Sebastian Ordoñez-Soto
Universidad Nacional de Colombia
Internship tutor: Sergey Barsuk
June 27th, 2024
IJCLab LHCb group meeting
S. Ordonez Soto
June 27th, 2024
S. Ordonez Soto
June 27th, 2024
\(m_{B_{c}} = (6274.47 \pm 0.32)\) MeV
\(\tau_{B_{c}} = (0.507 \pm 0.009) \) ps
Lowest-mass bound state of two heavy quarks of different flavors.
Discovered by the CDF collaboration in 1998.
Has no strong or electromagnetic decay channels.
Its weak decay yields a large branching fraction to final states containing a \(J/ \psi\)
Full decay width: \(\Gamma = \Gamma_{b} + \Gamma_{c} + \Gamma_{bc}\)
\(\Gamma_{b}: \bar{b}\rightarrow \bar{c}W^{+}\), with \(c\) as spectator (~ 20%)
\(\Gamma_{c}: c\rightarrow sW^{+}\), with \(\bar{b}\) as spectator (~ 70%)
\(\Gamma_{bc}: c\bar{b} \rightarrow W^{+}\), weak annihilation (~ 10%)
Introducing the \(B_{c}^{+}\) meson
S. Ordonez Soto
June 27th, 2024
The decay channel
\(B_{c}^{+}\rightarrow \eta_{c}\mu^{+}\nu_{\mu}\) is one of the possible \(B_{c}^{+}\) semileptonic (SL) decay channels.
\(B_{c}^{+}\rightarrow J/\psi\mu^{+}\nu_{\mu}\) was already measured by LHCb \(\rightarrow R(J/\psi)\).
S. Ordonez Soto
June 27th, 2024
Analysis strategy
The \(B_{c}^{+}\rightarrow \eta_{c}\mu^{+}\nu_{\mu}\) decay will be analyzed together with the \(B_{c}^{+}\rightarrow J/\psi\mu^{+}\nu_{\mu}\), which is used as normalization channel.
The ratio \(\frac{\mathcal{B}(B_{c}^{+}\rightarrow \eta_{c}\mu^{+}\nu_{\mu})}{\mathcal{B}(B_{c}^{+}\rightarrow J/\psi\mu^{+}\nu_{\mu})}\) can be calculated as:
Calculated from MC
Yield extraction from final fit
The \(R_{\eta_{c}}\) could be calculated as:
S. Ordonez Soto
June 27th, 2024
Data sample
LHCb run 2 data from proton-proton collisions, at \(\sqrt{s}=13 \text{TeV}\) and \(4 \text{fb}^{-1}\), collected from 2015 to 2017.
There are two main variables for the analysis:
The \(p\bar{p}\) invariant mass \(M(p\bar{p})\)
The \(p\bar{p}\mu\) corrected mass, defined as: \(M_{CORR} = \sqrt{M^{2}(p\bar{p}\mu) + p^{2}_{\bot}} + p_{\bot}\)
S. Ordonez Soto
June 27th, 2024
Simulation samples
There are Monte Carlo samples available for both signal and different backgrounds
Inclusive bkg: \(b\rightarrow \eta_{c}X\) and \(b\rightarrow J/\psi X\) decays
Peaking bkg:
S. Ordonez Soto
June 27th, 2024
Pre-selection
Charmonia optimization
A set of selection requirements is initially applied, including: vertex quality and PID requirements
Additional cuts are added to optimize charmonia:
S. Ordonez Soto
June 27th, 2024
Fit models to \(M_{CORR}\) distributions
Using the MC samples the shapes of the \(M_{CORR}\) distributions for signal and background decay channels are extracted.
\(B_{c}^{+}\rightarrow\eta_{c}\mu^{+}\nu_{\mu}\)
\(B_{c}^{+}\rightarrow J/\psi\mu^{+}\nu_{\mu}\)
S. Ordonez Soto
June 27th, 2024
Fit models to \(M_{CORR}\) distributions
\(B_{c}\rightarrow(\chi_{0}\rightarrow J/\psi\gamma)\mu\nu_{\mu}\)
\(B_{c}\rightarrow(\chi_{1}\rightarrow J/\psi\gamma)\mu\nu_{\mu}\)
\(B_{c}\rightarrow(\chi_{2}\rightarrow J/\psi\gamma)\mu\nu_{\mu}\)
\(B_{c}\rightarrow \eta_{c}(\tau\rightarrow\mu\nu_{\mu}\bar{\nu_{\tau}})\nu_{\tau}\)
\(B_{c}\rightarrow(h_{c}\rightarrow\eta_{c}\gamma)\mu\nu_{\mu}\)
\(B_{c}\rightarrow J/\psi(\tau\rightarrow\mu\nu_{\mu}\bar{\nu_{\tau}})\nu_{\tau}\)
\(B_{c}\rightarrow(\psi(2S)\rightarrow J/\psi \pi\pi)\mu\nu_{\mu}\)
S. Ordonez Soto
June 27th, 2024
Fit models to \(M_{CORR}\) distributions
\(b\rightarrow J/\psi X\)
\(b\rightarrow \eta_{c} X\)
S. Ordonez Soto
June 27th, 2024
Signal extraction
\(\eta_{c}\) and \(J/\psi\) yields are extracted from fits to the \(M(p\bar{p})\) distribution in bins of \(M_{CORR}\)
Data from this bin is extracted, and the charmonia fit model is used
S. Ordonez Soto
June 27th, 2024
Signal extraction
The yields from fits to the \(M(p\bar{p})\) in bins of \(M_{CORR}\) allow us to obtain the \(M_{CORR}\) distribution for true \(\eta_{c}\) and \(J/\psi\)
These true \(\eta_{c}\) and \(J/\psi\) don't necessarily come from \(B_{c}^{+}\rightarrow \eta_{c}\mu^{+}\nu_{\mu}\)
S. Ordonez Soto
June 27th, 2024
Final fit
We use the different shapes to fit these \(M_{CORR}\) distributions and extract the two yields: \(N_{B_{c}^{+}\rightarrow \eta_{c}\mu^{+}\nu_{\mu}}\) and \(N_{B_{c}^{+}\rightarrow J/\psi\mu^{+}\nu_{\mu}}\)
This is work in progress!
S. Ordonez Soto
June 27th, 2024
S. Ordonez Soto
June 27th, 2024
S. Ordonez Soto
June 27th, 2024
Stripping selection
S. Ordonez Soto
June 27th, 2024
\(M_{CORR}\) resolution study
Previous to the signal extraction, it is necessary to check the resolution in the \(M_{CORR}\) using signal MC .
Acceptance efficiency \(\epsilon_{acc}\) from generator-level simulations. The product \(\epsilon_{reco} \times \epsilon_{sel} \times \epsilon_{trig}\) can be calculated as follows:
\(\longrightarrow N_{processed} = 1\)M events
Total efficiency
S. Ordonez Soto
June 27th, 2024
Decay modes efficiency
S. Ordonez Soto
June 27th, 2024
The yields of the peaking background decays are fixed with respect to the yields of the signal with the values shown in the table: