CMS-PAS-HIN-19-005 | ||
Evidence for $\chi_{c1}\text{(3872)}$ in PbPb collisions and studies of its prompt production at ${\sqrt {\smash [b]{s_{_{\mathrm {NN}}}}}}=$ 5.02 TeV | ||
CMS Collaboration | ||
November 2019 | ||
Abstract: The first evidence for $\chi_{c1}\text{(3872)}$ in relativistic heavy ion collisions is reported. Prompt $\chi_{c1}\text{(3872)}$ production is studied in PbPb collisions at a center-of-mass energy of ${\sqrt {\smash [b]{s_{_{\mathrm {NN}}}}}} = $ 5.02 TeV per nucleon pair, using the decay chain $\chi_{c1}\text{(3872)} \rightarrow {\rm J}/\psi\pi^+\pi^-\rightarrow \mu^+\mu^-\pi^+\pi^-$. The data were recorded by the CMS detector in 2018 and correspond to an integrated luminosity of 1.7 $\pm$ 0.1 nb$^{-1}$. The measurement is performed in a kinematic range in which the $\chi_{c1}\text{(3872)}$ candidates have a transverse momentum 15 $ < p_{\mathrm{T}} < $ 50 GeV/$c$ and rapidity $|y| < $ 1.6. The statistical significance of the $\chi_{c1}\text{(3872)}$ signal is in excess of 3 standard deviations. The production and survival of the prompt $\chi_{c1}\text{(3872)}$ in the quark-gluon plasma is expected to depend upon its internal structure. The ratio of the $\chi_{c1}\text{(3872)}$ and $\psi\text{(2S)}$ yields is found to be $R = $ 1.10 $\pm$ 0.51(stat) $\pm$ 0.53 (syst). This results is compared to the similar ratio measured in pp collisions at $\sqrt{s} = $ 7 and 8 TeV. An indication of larger $R$ in PbPb collisions with respect to the pp reference is reported. | ||
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These preliminary results are superseded in this paper, Submitted to PRL. The superseded preliminary plots can be found here. |
Figures | Summary | Additional Figures | References | CMS Publications |
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Figures | |
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Figure 1:
Invariant mass distribution of $m_{\mu \mu \pi \pi}$ in PbPb collisions. The mass of the dimuon pair is forced to be equal to the nominal ${\mathrm{J}/\psi}$ mass [35]. The red line presents the unbinned maximum-likelihood fit result. The signal components of $\psi\text{(2S)}$ and $\chi_{c1}\text{(3872)}$ are shown by the blue and the green line respectively. The pull distribution is presented by the red boxes. |
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Figure 2:
The yield ratio $R$ of prompt $\chi_{c1}\text{(3872)}$ over $\psi\text{(2S)}$ in PbPb collisions at $ {\sqrt {\smash [b]{s_{_{\mathrm {NN}}}}}} = $ 5.02 TeV. The vertical bars (boxes) correspond to statistical (systematic) uncertainties. The yield ratio $R$ of prompt and nonprompt $\chi_{c1}\text{(3872)}$ over $\psi\text{(2S)}$ in pp collisions at $ {\sqrt {\smash [b]{s_{_{\mathrm {NN}}}}}} = $ 8 TeV from the ATLAS experiment [22] and $R$ of inclusive $\chi_{c1}\text{(3872)}$ over $\psi\text{(2S)}$ in pp collisions at $ {\sqrt {\smash [b]{s_{_{\mathrm {NN}}}}}} = $ 7 TeV from the CMS experiment [7] is also shown. |
Summary |
In summary, the first evidence for $\chi_{c1}\text{(3872)}$ production in heavy ion collisions is presented, using PbPb collisions at a center-of-mass energy of ${\sqrt {\smash [b]{s_{_{\mathrm {NN}}}}}} = $ 5.02 TeV per nucleon pair. The $\chi_{c1}\text{(3872)}$ state is reconstructed using the decay chain $\chi_{c1}\text{(3872)}\rightarrow {\rm J}/\psi\pi^+\pi^-\rightarrow \mu^+\mu^-\pi^+\pi^-$. The measurement is performed in a kinematic range in which the $\chi_{c1}\text{(3872)}$ candidates have a transverse momentum15 $ < p_{\mathrm{T}} < $ 50 GeV/$c$ and rapidity $ |y| < $ 1.6. The ratio $R$ of the prompt $\chi_{c1}\text{(3872)}$ and $\psi\text{(2S)}$ yields times their branching fractions into ${\rm J}/\psi\pi^+\pi^-$ is found to be 1.10 $\pm$ 0.51 (stat) $\pm$ 0.48 (syst). This result provides a unique experimental input to the theory community, towards elucidating the production mechanism and the nature of the $\chi_{c1}\text{(3872)}$ state. |
Additional Figures | |
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Additional Figure 1:
Pseudo-proper decay length ${l_{xy}}$ distributions of prompt and nonprompt signal X(3872) and $\psi$(2S) in PYTHIA+HYDJET Monte Carlo samples. |
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Additional Figure 2:
Invariant mass distribution of $m_{\mu \mu \pi \pi}$ in PbPb collisions with a nonprompt X(3872) enriched selection $ {l_{xy}} > $ 1 mm. The mass of dimuon pair is forced to be equal to the nominal ${{\mathrm {J} / \psi}} $ mass. The red line presents the unbinned maximum-likelihood fit result. The signal components of $\psi$(2S) and X(3872) are shown by the blue and the green line respectively. The pull distribution is presented by the red boxes. |
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Additional Figure 3:
The variation of the likelihood as a function of the number of X(3872) signals. The red lines indicate the values in the profile likelihood at the confidence level intervals of 68% and 95%. |
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Compact Muon Solenoid LHC, CERN |
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