cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.130198.v1/t18
title: "dcs17" of "Photoproduction of the omega meson off the proton near threshold"

description: Differential cross section at W= 1.8504 GeV
description: A2 Collaboration at MAMI.
An experimental study of $\omega$ photoproduction on the proton was
conducted by using the Crystal Ball and TAPS multiphoton
spectrometers together with the photon tagging facility at the Mainz
Microtron MAMI.
The $\gamma p \to \omega p$ differential cross sections are measured from
threshold to the incident-photon energy $E_{\gamma}$=1.4 GeV (W=1.87 GeV
for the center-of-mass energy) with 15-MeV binning in $E_{\gamma}$ and
full production-angle coverage. One contribution to the systematic
uncertainty comes from the uncertainty in the shape of the
background. It is not larger than 6%. Another contribution comes from
the determination of the detector acceptance and the photon-beam flux.
It was estimated as 5%.
The quality of the present data near threshold gives access to a 
variety of interesting physics aspects. As an example, an estimation 
of the $\omega$N scattering length is provided.
DOI: 10.17182/hepdata.130198.v1/t19
title: "dcs18" of "Photoproduction of the omega meson off the proton near threshold"

description: Differential cross section at W= 1.8581 GeV
description: A2 Collaboration at MAMI.
An experimental study of $\omega$ photoproduction on the proton was
conducted by using the Crystal Ball and TAPS multiphoton
spectrometers together with the photon tagging facility at the Mainz
Microtron MAMI.
The $\gamma p \to \omega p$ differential cross sections are measured from
threshold to the incident-photon energy $E_{\gamma}$=1.4 GeV (W=1.87 GeV
for the center-of-mass energy) with 15-MeV binning in $E_{\gamma}$ and
full production-angle coverage. One contribution to the systematic
uncertainty comes from the uncertainty in the shape of the
background. It is not larger than 6%. Another contribution comes from
the determination of the detector acceptance and the photon-beam flux.
It was estimated as 5%.
The quality of the present data near threshold gives access to a 
variety of interesting physics aspects. As an example, an estimation 
of the $\omega$N scattering length is provided.
DOI: 10.25549/vercoutere-ouc110611337
title: Partial view of 4 nude women

description: Four nude females: two yellow, one red, and one black. The red one is depicted from head to hip; the others show only bent legs. The background includes walls of red floral and brown and red bricks. See description of 001 for OT notes.
DOI: 10.17182/hepdata.130198.v1/t20
title: "dcs19" of "Photoproduction of the omega meson off the proton near threshold"

description: Differential cross section at W= 1.8657 GeV
description: A2 Collaboration at MAMI.
An experimental study of $\omega$ photoproduction on the proton was
conducted by using the Crystal Ball and TAPS multiphoton
spectrometers together with the photon tagging facility at the Mainz
Microtron MAMI.
The $\gamma p \to \omega p$ differential cross sections are measured from
threshold to the incident-photon energy $E_{\gamma}$=1.4 GeV (W=1.87 GeV
for the center-of-mass energy) with 15-MeV binning in $E_{\gamma}$ and
full production-angle coverage. One contribution to the systematic
uncertainty comes from the uncertainty in the shape of the
background. It is not larger than 6%. Another contribution comes from
the determination of the detector acceptance and the photon-beam flux.
It was estimated as 5%.
The quality of the present data near threshold gives access to a 
variety of interesting physics aspects. As an example, an estimation 
of the $\omega$N scattering length is provided.
DOI: 10.17182/hepdata.130198.v1/t21
title: "dcs20" of "Photoproduction of the omega meson off the proton near threshold"

description: Differential cross section at W= 1.8720 GeV
description: A2 Collaboration at MAMI.
An experimental study of $\omega$ photoproduction on the proton was
conducted by using the Crystal Ball and TAPS multiphoton
spectrometers together with the photon tagging facility at the Mainz
Microtron MAMI.
The $\gamma p \to \omega p$ differential cross sections are measured from
threshold to the incident-photon energy $E_{\gamma}$=1.4 GeV (W=1.87 GeV
for the center-of-mass energy) with 15-MeV binning in $E_{\gamma}$ and
full production-angle coverage. One contribution to the systematic
uncertainty comes from the uncertainty in the shape of the
background. It is not larger than 6%. Another contribution comes from
the determination of the detector acceptance and the photon-beam flux.
It was estimated as 5%.
The quality of the present data near threshold gives access to a 
variety of interesting physics aspects. As an example, an estimation 
of the $\omega$N scattering length is provided.
DOI: 10.17182/hepdata.130199.v1/t1
title: "Table of contents" of "Search for $B^{+}\to K^{+}\nu\bar{\nu}$ decays using an inclusive tagging method at Belle II"

description: - - - - - - - - Overview of HEPData Record - - - - - - - - <br><br> <b>Post-fit yields:</b> Y(4S) Off-resonance <b>Exclusion limit:</b> Expected limit and observed limit <b>Efficiency:</b> Selection efficiency as a function of $q^{2}$
description: SuperKEKB Belle II. Measurement of the branching fraction of $B^{+} \rightarrow K^{+} \nu \bar{\nu}$ at the Belle II experiment at the SuperKEKB. The analysed data sample corresponds to an integrated luminosity of 63 fb$^{−1}$ collected at the $\Upsilon(4S)$ resonance and a sample of 9 fb$^{−1}$ collected at an energy 60 MeV below the resonance between 2019-2021. Since no significant signal was observed, limit of $4.1\times 10^{-5}$ was set using CL$_{s}$ method.
DOI: 10.17182/hepdata.130199.v1/t2
title: "Postfit yields Y(4S)" of "Search for $B^{+}\to K^{+}\nu\bar{\nu}$ decays using an inclusive tagging method at Belle II"

description: Yields in on-resonance data and as predicted by the simultaneous fit to the on- and off-resonance data, corresponding to an integrated luminosity of 63 and 9 fb$^{−1}$, respectively. The predicted yields are shown individually for charged and neutral B-meson decays and the five continuum background categories. The leftmost three bins belong to the first control region (CR1) with BDT$_{2} \in [0.93; 0.95]$ and the other nine bins correspond to the signal region (SR), three for each range of BDT$_{2} \in [0.95; 0.97; 0.99; 1.0]$. Each set of three bins is defined by $p_{T}(K^{+}) \in [0.5; 2.0; 2.4; 3.5] \rm{GeV}/c^{2}$.
description: SuperKEKB Belle II. Measurement of the branching fraction of $B^{+} \rightarrow K^{+} \nu \bar{\nu}$ at the Belle II experiment at the SuperKEKB. The analysed data sample corresponds to an integrated luminosity of 63 fb$^{−1}$ collected at the $\Upsilon(4S)$ resonance and a sample of 9 fb$^{−1}$ collected at an energy 60 MeV below the resonance between 2019-2021. Since no significant signal was observed, limit of $4.1\times 10^{-5}$ was set using CL$_{s}$ method.
DOI: 10.17182/hepdata.130199.v1/t3
title: "Postfit yields off-resonance" of "Search for $B^{+}\to K^{+}\nu\bar{\nu}$ decays using an inclusive tagging method at Belle II"

description: Yields in off-resonance data and as predicted by the simultaneous fit to the on- and off-resonance data, corresponding to an integrated luminosity of 63 and 9 fb$^{−1}$, respectively. The predicted yields are shown individually for the five continuum background categories. The leftmost three bins belong to the third control region (CR3) with BDT$_{2} \in [0.93; 0.95]$ and the other nine bins correspond to the second control region (CR2), three for each range of BDT$_{2} \in [0.95; 0.97; 0.99; 1.0]$. Each set of three bins is defined by $p_{T}(K^{+}) \in [0.5; 2.0; 2.4; 3.5] \rm{GeV}/c^{2}$.
description: SuperKEKB Belle II. Measurement of the branching fraction of $B^{+} \rightarrow K^{+} \nu \bar{\nu}$ at the Belle II experiment at the SuperKEKB. The analysed data sample corresponds to an integrated luminosity of 63 fb$^{−1}$ collected at the $\Upsilon(4S)$ resonance and a sample of 9 fb$^{−1}$ collected at an energy 60 MeV below the resonance between 2019-2021. Since no significant signal was observed, limit of $4.1\times 10^{-5}$ was set using CL$_{s}$ method.
DOI: 10.17182/hepdata.130199.v1/t4
title: "Expected and observed limit" of "Search for $B^{+}\to K^{+}\nu\bar{\nu}$ decays using an inclusive tagging method at Belle II"

description: CL$_{s}$ value as a function of the branching fraction of $B^{+} \rightarrow K^{+} \nu \bar{\nu}$ for expected and observed signal yields and the corresponding upper limits at 90% confidence level (CL). The expected limit is derived for the background-only hypothesis. The observed limit is derived from a simultaneous fit to the on-resonance and off-resonance data, corresponding to an integrated luminosity of 63 fb$^{−1}$ and 9 fb$^{−1}$, respectively.
description: SuperKEKB Belle II. Measurement of the branching fraction of $B^{+} \rightarrow K^{+} \nu \bar{\nu}$ at the Belle II experiment at the SuperKEKB. The analysed data sample corresponds to an integrated luminosity of 63 fb$^{−1}$ collected at the $\Upsilon(4S)$ resonance and a sample of 9 fb$^{−1}$ collected at an energy 60 MeV below the resonance between 2019-2021. Since no significant signal was observed, limit of $4.1\times 10^{-5}$ was set using CL$_{s}$ method.
DOI: 10.17182/hepdata.130199.v1/t5
title: "Selection efficiency" of "Search for $B^{+}\to K^{+}\nu\bar{\nu}$ decays using an inclusive tagging method at Belle II"

description: Signal efficiency as a function of the dineutrino invariant mass squared $q^{2}$ for events in the signal region (SR) ($\rm{BDT}_{1} &gt; 0.9$ and $\rm{BDT}_{2} &gt; 0.95$). The error bars indicate the statistical uncertainty.
description: SuperKEKB Belle II. Measurement of the branching fraction of $B^{+} \rightarrow K^{+} \nu \bar{\nu}$ at the Belle II experiment at the SuperKEKB. The analysed data sample corresponds to an integrated luminosity of 63 fb$^{−1}$ collected at the $\Upsilon(4S)$ resonance and a sample of 9 fb$^{−1}$ collected at an energy 60 MeV below the resonance between 2019-2021. Since no significant signal was observed, limit of $4.1\times 10^{-5}$ was set using CL$_{s}$ method.
DOI: 10.17182/hepdata.130200.v1/t1
title: "Figures 3-9, PSI(2S)" of "Measurement of $\psi(2S)$ nuclear modification at backward and forward rapidity in $p$ $+$ $p$, $p$ $+$ Al, and $p$ $+$ Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: PSI(2S)--&gt;MU+MU- invariant yields in p+p, p+Al, and p+Au collisions as a function of rapidity. The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. An additional global systematic uncertainty is provided in each column heading, which applies to all data points per column.
description: BNL-RHIC. Suppression of the J/$\psi$ nuclear modification factor has been seen as a trademark signature of final state effects in large collision systems for decades. In small systems, the nuclear modification was attributed to cold nuclear matter effects until the observation of strong differential suppression of the $\psi$(2S) state in $p/d$+A collisions suggested the presence of final state effects. Results of J/$\psi$ and $\psi$(2S) measurements in the dimuon decay channel are presented here for $p$+$p$, $p$+Al, and $p$+Au collision systems at $\sqrt{s_NN} = 200$~GeV. The results are predominantly shown in the form of the nuclear modification factor, $R_{AB}$, the ratio of the $\psi$(2S) invariant yield per nucleon-nucleon collision in collisions of proton on target nucleus to that in $p$+$p$ collisions. Measurements of the J/$\psi$ and $\psi$(2S) nuclear modification factor are compared with shadowing and transport model predictions, as well as to complementary measurements at Large-Hadron-Collider energies.
DOI: 10.17182/hepdata.130200.v1/t2
title: "Figures 3-9, J/PSI(1S)" of "Measurement of $\psi(2S)$ nuclear modification at backward and forward rapidity in $p$ $+$ $p$, $p$ $+$ Al, and $p$ $+$ Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: J/PSI(1S)--&gt;MU+MU- invariant yields in p+p, p+Al, and p+Au collisions as a function of rapidity. The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. An additional global systematic uncertainty is provided in each column heading, which applies to all data points per column.
description: BNL-RHIC. Suppression of the J/$\psi$ nuclear modification factor has been seen as a trademark signature of final state effects in large collision systems for decades. In small systems, the nuclear modification was attributed to cold nuclear matter effects until the observation of strong differential suppression of the $\psi$(2S) state in $p/d$+A collisions suggested the presence of final state effects. Results of J/$\psi$ and $\psi$(2S) measurements in the dimuon decay channel are presented here for $p$+$p$, $p$+Al, and $p$+Au collision systems at $\sqrt{s_NN} = 200$~GeV. The results are predominantly shown in the form of the nuclear modification factor, $R_{AB}$, the ratio of the $\psi$(2S) invariant yield per nucleon-nucleon collision in collisions of proton on target nucleus to that in $p$+$p$ collisions. Measurements of the J/$\psi$ and $\psi$(2S) nuclear modification factor are compared with shadowing and transport model predictions, as well as to complementary measurements at Large-Hadron-Collider energies.
DOI: 10.17182/hepdata.130200.v1/t3
title: "Figure 3, PSI(2S)" of "Measurement of $\psi(2S)$ nuclear modification at backward and forward rapidity in $p$ $+$ $p$, $p$ $+$ Al, and $p$ $+$ Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: PSI(2S)--&gt;MU+MU- nuclear modification in p+Al collisions as a function of rapidity. The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. An additional global systematic uncertainty is provided in each column heading, which applies to all data points per column.
description: BNL-RHIC. Suppression of the J/$\psi$ nuclear modification factor has been seen as a trademark signature of final state effects in large collision systems for decades. In small systems, the nuclear modification was attributed to cold nuclear matter effects until the observation of strong differential suppression of the $\psi$(2S) state in $p/d$+A collisions suggested the presence of final state effects. Results of J/$\psi$ and $\psi$(2S) measurements in the dimuon decay channel are presented here for $p$+$p$, $p$+Al, and $p$+Au collision systems at $\sqrt{s_NN} = 200$~GeV. The results are predominantly shown in the form of the nuclear modification factor, $R_{AB}$, the ratio of the $\psi$(2S) invariant yield per nucleon-nucleon collision in collisions of proton on target nucleus to that in $p$+$p$ collisions. Measurements of the J/$\psi$ and $\psi$(2S) nuclear modification factor are compared with shadowing and transport model predictions, as well as to complementary measurements at Large-Hadron-Collider energies.
DOI: 10.17182/hepdata.130200.v1/t4
title: "Figure 3, J/PSI(1S)" of "Measurement of $\psi(2S)$ nuclear modification at backward and forward rapidity in $p$ $+$ $p$, $p$ $+$ Al, and $p$ $+$ Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: J/PSI(1S)--&gt;MU+MU- nuclear modification in p+Al collisions as a function of rapidity. The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. An additional global systematic uncertainty is provided in each column heading, which applies to all data points per column.
description: BNL-RHIC. Suppression of the J/$\psi$ nuclear modification factor has been seen as a trademark signature of final state effects in large collision systems for decades. In small systems, the nuclear modification was attributed to cold nuclear matter effects until the observation of strong differential suppression of the $\psi$(2S) state in $p/d$+A collisions suggested the presence of final state effects. Results of J/$\psi$ and $\psi$(2S) measurements in the dimuon decay channel are presented here for $p$+$p$, $p$+Al, and $p$+Au collision systems at $\sqrt{s_NN} = 200$~GeV. The results are predominantly shown in the form of the nuclear modification factor, $R_{AB}$, the ratio of the $\psi$(2S) invariant yield per nucleon-nucleon collision in collisions of proton on target nucleus to that in $p$+$p$ collisions. Measurements of the J/$\psi$ and $\psi$(2S) nuclear modification factor are compared with shadowing and transport model predictions, as well as to complementary measurements at Large-Hadron-Collider energies.
DOI: 10.17182/hepdata.130200.v1/t5
title: "Figures 4 and 9, PSI(2S)" of "Measurement of $\psi(2S)$ nuclear modification at backward and forward rapidity in $p$ $+$ $p$, $p$ $+$ Al, and $p$ $+$ Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: PSI(2S)--&gt;MU+MU- nuclear modification in p+Au collisions as a function of rapidity. The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. An additional global systematic uncertainty is provided in each column heading, which applies to all data points per column.
description: BNL-RHIC. Suppression of the J/$\psi$ nuclear modification factor has been seen as a trademark signature of final state effects in large collision systems for decades. In small systems, the nuclear modification was attributed to cold nuclear matter effects until the observation of strong differential suppression of the $\psi$(2S) state in $p/d$+A collisions suggested the presence of final state effects. Results of J/$\psi$ and $\psi$(2S) measurements in the dimuon decay channel are presented here for $p$+$p$, $p$+Al, and $p$+Au collision systems at $\sqrt{s_NN} = 200$~GeV. The results are predominantly shown in the form of the nuclear modification factor, $R_{AB}$, the ratio of the $\psi$(2S) invariant yield per nucleon-nucleon collision in collisions of proton on target nucleus to that in $p$+$p$ collisions. Measurements of the J/$\psi$ and $\psi$(2S) nuclear modification factor are compared with shadowing and transport model predictions, as well as to complementary measurements at Large-Hadron-Collider energies.
DOI: 10.17182/hepdata.130200.v1/t10
title: "Figure 8" of "Measurement of $\psi(2S)$ nuclear modification at backward and forward rapidity in $p$ $+$ $p$, $p$ $+$ Al, and $p$ $+$ Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: Invariant yield ratio of PSI(2S)--&gt;MU+MU- with respect to J/PSI(1S)--&gt;MU+MU- in p+p collisions at rapidity 1.2 &lt; |y| &lt; 2.2. The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. The global systematic uncertainty cancels when taking the ratio.
description: BNL-RHIC. Suppression of the J/$\psi$ nuclear modification factor has been seen as a trademark signature of final state effects in large collision systems for decades. In small systems, the nuclear modification was attributed to cold nuclear matter effects until the observation of strong differential suppression of the $\psi$(2S) state in $p/d$+A collisions suggested the presence of final state effects. Results of J/$\psi$ and $\psi$(2S) measurements in the dimuon decay channel are presented here for $p$+$p$, $p$+Al, and $p$+Au collision systems at $\sqrt{s_NN} = 200$~GeV. The results are predominantly shown in the form of the nuclear modification factor, $R_{AB}$, the ratio of the $\psi$(2S) invariant yield per nucleon-nucleon collision in collisions of proton on target nucleus to that in $p$+$p$ collisions. Measurements of the J/$\psi$ and $\psi$(2S) nuclear modification factor are compared with shadowing and transport model predictions, as well as to complementary measurements at Large-Hadron-Collider energies.
DOI: 10.17182/hepdata.130200.v1/t11
title: "Figure 8, FWD" of "Measurement of $\psi(2S)$ nuclear modification at backward and forward rapidity in $p$ $+$ $p$, $p$ $+$ Al, and $p$ $+$ Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: Invariant yield ratio of PSI(2S)--&gt;MU+MU- with respect to J/PSI(1S)--&gt;MU+MU- in p+Au collisions as a function of centrality at forward rapidity. The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. The global systematic uncertainty cancels when taking the ratio.
description: BNL-RHIC. Suppression of the J/$\psi$ nuclear modification factor has been seen as a trademark signature of final state effects in large collision systems for decades. In small systems, the nuclear modification was attributed to cold nuclear matter effects until the observation of strong differential suppression of the $\psi$(2S) state in $p/d$+A collisions suggested the presence of final state effects. Results of J/$\psi$ and $\psi$(2S) measurements in the dimuon decay channel are presented here for $p$+$p$, $p$+Al, and $p$+Au collision systems at $\sqrt{s_NN} = 200$~GeV. The results are predominantly shown in the form of the nuclear modification factor, $R_{AB}$, the ratio of the $\psi$(2S) invariant yield per nucleon-nucleon collision in collisions of proton on target nucleus to that in $p$+$p$ collisions. Measurements of the J/$\psi$ and $\psi$(2S) nuclear modification factor are compared with shadowing and transport model predictions, as well as to complementary measurements at Large-Hadron-Collider energies.
DOI: 10.17182/hepdata.130200.v1/t12
title: "Figure 8, BKWD" of "Measurement of $\psi(2S)$ nuclear modification at backward and forward rapidity in $p$ $+$ $p$, $p$ $+$ Al, and $p$ $+$ Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: Invariant yield ratio of PSI(2S)--&gt;MU+MU- with respect to J/PSI(1S)--&gt;MU+MU- in p+Au collisions as a function of centrality at backward rapidity. The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. The global systematic uncertainty cancels when taking the ratio.
description: BNL-RHIC. Suppression of the J/$\psi$ nuclear modification factor has been seen as a trademark signature of final state effects in large collision systems for decades. In small systems, the nuclear modification was attributed to cold nuclear matter effects until the observation of strong differential suppression of the $\psi$(2S) state in $p/d$+A collisions suggested the presence of final state effects. Results of J/$\psi$ and $\psi$(2S) measurements in the dimuon decay channel are presented here for $p$+$p$, $p$+Al, and $p$+Au collision systems at $\sqrt{s_NN} = 200$~GeV. The results are predominantly shown in the form of the nuclear modification factor, $R_{AB}$, the ratio of the $\psi$(2S) invariant yield per nucleon-nucleon collision in collisions of proton on target nucleus to that in $p$+$p$ collisions. Measurements of the J/$\psi$ and $\psi$(2S) nuclear modification factor are compared with shadowing and transport model predictions, as well as to complementary measurements at Large-Hadron-Collider energies.