cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.134068.v1/t175
title: "excl_c1c1_exp_down_dM" of "Search for direct pair production of sleptons and charginos decaying to two leptons and neutralinos with mass splittings near the $W$-boson mass in ${\sqrt{s}=13\,}$TeV $pp$ collisions with the ATLAS detector"

description: Observed and expected exclusion limits on SUSY simplified models for chargino-pair production with $W$-boson-mediated decays in the (a) $m(\tilde{\chi}_1^{\pm})-m(\tilde{\chi}_1^0)$ and (b) $m(\tilde{\chi}_1^{\pm})-\Delta m(\tilde{\chi}_1^{\pm},\tilde{\chi}_1^0)$ planes. The observed (solid thick line) and expected (thin dashed line) exclusion contours are indicated. The shaded band around the dashed line corresponds to the $\pm 1 \sigma$ variations in the expected limit, including all uncertainties except theoretical uncertainties in the signal cross-section. The dotted lines around the observed limit illustrate the change in the observed limit as the nominal signal cross-section is scaled up and down by the theoretical uncertainty. All limits are computed at 95% CL. The observed limits obtained at LEP and by the ATLAS experiment in previous searches are also shown. In case of the search performed on ATLAS Run 1 data at $\sqrt{s} = 8$ TeV no sensitivity was expected for the exclusion in the mass plane.
description: No data abstract available.
DOI: 10.17182/hepdata.134068.v1/t176
title: "pullplot_c1c1" of "Search for direct pair production of sleptons and charginos decaying to two leptons and neutralinos with mass splittings near the $W$-boson mass in ${\sqrt{s}=13\,}$TeV $pp$ collisions with the ATLAS detector"

description: The upper panel shows the observed number of events in the SRs defined in Table 3, together with the expected SM backgrounds obtained after the background fit in the CRs. `Others' include the non-dominant background sources, e.g.$t \bar{t}$+$V$, Higgs boson and Drell--Yan events. The uncertainty band includes systematic and statistical errors from all sources. Distributions for three benchmark signal points are overlaid for comparison. The lower panel shows the significance as defined in Ref. [115].
description: No data abstract available.
DOI: 10.17182/hepdata.134069.v3/t1
title: "Figure 1" of "Measurement of the dependence of the hadron production fraction ratio $f_\mathrm{s} / f_\mathrm{u}$ and $f_\mathrm{d} / f_ \mathrm{u}$ on B meson kinematic variables in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The $\mathrm{J/\psi \phi}$, $\mathrm{J/\psi K}$, and $\mathrm{J/\psi} \mathrm{K}^{*0}$ invariant mass distributions, for $\mathrm{B}$ meson candidates with $20 &lt; p_T &lt; 23$ GeV, and asociated fits as described in the text.
description: The dependence of the ratio between the $\mathrm{B}_\mathrm{s}$ and $\mathrm{B}^{+}$ hadron production fractions, $f_{s}/f_{u}$, on the transverse momentum ($p_T$) and rapidity of the $\mathrm{B}$ meson is studied using the decay channels $\mathrm{B}_\mathrm{s}\rightarrow\mathrm{J/\psi} \mathrm{\phi}$ and $\mathrm{B}^{+}\rightarrow \mathrm{J/\psi} \mathrm{K}^{+}$. The analysis uses a data sample of proton-proton collisions at a center-of-mass energy of 13TeV, collected by the CMS experiment in 2018 and corresponding to an integrated luminosity of 61.6 $\mathrm{fb}^{-1}$. The $f_{s}/f_{u}$ ratio is observed to depend on the $\mathrm{B}$ $p_T$, and to be consistent with becoming asymptotically constant at large $p_T$. No rapidity dependence is observed. The ratio of the $\mathrm{B}^{0}$ to $\mathrm{B}^{+}$ meson production fractions $f_{d}/f_{u}$, is also measured, for the first time at hadron colliders, using the $\mathrm{B}^{0} \rightarrow \mathrm{J/\psi} \mathrm{K}^{*0}$ decay channel. The result is found to be within one standard deviation of unity and independent of $p_T$ and rapidity, as expected from isospin invariance.
DOI: 10.17182/hepdata.134069.v3/t2
title: "Figure 2a" of "Measurement of the dependence of the hadron production fraction ratio $f_\mathrm{s} / f_\mathrm{u}$ and $f_\mathrm{d} / f_ \mathrm{u}$ on B meson kinematic variables in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Left pannel. The vertical bars (boxes) represent the statistical (bin-to-bin systematic) uncertainties, while the horizontal bars give the bin widths. The global uncertainty (of 2.3%) is not graphically represented. The blue line represents the average for $p_T &gt; 18$ GeV. For comparison, the LHCb measurement [10.1103/PhysRevLett.124.122002] is also shown. $ 12 &lt; \mathrm{B} \, p_T &lt; 70$ GeV and $ 0 &lt; |y| &lt; 2.4 $. Global uncertanties are not included in the table (2.3%)
description: The dependence of the ratio between the $\mathrm{B}_\mathrm{s}$ and $\mathrm{B}^{+}$ hadron production fractions, $f_{s}/f_{u}$, on the transverse momentum ($p_T$) and rapidity of the $\mathrm{B}$ meson is studied using the decay channels $\mathrm{B}_\mathrm{s}\rightarrow\mathrm{J/\psi} \mathrm{\phi}$ and $\mathrm{B}^{+}\rightarrow \mathrm{J/\psi} \mathrm{K}^{+}$. The analysis uses a data sample of proton-proton collisions at a center-of-mass energy of 13TeV, collected by the CMS experiment in 2018 and corresponding to an integrated luminosity of 61.6 $\mathrm{fb}^{-1}$. The $f_{s}/f_{u}$ ratio is observed to depend on the $\mathrm{B}$ $p_T$, and to be consistent with becoming asymptotically constant at large $p_T$. No rapidity dependence is observed. The ratio of the $\mathrm{B}^{0}$ to $\mathrm{B}^{+}$ meson production fractions $f_{d}/f_{u}$, is also measured, for the first time at hadron colliders, using the $\mathrm{B}^{0} \rightarrow \mathrm{J/\psi} \mathrm{K}^{*0}$ decay channel. The result is found to be within one standard deviation of unity and independent of $p_T$ and rapidity, as expected from isospin invariance.
DOI: 10.25549/vercoutere-ouc113056747
title: Publisher correspondence

description: Correspondence between Al Vercoutere and various publishers related to publication of patient artwork in textbooks. Arranged in chronological order includes letters and forms (101), check receipts (9), and envelopes (15)
DOI: 10.17182/hepdata.134069.v2/t1
title: "Figure 1" of "Measurement of the dependence of the hadron production fraction ratio $f_\mathrm{s} / f_\mathrm{u}$ and $f_\mathrm{d} / f_ \mathrm{u}$ on B meson kinematic variables in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The $\mathrm{J/\psi \phi}$, $\mathrm{J/\psi K}$, and $\mathrm{J/\psi} \mathrm{K}^{*0}$ invariant mass distributions, for $\mathrm{B}$ meson candidates with $20 &lt; p_T &lt; 23$ GeV, and asociated fits as described in the text.
description: The dependence of the ratio between the $\mathrm{B}_\mathrm{s}$ and $\mathrm{B}^{+}$ hadron production fractions, $f_{s}/f_{u}$, on the transverse momentum ($p_T$) and rapidity of the $\mathrm{B}$ meson is studied using the decay channels $\mathrm{B}_\mathrm{s}\rightarrow\mathrm{J/\psi} \mathrm{\phi}$ and $\mathrm{B}^{+}\rightarrow \mathrm{J/\psi} \mathrm{K}^{+}$. The analysis uses a data sample of proton-proton collisions at a center-of-mass energy of 13TeV, collected by the CMS experiment in 2018 and corresponding to an integrated luminosity of 61.6 $\mathrm{fb}^{-1}$. The $f_{s}/f_{u}$ ratio is observed to depend on the $\mathrm{B}$ $p_T$, and to be consistent with becoming asymptotically constant at large $p_T$. No rapidity dependence is observed. The ratio of the $\mathrm{B}^{0}$ to $\mathrm{B}^{+}$ meson production fractions $f_{d}/f_{u}$, is also measured, for the first time at hadron colliders, using the $\mathrm{B}^{0} \rightarrow \mathrm{J/\psi} \mathrm{K}^{*0}$ decay channel. The result is found to be within one standard deviation of unity and independent of $p_T$ and rapidity, as expected from isospin invariance.
DOI: 10.17182/hepdata.134069.v2/t2
title: "Figure 2a" of "Measurement of the dependence of the hadron production fraction ratio $f_\mathrm{s} / f_\mathrm{u}$ and $f_\mathrm{d} / f_ \mathrm{u}$ on B meson kinematic variables in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Left pannel. The vertical bars (boxes) represent the statistical (bin-to-bin systematic) uncertainties, while the horizontal bars give the bin widths. The global uncertainty (of 2.3%) is not graphically represented. The blue line represents the average for $p_T &gt; 18$ GeV. For comparison, the LHCb measurement [10.1103/PhysRevLett.124.122002] is also shown. $ 12 &lt; \mathrm{B} \, p_T &lt; 70$ GeV and $ 0 &lt; |y| &lt; 2.4 $. Global uncertanties are not included in the table (2.3%)
description: The dependence of the ratio between the $\mathrm{B}_\mathrm{s}$ and $\mathrm{B}^{+}$ hadron production fractions, $f_{s}/f_{u}$, on the transverse momentum ($p_T$) and rapidity of the $\mathrm{B}$ meson is studied using the decay channels $\mathrm{B}_\mathrm{s}\rightarrow\mathrm{J/\psi} \mathrm{\phi}$ and $\mathrm{B}^{+}\rightarrow \mathrm{J/\psi} \mathrm{K}^{+}$. The analysis uses a data sample of proton-proton collisions at a center-of-mass energy of 13TeV, collected by the CMS experiment in 2018 and corresponding to an integrated luminosity of 61.6 $\mathrm{fb}^{-1}$. The $f_{s}/f_{u}$ ratio is observed to depend on the $\mathrm{B}$ $p_T$, and to be consistent with becoming asymptotically constant at large $p_T$. No rapidity dependence is observed. The ratio of the $\mathrm{B}^{0}$ to $\mathrm{B}^{+}$ meson production fractions $f_{d}/f_{u}$, is also measured, for the first time at hadron colliders, using the $\mathrm{B}^{0} \rightarrow \mathrm{J/\psi} \mathrm{K}^{*0}$ decay channel. The result is found to be within one standard deviation of unity and independent of $p_T$ and rapidity, as expected from isospin invariance.
DOI: 10.17182/hepdata.134069.v2/t3
title: "Figure 2b" of "Measurement of the dependence of the hadron production fraction ratio $f_\mathrm{s} / f_\mathrm{u}$ and $f_\mathrm{d} / f_ \mathrm{u}$ on B meson kinematic variables in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Right pannel. The vertical bars (boxes) represent the statistical (bin-to-bin systematic) uncertainties, while the horizontal bars give the bin widths. The global uncertainty (of 2.3%) is not graphically represented. The blue line represents the average for $p_T &gt; 18$ GeV. For comparison, the LHCb measurement [10.1103/PhysRevLett.124.122002] is also shown. $ 12 &lt; \mathrm{B} \, p_T &lt; 70$ GeV and $ 0 &lt; |y| &lt; 2.4 $. Global uncertanties are not included in the table (2.3%)
description: The dependence of the ratio between the $\mathrm{B}_\mathrm{s}$ and $\mathrm{B}^{+}$ hadron production fractions, $f_{s}/f_{u}$, on the transverse momentum ($p_T$) and rapidity of the $\mathrm{B}$ meson is studied using the decay channels $\mathrm{B}_\mathrm{s}\rightarrow\mathrm{J/\psi} \mathrm{\phi}$ and $\mathrm{B}^{+}\rightarrow \mathrm{J/\psi} \mathrm{K}^{+}$. The analysis uses a data sample of proton-proton collisions at a center-of-mass energy of 13TeV, collected by the CMS experiment in 2018 and corresponding to an integrated luminosity of 61.6 $\mathrm{fb}^{-1}$. The $f_{s}/f_{u}$ ratio is observed to depend on the $\mathrm{B}$ $p_T$, and to be consistent with becoming asymptotically constant at large $p_T$. No rapidity dependence is observed. The ratio of the $\mathrm{B}^{0}$ to $\mathrm{B}^{+}$ meson production fractions $f_{d}/f_{u}$, is also measured, for the first time at hadron colliders, using the $\mathrm{B}^{0} \rightarrow \mathrm{J/\psi} \mathrm{K}^{*0}$ decay channel. The result is found to be within one standard deviation of unity and independent of $p_T$ and rapidity, as expected from isospin invariance.
DOI: 10.17182/hepdata.134069.v3/t3
title: "Figure 2b" of "Measurement of the dependence of the hadron production fraction ratio $f_\mathrm{s} / f_\mathrm{u}$ and $f_\mathrm{d} / f_ \mathrm{u}$ on B meson kinematic variables in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Right pannel. The vertical bars (boxes) represent the statistical (bin-to-bin systematic) uncertainties, while the horizontal bars give the bin widths. The global uncertainty (of 2.3%) is not graphically represented. The blue line represents the average for $p_T &gt; 18$ GeV. For comparison, the LHCb measurement [10.1103/PhysRevLett.124.122002] is also shown. $ 12 &lt; \mathrm{B} \, p_T &lt; 70$ GeV and $ 0 &lt; |y| &lt; 2.4 $. Global uncertanties are not included in the table (2.3%)
description: The dependence of the ratio between the $\mathrm{B}_\mathrm{s}$ and $\mathrm{B}^{+}$ hadron production fractions, $f_{s}/f_{u}$, on the transverse momentum ($p_T$) and rapidity of the $\mathrm{B}$ meson is studied using the decay channels $\mathrm{B}_\mathrm{s}\rightarrow\mathrm{J/\psi} \mathrm{\phi}$ and $\mathrm{B}^{+}\rightarrow \mathrm{J/\psi} \mathrm{K}^{+}$. The analysis uses a data sample of proton-proton collisions at a center-of-mass energy of 13TeV, collected by the CMS experiment in 2018 and corresponding to an integrated luminosity of 61.6 $\mathrm{fb}^{-1}$. The $f_{s}/f_{u}$ ratio is observed to depend on the $\mathrm{B}$ $p_T$, and to be consistent with becoming asymptotically constant at large $p_T$. No rapidity dependence is observed. The ratio of the $\mathrm{B}^{0}$ to $\mathrm{B}^{+}$ meson production fractions $f_{d}/f_{u}$, is also measured, for the first time at hadron colliders, using the $\mathrm{B}^{0} \rightarrow \mathrm{J/\psi} \mathrm{K}^{*0}$ decay channel. The result is found to be within one standard deviation of unity and independent of $p_T$ and rapidity, as expected from isospin invariance.
DOI: 10.17182/hepdata.134069.v3/t4
title: "Figure 3a" of "Measurement of the dependence of the hadron production fraction ratio $f_\mathrm{s} / f_\mathrm{u}$ and $f_\mathrm{d} / f_ \mathrm{u}$ on B meson kinematic variables in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Left panel.The vertical bars (boxes) represent the statistical (bin-to-bin systematic) uncertainties, while the horizontal bars give the bin widths. The global uncertainty (of 5.7%) is not graphically represented. The blue line represents the average of all the points. $ 12 &lt; \mathrm{B} \, p_T &lt; 70$ GeV and $ 0 &lt; |y| &lt; 2.4 $. Global uncertanties are not included in the table (5.7%)
description: The dependence of the ratio between the $\mathrm{B}_\mathrm{s}$ and $\mathrm{B}^{+}$ hadron production fractions, $f_{s}/f_{u}$, on the transverse momentum ($p_T$) and rapidity of the $\mathrm{B}$ meson is studied using the decay channels $\mathrm{B}_\mathrm{s}\rightarrow\mathrm{J/\psi} \mathrm{\phi}$ and $\mathrm{B}^{+}\rightarrow \mathrm{J/\psi} \mathrm{K}^{+}$. The analysis uses a data sample of proton-proton collisions at a center-of-mass energy of 13TeV, collected by the CMS experiment in 2018 and corresponding to an integrated luminosity of 61.6 $\mathrm{fb}^{-1}$. The $f_{s}/f_{u}$ ratio is observed to depend on the $\mathrm{B}$ $p_T$, and to be consistent with becoming asymptotically constant at large $p_T$. No rapidity dependence is observed. The ratio of the $\mathrm{B}^{0}$ to $\mathrm{B}^{+}$ meson production fractions $f_{d}/f_{u}$, is also measured, for the first time at hadron colliders, using the $\mathrm{B}^{0} \rightarrow \mathrm{J/\psi} \mathrm{K}^{*0}$ decay channel. The result is found to be within one standard deviation of unity and independent of $p_T$ and rapidity, as expected from isospin invariance.
DOI: 10.17182/hepdata.134069.v3/t5
title: "Figure 3b" of "Measurement of the dependence of the hadron production fraction ratio $f_\mathrm{s} / f_\mathrm{u}$ and $f_\mathrm{d} / f_ \mathrm{u}$ on B meson kinematic variables in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Right panel.The vertical bars (boxes) represent the statistical (bin-to-bin systematic) uncertainties, while the horizontal bars give the bin widths. The global uncertainty (of 5.7%) is not graphically represented. The blue line represents the average of all the points. $ 12 &lt; \mathrm{B} \, p_T &lt; 70$ GeV and $ 0 &lt; |y| &lt; 2.4 $. Global uncertanties are not included in the table (5.7%)
description: The dependence of the ratio between the $\mathrm{B}_\mathrm{s}$ and $\mathrm{B}^{+}$ hadron production fractions, $f_{s}/f_{u}$, on the transverse momentum ($p_T$) and rapidity of the $\mathrm{B}$ meson is studied using the decay channels $\mathrm{B}_\mathrm{s}\rightarrow\mathrm{J/\psi} \mathrm{\phi}$ and $\mathrm{B}^{+}\rightarrow \mathrm{J/\psi} \mathrm{K}^{+}$. The analysis uses a data sample of proton-proton collisions at a center-of-mass energy of 13TeV, collected by the CMS experiment in 2018 and corresponding to an integrated luminosity of 61.6 $\mathrm{fb}^{-1}$. The $f_{s}/f_{u}$ ratio is observed to depend on the $\mathrm{B}$ $p_T$, and to be consistent with becoming asymptotically constant at large $p_T$. No rapidity dependence is observed. The ratio of the $\mathrm{B}^{0}$ to $\mathrm{B}^{+}$ meson production fractions $f_{d}/f_{u}$, is also measured, for the first time at hadron colliders, using the $\mathrm{B}^{0} \rightarrow \mathrm{J/\psi} \mathrm{K}^{*0}$ decay channel. The result is found to be within one standard deviation of unity and independent of $p_T$ and rapidity, as expected from isospin invariance.
DOI: 10.17182/hepdata.134069.v1/t1
title: "Figure 1" of "Measurement of the dependence of the hadron production fraction ratio $f_\mathrm{s} / f_\mathrm{u}$ and $f_\mathrm{d} / f_ \mathrm{u}$ on B meson kinematic variables in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The $\mathrm{J/\psi \phi}$, $\mathrm{J/\psi K}$, and $\mathrm{J/\psi} \mathrm{K}^{*0}$ invariant mass distributions, for $\mathrm{B}$ meson candidates with $20 &lt; p_T &lt; 23$ GeV, and asociated fits as described in the text.
description: The dependence of the ratio between the $\mathrm{B}_\mathrm{s}$ and $\mathrm{B}^{+}$ hadron production fractions, $f_{s}/f_{u}$, on the transverse momentum ($p_T$) and rapidity of the $\mathrm{B}$ meson is studied using the decay channels $\mathrm{B}_\mathrm{s}\rightarrow\mathrm{J/\psi} \mathrm{\phi}$ and $\mathrm{B}^{+}\rightarrow \mathrm{J/\psi} \mathrm{K}^{+}$. The analysis uses a data sample of proton-proton collisions at a center-of-mass energy of 13TeV, collected by the CMS experiment in 2018 and corresponding to an integrated luminosity of 61.6 $\mathrm{fb}^{-1}$. The $f_{s}/f_{u}$ ratio is observed to depend on the $\mathrm{B}$ $p_T$, and to be consistent with becoming asymptotically constant at large $p_T$. No rapidity dependence is observed. The ratio of the $\mathrm{B}^{0}$ to $\mathrm{B}^{+}$ hadron production fractions $f_{d}/f_{u}$, measured using the $\mathrm{B}^{0} \rightarrow \mathrm{J/\psi} \mathrm{K}^{*0}$ decay channel, is found to be consistent with unity and independent of $p_T$ and rapidity.
DOI: 10.17182/hepdata.134069.v1/t2
title: "Figure 2a" of "Measurement of the dependence of the hadron production fraction ratio $f_\mathrm{s} / f_\mathrm{u}$ and $f_\mathrm{d} / f_ \mathrm{u}$ on B meson kinematic variables in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Left pannel. The vertical bars (boxes) represent the statistical (bin-to-bin systematic) uncertainties, while the horizontal bars give the bin widths. The global uncertainty (of 2.3%) is not graphically represented. The blue line represents the average for $p_T &gt; 18$ GeV. For comparison, the LHCb measurement [10.1103/PhysRevLett.124.122002] is also shown. $ 12 &lt; \mathrm{B} \, p_T &lt; 70$ GeV and $ 0 &lt; |y| &lt; 2.4 $. Global uncertanties are not included in the table (2.3%)
description: The dependence of the ratio between the $\mathrm{B}_\mathrm{s}$ and $\mathrm{B}^{+}$ hadron production fractions, $f_{s}/f_{u}$, on the transverse momentum ($p_T$) and rapidity of the $\mathrm{B}$ meson is studied using the decay channels $\mathrm{B}_\mathrm{s}\rightarrow\mathrm{J/\psi} \mathrm{\phi}$ and $\mathrm{B}^{+}\rightarrow \mathrm{J/\psi} \mathrm{K}^{+}$. The analysis uses a data sample of proton-proton collisions at a center-of-mass energy of 13TeV, collected by the CMS experiment in 2018 and corresponding to an integrated luminosity of 61.6 $\mathrm{fb}^{-1}$. The $f_{s}/f_{u}$ ratio is observed to depend on the $\mathrm{B}$ $p_T$, and to be consistent with becoming asymptotically constant at large $p_T$. No rapidity dependence is observed. The ratio of the $\mathrm{B}^{0}$ to $\mathrm{B}^{+}$ hadron production fractions $f_{d}/f_{u}$, measured using the $\mathrm{B}^{0} \rightarrow \mathrm{J/\psi} \mathrm{K}^{*0}$ decay channel, is found to be consistent with unity and independent of $p_T$ and rapidity.
DOI: 10.17182/hepdata.134069.v1/t3
title: "Figure 2b" of "Measurement of the dependence of the hadron production fraction ratio $f_\mathrm{s} / f_\mathrm{u}$ and $f_\mathrm{d} / f_ \mathrm{u}$ on B meson kinematic variables in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Right pannel. The vertical bars (boxes) represent the statistical (bin-to-bin systematic) uncertainties, while the horizontal bars give the bin widths. The global uncertainty (of 2.3%) is not graphically represented. The blue line represents the average for $p_T &gt; 18$ GeV. For comparison, the LHCb measurement [10.1103/PhysRevLett.124.122002] is also shown. $ 12 &lt; \mathrm{B} \, p_T &lt; 70$ GeV and $ 0 &lt; |y| &lt; 2.4 $. Global uncertanties are not included in the table (2.3%)
description: The dependence of the ratio between the $\mathrm{B}_\mathrm{s}$ and $\mathrm{B}^{+}$ hadron production fractions, $f_{s}/f_{u}$, on the transverse momentum ($p_T$) and rapidity of the $\mathrm{B}$ meson is studied using the decay channels $\mathrm{B}_\mathrm{s}\rightarrow\mathrm{J/\psi} \mathrm{\phi}$ and $\mathrm{B}^{+}\rightarrow \mathrm{J/\psi} \mathrm{K}^{+}$. The analysis uses a data sample of proton-proton collisions at a center-of-mass energy of 13TeV, collected by the CMS experiment in 2018 and corresponding to an integrated luminosity of 61.6 $\mathrm{fb}^{-1}$. The $f_{s}/f_{u}$ ratio is observed to depend on the $\mathrm{B}$ $p_T$, and to be consistent with becoming asymptotically constant at large $p_T$. No rapidity dependence is observed. The ratio of the $\mathrm{B}^{0}$ to $\mathrm{B}^{+}$ hadron production fractions $f_{d}/f_{u}$, measured using the $\mathrm{B}^{0} \rightarrow \mathrm{J/\psi} \mathrm{K}^{*0}$ decay channel, is found to be consistent with unity and independent of $p_T$ and rapidity.
DOI: 10.17182/hepdata.134069.v1/t4
title: "Figure 3a" of "Measurement of the dependence of the hadron production fraction ratio $f_\mathrm{s} / f_\mathrm{u}$ and $f_\mathrm{d} / f_ \mathrm{u}$ on B meson kinematic variables in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Left panel.The vertical bars (boxes) represent the statistical (bin-to-bin systematic) uncertainties, while the horizontal bars give the bin widths. The global uncertainty (of 4.9\%) is not graphically represented. The blue line represents the average of all the points. $ 12 &lt; \mathrm{B} \, p_T &lt; 70$ GeV and $ 0 &lt; |y| &lt; 2.4 $. Global uncertanties are not included in the table (4.9%)
description: The dependence of the ratio between the $\mathrm{B}_\mathrm{s}$ and $\mathrm{B}^{+}$ hadron production fractions, $f_{s}/f_{u}$, on the transverse momentum ($p_T$) and rapidity of the $\mathrm{B}$ meson is studied using the decay channels $\mathrm{B}_\mathrm{s}\rightarrow\mathrm{J/\psi} \mathrm{\phi}$ and $\mathrm{B}^{+}\rightarrow \mathrm{J/\psi} \mathrm{K}^{+}$. The analysis uses a data sample of proton-proton collisions at a center-of-mass energy of 13TeV, collected by the CMS experiment in 2018 and corresponding to an integrated luminosity of 61.6 $\mathrm{fb}^{-1}$. The $f_{s}/f_{u}$ ratio is observed to depend on the $\mathrm{B}$ $p_T$, and to be consistent with becoming asymptotically constant at large $p_T$. No rapidity dependence is observed. The ratio of the $\mathrm{B}^{0}$ to $\mathrm{B}^{+}$ hadron production fractions $f_{d}/f_{u}$, measured using the $\mathrm{B}^{0} \rightarrow \mathrm{J/\psi} \mathrm{K}^{*0}$ decay channel, is found to be consistent with unity and independent of $p_T$ and rapidity.