Estimating decay yields from fits to these distributions

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SUMMARY

This discussion focuses on the methodology for estimating decay yields in rare B-decays, specifically the measurement of the ratio RK using an unbinned extended maximum-likelihood fit to the mass distributions of K+e+e− and K+µ+µ−. The LHCb collaboration's approach incorporates constraints from resonant decay modes and simultaneously fits various parameters, including selection efficiencies and trigger categories. The extraction of yields from the mass data points relies on maximum likelihood estimations, where the fitted function includes yield as a free parameter, allowing for the determination of optimal values and their uncertainties.

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  • Understanding of unbinned extended maximum-likelihood fitting techniques
  • Familiarity with B-decay processes and Lepton Flavour Universality
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Floyd_13
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I'm currently reading various papers on the violation of Lepton Flavour Universality in rare B-decays and I would appreciate some help in understanding the methodology for measuring the ratios in these decays.

Here is a quote from a recent paper from the LHCb collaboration (p.5):

An unbinned extended maximum-likelihood fit to the m(K+e+e) and m(K+µ+µ) distributions of nonresonant candidates is used to determine RK [the ratio]. In order to take into account the correlation between the selection efficiencies, the different trigger categories and data-taking periods are fitted simultaneously. The resonant decay mode yields are incorporated as constraints in this fit, such that the B+→K+µ+µ- yield and RK are fit parameters.

My question is how exactly are the yields extracted from the fits performed on the mass data points using maximum likelihood estimations? Does this mean that the fitted function has to be a function of the yield N? If yes, how is this achieved?
 
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For details you would have to ask the people doing the analysis, but the non-resonant yield and the ratio are free parameters in the fit function. The fit then determines the optimal values and their uncertainties.
 
Plotting the invariant mass of the final state particles gives a mass distribution of the B meson. In this distribution, the events are not only real B meson decays but they could come from different sources of background. Almost always you will have combinatorial background and, as it is the case in the analysis you are referring to, partially reconstructed background (see Fig 2, top-left). Some functions/shapes are then used to model these several contributions that add up to the observed mass distribution. For example, combinatorial background is usually fitted only with an exponential function, while the (non-resonant, i.e. non-Jpsi mode) signal is fitted probably with a Gaussian with exponential tails (DSCB).

What they mean by (signal) yield is actually the number of events in the initial mass distribution that fall under the signal shape in their fit model. The yield along with its uncertainty are determined by the fit.
 
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