cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.130236.v1/t2
title: "K0L0-tcs.yaml" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Total cross section as a function of c.m. energy W.
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.25549/vercoutere-ouc110611400
title: 3 nude black and red women beside a window

description: Three nude females: one is black outlined in red depicted from breasts to feet is jumping up and is in front of the other two female; one is red and white depicted from the back side from neck to calves and is standing; one is pink depicted from chest to ankle and is standing beside the red and white female. Large arched window with lines of various colored designs is next to the females wotj a background of solid dark green. See description of 001 for OT notes.
DOI: 10.17182/hepdata.130236.v1/t10
title: "K0Sp-dcs07" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.855 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t3
title: "K0S0-tcs.yaml" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Total cross section as a function of c.m. energy W.
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t4
title: "K0Sp-dcs01" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.720 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t5
title: "K0Sp-dcs02" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.750 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t6
title: "K0Sp-dcs03" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.775 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t7
title: "K0Sp-dcs04" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.795 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t8
title: "K0Sp-dcs05" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.815 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t9
title: "K0Sp-dcs06" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.835 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t11
title: "K0L0-dcs01" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.630 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t12
title: "K0L0-dcs02" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.660 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t13
title: "K0L0-dcs03" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.690 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t14
title: "K0L0-dcs04" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.720 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t15
title: "K0L0-dcs05" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.750 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t16
title: "K0L0-dcs06" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.775 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t17
title: "K0L0-dcs07" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.795 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t18
title: "K0L0-dcs08" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.815 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t19
title: "K0L0-dcs09" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.835 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.