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Luka Santelj

Publications and source records attributed to Luka Santelj.

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Recent advances and trends in pattern recognition and data analysis for RICH detectors

Ring Imaging Cherenkov (RICH) detectors are a key component of particle identification systems in many particle, nuclear and astroparticle physics experiments. Their ultimate performance depends not only on detector design and hardware implementation, but also crucially on the quality of pattern recognition and data analysis algorithms used to reconstruct Cherenkov ring images and to perform particle identification. In recent years, significant advances have been made both in traditional reconstruction approaches, such as likelihood-based methods and Hough-transform techniques, and in the application of modern machine learning tools. This contribution reviews the current state of RICH reconstruction algorithms, highlights representative use cases from operating experiments, and discusses emerging trends including global particle identification strategies and generative machine learning approaches for fast simulation and reconstruction.

physics.data-an

Recent developments in data reconstruction for aerogel RICH at Belle II

In the forward end-cap of the Belle II spectrometer, particle identification is provided by a proximity focusing RICH detector with an aerogel radiator (ARICH). The ARICH's primary function is to effectively distinguish between pions and kaons in the momentum range of 0.5 GeV/c to about 4 GeV/c, as well as to contribute to identification of low-momentum leptons. Since its operation began, Belle II has collected over 420 fb-1 of data. Based on this large data sample, studies of several effects that impact the performance of the ARICH detector were carried out. In this paper, we present a comparison of the observed Cherenkov ring image and detector particle identification performance in the measured data and detector simulation. Furthermore, we highlight recent efforts aimed at enhancing the ARICH's performance by taking into account the effects of particle decay in flight and scattering in materials before the detector, as well as by refining the probability density function used for particle identification likelihood evaluation.

physics.ins-det

Measurements of Beam Backgrounds in SuperKEKB Phase 2

The high design luminosity of the SuperKEKB electron-positron collider will result in challenging levels of beam-induced backgro\ unds in the interaction region. Understanding and mitigating these backgrounds is critical to the success of the Belle~II experi\ ment. We report on the first background measurements performed after roll-in of the Belle II detector, a period known as SuperKE\ KB Phase 2, utilizing both the BEAST II system of dedicated background detectors and the Belle II detector itself. We also repor\ t on first revisions to the background simulation made in response to our findings. Backgrounds measured include contributions f\ rom synchrotron radiation, beam-gas, Touschek, and injection backgrounds. At the end of Phase 2, single-beam backgrounds origina\ ting from the 4 GeV positron Low Energy Ring (LER) agree reasonably well with simulation, while backgrounds from the 7 GeV elect\ ron High Energy Ring (HER) are approximately one order of magnitude higher than simulation. We extrapolate these backgrounds for\ ward and conclude it is safe to install the Belle II vertex detector.

physics.ins-det

Time-dependent CP violation in $B$ decays at Belle

Using the full data sample collected with the Belle detector at the KEKB asymmetric-energy $e^+e^-$ collider, we present three recent measurements of time-dependent CP violation in $B$ decays, and a measurement of branching fraction of the $B^0\toρ^0ρ^0$ decay. We studied $B\toωK$ decays and measured the values of CP violation parameters in $B^0\toωK^0_S$ to be $A_{ωK^0_S} =-0.36\pm 0.19(stat)\pm 0.05(syst)$ and $S_{ωK^0_S}= +0.91\pm 0.32 \pm 0.05 $, which gives the first evidence of CP violation in this decay. In addition, we measured the direct CP violation in $B^+\toωK^+$ to be $A_{CP} (B^+ \to ωK^+)=-0.03\pm 0.04 \pm 0.01$, and two branching fractions $B(B^0 \to ωK^0)=(4.5\pm 0.4\pm 0.3) \times 10^{-6}$ and $B(B^+ \to ωK^+)=(6.8\pm 0.4 \pm 0.4) \times 10^{-6}$ (preliminary). From the measurement of CP violation parameters in the $B^0\toη'K^0$ decay we obtain $S_{η'K^0} = 0.68 \pm 0.07\pm 0.03$ and $A_{η'K^0} = +0.03 \pm 0.05\pm 0.04$ (preliminary), which are the world's most precise values to date. Measuring CP violating parameters in the $B^0\toπ^+π^-$ decay gives $A_{π^+π^-} = +0.33\pm 0.06\pm 0.03$ and $S_{π^+π^-} = -0.64\pm 0.08\pm 0.03$. This result is used in an isospin analysis to constrain the $ϕ_2$ angle of the unitarity triangle, with which we rule out the region $23.8^\circ < ϕ_2 < 66.8^\circ$ at the $1σ$ confidence level. The measured branching fraction of the $B^0\toρ^0ρ^0$ decay is $B(B^0\toρ^0ρ^0) = (1.02\pm 0.30\pm 0.15)\times 10^{-6}$, with the fraction of longitudinally polarized $ρ^0$ mesons being $f_L = 0.21^{+0.18}_{-0.22}\pm 0.13$. We obtain also the first evidence of the $B^0\to f_0ρ^0$ decay, by measuring $B(B^0\to f_0 ρ^0)\times B(f_0\to π^+π^-) = (0.86\pm 0.27 \pm 0.14)\times 10^{-6}$.

hep-ex

Pion wave function from lattice QCD vs. chiral quark models

We analyze the equal-time Bethe-Salpeter quark wave function of the pion obtained from a quenched lattice QCD calculation with delocalized quark interpolators. We find that the result agrees remarkably well with the predictions of the Nambu--Jona-Lasinio model in all channels. We choose the quenched lattice QCD, since it is closer to the large-Nc limit of the Nambu--Jona-Lasinio model. We also show how transversity information, relevant for the light-cone physics, can be obtained from our equal-time rest-frame lattice calculations.

hep-ph