{"title":"在$\\sqrt{s_{mathrm{NN}}} = 5.02$ TeV的p-Pb对撞中通过非突变粲强子测量美的产生","authors":"ALICE Collaboration","doi":"arxiv-2407.10593","DOIUrl":null,"url":null,"abstract":"The production cross sections of $\\mathrm {D^0}$, $\\mathrm {D^+}$, and\n$\\mathrm {\\Lambda_{c}^{+}}$ hadrons originating from beauty-hadron decays (i.e.\nnon-prompt) were measured for the first time at midrapidity in proton$-$lead\n(p$-$Pb) collisions at the center-of-mass energy per nucleon pair of\n$\\sqrt{s_{\\mathrm{NN}}} = 5.02$ TeV. Nuclear modification factors ($R_{\\mathrm\n{pPb}}$) of non-prompt $\\mathrm {D^0}$, $\\mathrm {D^+}$, and $\\mathrm\n{\\Lambda_{c}^{+}}$ are calculated as a function of the transverse momentum\n($p_{\\mathrm T}$) to investigate the modification of the momentum spectra\nmeasured in p$-$Pb collisions with respect to those measured in proton$-$proton\n(pp) collisions at the same energy. The $R_{\\mathrm {pPb}}$ measurements are\ncompatible with unity and with the measurements in the prompt charm sector, and\ndo not show a significant $p_{\\mathrm T}$ dependence. The $p_{\\mathrm\nT}$-integrated cross sections and $p_{\\mathrm T}$-integrated $R_{\\mathrm\n{pPb}}$ of non-prompt $\\mathrm {D^0}$ and $\\mathrm {D^+}$ mesons are also\ncomputed by extrapolating the visible cross sections down to $p_{\\mathrm T}$ =\n0. The non-prompt D-meson $R_{\\mathrm {pPb}}$ integrated over $p_{\\mathrm T}$\nis compatible with unity and with model calculations implementing modification\nof the parton distribution functions of nucleons bound in nuclei with respect\nto free nucleons. The non-prompt $\\mathrm {\\Lambda_{c}^{+}/D^{0}}$ and\n$\\mathrm{D^+/D^0}$ production ratios are computed to investigate hadronisation\nmechanisms of beauty quarks into mesons and baryons. The measured ratios as a\nfunction of $p_{\\mathrm T}$ display a similar trend to that measured for charm\nhadrons in the same collision system.","PeriodicalId":501206,"journal":{"name":"arXiv - PHYS - Nuclear Experiment","volume":"5 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-07-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Measurement of beauty production via non-prompt charm hadrons in p-Pb collisions at $\\\\sqrt{s_{\\\\mathrm{NN}}} = 5.02$ TeV\",\"authors\":\"ALICE Collaboration\",\"doi\":\"arxiv-2407.10593\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The production cross sections of $\\\\mathrm {D^0}$, $\\\\mathrm {D^+}$, and\\n$\\\\mathrm {\\\\Lambda_{c}^{+}}$ hadrons originating from beauty-hadron decays (i.e.\\nnon-prompt) were measured for the first time at midrapidity in proton$-$lead\\n(p$-$Pb) collisions at the center-of-mass energy per nucleon pair of\\n$\\\\sqrt{s_{\\\\mathrm{NN}}} = 5.02$ TeV. Nuclear modification factors ($R_{\\\\mathrm\\n{pPb}}$) of non-prompt $\\\\mathrm {D^0}$, $\\\\mathrm {D^+}$, and $\\\\mathrm\\n{\\\\Lambda_{c}^{+}}$ are calculated as a function of the transverse momentum\\n($p_{\\\\mathrm T}$) to investigate the modification of the momentum spectra\\nmeasured in p$-$Pb collisions with respect to those measured in proton$-$proton\\n(pp) collisions at the same energy. The $R_{\\\\mathrm {pPb}}$ measurements are\\ncompatible with unity and with the measurements in the prompt charm sector, and\\ndo not show a significant $p_{\\\\mathrm T}$ dependence. The $p_{\\\\mathrm\\nT}$-integrated cross sections and $p_{\\\\mathrm T}$-integrated $R_{\\\\mathrm\\n{pPb}}$ of non-prompt $\\\\mathrm {D^0}$ and $\\\\mathrm {D^+}$ mesons are also\\ncomputed by extrapolating the visible cross sections down to $p_{\\\\mathrm T}$ =\\n0. The non-prompt D-meson $R_{\\\\mathrm {pPb}}$ integrated over $p_{\\\\mathrm T}$\\nis compatible with unity and with model calculations implementing modification\\nof the parton distribution functions of nucleons bound in nuclei with respect\\nto free nucleons. The non-prompt $\\\\mathrm {\\\\Lambda_{c}^{+}/D^{0}}$ and\\n$\\\\mathrm{D^+/D^0}$ production ratios are computed to investigate hadronisation\\nmechanisms of beauty quarks into mesons and baryons. The measured ratios as a\\nfunction of $p_{\\\\mathrm T}$ display a similar trend to that measured for charm\\nhadrons in the same collision system.\",\"PeriodicalId\":501206,\"journal\":{\"name\":\"arXiv - PHYS - Nuclear Experiment\",\"volume\":\"5 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-07-15\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - Nuclear Experiment\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2407.10593\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Nuclear Experiment","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2407.10593","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Measurement of beauty production via non-prompt charm hadrons in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV
The production cross sections of $\mathrm {D^0}$, $\mathrm {D^+}$, and
$\mathrm {\Lambda_{c}^{+}}$ 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
$\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV. Nuclear modification factors ($R_{\mathrm
{pPb}}$) of non-prompt $\mathrm {D^0}$, $\mathrm {D^+}$, and $\mathrm
{\Lambda_{c}^{+}}$ 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 $\mathrm {\Lambda_{c}^{+}/D^{0}}$ and
$\mathrm{D^+/D^0}$ 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.