cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.130796.v1/t10
title: "K+L0_dcs10" of "$K^+\Lambda$ and $K^+\Sigma^0$ photoproduction with fine center-of-mass energy resolution"

description: Excitation function at cos(Theta_K+)cm = 0.1
description: A2 Collaboration at MAMI.
Measurements of $\gamma p \to K^+ \Lambda$ and $\gamma p \to K^+ \Sigma^0$
cross-sections have been obtained with the photon tagging facility
and the Crystal Ball calorimeter at MAMI-C. The measurement uses
a novel $K^+$ meson identification technique in which the weak decay
products are characterized using the energy and timing
characteristics of the energy deposit in the calorimeter, a method
that has the potential to be applied at many other facilities. The
fine center-of-mass energy (W) resolution and statistical accuracy
of the new data results in a significant impact on partial wave
analyses aiming to better establish the excitation spectrum of the
nucleon. Systematic effects from the modeling of the experimental
trigger in the simulation were typically 4% near threshold for
$K^+ \Lambda$ and reducing with the beam energy. For $K^+ \Sigma^0$,
the uncertainty was 2–3% near threshold and only at very backward
angles. Systematic errors from non-hydrogen components of the target
cell, target cell length and PID efficiency were each less than 1%.
DOI: 10.17182/hepdata.130796.v1/t11
title: "K+L0_dcs11" of "$K^+\Lambda$ and $K^+\Sigma^0$ photoproduction with fine center-of-mass energy resolution"

description: Excitation function at cos(Theta_K+)cm = 0.2
description: A2 Collaboration at MAMI.
Measurements of $\gamma p \to K^+ \Lambda$ and $\gamma p \to K^+ \Sigma^0$
cross-sections have been obtained with the photon tagging facility
and the Crystal Ball calorimeter at MAMI-C. The measurement uses
a novel $K^+$ meson identification technique in which the weak decay
products are characterized using the energy and timing
characteristics of the energy deposit in the calorimeter, a method
that has the potential to be applied at many other facilities. The
fine center-of-mass energy (W) resolution and statistical accuracy
of the new data results in a significant impact on partial wave
analyses aiming to better establish the excitation spectrum of the
nucleon. Systematic effects from the modeling of the experimental
trigger in the simulation were typically 4% near threshold for
$K^+ \Lambda$ and reducing with the beam energy. For $K^+ \Sigma^0$,
the uncertainty was 2–3% near threshold and only at very backward
angles. Systematic errors from non-hydrogen components of the target
cell, target cell length and PID efficiency were each less than 1%.
DOI: 10.17182/hepdata.130796.v1/t12
title: "K+L0_dcs12" of "$K^+\Lambda$ and $K^+\Sigma^0$ photoproduction with fine center-of-mass energy resolution"

description: Excitation function at cos(Theta_K+)cm = 0.3
description: A2 Collaboration at MAMI.
Measurements of $\gamma p \to K^+ \Lambda$ and $\gamma p \to K^+ \Sigma^0$
cross-sections have been obtained with the photon tagging facility
and the Crystal Ball calorimeter at MAMI-C. The measurement uses
a novel $K^+$ meson identification technique in which the weak decay
products are characterized using the energy and timing
characteristics of the energy deposit in the calorimeter, a method
that has the potential to be applied at many other facilities. The
fine center-of-mass energy (W) resolution and statistical accuracy
of the new data results in a significant impact on partial wave
analyses aiming to better establish the excitation spectrum of the
nucleon. Systematic effects from the modeling of the experimental
trigger in the simulation were typically 4% near threshold for
$K^+ \Lambda$ and reducing with the beam energy. For $K^+ \Sigma^0$,
the uncertainty was 2–3% near threshold and only at very backward
angles. Systematic errors from non-hydrogen components of the target
cell, target cell length and PID efficiency were each less than 1%.
DOI: 10.17182/hepdata.130796.v1/t5
title: "K+L0_dcs05" of "$K^+\Lambda$ and $K^+\Sigma^0$ photoproduction with fine center-of-mass energy resolution"

description: Excitation function at cos(Theta_K+)cm = -0.4
description: A2 Collaboration at MAMI.
Measurements of $\gamma p \to K^+ \Lambda$ and $\gamma p \to K^+ \Sigma^0$
cross-sections have been obtained with the photon tagging facility
and the Crystal Ball calorimeter at MAMI-C. The measurement uses
a novel $K^+$ meson identification technique in which the weak decay
products are characterized using the energy and timing
characteristics of the energy deposit in the calorimeter, a method
that has the potential to be applied at many other facilities. The
fine center-of-mass energy (W) resolution and statistical accuracy
of the new data results in a significant impact on partial wave
analyses aiming to better establish the excitation spectrum of the
nucleon. Systematic effects from the modeling of the experimental
trigger in the simulation were typically 4% near threshold for
$K^+ \Lambda$ and reducing with the beam energy. For $K^+ \Sigma^0$,
the uncertainty was 2–3% near threshold and only at very backward
angles. Systematic errors from non-hydrogen components of the target
cell, target cell length and PID efficiency were each less than 1%.
DOI: 10.17182/hepdata.130796.v1/t6
title: "K+L0_dcs06" of "$K^+\Lambda$ and $K^+\Sigma^0$ photoproduction with fine center-of-mass energy resolution"

description: Excitation function at cos(Theta_K+)cm = -0.3
description: A2 Collaboration at MAMI.
Measurements of $\gamma p \to K^+ \Lambda$ and $\gamma p \to K^+ \Sigma^0$
cross-sections have been obtained with the photon tagging facility
and the Crystal Ball calorimeter at MAMI-C. The measurement uses
a novel $K^+$ meson identification technique in which the weak decay
products are characterized using the energy and timing
characteristics of the energy deposit in the calorimeter, a method
that has the potential to be applied at many other facilities. The
fine center-of-mass energy (W) resolution and statistical accuracy
of the new data results in a significant impact on partial wave
analyses aiming to better establish the excitation spectrum of the
nucleon. Systematic effects from the modeling of the experimental
trigger in the simulation were typically 4% near threshold for
$K^+ \Lambda$ and reducing with the beam energy. For $K^+ \Sigma^0$,
the uncertainty was 2–3% near threshold and only at very backward
angles. Systematic errors from non-hydrogen components of the target
cell, target cell length and PID efficiency were each less than 1%.
DOI: 10.17182/hepdata.130796.v1/t7
title: "K+L0_dcs07" of "$K^+\Lambda$ and $K^+\Sigma^0$ photoproduction with fine center-of-mass energy resolution"

description: Excitation function at cos(Theta_K+)cm = -0.2
description: A2 Collaboration at MAMI.
Measurements of $\gamma p \to K^+ \Lambda$ and $\gamma p \to K^+ \Sigma^0$
cross-sections have been obtained with the photon tagging facility
and the Crystal Ball calorimeter at MAMI-C. The measurement uses
a novel $K^+$ meson identification technique in which the weak decay
products are characterized using the energy and timing
characteristics of the energy deposit in the calorimeter, a method
that has the potential to be applied at many other facilities. The
fine center-of-mass energy (W) resolution and statistical accuracy
of the new data results in a significant impact on partial wave
analyses aiming to better establish the excitation spectrum of the
nucleon. Systematic effects from the modeling of the experimental
trigger in the simulation were typically 4% near threshold for
$K^+ \Lambda$ and reducing with the beam energy. For $K^+ \Sigma^0$,
the uncertainty was 2–3% near threshold and only at very backward
angles. Systematic errors from non-hydrogen components of the target
cell, target cell length and PID efficiency were each less than 1%.
DOI: 10.17182/hepdata.130796.v1/t8
title: "K+L0_dcs08" of "$K^+\Lambda$ and $K^+\Sigma^0$ photoproduction with fine center-of-mass energy resolution"

description: Excitation function at cos(Theta_K+)cm = -0.1
description: A2 Collaboration at MAMI.
Measurements of $\gamma p \to K^+ \Lambda$ and $\gamma p \to K^+ \Sigma^0$
cross-sections have been obtained with the photon tagging facility
and the Crystal Ball calorimeter at MAMI-C. The measurement uses
a novel $K^+$ meson identification technique in which the weak decay
products are characterized using the energy and timing
characteristics of the energy deposit in the calorimeter, a method
that has the potential to be applied at many other facilities. The
fine center-of-mass energy (W) resolution and statistical accuracy
of the new data results in a significant impact on partial wave
analyses aiming to better establish the excitation spectrum of the
nucleon. Systematic effects from the modeling of the experimental
trigger in the simulation were typically 4% near threshold for
$K^+ \Lambda$ and reducing with the beam energy. For $K^+ \Sigma^0$,
the uncertainty was 2–3% near threshold and only at very backward
angles. Systematic errors from non-hydrogen components of the target
cell, target cell length and PID efficiency were each less than 1%.
DOI: 10.17182/hepdata.130796.v1/t9
title: "K+L0_dcs09" of "$K^+\Lambda$ and $K^+\Sigma^0$ photoproduction with fine center-of-mass energy resolution"

description: Excitation function at cos(Theta_K+)cm = 0.0
description: A2 Collaboration at MAMI.
Measurements of $\gamma p \to K^+ \Lambda$ and $\gamma p \to K^+ \Sigma^0$
cross-sections have been obtained with the photon tagging facility
and the Crystal Ball calorimeter at MAMI-C. The measurement uses
a novel $K^+$ meson identification technique in which the weak decay
products are characterized using the energy and timing
characteristics of the energy deposit in the calorimeter, a method
that has the potential to be applied at many other facilities. The
fine center-of-mass energy (W) resolution and statistical accuracy
of the new data results in a significant impact on partial wave
analyses aiming to better establish the excitation spectrum of the
nucleon. Systematic effects from the modeling of the experimental
trigger in the simulation were typically 4% near threshold for
$K^+ \Lambda$ and reducing with the beam energy. For $K^+ \Sigma^0$,
the uncertainty was 2–3% near threshold and only at very backward
angles. Systematic errors from non-hydrogen components of the target
cell, target cell length and PID efficiency were each less than 1%.
DOI: 10.25549/vercoutere-ouc110610466
title: Woman in harem pants plus word salad

description: One orange female with brown hair wearing a red bra and red harem pants standing with one hand to her head and one arm raised; area around the figure is green; a word salad written in magenta cursive writing is in the left lower section of the page next to the figure; remainder of the page is blank. See description of 347 for OT notes.
DOI: 10.17182/hepdata.130796.v1/t13
title: "K+L0_dcs13" of "$K^+\Lambda$ and $K^+\Sigma^0$ photoproduction with fine center-of-mass energy resolution"

description: Excitation function at cos(Theta_K+)cm = 0.4
description: A2 Collaboration at MAMI.
Measurements of $\gamma p \to K^+ \Lambda$ and $\gamma p \to K^+ \Sigma^0$
cross-sections have been obtained with the photon tagging facility
and the Crystal Ball calorimeter at MAMI-C. The measurement uses
a novel $K^+$ meson identification technique in which the weak decay
products are characterized using the energy and timing
characteristics of the energy deposit in the calorimeter, a method
that has the potential to be applied at many other facilities. The
fine center-of-mass energy (W) resolution and statistical accuracy
of the new data results in a significant impact on partial wave
analyses aiming to better establish the excitation spectrum of the
nucleon. Systematic effects from the modeling of the experimental
trigger in the simulation were typically 4% near threshold for
$K^+ \Lambda$ and reducing with the beam energy. For $K^+ \Sigma^0$,
the uncertainty was 2–3% near threshold and only at very backward
angles. Systematic errors from non-hydrogen components of the target
cell, target cell length and PID efficiency were each less than 1%.
DOI: 10.17182/hepdata.130796.v1/t14
title: "K0S0_dcs01" of "$K^+\Lambda$ and $K^+\Sigma^0$ photoproduction with fine center-of-mass energy resolution"

description: Excitation function at cos(Theta_K+)cm = -0.8
description: A2 Collaboration at MAMI.
Measurements of $\gamma p \to K^+ \Lambda$ and $\gamma p \to K^+ \Sigma^0$
cross-sections have been obtained with the photon tagging facility
and the Crystal Ball calorimeter at MAMI-C. The measurement uses
a novel $K^+$ meson identification technique in which the weak decay
products are characterized using the energy and timing
characteristics of the energy deposit in the calorimeter, a method
that has the potential to be applied at many other facilities. The
fine center-of-mass energy (W) resolution and statistical accuracy
of the new data results in a significant impact on partial wave
analyses aiming to better establish the excitation spectrum of the
nucleon. Systematic effects from the modeling of the experimental
trigger in the simulation were typically 4% near threshold for
$K^+ \Lambda$ and reducing with the beam energy. For $K^+ \Sigma^0$,
the uncertainty was 2–3% near threshold and only at very backward
angles. Systematic errors from non-hydrogen components of the target
cell, target cell length and PID efficiency were each less than 1%.
DOI: 10.17182/hepdata.130796.v1/t15
title: "K0S0_dcs02" of "$K^+\Lambda$ and $K^+\Sigma^0$ photoproduction with fine center-of-mass energy resolution"

description: Excitation function at cos(Theta_K+)cm = -0.7
description: A2 Collaboration at MAMI.
Measurements of $\gamma p \to K^+ \Lambda$ and $\gamma p \to K^+ \Sigma^0$
cross-sections have been obtained with the photon tagging facility
and the Crystal Ball calorimeter at MAMI-C. The measurement uses
a novel $K^+$ meson identification technique in which the weak decay
products are characterized using the energy and timing
characteristics of the energy deposit in the calorimeter, a method
that has the potential to be applied at many other facilities. The
fine center-of-mass energy (W) resolution and statistical accuracy
of the new data results in a significant impact on partial wave
analyses aiming to better establish the excitation spectrum of the
nucleon. Systematic effects from the modeling of the experimental
trigger in the simulation were typically 4% near threshold for
$K^+ \Lambda$ and reducing with the beam energy. For $K^+ \Sigma^0$,
the uncertainty was 2–3% near threshold and only at very backward
angles. Systematic errors from non-hydrogen components of the target
cell, target cell length and PID efficiency were each less than 1%.
DOI: 10.17182/hepdata.130796.v1/t16
title: "K0S0_dcs03" of "$K^+\Lambda$ and $K^+\Sigma^0$ photoproduction with fine center-of-mass energy resolution"

description: Excitation function at cos(Theta_K+)cm = -0.6
description: A2 Collaboration at MAMI.
Measurements of $\gamma p \to K^+ \Lambda$ and $\gamma p \to K^+ \Sigma^0$
cross-sections have been obtained with the photon tagging facility
and the Crystal Ball calorimeter at MAMI-C. The measurement uses
a novel $K^+$ meson identification technique in which the weak decay
products are characterized using the energy and timing
characteristics of the energy deposit in the calorimeter, a method
that has the potential to be applied at many other facilities. The
fine center-of-mass energy (W) resolution and statistical accuracy
of the new data results in a significant impact on partial wave
analyses aiming to better establish the excitation spectrum of the
nucleon. Systematic effects from the modeling of the experimental
trigger in the simulation were typically 4% near threshold for
$K^+ \Lambda$ and reducing with the beam energy. For $K^+ \Sigma^0$,
the uncertainty was 2–3% near threshold and only at very backward
angles. Systematic errors from non-hydrogen components of the target
cell, target cell length and PID efficiency were each less than 1%.
DOI: 10.17182/hepdata.130796.v1/t17
title: "K0S0_dcs04" of "$K^+\Lambda$ and $K^+\Sigma^0$ photoproduction with fine center-of-mass energy resolution"

description: Excitation function at cos(Theta_K+)cm = -0.5
description: A2 Collaboration at MAMI.
Measurements of $\gamma p \to K^+ \Lambda$ and $\gamma p \to K^+ \Sigma^0$
cross-sections have been obtained with the photon tagging facility
and the Crystal Ball calorimeter at MAMI-C. The measurement uses
a novel $K^+$ meson identification technique in which the weak decay
products are characterized using the energy and timing
characteristics of the energy deposit in the calorimeter, a method
that has the potential to be applied at many other facilities. The
fine center-of-mass energy (W) resolution and statistical accuracy
of the new data results in a significant impact on partial wave
analyses aiming to better establish the excitation spectrum of the
nucleon. Systematic effects from the modeling of the experimental
trigger in the simulation were typically 4% near threshold for
$K^+ \Lambda$ and reducing with the beam energy. For $K^+ \Sigma^0$,
the uncertainty was 2–3% near threshold and only at very backward
angles. Systematic errors from non-hydrogen components of the target
cell, target cell length and PID efficiency were each less than 1%.
DOI: 10.17182/hepdata.130796.v1/t18
title: "K0S0_dcs05" of "$K^+\Lambda$ and $K^+\Sigma^0$ photoproduction with fine center-of-mass energy resolution"

description: Excitation function at cos(Theta_K+)cm = -0.4
description: A2 Collaboration at MAMI.
Measurements of $\gamma p \to K^+ \Lambda$ and $\gamma p \to K^+ \Sigma^0$
cross-sections have been obtained with the photon tagging facility
and the Crystal Ball calorimeter at MAMI-C. The measurement uses
a novel $K^+$ meson identification technique in which the weak decay
products are characterized using the energy and timing
characteristics of the energy deposit in the calorimeter, a method
that has the potential to be applied at many other facilities. The
fine center-of-mass energy (W) resolution and statistical accuracy
of the new data results in a significant impact on partial wave
analyses aiming to better establish the excitation spectrum of the
nucleon. Systematic effects from the modeling of the experimental
trigger in the simulation were typically 4% near threshold for
$K^+ \Lambda$ and reducing with the beam energy. For $K^+ \Sigma^0$,
the uncertainty was 2–3% near threshold and only at very backward
angles. Systematic errors from non-hydrogen components of the target
cell, target cell length and PID efficiency were each less than 1%.
DOI: 10.17182/hepdata.130796.v1/t19
title: "K0S0_dcs06" of "$K^+\Lambda$ and $K^+\Sigma^0$ photoproduction with fine center-of-mass energy resolution"

description: Excitation function at cos(Theta_K+)cm = -0.3
description: A2 Collaboration at MAMI.
Measurements of $\gamma p \to K^+ \Lambda$ and $\gamma p \to K^+ \Sigma^0$
cross-sections have been obtained with the photon tagging facility
and the Crystal Ball calorimeter at MAMI-C. The measurement uses
a novel $K^+$ meson identification technique in which the weak decay
products are characterized using the energy and timing
characteristics of the energy deposit in the calorimeter, a method
that has the potential to be applied at many other facilities. The
fine center-of-mass energy (W) resolution and statistical accuracy
of the new data results in a significant impact on partial wave
analyses aiming to better establish the excitation spectrum of the
nucleon. Systematic effects from the modeling of the experimental
trigger in the simulation were typically 4% near threshold for
$K^+ \Lambda$ and reducing with the beam energy. For $K^+ \Sigma^0$,
the uncertainty was 2–3% near threshold and only at very backward
angles. Systematic errors from non-hydrogen components of the target
cell, target cell length and PID efficiency were each less than 1%.
DOI: 10.17182/hepdata.130796.v1/t20
title: "K0S0_dcs07" of "$K^+\Lambda$ and $K^+\Sigma^0$ photoproduction with fine center-of-mass energy resolution"

description: Excitation function at cos(Theta_K+)cm = -0.2
description: A2 Collaboration at MAMI.
Measurements of $\gamma p \to K^+ \Lambda$ and $\gamma p \to K^+ \Sigma^0$
cross-sections have been obtained with the photon tagging facility
and the Crystal Ball calorimeter at MAMI-C. The measurement uses
a novel $K^+$ meson identification technique in which the weak decay
products are characterized using the energy and timing
characteristics of the energy deposit in the calorimeter, a method
that has the potential to be applied at many other facilities. The
fine center-of-mass energy (W) resolution and statistical accuracy
of the new data results in a significant impact on partial wave
analyses aiming to better establish the excitation spectrum of the
nucleon. Systematic effects from the modeling of the experimental
trigger in the simulation were typically 4% near threshold for
$K^+ \Lambda$ and reducing with the beam energy. For $K^+ \Sigma^0$,
the uncertainty was 2–3% near threshold and only at very backward
angles. Systematic errors from non-hydrogen components of the target
cell, target cell length and PID efficiency were each less than 1%.
DOI: 10.17182/hepdata.130796.v1/t21
title: "K0S0_dcs08" of "$K^+\Lambda$ and $K^+\Sigma^0$ photoproduction with fine center-of-mass energy resolution"

description: Excitation function at cos(Theta_K+)cm = -0.1
description: A2 Collaboration at MAMI.
Measurements of $\gamma p \to K^+ \Lambda$ and $\gamma p \to K^+ \Sigma^0$
cross-sections have been obtained with the photon tagging facility
and the Crystal Ball calorimeter at MAMI-C. The measurement uses
a novel $K^+$ meson identification technique in which the weak decay
products are characterized using the energy and timing
characteristics of the energy deposit in the calorimeter, a method
that has the potential to be applied at many other facilities. The
fine center-of-mass energy (W) resolution and statistical accuracy
of the new data results in a significant impact on partial wave
analyses aiming to better establish the excitation spectrum of the
nucleon. Systematic effects from the modeling of the experimental
trigger in the simulation were typically 4% near threshold for
$K^+ \Lambda$ and reducing with the beam energy. For $K^+ \Sigma^0$,
the uncertainty was 2–3% near threshold and only at very backward
angles. Systematic errors from non-hydrogen components of the target
cell, target cell length and PID efficiency were each less than 1%.
DOI: 10.17182/hepdata.130796.v1/t22
title: "K0S0_dcs09" of "$K^+\Lambda$ and $K^+\Sigma^0$ photoproduction with fine center-of-mass energy resolution"

description: Excitation function at cos(Theta_K+)cm = 0.0
description: A2 Collaboration at MAMI.
Measurements of $\gamma p \to K^+ \Lambda$ and $\gamma p \to K^+ \Sigma^0$
cross-sections have been obtained with the photon tagging facility
and the Crystal Ball calorimeter at MAMI-C. The measurement uses
a novel $K^+$ meson identification technique in which the weak decay
products are characterized using the energy and timing
characteristics of the energy deposit in the calorimeter, a method
that has the potential to be applied at many other facilities. The
fine center-of-mass energy (W) resolution and statistical accuracy
of the new data results in a significant impact on partial wave
analyses aiming to better establish the excitation spectrum of the
nucleon. Systematic effects from the modeling of the experimental
trigger in the simulation were typically 4% near threshold for
$K^+ \Lambda$ and reducing with the beam energy. For $K^+ \Sigma^0$,
the uncertainty was 2–3% near threshold and only at very backward
angles. Systematic errors from non-hydrogen components of the target
cell, target cell length and PID efficiency were each less than 1%.