cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.135498.v1/t1
title: "Table 1" of "A measurement of the $K^{+} \to \pi^{+} \mu^{+} \mu^{-}$ decay"

description: Reconstructed $K^+ \to \pi^+ \mu^+ \mu^-$ differential decay width. Only statistical errors are provided. The 4-body differential decay width (shown in green in Figure 3-left) is, in general, required to fit these data points; fitting the squared modulus of the form factor may therefore be preferable.
description: CERN-NA-062. A sample of $2.8 \times 10^4$ $K^+ \to \pi^+ \mu^+ \mu^-$ candidates with negligible background was collected by the NA62 experiment at the CERN SPS in 2017--2018. The model-independent branching fraction is measured to be $(9.15 \pm 0.08)\times 10^{-8}$, a factor three more precise than previous measurements. The decay form factor is presented as a function of the squared dimuon mass. A measurement of the form factor parameters and their uncertainties is performed using a description based on Chiral Perturbation Theory at $\mathcal{O}(p^6)$.
DOI: 10.17182/hepdata.135498.v1/t2
title: "Table 2" of "A measurement of the $K^{+} \to \pi^{+} \mu^{+} \mu^{-}$ decay"

description: Reconstructed squared modulus of the $K^+ \to \pi^+ \mu^+ \mu^-$ form factor. Only statistical errors are provided.
description: CERN-NA-062. A sample of $2.8 \times 10^4$ $K^+ \to \pi^+ \mu^+ \mu^-$ candidates with negligible background was collected by the NA62 experiment at the CERN SPS in 2017--2018. The model-independent branching fraction is measured to be $(9.15 \pm 0.08)\times 10^{-8}$, a factor three more precise than previous measurements. The decay form factor is presented as a function of the squared dimuon mass. A measurement of the form factor parameters and their uncertainties is performed using a description based on Chiral Perturbation Theory at $\mathcal{O}(p^6)$.
DOI: 10.17182/hepdata.135675.v1/t1
title: "Results" of "Measurement of the B$^0_\mathrm{S}$$\to$$\mu^+\mu^-$ decay properties and search for the B$^0$$\to$$\mu^+\mu^-$ decay in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The measured branching fraction and effective lifetime for Bs to mu+mu- decay; the branching fraction and upper limits for B0 to mu+mu- decay.
description: CMS-BPH-21-006: We report a measurement of the Bs to mu+mu- branching fraction and its effective lifetime, as well as results of a search for the B0 to mu+mu-
decay in proton-proton collisions at 13 TeV at the LHC. The analysis is based on data collected with the CMS detector in 2016-2018 corresponding to an integrated luminosity of 140 fb-1
The measured branching fraction of the Bs to mu+mu- decay and the effective Bs lifetime are the most precise measurements to date. No evidence for the B0 to mu+mu-
decay has been found. All results are found to be consistent with the standard model predictions.
DOI: 10.17182/hepdata.135675.v1/t2
title: "Figure 2-a" of "Measurement of the B$^0_\mathrm{S}$$\to$$\mu^+\mu^-$ decay properties and search for the B$^0$$\to$$\mu^+\mu^-$ decay in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distribution of the B+ meson pT after the sPlot background subtraction in data and simulation for B+ to J/psi K+ events. The MC distribution is normalized to the data integral.
description: CMS-BPH-21-006: We report a measurement of the Bs to mu+mu- branching fraction and its effective lifetime, as well as results of a search for the B0 to mu+mu-
decay in proton-proton collisions at 13 TeV at the LHC. The analysis is based on data collected with the CMS detector in 2016-2018 corresponding to an integrated luminosity of 140 fb-1
The measured branching fraction of the Bs to mu+mu- decay and the effective Bs lifetime are the most precise measurements to date. No evidence for the B0 to mu+mu-
decay has been found. All results are found to be consistent with the standard model predictions.
DOI: 10.17182/hepdata.135675.v1/t3
title: "Figure 2-b" of "Measurement of the B$^0_\mathrm{S}$$\to$$\mu^+\mu^-$ decay properties and search for the B$^0$$\to$$\mu^+\mu^-$ decay in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distribution of the Bs meson pT after the sPlot background subtraction in data and simulation for Bs to mu+mu- events. The MC distribution is normalized to the data integral.
description: CMS-BPH-21-006: We report a measurement of the Bs to mu+mu- branching fraction and its effective lifetime, as well as results of a search for the B0 to mu+mu-
decay in proton-proton collisions at 13 TeV at the LHC. The analysis is based on data collected with the CMS detector in 2016-2018 corresponding to an integrated luminosity of 140 fb-1
The measured branching fraction of the Bs to mu+mu- decay and the effective Bs lifetime are the most precise measurements to date. No evidence for the B0 to mu+mu-
decay has been found. All results are found to be consistent with the standard model predictions.
DOI: 10.17182/hepdata.135675.v1/t4
title: "Figure 4-c" of "Measurement of the B$^0_\mathrm{S}$$\to$$\mu^+\mu^-$ decay properties and search for the B$^0$$\to$$\mu^+\mu^-$ decay in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The profile likelihood scan as a function of Bs to mu+mu- and B0 to mu+mu- decay branching fractions in 2D.
description: CMS-BPH-21-006: We report a measurement of the Bs to mu+mu- branching fraction and its effective lifetime, as well as results of a search for the B0 to mu+mu-
decay in proton-proton collisions at 13 TeV at the LHC. The analysis is based on data collected with the CMS detector in 2016-2018 corresponding to an integrated luminosity of 140 fb-1
The measured branching fraction of the Bs to mu+mu- decay and the effective Bs lifetime are the most precise measurements to date. No evidence for the B0 to mu+mu-
decay has been found. All results are found to be consistent with the standard model predictions.
DOI: 10.17182/hepdata.135702.v1/t1
title: "figure 3 left" of "Measurement of the electroweak production of W$\gamma$ in association with two jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 2D distributions used in the fit for the total EW W$\gamma$ cross section measurement. The hatched bands represent the systematic uncertainties in the predicted yields. The expectation is shown after the fit to the data and overflow bin has been considered.
description: A measurement is presented for the electroweak production of a W boson, a photon(γ), and two jets (j) in proton-proton collisions. The leptonic decay of the W boson is selected by requiring one identified electron or muon and large missing transverse momentum. The two jets are required to have large invariant dijet mass and large separation in pseudorapidity. The measurement is performed with the data collected by the CMS detector at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of $138 fb^{−1}$. The cross section for the electroweak Wγjj production in a fiducial region is $23.5^{+4.9}_{−4.7} fb$, while the total cross section for Wγjj production in the same fiducial region is 113 ± 13 fb. Differential cross sections are also measured with the distributions unfolded to the parton level. Constraints are placed on anomalous quartic gauge couplings (aQGC) in terms of dimension-8 effective field theory operators and found to be the most stringent limits to date on the aQGC parameters $f_{M,2–5}/Λ^4$ and $f_{T,6–7}/Λ^4$. All results are in agreement with the standard model expectations.
DOI: 10.17182/hepdata.135702.v1/t2
title: "figure 3 right" of "Measurement of the electroweak production of W$\gamma$ in association with two jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 2D distributions used in the fit for the total EW W$\gamma$ cross section measurement. The hatched bands represent the systematic uncertainties in the predicted yields. The expectation is shown after the fit to the data and overflow bin has been considered.
description: A measurement is presented for the electroweak production of a W boson, a photon(γ), and two jets (j) in proton-proton collisions. The leptonic decay of the W boson is selected by requiring one identified electron or muon and large missing transverse momentum. The two jets are required to have large invariant dijet mass and large separation in pseudorapidity. The measurement is performed with the data collected by the CMS detector at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of $138 fb^{−1}$. The cross section for the electroweak Wγjj production in a fiducial region is $23.5^{+4.9}_{−4.7} fb$, while the total cross section for Wγjj production in the same fiducial region is 113 ± 13 fb. Differential cross sections are also measured with the distributions unfolded to the parton level. Constraints are placed on anomalous quartic gauge couplings (aQGC) in terms of dimension-8 effective field theory operators and found to be the most stringent limits to date on the aQGC parameters $f_{M,2–5}/Λ^4$ and $f_{T,6–7}/Λ^4$. All results are in agreement with the standard model expectations.
DOI: 10.17182/hepdata.135702.v1/t3
title: "figure 4 up-left" of "Measurement of the electroweak production of W$\gamma$ in association with two jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Differential cross sections for the EW W$\gamma$jj production. Given that the ranges of some variables extend to infinity, the last bins accommodate all the events up to infinity as marked by the bin label.
description: A measurement is presented for the electroweak production of a W boson, a photon(γ), and two jets (j) in proton-proton collisions. The leptonic decay of the W boson is selected by requiring one identified electron or muon and large missing transverse momentum. The two jets are required to have large invariant dijet mass and large separation in pseudorapidity. The measurement is performed with the data collected by the CMS detector at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of $138 fb^{−1}$. The cross section for the electroweak Wγjj production in a fiducial region is $23.5^{+4.9}_{−4.7} fb$, while the total cross section for Wγjj production in the same fiducial region is 113 ± 13 fb. Differential cross sections are also measured with the distributions unfolded to the parton level. Constraints are placed on anomalous quartic gauge couplings (aQGC) in terms of dimension-8 effective field theory operators and found to be the most stringent limits to date on the aQGC parameters $f_{M,2–5}/Λ^4$ and $f_{T,6–7}/Λ^4$. All results are in agreement with the standard model expectations.
DOI: 10.17182/hepdata.135702.v1/t4
title: "figure 4 up-right" of "Measurement of the electroweak production of W$\gamma$ in association with two jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Differential cross sections for the EW W$\gamma$jj production. Given that the ranges of some variables extend to infinity, the last bins accommodate all the events up to infinity as marked by the bin label.
description: A measurement is presented for the electroweak production of a W boson, a photon(γ), and two jets (j) in proton-proton collisions. The leptonic decay of the W boson is selected by requiring one identified electron or muon and large missing transverse momentum. The two jets are required to have large invariant dijet mass and large separation in pseudorapidity. The measurement is performed with the data collected by the CMS detector at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of $138 fb^{−1}$. The cross section for the electroweak Wγjj production in a fiducial region is $23.5^{+4.9}_{−4.7} fb$, while the total cross section for Wγjj production in the same fiducial region is 113 ± 13 fb. Differential cross sections are also measured with the distributions unfolded to the parton level. Constraints are placed on anomalous quartic gauge couplings (aQGC) in terms of dimension-8 effective field theory operators and found to be the most stringent limits to date on the aQGC parameters $f_{M,2–5}/Λ^4$ and $f_{T,6–7}/Λ^4$. All results are in agreement with the standard model expectations.
DOI: 10.17182/hepdata.135702.v1/t5
title: "figure 4 middle-left" of "Measurement of the electroweak production of W$\gamma$ in association with two jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Differential cross sections for the EW W$\gamma$jj production. Given that the ranges of some variables extend to infinity, the last bins accommodate all the events up to infinity as marked by the bin label.
description: A measurement is presented for the electroweak production of a W boson, a photon(γ), and two jets (j) in proton-proton collisions. The leptonic decay of the W boson is selected by requiring one identified electron or muon and large missing transverse momentum. The two jets are required to have large invariant dijet mass and large separation in pseudorapidity. The measurement is performed with the data collected by the CMS detector at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of $138 fb^{−1}$. The cross section for the electroweak Wγjj production in a fiducial region is $23.5^{+4.9}_{−4.7} fb$, while the total cross section for Wγjj production in the same fiducial region is 113 ± 13 fb. Differential cross sections are also measured with the distributions unfolded to the parton level. Constraints are placed on anomalous quartic gauge couplings (aQGC) in terms of dimension-8 effective field theory operators and found to be the most stringent limits to date on the aQGC parameters $f_{M,2–5}/Λ^4$ and $f_{T,6–7}/Λ^4$. All results are in agreement with the standard model expectations.
DOI: 10.17182/hepdata.135702.v1/t6
title: "figure 4 middle-right" of "Measurement of the electroweak production of W$\gamma$ in association with two jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Differential cross sections for the EW W$\gamma$jj production. Given that the ranges of some variables extend to infinity, the last bins accommodate all the events up to infinity as marked by the bin label.
description: A measurement is presented for the electroweak production of a W boson, a photon(γ), and two jets (j) in proton-proton collisions. The leptonic decay of the W boson is selected by requiring one identified electron or muon and large missing transverse momentum. The two jets are required to have large invariant dijet mass and large separation in pseudorapidity. The measurement is performed with the data collected by the CMS detector at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of $138 fb^{−1}$. The cross section for the electroweak Wγjj production in a fiducial region is $23.5^{+4.9}_{−4.7} fb$, while the total cross section for Wγjj production in the same fiducial region is 113 ± 13 fb. Differential cross sections are also measured with the distributions unfolded to the parton level. Constraints are placed on anomalous quartic gauge couplings (aQGC) in terms of dimension-8 effective field theory operators and found to be the most stringent limits to date on the aQGC parameters $f_{M,2–5}/Λ^4$ and $f_{T,6–7}/Λ^4$. All results are in agreement with the standard model expectations.
DOI: 10.17182/hepdata.135702.v1/t10
title: "figure 5 up-right" of "Measurement of the electroweak production of W$\gamma$ in association with two jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Differential cross sections for the EW +QCD W$\gamma$jj production. Given that the ranges of some variables extend to infinity, the last bins accommodate all the events up to infinity as marked by the bin label.
description: A measurement is presented for the electroweak production of a W boson, a photon(γ), and two jets (j) in proton-proton collisions. The leptonic decay of the W boson is selected by requiring one identified electron or muon and large missing transverse momentum. The two jets are required to have large invariant dijet mass and large separation in pseudorapidity. The measurement is performed with the data collected by the CMS detector at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of $138 fb^{−1}$. The cross section for the electroweak Wγjj production in a fiducial region is $23.5^{+4.9}_{−4.7} fb$, while the total cross section for Wγjj production in the same fiducial region is 113 ± 13 fb. Differential cross sections are also measured with the distributions unfolded to the parton level. Constraints are placed on anomalous quartic gauge couplings (aQGC) in terms of dimension-8 effective field theory operators and found to be the most stringent limits to date on the aQGC parameters $f_{M,2–5}/Λ^4$ and $f_{T,6–7}/Λ^4$. All results are in agreement with the standard model expectations.
DOI: 10.17182/hepdata.135702.v1/t11
title: "figure 5 middle-left" of "Measurement of the electroweak production of W$\gamma$ in association with two jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Differential cross sections for the EW + QCD W$\gamma$jj production. Given that the ranges of some variables extend to infinity, the last bins accommodate all the events up to infinity as marked by the bin label.
description: A measurement is presented for the electroweak production of a W boson, a photon(γ), and two jets (j) in proton-proton collisions. The leptonic decay of the W boson is selected by requiring one identified electron or muon and large missing transverse momentum. The two jets are required to have large invariant dijet mass and large separation in pseudorapidity. The measurement is performed with the data collected by the CMS detector at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of $138 fb^{−1}$. The cross section for the electroweak Wγjj production in a fiducial region is $23.5^{+4.9}_{−4.7} fb$, while the total cross section for Wγjj production in the same fiducial region is 113 ± 13 fb. Differential cross sections are also measured with the distributions unfolded to the parton level. Constraints are placed on anomalous quartic gauge couplings (aQGC) in terms of dimension-8 effective field theory operators and found to be the most stringent limits to date on the aQGC parameters $f_{M,2–5}/Λ^4$ and $f_{T,6–7}/Λ^4$. All results are in agreement with the standard model expectations.
DOI: 10.17182/hepdata.135702.v1/t12
title: "figure 5 middle-right" of "Measurement of the electroweak production of W$\gamma$ in association with two jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Differential cross sections for the EW + QCD W$\gamma$jj production. Given that the ranges of some variables extend to infinity, the last bins accommodate all the events up to infinity as marked by the bin label.
description: A measurement is presented for the electroweak production of a W boson, a photon(γ), and two jets (j) in proton-proton collisions. The leptonic decay of the W boson is selected by requiring one identified electron or muon and large missing transverse momentum. The two jets are required to have large invariant dijet mass and large separation in pseudorapidity. The measurement is performed with the data collected by the CMS detector at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of $138 fb^{−1}$. The cross section for the electroweak Wγjj production in a fiducial region is $23.5^{+4.9}_{−4.7} fb$, while the total cross section for Wγjj production in the same fiducial region is 113 ± 13 fb. Differential cross sections are also measured with the distributions unfolded to the parton level. Constraints are placed on anomalous quartic gauge couplings (aQGC) in terms of dimension-8 effective field theory operators and found to be the most stringent limits to date on the aQGC parameters $f_{M,2–5}/Λ^4$ and $f_{T,6–7}/Λ^4$. All results are in agreement with the standard model expectations.
DOI: 10.17182/hepdata.135702.v1/t13
title: "figure 5 down-left" of "Measurement of the electroweak production of W$\gamma$ in association with two jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Differential cross sections for the EW + QCD W$\gamma$jj production. Given that the ranges of some variables extend to infinity, the last bins accommodate all the events up to infinity as marked by the bin label.
description: A measurement is presented for the electroweak production of a W boson, a photon(γ), and two jets (j) in proton-proton collisions. The leptonic decay of the W boson is selected by requiring one identified electron or muon and large missing transverse momentum. The two jets are required to have large invariant dijet mass and large separation in pseudorapidity. The measurement is performed with the data collected by the CMS detector at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of $138 fb^{−1}$. The cross section for the electroweak Wγjj production in a fiducial region is $23.5^{+4.9}_{−4.7} fb$, while the total cross section for Wγjj production in the same fiducial region is 113 ± 13 fb. Differential cross sections are also measured with the distributions unfolded to the parton level. Constraints are placed on anomalous quartic gauge couplings (aQGC) in terms of dimension-8 effective field theory operators and found to be the most stringent limits to date on the aQGC parameters $f_{M,2–5}/Λ^4$ and $f_{T,6–7}/Λ^4$. All results are in agreement with the standard model expectations.
DOI: 10.17182/hepdata.135702.v1/t14
title: "figure 5 down-right" of "Measurement of the electroweak production of W$\gamma$ in association with two jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Differential cross sections for the EW + QCD W$\gamma$jj production. Given that the ranges of some variables extend to infinity, the last bins accommodate all the events up to infinity as marked by the bin label.
description: A measurement is presented for the electroweak production of a W boson, a photon(γ), and two jets (j) in proton-proton collisions. The leptonic decay of the W boson is selected by requiring one identified electron or muon and large missing transverse momentum. The two jets are required to have large invariant dijet mass and large separation in pseudorapidity. The measurement is performed with the data collected by the CMS detector at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of $138 fb^{−1}$. The cross section for the electroweak Wγjj production in a fiducial region is $23.5^{+4.9}_{−4.7} fb$, while the total cross section for Wγjj production in the same fiducial region is 113 ± 13 fb. Differential cross sections are also measured with the distributions unfolded to the parton level. Constraints are placed on anomalous quartic gauge couplings (aQGC) in terms of dimension-8 effective field theory operators and found to be the most stringent limits to date on the aQGC parameters $f_{M,2–5}/Λ^4$ and $f_{T,6–7}/Λ^4$. All results are in agreement with the standard model expectations.