cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.102953.v1/t16
title: "Figure 6.0.1" of "Invariant Jet Mass Measurements in $pp$ Collisions at $\sqrt{s} = 200$ GeV at RHIC"

description: The mean of the fully corrected jet mass distribution for $R=0.4$ anti-$k_{\rm{T}}$ jets as a function of $p_{\rm{T,jet}}$.
description: We present the first inclusive measurements of the invariant and SoftDrop jet mass in proton-proton collisions at $\sqrt{s} = 200$ GeV at STAR. The measurements are fully corrected for detector effects, and reported differentially in both the jet transverse momentum and jet radius parameter. We compare the measurements to established leading-order Monte Carlo event generators and find that STAR-tuned PYTHIA-6 reproduces the data while LHC tunes of PYTHIA-8 and HERWIG-7 do not agree with the data, providing further constraints on parameter tuning. Finally, we observe that SoftDrop grooming, for which the contribution of wide-angle non-perturbative radiation is suppressed, shifts the jet mass distributions into closer agreement with the partonic jet mass as determined by both PYTHIA-8 and a next-to-leading-logarithmic accuracy perturbative QCD calculation. These measurements complement recent LHC measurements in a different kinematic region, as well as establish a baseline for future jet mass measurements in heavy-ion collisions at RHIC.
DOI: 10.17182/hepdata.102953.v1/t17
title: "Figure 6.0.2" of "Invariant Jet Mass Measurements in $pp$ Collisions at $\sqrt{s} = 200$ GeV at RHIC"

description: The mean of the fully corrected jet mass distribution for $R=0.6$ anti-$k_{\rm{T}}$ jets as a function of $p_{\rm{T,jet}}$.
description: We present the first inclusive measurements of the invariant and SoftDrop jet mass in proton-proton collisions at $\sqrt{s} = 200$ GeV at STAR. The measurements are fully corrected for detector effects, and reported differentially in both the jet transverse momentum and jet radius parameter. We compare the measurements to established leading-order Monte Carlo event generators and find that STAR-tuned PYTHIA-6 reproduces the data while LHC tunes of PYTHIA-8 and HERWIG-7 do not agree with the data, providing further constraints on parameter tuning. Finally, we observe that SoftDrop grooming, for which the contribution of wide-angle non-perturbative radiation is suppressed, shifts the jet mass distributions into closer agreement with the partonic jet mass as determined by both PYTHIA-8 and a next-to-leading-logarithmic accuracy perturbative QCD calculation. These measurements complement recent LHC measurements in a different kinematic region, as well as establish a baseline for future jet mass measurements in heavy-ion collisions at RHIC.
DOI: 10.17182/hepdata.102953.v1/t18
title: "Figure 6.1.0" of "Invariant Jet Mass Measurements in $pp$ Collisions at $\sqrt{s} = 200$ GeV at RHIC"

description: The mean of the fully corrected SoftDrop groomed jet mass distribution for $R=0.2$ anti-$k_{\rm{T}}$ jets as a function of $p_{\rm{T,jet}}$.
description: We present the first inclusive measurements of the invariant and SoftDrop jet mass in proton-proton collisions at $\sqrt{s} = 200$ GeV at STAR. The measurements are fully corrected for detector effects, and reported differentially in both the jet transverse momentum and jet radius parameter. We compare the measurements to established leading-order Monte Carlo event generators and find that STAR-tuned PYTHIA-6 reproduces the data while LHC tunes of PYTHIA-8 and HERWIG-7 do not agree with the data, providing further constraints on parameter tuning. Finally, we observe that SoftDrop grooming, for which the contribution of wide-angle non-perturbative radiation is suppressed, shifts the jet mass distributions into closer agreement with the partonic jet mass as determined by both PYTHIA-8 and a next-to-leading-logarithmic accuracy perturbative QCD calculation. These measurements complement recent LHC measurements in a different kinematic region, as well as establish a baseline for future jet mass measurements in heavy-ion collisions at RHIC.
DOI: 10.17182/hepdata.102953.v1/t19
title: "Figure 6.1.1" of "Invariant Jet Mass Measurements in $pp$ Collisions at $\sqrt{s} = 200$ GeV at RHIC"

description: The mean of the fully corrected SoftDrop groomed jet mass distribution for $R=0.4$ anti-$k_{\rm{T}}$ jets as a function of $p_{\rm{T,jet}}$.
description: We present the first inclusive measurements of the invariant and SoftDrop jet mass in proton-proton collisions at $\sqrt{s} = 200$ GeV at STAR. The measurements are fully corrected for detector effects, and reported differentially in both the jet transverse momentum and jet radius parameter. We compare the measurements to established leading-order Monte Carlo event generators and find that STAR-tuned PYTHIA-6 reproduces the data while LHC tunes of PYTHIA-8 and HERWIG-7 do not agree with the data, providing further constraints on parameter tuning. Finally, we observe that SoftDrop grooming, for which the contribution of wide-angle non-perturbative radiation is suppressed, shifts the jet mass distributions into closer agreement with the partonic jet mass as determined by both PYTHIA-8 and a next-to-leading-logarithmic accuracy perturbative QCD calculation. These measurements complement recent LHC measurements in a different kinematic region, as well as establish a baseline for future jet mass measurements in heavy-ion collisions at RHIC.
DOI: 10.17182/hepdata.102953.v1/t5
title: "Figure 4.0.2" of "Invariant Jet Mass Measurements in $pp$ Collisions at $\sqrt{s} = 200$ GeV at RHIC"

description: The fully corrected jet mass distribution for $R = 0.4$ anti-$k_{\rm{T}}$ jets with $30 &lt; p_{\rm{T,jet}} &lt; 40$ GeV$/c$. Data are reported beyond the x-axis upper limit of the figure, for future reference.
description: We present the first inclusive measurements of the invariant and SoftDrop jet mass in proton-proton collisions at $\sqrt{s} = 200$ GeV at STAR. The measurements are fully corrected for detector effects, and reported differentially in both the jet transverse momentum and jet radius parameter. We compare the measurements to established leading-order Monte Carlo event generators and find that STAR-tuned PYTHIA-6 reproduces the data while LHC tunes of PYTHIA-8 and HERWIG-7 do not agree with the data, providing further constraints on parameter tuning. Finally, we observe that SoftDrop grooming, for which the contribution of wide-angle non-perturbative radiation is suppressed, shifts the jet mass distributions into closer agreement with the partonic jet mass as determined by both PYTHIA-8 and a next-to-leading-logarithmic accuracy perturbative QCD calculation. These measurements complement recent LHC measurements in a different kinematic region, as well as establish a baseline for future jet mass measurements in heavy-ion collisions at RHIC.
DOI: 10.17182/hepdata.102953.v1/t9
title: "Figure 5.0.0" of "Invariant Jet Mass Measurements in $pp$ Collisions at $\sqrt{s} = 200$ GeV at RHIC"

description: The fully corrected jet mass distribution for $R = 0.2$ anti-$k_{\rm{T}}$ jets with $30 &lt; p_{\rm{T,jet}} &lt; 40$ GeV$/c$.
description: We present the first inclusive measurements of the invariant and SoftDrop jet mass in proton-proton collisions at $\sqrt{s} = 200$ GeV at STAR. The measurements are fully corrected for detector effects, and reported differentially in both the jet transverse momentum and jet radius parameter. We compare the measurements to established leading-order Monte Carlo event generators and find that STAR-tuned PYTHIA-6 reproduces the data while LHC tunes of PYTHIA-8 and HERWIG-7 do not agree with the data, providing further constraints on parameter tuning. Finally, we observe that SoftDrop grooming, for which the contribution of wide-angle non-perturbative radiation is suppressed, shifts the jet mass distributions into closer agreement with the partonic jet mass as determined by both PYTHIA-8 and a next-to-leading-logarithmic accuracy perturbative QCD calculation. These measurements complement recent LHC measurements in a different kinematic region, as well as establish a baseline for future jet mass measurements in heavy-ion collisions at RHIC.
DOI: 10.25549/vercoutere-ouc110610993
title: Woman's face surrounded by other faces

description: Female with green face, black lips, orange hair or scarf, blue neck, orange neck kerchief, and yellow, brown, and orange shirt; handgun on sleeve; other faces included in the background of green pink, red, orange, and black. Notes left by OT: Fourteen year old 'F' had crawled under the fence at the Boys School in Paso Robles, California. Always the day before he was to be released to his home in Los Angeles. The staff at the Boys School were confused because the pattern was always the same. He was told that he was going home and within the next few hours he would crawl under the fence and steal a staff car from the parking lot. Staff cars only filled their cars before they left the facility and were habitualy left parked with a small amount of gas so the boy did not get very far. They sent him to the State Hospital because he had escaped and that was against the law. He certainly didn't belong in a hospital with 800 sex psychopaths. I kept him with me. Six hours in the OT clinic was a partial solution for providing a safe environment. He had no art training but he was handy with a brush and colors. ..... Picture #2. Appears to be a woman, again with several faces surrounding this main subject. There is a handgun on her/his sleeve. He wouldn't talk about his family, bu the pictures began to tell a story. ... I packed the pictures of the family and sent them to his social worker. He was released to a foster family in Northern California.
DOI: 10.17182/hepdata.102953.v1/t20
title: "Figure 6.1.2" of "Invariant Jet Mass Measurements in $pp$ Collisions at $\sqrt{s} = 200$ GeV at RHIC"

description: The mean of the fully corrected SoftDrop groomed jet mass distribution for $R=0.6$ anti-$k_{\rm{T}}$ jets as a function of $p_{\rm{T,jet}}$.
description: We present the first inclusive measurements of the invariant and SoftDrop jet mass in proton-proton collisions at $\sqrt{s} = 200$ GeV at STAR. The measurements are fully corrected for detector effects, and reported differentially in both the jet transverse momentum and jet radius parameter. We compare the measurements to established leading-order Monte Carlo event generators and find that STAR-tuned PYTHIA-6 reproduces the data while LHC tunes of PYTHIA-8 and HERWIG-7 do not agree with the data, providing further constraints on parameter tuning. Finally, we observe that SoftDrop grooming, for which the contribution of wide-angle non-perturbative radiation is suppressed, shifts the jet mass distributions into closer agreement with the partonic jet mass as determined by both PYTHIA-8 and a next-to-leading-logarithmic accuracy perturbative QCD calculation. These measurements complement recent LHC measurements in a different kinematic region, as well as establish a baseline for future jet mass measurements in heavy-ion collisions at RHIC.
DOI: 10.17182/hepdata.102953.v1/t21
title: "Figure 7.0.0" of "Invariant Jet Mass Measurements in $pp$ Collisions at $\sqrt{s} = 200$ GeV at RHIC"

description: The fully corrected jet mass distribution for $R = 0.6$ anti-$k_{\rm{T}}$ jets with $20 &lt; p_{\rm{T,jet}} &lt; 25$ GeV$/c$. Data are reported beyond the x-axis upper limit of the figure, for future reference.
description: We present the first inclusive measurements of the invariant and SoftDrop jet mass in proton-proton collisions at $\sqrt{s} = 200$ GeV at STAR. The measurements are fully corrected for detector effects, and reported differentially in both the jet transverse momentum and jet radius parameter. We compare the measurements to established leading-order Monte Carlo event generators and find that STAR-tuned PYTHIA-6 reproduces the data while LHC tunes of PYTHIA-8 and HERWIG-7 do not agree with the data, providing further constraints on parameter tuning. Finally, we observe that SoftDrop grooming, for which the contribution of wide-angle non-perturbative radiation is suppressed, shifts the jet mass distributions into closer agreement with the partonic jet mass as determined by both PYTHIA-8 and a next-to-leading-logarithmic accuracy perturbative QCD calculation. These measurements complement recent LHC measurements in a different kinematic region, as well as establish a baseline for future jet mass measurements in heavy-ion collisions at RHIC.
DOI: 10.17182/hepdata.102953.v1/t22
title: "Figure 7.1.0" of "Invariant Jet Mass Measurements in $pp$ Collisions at $\sqrt{s} = 200$ GeV at RHIC"

description: The fully corrected SoftDrop groomed jet mass distribution for $R = 0.6$ anti-$k_{\rm{T}}$ jets with $20 &lt; p_{\rm{T,jet}} &lt; 25$ GeV$/c$. Data are reported beyond the x-axis upper limit of the figure, for future reference.
description: We present the first inclusive measurements of the invariant and SoftDrop jet mass in proton-proton collisions at $\sqrt{s} = 200$ GeV at STAR. The measurements are fully corrected for detector effects, and reported differentially in both the jet transverse momentum and jet radius parameter. We compare the measurements to established leading-order Monte Carlo event generators and find that STAR-tuned PYTHIA-6 reproduces the data while LHC tunes of PYTHIA-8 and HERWIG-7 do not agree with the data, providing further constraints on parameter tuning. Finally, we observe that SoftDrop grooming, for which the contribution of wide-angle non-perturbative radiation is suppressed, shifts the jet mass distributions into closer agreement with the partonic jet mass as determined by both PYTHIA-8 and a next-to-leading-logarithmic accuracy perturbative QCD calculation. These measurements complement recent LHC measurements in a different kinematic region, as well as establish a baseline for future jet mass measurements in heavy-ion collisions at RHIC.
DOI: 10.17182/hepdata.102954.v1/t1
title: "Table 1" of "Measurement of the electroweak production of Z$\gamma$ and two jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV and constraints on anomalous quartic gauge couplings"

description: The measured inclusive fiducial cross section for the pure electroweak Z$\gamma$jj production. The uncertainty of the observed results includes the stastical uncertianty and the systematic uncertainty, while the uncertainty of the predicted results is the theoretical uncertainty from the MadGraph5_aMC@NLO.
description: The first observation of the electroweak (EW) production of a Z boson, a photon, and two forward jets (Z$\gamma$jj) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented. A data set corresponding to an integrated luminosity of 137 fb$^{-1}$, collected by the CMS experiment at the LHC in 2016--2018 is used. The measured fiducial cross section for EW Z$\gamma$jj is $\sigma_{\mathrm{EW}}=5.21\pm0.52\,\mathrm{stat}\,\pm0.56\,\mathrm{syst}\,\mathrm{fb}=5.21\pm0.76\mathrm{fb}$. Single-differential cross sections in photon, leading lepton, and leading jet transverse momenta, and double-differential cross sections in $m_{\mathrm{jj}}$ and $|\Delta\eta_{\mathrm{jj}}|$ are also measured. Exclusion limits on anomalous quartic gauge couplings are derived at 95\% confidence level in terms of the effective field theory operators $\mathrm{M}_{0}$ to $\mathrm{M}_{5}$, $\mathrm{M}_{7}$, $\mathrm{T}_{0}$ to $\mathrm{T}_{2}$, and $\mathrm{T}_{5}$ to $\mathrm{T}_{9}$.
The fiducial region is defined as (selection is in the generator-level):
- $p_{\mathrm{T}}^{l}&gt;$ 20 GeV (25 GeV) && $|\eta^{l}|&lt;$ 2.4 (2.5) for muon(electron)
- 70 $$ 20 GeV && $|\eta^{\gamma}|&lt;$ 1.4442 or ($|\eta^{\gamma}&gt;|$ 1.566 && $|\eta^{\gamma}|&lt;$ 2.5)
- $p_{\mathrm{T}}^{j}&gt;$ 30 GeV && $|\eta^{j}|&lt;$ 4.7
- $m_{jj}&gt;$ 500 GeV && $|\Delta\eta_{jj}|&gt;$ 2.5
- $\Delta R(l,\gamma)&gt;$0.7 && $\Delta R(l,j)&gt;$ 0.5 && $\Delta R(\gamma,j)&gt;$ 0.5 && $\Delta R(j,j)&gt;$ 0.5
- leptons are dressed with photons whose $\Delta R(l,\gamma)&lt;$ 0.1
Selection for aQGC limits are defined as (selection is in the reconstruction-level):
- $p_{\mathrm{T}}^{l}&gt;20$ GeV (25 GeV) && $|\eta^{l}|&lt;$ 2.4 (2.5) for muon(electron)
- 70 $$ 120 GeV && $|\eta^{\gamma}|&lt;$ 1.4442 or ($|\eta^{\gamma}|&gt;$ 1.566 && $|\eta^{\gamma}|&lt;$ 2.5)
- $p_{\mathrm{T}}^{j}&gt;$ 30 GeV && $|\eta^{j}|&lt;$ 4.7
- $m_{jj}&gt;$ 500 GeV && $|\Delta\eta_{jj}|&gt;$ 2.5
- $\Delta R(l,\gamma)&gt;$0.7 && $\Delta R(l,j)&gt;$ 0.5 && $\Delta R(\gamma,j)&gt;$ 0.5 && $\Delta R(j,j)&gt;$ 0.5
DOI: 10.17182/hepdata.102954.v1/t3
title: "Table 3a" of "Measurement of the electroweak production of Z$\gamma$ and two jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV and constraints on anomalous quartic gauge couplings"

description: The measured single-differential cross sections in photon transverse momenta for the pure electroweak Z$\gamma$jj production. The total uncertainty of the observed results includes the stastical uncertianty and the systematic uncertainty, while the uncertainty of the predicted results is the theoretical uncertainty from the MadGraph5_aMC@NLO. The last bin includes overflow events.
description: The first observation of the electroweak (EW) production of a Z boson, a photon, and two forward jets (Z$\gamma$jj) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented. A data set corresponding to an integrated luminosity of 137 fb$^{-1}$, collected by the CMS experiment at the LHC in 2016--2018 is used. The measured fiducial cross section for EW Z$\gamma$jj is $\sigma_{\mathrm{EW}}=5.21\pm0.52\,\mathrm{stat}\,\pm0.56\,\mathrm{syst}\,\mathrm{fb}=5.21\pm0.76\mathrm{fb}$. Single-differential cross sections in photon, leading lepton, and leading jet transverse momenta, and double-differential cross sections in $m_{\mathrm{jj}}$ and $|\Delta\eta_{\mathrm{jj}}|$ are also measured. Exclusion limits on anomalous quartic gauge couplings are derived at 95\% confidence level in terms of the effective field theory operators $\mathrm{M}_{0}$ to $\mathrm{M}_{5}$, $\mathrm{M}_{7}$, $\mathrm{T}_{0}$ to $\mathrm{T}_{2}$, and $\mathrm{T}_{5}$ to $\mathrm{T}_{9}$.
The fiducial region is defined as (selection is in the generator-level):
- $p_{\mathrm{T}}^{l}&gt;$ 20 GeV (25 GeV) && $|\eta^{l}|&lt;$ 2.4 (2.5) for muon(electron)
- 70 $$ 20 GeV && $|\eta^{\gamma}|&lt;$ 1.4442 or ($|\eta^{\gamma}&gt;|$ 1.566 && $|\eta^{\gamma}|&lt;$ 2.5)
- $p_{\mathrm{T}}^{j}&gt;$ 30 GeV && $|\eta^{j}|&lt;$ 4.7
- $m_{jj}&gt;$ 500 GeV && $|\Delta\eta_{jj}|&gt;$ 2.5
- $\Delta R(l,\gamma)&gt;$0.7 && $\Delta R(l,j)&gt;$ 0.5 && $\Delta R(\gamma,j)&gt;$ 0.5 && $\Delta R(j,j)&gt;$ 0.5
- leptons are dressed with photons whose $\Delta R(l,\gamma)&lt;$ 0.1
Selection for aQGC limits are defined as (selection is in the reconstruction-level):
- $p_{\mathrm{T}}^{l}&gt;20$ GeV (25 GeV) && $|\eta^{l}|&lt;$ 2.4 (2.5) for muon(electron)
- 70 $$ 120 GeV && $|\eta^{\gamma}|&lt;$ 1.4442 or ($|\eta^{\gamma}|&gt;$ 1.566 && $|\eta^{\gamma}|&lt;$ 2.5)
- $p_{\mathrm{T}}^{j}&gt;$ 30 GeV && $|\eta^{j}|&lt;$ 4.7
- $m_{jj}&gt;$ 500 GeV && $|\Delta\eta_{jj}|&gt;$ 2.5
- $\Delta R(l,\gamma)&gt;$0.7 && $\Delta R(l,j)&gt;$ 0.5 && $\Delta R(\gamma,j)&gt;$ 0.5 && $\Delta R(j,j)&gt;$ 0.5
DOI: 10.17182/hepdata.102954.v1/t2
title: "Table 2" of "Measurement of the electroweak production of Z$\gamma$ and two jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV and constraints on anomalous quartic gauge couplings"

description: The measured inclusive fiducial cross section for the combined QCD-induced and electroweak Z$\gamma$jj production. The uncertainty of the observed results includes the stastical uncertianty and the systematic uncertainty, while the uncertainty of the predicted results is the theoretical uncertainty from the MadGraph5_aMC@NLO.
description: The first observation of the electroweak (EW) production of a Z boson, a photon, and two forward jets (Z$\gamma$jj) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented. A data set corresponding to an integrated luminosity of 137 fb$^{-1}$, collected by the CMS experiment at the LHC in 2016--2018 is used. The measured fiducial cross section for EW Z$\gamma$jj is $\sigma_{\mathrm{EW}}=5.21\pm0.52\,\mathrm{stat}\,\pm0.56\,\mathrm{syst}\,\mathrm{fb}=5.21\pm0.76\mathrm{fb}$. Single-differential cross sections in photon, leading lepton, and leading jet transverse momenta, and double-differential cross sections in $m_{\mathrm{jj}}$ and $|\Delta\eta_{\mathrm{jj}}|$ are also measured. Exclusion limits on anomalous quartic gauge couplings are derived at 95\% confidence level in terms of the effective field theory operators $\mathrm{M}_{0}$ to $\mathrm{M}_{5}$, $\mathrm{M}_{7}$, $\mathrm{T}_{0}$ to $\mathrm{T}_{2}$, and $\mathrm{T}_{5}$ to $\mathrm{T}_{9}$.
The fiducial region is defined as (selection is in the generator-level):
- $p_{\mathrm{T}}^{l}&gt;$ 20 GeV (25 GeV) && $|\eta^{l}|&lt;$ 2.4 (2.5) for muon(electron)
- 70 $$ 20 GeV && $|\eta^{\gamma}|&lt;$ 1.4442 or ($|\eta^{\gamma}&gt;|$ 1.566 && $|\eta^{\gamma}|&lt;$ 2.5)
- $p_{\mathrm{T}}^{j}&gt;$ 30 GeV && $|\eta^{j}|&lt;$ 4.7
- $m_{jj}&gt;$ 500 GeV && $|\Delta\eta_{jj}|&gt;$ 2.5
- $\Delta R(l,\gamma)&gt;$0.7 && $\Delta R(l,j)&gt;$ 0.5 && $\Delta R(\gamma,j)&gt;$ 0.5 && $\Delta R(j,j)&gt;$ 0.5
- leptons are dressed with photons whose $\Delta R(l,\gamma)&lt;$ 0.1
Selection for aQGC limits are defined as (selection is in the reconstruction-level):
- $p_{\mathrm{T}}^{l}&gt;20$ GeV (25 GeV) && $|\eta^{l}|&lt;$ 2.4 (2.5) for muon(electron)
- 70 $$ 120 GeV && $|\eta^{\gamma}|&lt;$ 1.4442 or ($|\eta^{\gamma}|&gt;$ 1.566 && $|\eta^{\gamma}|&lt;$ 2.5)
- $p_{\mathrm{T}}^{j}&gt;$ 30 GeV && $|\eta^{j}|&lt;$ 4.7
- $m_{jj}&gt;$ 500 GeV && $|\Delta\eta_{jj}|&gt;$ 2.5
- $\Delta R(l,\gamma)&gt;$0.7 && $\Delta R(l,j)&gt;$ 0.5 && $\Delta R(\gamma,j)&gt;$ 0.5 && $\Delta R(j,j)&gt;$ 0.5