cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.155497.v1/t32
title: "Table 13f" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $g^{(2)}_{ZZ}$ vs. $g^{(4)}_{ZZ}$ while other coefficients are fixed at their SM values.
description: No data abstract available.
DOI: 10.17182/hepdata.155498.v1/t1
title: "Spin-1\2 limits" of "Search for pair production of heavy particles decaying to a top quark and a gluon in the lepton+jets final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL upper limits on the product of the $t^{*} \overline{t}^{*}$ production cross section and the branching fraction squared $BR^2(t^{*} \rightarrow tg)$ for a spin-1/2 $t^{*}$ as a function of $m_{t^{*}}$. The inner (green) and outer (yellow) bands give the central probability intervals containing 68 and 95% of the expected upper limits under the background-only hypothesis. The cross section predicted by theory, following an EFT approach, is shown in blue, assuming $BR(t^{*} \rightarrow tg)=1$.
description: A search is presented for the pair production of new heavy resonances, each decaying into a top quark or antiquark and a gluon. The analysis uses data recorded with the CMS detector from proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 $fb^{-1}$. Events with one muon or electron, multiple jets, and missing transverse momentum are selected. After using a deep neural network to enrich the data sample with signal-like events, distributions in the scalar sum of the transverse momenta of all reconstructed objects are analyzed in search for a signal. No significant deviations from the standard model predictions are found. Upper limits at 95% confidence level are set on the product of cross section and branching fraction squared for the pair production of excited top quarks in the $t^{*} \rightarrow tg$ decay channel. The upper limits range from 0.12 $pb$ to 0.8 $fb$ for a $t^{*}$ with spin-1/2 and from 0.015 $pb$ to 1.0 $fb$ for a t^{*} with spin-3/2. These correspond to mass exclusion limits up to 1050 and 1700 GeV for spin-1/2 and spin-3/2 $t^{*}$ particles, respectively.
DOI: 10.17182/hepdata.155498.v1/t2
title: "Spin-3\2 limits" of "Search for pair production of heavy particles decaying to a top quark and a gluon in the lepton+jets final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL upper limits on the product of the $t^{*} \overline{t}^{*}$ production cross section and the branching fraction squared $BR^2(t^{*} \rightarrow tg)$ for a spin-3/2 $t^{*}$ as a function of $m_{t^{*}}$. The inner (green) and outer (yellow) bands give the central probability intervals containing 68 and 95% of the expected upper limits under the background-only hypothesis. The cross section predicted by theory, following an EFT approach, is shown in blue, assuming $BR(t^{*} \rightarrow tg)=1$. The results of the previous CMS analysis, using data corresponding to an integrated luminosity of 35.9 $fb^{-1}$, are shown in red.
description: A search is presented for the pair production of new heavy resonances, each decaying into a top quark or antiquark and a gluon. The analysis uses data recorded with the CMS detector from proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 $fb^{-1}$. Events with one muon or electron, multiple jets, and missing transverse momentum are selected. After using a deep neural network to enrich the data sample with signal-like events, distributions in the scalar sum of the transverse momenta of all reconstructed objects are analyzed in search for a signal. No significant deviations from the standard model predictions are found. Upper limits at 95% confidence level are set on the product of cross section and branching fraction squared for the pair production of excited top quarks in the $t^{*} \rightarrow tg$ decay channel. The upper limits range from 0.12 $pb$ to 0.8 $fb$ for a $t^{*}$ with spin-1/2 and from 0.015 $pb$ to 1.0 $fb$ for a t^{*} with spin-3/2. These correspond to mass exclusion limits up to 1050 and 1700 GeV for spin-1/2 and spin-3/2 $t^{*}$ particles, respectively.
DOI: 10.17182/hepdata.155498.v1/t3
title: "$S_T$ distribution, SR, muon channel" of "Search for pair production of heavy particles decaying to a top quark and a gluon in the lepton+jets final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distributions in $S_T$ in the SR for the muon channel, after a background-only fit to the data. The signal distributions are scaled to the cross section predicted by the theory. The hatched bands show the post-fit uncertainty band, combining all sources of uncertainty. The ratio of data to the background predictions is shown in the panels below the distributions.
description: A search is presented for the pair production of new heavy resonances, each decaying into a top quark or antiquark and a gluon. The analysis uses data recorded with the CMS detector from proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 $fb^{-1}$. Events with one muon or electron, multiple jets, and missing transverse momentum are selected. After using a deep neural network to enrich the data sample with signal-like events, distributions in the scalar sum of the transverse momenta of all reconstructed objects are analyzed in search for a signal. No significant deviations from the standard model predictions are found. Upper limits at 95% confidence level are set on the product of cross section and branching fraction squared for the pair production of excited top quarks in the $t^{*} \rightarrow tg$ decay channel. The upper limits range from 0.12 $pb$ to 0.8 $fb$ for a $t^{*}$ with spin-1/2 and from 0.015 $pb$ to 1.0 $fb$ for a t^{*} with spin-3/2. These correspond to mass exclusion limits up to 1050 and 1700 GeV for spin-1/2 and spin-3/2 $t^{*}$ particles, respectively.
DOI: 10.17182/hepdata.155498.v1/t4
title: "$S_T$ distribution, SR, electron channel" of "Search for pair production of heavy particles decaying to a top quark and a gluon in the lepton+jets final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distributions in $S_T$ in the SR for the electron channel, after a background-only fit to the data. The signal distributions are scaled to the cross section predicted by the theory. The hatched bands show the post-fit uncertainty band, combining all sources of uncertainty. The ratio of data to the background predictions is shown in the panels below the distributions.
description: A search is presented for the pair production of new heavy resonances, each decaying into a top quark or antiquark and a gluon. The analysis uses data recorded with the CMS detector from proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 $fb^{-1}$. Events with one muon or electron, multiple jets, and missing transverse momentum are selected. After using a deep neural network to enrich the data sample with signal-like events, distributions in the scalar sum of the transverse momenta of all reconstructed objects are analyzed in search for a signal. No significant deviations from the standard model predictions are found. Upper limits at 95% confidence level are set on the product of cross section and branching fraction squared for the pair production of excited top quarks in the $t^{*} \rightarrow tg$ decay channel. The upper limits range from 0.12 $pb$ to 0.8 $fb$ for a $t^{*}$ with spin-1/2 and from 0.015 $pb$ to 1.0 $fb$ for a t^{*} with spin-3/2. These correspond to mass exclusion limits up to 1050 and 1700 GeV for spin-1/2 and spin-3/2 $t^{*}$ particles, respectively.
DOI: 10.17182/hepdata.155514.v1/t1
title: "Table 1" of "Measurement of beauty production via non-prompt charm hadrons in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV"

description: Non-prompt $\mathrm{D}^0$ $p_\mathrm{{T}}$-differential production cross section $\mathrm{d}^2\sigma/\mathrm{d}p_\mathrm{T}\mathrm{d}y$ in p--Pb collisions at $\sqrt{{s_\mathrm{NN}}}=5.02~\mathrm{{TeV}}$ in the rapidity interval $-0.96 &lt; y_{\mathrm{cms}} &lt; 0.04$.
description: The production cross sections of $\mathrm{D}^0$, $\mathrm{D}^+$, and $\Lambda_{c}^{+}$ hadrons originating from beauty-hadron decays(i.e. non-prompt) were measured for the first time at midrapidity in proton--lead (p--Pb) collisions at the center-of-mass energy per nucleon pair of $\sqrt{{s_\mathrm{NN}}}=5.02 \mathrm{{TeV}}$. Nuclear modification factors ($R_{\mathrm{pPb}}$) of non-prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\Lambda_{c}^{+}$ are calculated as a function of the transverse momentum ($p_\mathrm{{T}}$)to investigate the modification of the momentum spectra measured in p--Pb collisions with respect to those measured in proton-proton (pp) collisions at the same energy. The $R_{\mathrm{pPb}}$ measurements are compatible with unity and with the measurements in the prompt charm sector, and do not show a significant $p_\mathrm{{T}}$ dependence. The $p_\mathrm{{T}}$-integrated cross sections and $p_\mathrm{{T}}$-integrated $R_{\mathrm{pPb}}$ of non-prompt $\mathrm{D}^0$ and $\mathrm{D}^+$ mesons are also computed by extrapolating the visible cross sections down to $p_\mathrm{{T}}$ = 0.The non-prompt D-meson $R_{\mathrm{pPb}}$ integrated over $p_\mathrm{{T}}$ is compatible with unity and with model calculations implementing modification of the parton distribution functions of nucleons bound in nuclei with respect to free nucleons. The non-prompt $\Lambda_{c}^{+}/\mathrm{D}^0$ and $\mathrm{D}^+/\mathrm{D}^0$ production ratios are computed to investigate hadronisation mechanisms of beauty quarks into mesons and baryons. The measured ratios as a function of $p_\mathrm{{T}}$ display a similar trend to that measured for charm hadrons in the same collision system.
DOI: 10.17182/hepdata.155514.v1/t2
title: "Table 2" of "Measurement of beauty production via non-prompt charm hadrons in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV"

description: Non-prompt $\mathrm{D}^+$ $p_\mathrm{{T}}$-differential production cross section $\mathrm{d}^2\sigma/\mathrm{d}p_\mathrm{T}\mathrm{d}y$ in p--Pb collisions at $\sqrt{{s_\mathrm{NN}}}=5.02~\mathrm{{TeV}}$ in the rapidity interval $-0.96 &lt; y_{\mathrm{cms}} &lt; 0.04$.
description: The production cross sections of $\mathrm{D}^0$, $\mathrm{D}^+$, and $\Lambda_{c}^{+}$ hadrons originating from beauty-hadron decays(i.e. non-prompt) were measured for the first time at midrapidity in proton--lead (p--Pb) collisions at the center-of-mass energy per nucleon pair of $\sqrt{{s_\mathrm{NN}}}=5.02 \mathrm{{TeV}}$. Nuclear modification factors ($R_{\mathrm{pPb}}$) of non-prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\Lambda_{c}^{+}$ are calculated as a function of the transverse momentum ($p_\mathrm{{T}}$)to investigate the modification of the momentum spectra measured in p--Pb collisions with respect to those measured in proton-proton (pp) collisions at the same energy. The $R_{\mathrm{pPb}}$ measurements are compatible with unity and with the measurements in the prompt charm sector, and do not show a significant $p_\mathrm{{T}}$ dependence. The $p_\mathrm{{T}}$-integrated cross sections and $p_\mathrm{{T}}$-integrated $R_{\mathrm{pPb}}$ of non-prompt $\mathrm{D}^0$ and $\mathrm{D}^+$ mesons are also computed by extrapolating the visible cross sections down to $p_\mathrm{{T}}$ = 0.The non-prompt D-meson $R_{\mathrm{pPb}}$ integrated over $p_\mathrm{{T}}$ is compatible with unity and with model calculations implementing modification of the parton distribution functions of nucleons bound in nuclei with respect to free nucleons. The non-prompt $\Lambda_{c}^{+}/\mathrm{D}^0$ and $\mathrm{D}^+/\mathrm{D}^0$ production ratios are computed to investigate hadronisation mechanisms of beauty quarks into mesons and baryons. The measured ratios as a function of $p_\mathrm{{T}}$ display a similar trend to that measured for charm hadrons in the same collision system.
DOI: 10.17182/hepdata.155514.v1/t3
title: "Table 3" of "Measurement of beauty production via non-prompt charm hadrons in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV"

description: Non-prompt $\Lambda_{c}^{+}$ $p_\mathrm{{T}}$-differential production cross section $\mathrm{d}^2\sigma/\mathrm{d}p_\mathrm{T}\mathrm{d}y$ in p--Pb collisions at $\sqrt{{s_\mathrm{NN}}}=5.02~\mathrm{{TeV}}$ in the rapidity interval $-0.96 &lt; y_{\mathrm{cms}} &lt; 0.04$.
description: The production cross sections of $\mathrm{D}^0$, $\mathrm{D}^+$, and $\Lambda_{c}^{+}$ hadrons originating from beauty-hadron decays(i.e. non-prompt) were measured for the first time at midrapidity in proton--lead (p--Pb) collisions at the center-of-mass energy per nucleon pair of $\sqrt{{s_\mathrm{NN}}}=5.02 \mathrm{{TeV}}$. Nuclear modification factors ($R_{\mathrm{pPb}}$) of non-prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\Lambda_{c}^{+}$ are calculated as a function of the transverse momentum ($p_\mathrm{{T}}$)to investigate the modification of the momentum spectra measured in p--Pb collisions with respect to those measured in proton-proton (pp) collisions at the same energy. The $R_{\mathrm{pPb}}$ measurements are compatible with unity and with the measurements in the prompt charm sector, and do not show a significant $p_\mathrm{{T}}$ dependence. The $p_\mathrm{{T}}$-integrated cross sections and $p_\mathrm{{T}}$-integrated $R_{\mathrm{pPb}}$ of non-prompt $\mathrm{D}^0$ and $\mathrm{D}^+$ mesons are also computed by extrapolating the visible cross sections down to $p_\mathrm{{T}}$ = 0.The non-prompt D-meson $R_{\mathrm{pPb}}$ integrated over $p_\mathrm{{T}}$ is compatible with unity and with model calculations implementing modification of the parton distribution functions of nucleons bound in nuclei with respect to free nucleons. The non-prompt $\Lambda_{c}^{+}/\mathrm{D}^0$ and $\mathrm{D}^+/\mathrm{D}^0$ production ratios are computed to investigate hadronisation mechanisms of beauty quarks into mesons and baryons. The measured ratios as a function of $p_\mathrm{{T}}$ display a similar trend to that measured for charm hadrons in the same collision system.
DOI: 10.17182/hepdata.155514.v1/t4
title: "Table 4" of "Measurement of beauty production via non-prompt charm hadrons in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV"

description: Non-prompt $\mathrm{D}^0$ and $\mathrm{D}^+$ average $p_\mathrm{{T}}$-differential $R_{\mathrm{pPb}}$ in p--Pb collisions at $\sqrt{{s_\mathrm{NN}}}=5.02~\mathrm{{TeV}}$ in the rapidity interval $-0.96 &lt; y_{\mathrm{cms}} &lt; 0.04$.
description: The production cross sections of $\mathrm{D}^0$, $\mathrm{D}^+$, and $\Lambda_{c}^{+}$ hadrons originating from beauty-hadron decays(i.e. non-prompt) were measured for the first time at midrapidity in proton--lead (p--Pb) collisions at the center-of-mass energy per nucleon pair of $\sqrt{{s_\mathrm{NN}}}=5.02 \mathrm{{TeV}}$. Nuclear modification factors ($R_{\mathrm{pPb}}$) of non-prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\Lambda_{c}^{+}$ are calculated as a function of the transverse momentum ($p_\mathrm{{T}}$)to investigate the modification of the momentum spectra measured in p--Pb collisions with respect to those measured in proton-proton (pp) collisions at the same energy. The $R_{\mathrm{pPb}}$ measurements are compatible with unity and with the measurements in the prompt charm sector, and do not show a significant $p_\mathrm{{T}}$ dependence. The $p_\mathrm{{T}}$-integrated cross sections and $p_\mathrm{{T}}$-integrated $R_{\mathrm{pPb}}$ of non-prompt $\mathrm{D}^0$ and $\mathrm{D}^+$ mesons are also computed by extrapolating the visible cross sections down to $p_\mathrm{{T}}$ = 0.The non-prompt D-meson $R_{\mathrm{pPb}}$ integrated over $p_\mathrm{{T}}$ is compatible with unity and with model calculations implementing modification of the parton distribution functions of nucleons bound in nuclei with respect to free nucleons. The non-prompt $\Lambda_{c}^{+}/\mathrm{D}^0$ and $\mathrm{D}^+/\mathrm{D}^0$ production ratios are computed to investigate hadronisation mechanisms of beauty quarks into mesons and baryons. The measured ratios as a function of $p_\mathrm{{T}}$ display a similar trend to that measured for charm hadrons in the same collision system.
DOI: 10.17182/hepdata.155514.v1/t5
title: "Table 5" of "Measurement of beauty production via non-prompt charm hadrons in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV"

description: Non-prompt $\Lambda_{c}^{+}$ $p_\mathrm{{T}}$-differential $R_{\mathrm{pPb}}$ in p--Pb collisions at $\sqrt{{s_\mathrm{NN}}}=5.02~\mathrm{{TeV}}$ in the rapidity interval $-0.96 &lt; y_{\mathrm{cms}} &lt; 0.04$.
description: The production cross sections of $\mathrm{D}^0$, $\mathrm{D}^+$, and $\Lambda_{c}^{+}$ hadrons originating from beauty-hadron decays(i.e. non-prompt) were measured for the first time at midrapidity in proton--lead (p--Pb) collisions at the center-of-mass energy per nucleon pair of $\sqrt{{s_\mathrm{NN}}}=5.02 \mathrm{{TeV}}$. Nuclear modification factors ($R_{\mathrm{pPb}}$) of non-prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\Lambda_{c}^{+}$ are calculated as a function of the transverse momentum ($p_\mathrm{{T}}$)to investigate the modification of the momentum spectra measured in p--Pb collisions with respect to those measured in proton-proton (pp) collisions at the same energy. The $R_{\mathrm{pPb}}$ measurements are compatible with unity and with the measurements in the prompt charm sector, and do not show a significant $p_\mathrm{{T}}$ dependence. The $p_\mathrm{{T}}$-integrated cross sections and $p_\mathrm{{T}}$-integrated $R_{\mathrm{pPb}}$ of non-prompt $\mathrm{D}^0$ and $\mathrm{D}^+$ mesons are also computed by extrapolating the visible cross sections down to $p_\mathrm{{T}}$ = 0.The non-prompt D-meson $R_{\mathrm{pPb}}$ integrated over $p_\mathrm{{T}}$ is compatible with unity and with model calculations implementing modification of the parton distribution functions of nucleons bound in nuclei with respect to free nucleons. The non-prompt $\Lambda_{c}^{+}/\mathrm{D}^0$ and $\mathrm{D}^+/\mathrm{D}^0$ production ratios are computed to investigate hadronisation mechanisms of beauty quarks into mesons and baryons. The measured ratios as a function of $p_\mathrm{{T}}$ display a similar trend to that measured for charm hadrons in the same collision system.
DOI: 10.17182/hepdata.155514.v1/t7
title: "Table 7" of "Measurement of beauty production via non-prompt charm hadrons in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV"

description: Non-prompt $\mathrm{D}^+$ $p_\mathrm{{T}}$-integrated $R_{\mathrm{pPb}}$ p--Pb collisions at $\sqrt{{s_\mathrm{NN}}}=5.02~\mathrm{{TeV}}$ in the rapidity interval $-0.96 &lt; y_{\mathrm{cms}} &lt; 0.04$.
description: The production cross sections of $\mathrm{D}^0$, $\mathrm{D}^+$, and $\Lambda_{c}^{+}$ hadrons originating from beauty-hadron decays(i.e. non-prompt) were measured for the first time at midrapidity in proton--lead (p--Pb) collisions at the center-of-mass energy per nucleon pair of $\sqrt{{s_\mathrm{NN}}}=5.02 \mathrm{{TeV}}$. Nuclear modification factors ($R_{\mathrm{pPb}}$) of non-prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\Lambda_{c}^{+}$ are calculated as a function of the transverse momentum ($p_\mathrm{{T}}$)to investigate the modification of the momentum spectra measured in p--Pb collisions with respect to those measured in proton-proton (pp) collisions at the same energy. The $R_{\mathrm{pPb}}$ measurements are compatible with unity and with the measurements in the prompt charm sector, and do not show a significant $p_\mathrm{{T}}$ dependence. The $p_\mathrm{{T}}$-integrated cross sections and $p_\mathrm{{T}}$-integrated $R_{\mathrm{pPb}}$ of non-prompt $\mathrm{D}^0$ and $\mathrm{D}^+$ mesons are also computed by extrapolating the visible cross sections down to $p_\mathrm{{T}}$ = 0.The non-prompt D-meson $R_{\mathrm{pPb}}$ integrated over $p_\mathrm{{T}}$ is compatible with unity and with model calculations implementing modification of the parton distribution functions of nucleons bound in nuclei with respect to free nucleons. The non-prompt $\Lambda_{c}^{+}/\mathrm{D}^0$ and $\mathrm{D}^+/\mathrm{D}^0$ production ratios are computed to investigate hadronisation mechanisms of beauty quarks into mesons and baryons. The measured ratios as a function of $p_\mathrm{{T}}$ display a similar trend to that measured for charm hadrons in the same collision system.
DOI: 10.17182/hepdata.155514.v1/t10
title: "Table 10" of "Measurement of beauty production via non-prompt charm hadrons in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV"

description: Ratio of the $p_\mathrm{{T}}$-integrated ($2 &lt; p_\mathrm{{T}} &lt; 24$ $\mathrm{{GeV}}/c$) $R_{\mathrm{pPb}}$ of non-prompt $\Lambda_{c}^{+}$ and non-prompt $\mathrm{D}^0$ in p--Pb collisions at $\sqrt{{s_\mathrm{NN}}}=5.02~\mathrm{{TeV}}$ in the rapidity interval $-0.96 &lt; y_{\mathrm{cms}} &lt; 0.04$.
description: The production cross sections of $\mathrm{D}^0$, $\mathrm{D}^+$, and $\Lambda_{c}^{+}$ hadrons originating from beauty-hadron decays(i.e. non-prompt) were measured for the first time at midrapidity in proton--lead (p--Pb) collisions at the center-of-mass energy per nucleon pair of $\sqrt{{s_\mathrm{NN}}}=5.02 \mathrm{{TeV}}$. Nuclear modification factors ($R_{\mathrm{pPb}}$) of non-prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\Lambda_{c}^{+}$ are calculated as a function of the transverse momentum ($p_\mathrm{{T}}$)to investigate the modification of the momentum spectra measured in p--Pb collisions with respect to those measured in proton-proton (pp) collisions at the same energy. The $R_{\mathrm{pPb}}$ measurements are compatible with unity and with the measurements in the prompt charm sector, and do not show a significant $p_\mathrm{{T}}$ dependence. The $p_\mathrm{{T}}$-integrated cross sections and $p_\mathrm{{T}}$-integrated $R_{\mathrm{pPb}}$ of non-prompt $\mathrm{D}^0$ and $\mathrm{D}^+$ mesons are also computed by extrapolating the visible cross sections down to $p_\mathrm{{T}}$ = 0.The non-prompt D-meson $R_{\mathrm{pPb}}$ integrated over $p_\mathrm{{T}}$ is compatible with unity and with model calculations implementing modification of the parton distribution functions of nucleons bound in nuclei with respect to free nucleons. The non-prompt $\Lambda_{c}^{+}/\mathrm{D}^0$ and $\mathrm{D}^+/\mathrm{D}^0$ production ratios are computed to investigate hadronisation mechanisms of beauty quarks into mesons and baryons. The measured ratios as a function of $p_\mathrm{{T}}$ display a similar trend to that measured for charm hadrons in the same collision system.