cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.116551.v1/t19
title: "Table_T19" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.6491 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t21
title: "Table_T21" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.6828 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t22
title: "Table_T22" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.6995 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t24
title: "Table_T24" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.7323 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t25
title: "Table_T25" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.7485 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t27
title: "Table_T27" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.7804 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.25549/vercoutere-ouc110611934
title: Woven wall hanging in white and black

description: Black warp thread and white weft yarn creating a center diamond design flanked by a zig zag design on each side. Gold metallic thread interwoven with black thread. Black border on each vertical end next to the fringe.
DOI: 10.17182/hepdata.116551.v1/t26
title: "Table_T26" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.7645 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t31
title: "Table_T31" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.8425 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t23
title: "Table_T23" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.7160 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t30
title: "Table_T30" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.8272 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t32
title: "Table_T32" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.8577 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t28
title: "Table_T28" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.7961 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t29
title: "Table_T29" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.8117 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t34
title: "Table_T34" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.8878 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t38
title: "Table_F04" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Beam-target asymmetry F for c.m. energy W= 1.3693 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t39
title: "Table_F05" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Beam-target asymmetry F for c.m. energy W= 1.3897 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t40
title: "Table_F06" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Beam-target asymmetry F for c.m. energy W= 1.4098 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.25549/vercoutere-ouc110637185
title: Woman's head sculpture with ash tray molded in clay

description: White glazed molded clay sculpture of a woman with shoulder length hair; includes a small receptacle for ashes or other at the ottom front
DOI: 10.17182/hepdata.116551.v1/t33
title: "Table_T33" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Target asymmetry T for c.m. energy W= 1.8728 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t35
title: "Table_F01" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Beam-target asymmetry F for c.m. energy W= 1.3062 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t36
title: "Table_F02" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Beam-target asymmetry F for c.m. energy W= 1.3275 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t37
title: "Table_F03" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Beam-target asymmetry F for c.m. energy W= 1.3486 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t44
title: "Table_F10" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Beam-target asymmetry F for c.m. energy W= 1.4875 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t45
title: "Table_F11" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Beam-target asymmetry F for c.m. energy W= 1.5063 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t47
title: "Table_F13" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Beam-target asymmetry F for c.m. energy W= 1.5432 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.
DOI: 10.17182/hepdata.116551.v1/t48
title: "Table_F14" of "T and F asymmetries in $π^0$ photoproduction on the proton"

description: Beam-target asymmetry F for c.m. energy W= 1.5614 GeV
description: A2 at MAMI. The $\gamma p \to \pi^0 p$ reaction was studied at laboratory photon
energies from 425 to 1445 MeV with a transversely polarized target and a longitudinally
polarized beam. The beam-target asymmetry F was measured for the first time and new
high precision data for the target asymmetry T were obtained. 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 experiment was performed at the photon tagging facility of
the Mainz Microtron (MAMI) using the Crystal Ball/TAPS detector setup.