/TAPS detector setup at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.116552.v1/t24
title: "Table_F12" of "Measurement of the transverse target and beam-target asymmetries in $\eta$ meson photoproduction at MAMI"

description: Beam-target asymmetry F for c.m. energy W= 1.8476 GeV
description: A2 at MAMI. We present new data for the transverse target asymmetry T and the very first data for the beam-target
asymmetry F in the $\gamma p \to \eta p$ reaction up to a center-of-mass energy of W = 1.9 GeV.
The systematic uncertainty is dominated by the determination of the degree of proton polarization (4%), the
degree of photon beam polarization (2%), and the background subtraction procedure (3%–4%). By adding all
contributions in quadrature, a total systematic uncertainty of less than 6% is obtained.
The data were obtained with the Crystal Ball/TAPS detector setup at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.126971.v1/t1
title: "Run1_tcs" of "Measurement of pi^0 photoproduction on the proton at MAMI C"

description: Run 1. Total cross section as a function of c.m. energy W.
description: A2 Collaboration at MAMI.
Differential cross sections for the $\gamma p \to \pi^0 p$ reaction have been
measured with the A2 tagged-photon facilities at the Mainz Microtron, MAMI C,
up to the center-of-mass energy W = 1.9 GeV. Data was obtained with a fine
energy and angular binning, the unprecedented statistical accuracy, and the full
angular coverage (Run 1). The total cross sections were determined by integrating
the differential cross sections for the data obtained from Run 1. 
The overall systematic uncertainty due to the calculation of the detection efficiency
and the photon-beam flux was estimated to be 4% for the data taken in Run 1 and 5% 
for the data taken in Run 2. The average systematic uncertainty in the differential 
cross sections due to the resolution in the c.m. $\Theta$ and possible imperfections 
in the angular acceptance was estimated to be 2% for the results of Run 1. The corresponding
systematic uncertainty for the results of Run 2 is at least twice as high.
The data was obtained with Crystal Ball/TAPS experimental setup.
DOI: 10.17182/hepdata.126971.v1/t2
title: "Run1_dcs01" of "Measurement of pi^0 photoproduction on the proton at MAMI C"

description: Excitation function at cos(Theta_eta)= -0.967
description: A2 Collaboration at MAMI.
Differential cross sections for the $\gamma p \to \pi^0 p$ reaction have been
measured with the A2 tagged-photon facilities at the Mainz Microtron, MAMI C,
up to the center-of-mass energy W = 1.9 GeV. Data was obtained with a fine
energy and angular binning, the unprecedented statistical accuracy, and the full
angular coverage (Run 1). The total cross sections were determined by integrating
the differential cross sections for the data obtained from Run 1. 
The overall systematic uncertainty due to the calculation of the detection efficiency
and the photon-beam flux was estimated to be 4% for the data taken in Run 1 and 5% 
for the data taken in Run 2. The average systematic uncertainty in the differential 
cross sections due to the resolution in the c.m. $\Theta$ and possible imperfections 
in the angular acceptance was estimated to be 2% for the results of Run 1. The corresponding
systematic uncertainty for the results of Run 2 is at least twice as high.
The data was obtained with Crystal Ball/TAPS experimental setup.
DOI: 10.17182/hepdata.126971.v1/t3
title: "Run1_dcs02" of "Measurement of pi^0 photoproduction on the proton at MAMI C"

description: Excitation function at cos(Theta_eta)= -0.900
description: A2 Collaboration at MAMI.
Differential cross sections for the $\gamma p \to \pi^0 p$ reaction have been
measured with the A2 tagged-photon facilities at the Mainz Microtron, MAMI C,
up to the center-of-mass energy W = 1.9 GeV. Data was obtained with a fine
energy and angular binning, the unprecedented statistical accuracy, and the full
angular coverage (Run 1). The total cross sections were determined by integrating
the differential cross sections for the data obtained from Run 1. 
The overall systematic uncertainty due to the calculation of the detection efficiency
and the photon-beam flux was estimated to be 4% for the data taken in Run 1 and 5% 
for the data taken in Run 2. The average systematic uncertainty in the differential 
cross sections due to the resolution in the c.m. $\Theta$ and possible imperfections 
in the angular acceptance was estimated to be 2% for the results of Run 1. The corresponding
systematic uncertainty for the results of Run 2 is at least twice as high.
The data was obtained with Crystal Ball/TAPS experimental setup.
DOI: 10.17182/hepdata.126971.v1/t4
title: "Run1_dcs03" of "Measurement of pi^0 photoproduction on the proton at MAMI C"

description: Excitation function at cos(Theta_eta)= -0.833
description: A2 Collaboration at MAMI.
Differential cross sections for the $\gamma p \to \pi^0 p$ reaction have been
measured with the A2 tagged-photon facilities at the Mainz Microtron, MAMI C,
up to the center-of-mass energy W = 1.9 GeV. Data was obtained with a fine
energy and angular binning, the unprecedented statistical accuracy, and the full
angular coverage (Run 1). The total cross sections were determined by integrating
the differential cross sections for the data obtained from Run 1. 
The overall systematic uncertainty due to the calculation of the detection efficiency
and the photon-beam flux was estimated to be 4% for the data taken in Run 1 and 5% 
for the data taken in Run 2. The average systematic uncertainty in the differential 
cross sections due to the resolution in the c.m. $\Theta$ and possible imperfections 
in the angular acceptance was estimated to be 2% for the results of Run 1. The corresponding
systematic uncertainty for the results of Run 2 is at least twice as high.
The data was obtained with Crystal Ball/TAPS experimental setup.
DOI: 10.17182/hepdata.126971.v1/t10
title: "Run1_dcs09" of "Measurement of pi^0 photoproduction on the proton at MAMI C"

description: Excitation function at cos(Theta_eta)= -0.433
description: A2 Collaboration at MAMI.
Differential cross sections for the $\gamma p \to \pi^0 p$ reaction have been
measured with the A2 tagged-photon facilities at the Mainz Microtron, MAMI C,
up to the center-of-mass energy W = 1.9 GeV. Data was obtained with a fine
energy and angular binning, the unprecedented statistical accuracy, and the full
angular coverage (Run 1). The total cross sections were determined by integrating
the differential cross sections for the data obtained from Run 1. 
The overall systematic uncertainty due to the calculation of the detection efficiency
and the photon-beam flux was estimated to be 4% for the data taken in Run 1 and 5% 
for the data taken in Run 2. The average systematic uncertainty in the differential 
cross sections due to the resolution in the c.m. $\Theta$ and possible imperfections 
in the angular acceptance was estimated to be 2% for the results of Run 1. The corresponding
systematic uncertainty for the results of Run 2 is at least twice as high.
The data was obtained with Crystal Ball/TAPS experimental setup.
DOI: 10.17182/hepdata.126971.v1/t11
title: "Run1_dcs10" of "Measurement of pi^0 photoproduction on the proton at MAMI C"

description: Excitation function at cos(Theta_eta)= -0.367
description: A2 Collaboration at MAMI.
Differential cross sections for the $\gamma p \to \pi^0 p$ reaction have been
measured with the A2 tagged-photon facilities at the Mainz Microtron, MAMI C,
up to the center-of-mass energy W = 1.9 GeV. Data was obtained with a fine
energy and angular binning, the unprecedented statistical accuracy, and the full
angular coverage (Run 1). The total cross sections were determined by integrating
the differential cross sections for the data obtained from Run 1. 
The overall systematic uncertainty due to the calculation of the detection efficiency
and the photon-beam flux was estimated to be 4% for the data taken in Run 1 and 5% 
for the data taken in Run 2. The average systematic uncertainty in the differential 
cross sections due to the resolution in the c.m. $\Theta$ and possible imperfections 
in the angular acceptance was estimated to be 2% for the results of Run 1. The corresponding
systematic uncertainty for the results of Run 2 is at least twice as high.
The data was obtained with Crystal Ball/TAPS experimental setup.
DOI: 10.17182/hepdata.126971.v1/t12
title: "Run1_dcs11" of "Measurement of pi^0 photoproduction on the proton at MAMI C"

description: Excitation function at cos(Theta_eta)= -0.300
description: A2 Collaboration at MAMI.
Differential cross sections for the $\gamma p \to \pi^0 p$ reaction have been
measured with the A2 tagged-photon facilities at the Mainz Microtron, MAMI C,
up to the center-of-mass energy W = 1.9 GeV. Data was obtained with a fine
energy and angular binning, the unprecedented statistical accuracy, and the full
angular coverage (Run 1). The total cross sections were determined by integrating
the differential cross sections for the data obtained from Run 1. 
The overall systematic uncertainty due to the calculation of the detection efficiency
and the photon-beam flux was estimated to be 4% for the data taken in Run 1 and 5% 
for the data taken in Run 2. The average systematic uncertainty in the differential 
cross sections due to the resolution in the c.m. $\Theta$ and possible imperfections 
in the angular acceptance was estimated to be 2% for the results of Run 1. The corresponding
systematic uncertainty for the results of Run 2 is at least twice as high.
The data was obtained with Crystal Ball/TAPS experimental setup.
DOI: 10.17182/hepdata.126971.v1/t5
title: "Run1_dcs04" of "Measurement of pi^0 photoproduction on the proton at MAMI C"

description: Excitation function at cos(Theta_eta)= -0.767
description: A2 Collaboration at MAMI.
Differential cross sections for the $\gamma p \to \pi^0 p$ reaction have been
measured with the A2 tagged-photon facilities at the Mainz Microtron, MAMI C,
up to the center-of-mass energy W = 1.9 GeV. Data was obtained with a fine
energy and angular binning, the unprecedented statistical accuracy, and the full
angular coverage (Run 1). The total cross sections were determined by integrating
the differential cross sections for the data obtained from Run 1. 
The overall systematic uncertainty due to the calculation of the detection efficiency
and the photon-beam flux was estimated to be 4% for the data taken in Run 1 and 5% 
for the data taken in Run 2. The average systematic uncertainty in the differential 
cross sections due to the resolution in the c.m. $\Theta$ and possible imperfections 
in the angular acceptance was estimated to be 2% for the results of Run 1. The corresponding
systematic uncertainty for the results of Run 2 is at least twice as high.
The data was obtained with Crystal Ball/TAPS experimental setup.
DOI: 10.17182/hepdata.126971.v1/t6
title: "Run1_dcs05" of "Measurement of pi^0 photoproduction on the proton at MAMI C"

description: Excitation function at cos(Theta_eta)= -0.700
description: A2 Collaboration at MAMI.
Differential cross sections for the $\gamma p \to \pi^0 p$ reaction have been
measured with the A2 tagged-photon facilities at the Mainz Microtron, MAMI C,
up to the center-of-mass energy W = 1.9 GeV. Data was obtained with a fine
energy and angular binning, the unprecedented statistical accuracy, and the full
angular coverage (Run 1). The total cross sections were determined by integrating
the differential cross sections for the data obtained from Run 1. 
The overall systematic uncertainty due to the calculation of the detection efficiency
and the photon-beam flux was estimated to be 4% for the data taken in Run 1 and 5% 
for the data taken in Run 2. The average systematic uncertainty in the differential 
cross sections due to the resolution in the c.m. $\Theta$ and possible imperfections 
in the angular acceptance was estimated to be 2% for the results of Run 1. The corresponding
systematic uncertainty for the results of Run 2 is at least twice as high.
The data was obtained with Crystal Ball/TAPS experimental setup.