27–31 May 2024
Chulalongkorn University
Asia/Bangkok timezone

Contribution List

101 out of 101 displayed
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  1. 27/05/2024, 09:00
  2. Marco Fedele
    27/05/2024, 09:30
    Rare decays of hadrons and leptons
    Plenary session
  3. Michael Schmidt (UNSW Sydney)
    27/05/2024, 10:00
    Rare decays of hadrons and leptons
    Plenary session
  4. Dr Chris Bouchard (University of Glasgow)
    27/05/2024, 11:10
    Rare decays of hadrons and leptons
    Plenary session
  5. Dr Ami Rostomyan (DESY)
    27/05/2024, 11:40
    Rare decays of hadrons and leptons
    Plenary session
  6. Luyan Tao
    27/05/2024, 12:05
    Rare decays of hadrons and leptons
    Plenary session
  7. Junxi Cui (Southeast University)
    27/05/2024, 14:00
    CP violation in hadrons and leptons, EDMs
    Parallel session

    The Belle and Belle$~$II experiments have collected a $1.4~\mathrm{ab}^{-1}$ sample of $e^+e^-$ collision data at centre-of-mass energies near the $\Upsilon(nS)$ resonances. These samples contain a large number of $e^+e^-\to c\bar{c}$ events that produce charmed mesons. Direct $C\!P$ violation is searched for in $D^0\to K^0_{\rm S}K^0_{\rm S}$ decays and $D$-meson decays to a four-body final...

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  8. mitesh behera
    27/05/2024, 14:00
    Neutrino physics
    Parallel session

    This work's novelty lies in using the simplest group i.e. $\Gamma_2 \cong S_3$ modular symmetry implemented on the canonical seesaw to explain neutrino phenomenology. Here, we construct and classify models based on the doublet and singlet representations of supermultiplets under $S_3$ discrete symmetry along with their respective modular weights, allowing a mass matrix for the neutrino sector...

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  9. Jolanta Brodzicka (INP PAS Krakow), Jolanta Brodzicka (Polish Academy of Sciences (PL))
    27/05/2024, 14:00
    Rare decays of hadrons and leptons
    Parallel session

    Charm measurements allow for testing the Standard Model in a way complementary to measurements in b-quark sector. LHCb experiment, with its large data sample and excellent performance, provides sensitivity approaching the Standard Model predictions for rare charm decays. In this talk, recent LHCb results on rare decays of charm hadrons will be presented.

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  10. Tadeusz Lesiak (Polish Academy of Sciences (PL)), Tadeusz Lesiak
    27/05/2024, 14:15
    Exotic quarkonium-like states
    Parallel session

    Studies of exotic hadrons comprise a natural and privileged playground for a more thorough elucidation of the nature of quantum chromodynamics. In this contest the LHCb experiment, dedicated to study heavy flavor hadrons produced from pp collision at the LHC, plays a vital role, already providing evidence for several exotic hadrons. The talk will deliver an overview of the selected, latest...

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  11. Raktima Kalita (Cotton University)
    27/05/2024, 14:15
    Neutrino physics
    Parallel session

    In our work, we have used modular invariance approach to construct a neutrino mass model in the framework of the inverse seesaw(2,3) mechanism with modular S4 flavor symmetry. The use of modular invariance requires less number of flavon fields which increases the predictability of the model. The phenomenological study of the neutrino mass matrix is carried out using the current 3σ ranges of...

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  12. Marcela Garcia Hernandez
    27/05/2024, 14:15
    Rare decays of hadrons and leptons
    Parallel session

    The Belle II experiment has collected a 424fb$^{-1}$ sample of $e^{+}e^{-}$ collision data at center-of-mass energies near the resonances $\Upsilon(nS)$. This sample contains 389 million $e^{+}e^{-} \to \tau^{+}\tau^{-}$ events, which we use for precision tests of the standard model. In this talk, we focused on the measurements of the tau-lepton mass and
    tests of Lepton Flavor Universality...

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  13. Mr UTKARSH PATEL (Indian Institute of Technology, Bhilai)
    27/05/2024, 14:30
    Neutrino physics
    Parallel session

    We explore the connection between low-scale CP-violating Dirac phase $(\delta)$ and high-scale leptogenesis in a Left-Right Symmetric Model (LRSM) with scalar bidoublet and doublets. The fermion sector of the model is extended with one sterile neutrino $(S_L)$ per generation to implement a double seesaw mechanism in the neutral fermion mass matrix. The double seesaw is performed via the...

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  14. Mr Debjit Ghosh (INFN Trieste)
    27/05/2024, 14:30
    Rare decays of hadrons and leptons
    Parallel session

    The Belle and Belle$~$II experiments have collected a 1.1$~$ab$^{-1}$ sample of $e^+ e^-\to B\bar{B}$ collisions at the $\Upsilon(4S)$ resonance. These data, with low particle multiplicity and constrained initial state kinematics, are an ideal environment to search for rare $B$ meson decays proceeding via electroweak and radiative penguin processes. Results include those of the decay $B^+\to...

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  15. Vladimir Sergeychik (Moscow Institute of Physics and Technology State University (RU))
    27/05/2024, 14:30
    CP violation in hadrons and leptons, EDMs
    Parallel session

    Recent results on CP violation in charm and beauty sector, as well as lifetime measurements, by the CMS experiment at the LHC are presented. The analyses are based on 13 TeV pp collision data.

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  16. Dr Hai Yang Cheng (Academia Sinica)
    27/05/2024, 14:45
    Heavy quark decays and CKM
    Parallel session

    Inspired by the recent BESIII measurement of the decay asymmetry in the decay $\Lambda_c^+\to \Xi^0K^+$, we perform a global fit to the experimental data of two-body charmed baryon decays based on the topological diagrammatic approach (TDA) which has the advantage that it is more intuitive, graphic and easier to implement model calculations. The measured branching fractions and decay...

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  17. Aditya Gadam
    27/05/2024, 14:45
    Rare decays of hadrons and leptons
    Parallel session

    Highly suppressed (Rare) $b$-quark processes provide an excellent probe into heavy New Physics (NP) scenarios in conjunction with stringent tests of the Standard Model (SM). Rare decays of the form $b \rightarrow s \nu \bar{\nu}$ appear in the $\Lambda_b \rightarrow \Lambda \nu \bar{nu}$ channel, that has not yet been observed, but is a promising avenue of exploration at future $e^+e^-$...

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  18. Rukmani Mohanta
    27/05/2024, 14:45
    Neutrino physics
    Parallel session

    We illustrate neutrino mass and magnetic moment along with dark matter phenomenology in a Type-III radiative scenario. The Standard Model is enriched with three vector-like fermion triplets and two inert doublets to provide a suitable platform for the above phenomenological aspects. The inert scalars contribute to total relic density of dark matter in the Universe. Neutrino aspects are...

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  19. Haritha c.p (University of Hyderabad)
    27/05/2024, 15:00
    Heavy quark decays and CKM
    Parallel session

    Observations of flavor anomalies in the $b$-sector, particularly the deviations in the measurements of the lepton flavor universality ratios in the $b \rightarrow c \tau \nu_\tau$ transitions from the standard model (SM) predictions, suggest the existence of possible new physics beyond the SM. In the pursuit of new physics in similar decays involving $b\to c \ell \nu_{\ell}$ transitions, we...

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  20. Nayana Gautam
    27/05/2024, 15:00
    Neutrino physics
    Parallel session

    We study maximal texture zeros of the Dirac matrix in a minimal inverse seesaw ISS (2,3) model with $S_4$ flavor symmetry. The seesaw model is extended with the addition of 2 Right Handed neutrinos and 3 sterile states in the intermediate-mass range. To make the model more predictive, we have considered the maximum possible texture zeros in Dirac neutrino mass matrix $M_D$, heavy right-handed...

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  21. SANGEETA DEY (COTTON UNIVERSITY, ASSAM, INDIA)
    27/05/2024, 15:15
    Neutrino physics
    Parallel session

    In this work we carry out a systematic texture study of the neutrino mass matrix with the ansatzes - (i) one vanishing minor and (ii) the zero sum of the mass eigenvalues with the CP phases (henceforth vanishing trace). There are six possible textures of a neutrino mass matrix with one vanishing minor. The viability of each texture is checked with $3\sigma$ values of current neutrino data by...

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  22. Prof. Jian Tang (Sun Yat-Sen University(CN))
    27/05/2024, 16:05
    Neutrino physics
    Plenary session

    Results of a global data analysis can constrain the default 3-neutrino mixing scheme given unitarity assumption, based on recent data from the reactor, solar and long-baseline accelerator neutrino oscillation experiments. It is straightforward to extend the analysis towards the non-unitary assumption. Meanwhile, global neutrino data scrutiny serves as a probe of new physics such as whether...

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  23. Aikaterini Tzamarioudaki (Nat. Cent. for Sci. Res. Demokritos (GR)), Ekaterini Tzamariudaki (NCSR Demokritos)
    27/05/2024, 16:35
    Neutrino physics
    Plenary session

    The KM3NeT research infrastructure is building second-generation neutrino telescopes in the depths of the Mediterranean Sea. The KM3NeT/ARCA detector at a depth of 3500 m off the coast of Sicily, Italy, focuses on the detection of high energy (E>TeV) neutrinos from astrophysical sources. The KM3NeT/ORCA detector at a depth of 2500 m off the coast of Toulon, France, is aimed at studying low...

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  24. Aparajita Mazumdar
    27/05/2024, 17:00
    Neutrino physics
    Plenary session
  25. Dr Larisa Thorne (Johannes Gutenberg University Mainz)
    27/05/2024, 17:25
    Neutrino physics
    Plenary session

    Nearly 70 years since the neutrino was discovered, and 25 years since discovery of neutrino oscillations established its non-zero mass, the absolute neutrino-mass scale remains unknown. Due to its unique characteristics, determining this neutrino property requires new measurement techniques to be developed. Currently, there are four measurement approaches: using cosmological models, inference...

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  26. Hongyue Duyang (Shandong University)
    27/05/2024, 17:50
    Neutrino physics
    Plenary session
  27. Rahul Tiwary (Tata Institute of Fundamental Research, Mumbai)
    28/05/2024, 09:00
    Rare decays of hadrons and leptons
    Plenary session
  28. Rishabh Raturi (Indian Institute of Technology Bhubaneshar), Mr Rishabh Raturi (Indian Institute of Technology Bhubaneswar)
    28/05/2024, 09:30
    Rare decays of hadrons and leptons
    Plenary session
  29. Kai-Feng Chen (National Taiwan University (TW))
    28/05/2024, 09:55
    Rare decays of hadrons and leptons
    Plenary session

    Recent CMS results on rare decays are presented. The results are based on data collected in proton-proton collisions at sqrt(s) = 13 TeV.

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  30. Lakshan Madhan (University of Cambridge (GB)), Lakshan Ram Madhan Mohan (University of Bristol)
    28/05/2024, 10:20
    Rare decays of hadrons and leptons
    Plenary session

    In the Standard Model, decays mediated by $b\rightarrow sll$ are very suppressed making them sensitive to possible non-SM contributions.
    The latest LHCb measurement of the branching fraction ratio of this process between electrons and muons was shown to be consistent with the Standard Model.
    However, measurements of branching fraction and angular observables of $b\rightarrow s\mu \mu$ have...

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  31. Nathan Barry Heatley (University of London (GB))
    28/05/2024, 11:15
    Rare decays of hadrons and leptons
    Plenary session

    Overview and recent results on spectroscopy of exotic hadrons in ATLAS with Run-2 data are presented. Four-muon mass spectrum is studied, investigating the structures earlier observed by LHCb experiment in di-$J/\psi$ channel, using di-$J/\psi$ and $J/\psi+\psi(2S)$ final states. Search for exotic resonances is also performed in $\Upsilon(1S)+2\mu$ final state. ATLAS measurement of...

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  32. Steven Robertson (IPP / University of Alberta)
    28/05/2024, 11:40
    Heavy quark decays and CKM
    Plenary session
  33. Guglielmo De Nardo, Guglielmo De Nardo (Universita Federico II e INFN Sezione di Napoli (IT))
    28/05/2024, 12:05
    Heavy quark decays and CKM
    Plenary session
  34. Jake Bennett, Nazila Mahmoudi (CERN and Lyon University (FR)), Roy Briere, Xiao-Gang He
    28/05/2024, 12:30

    Topic: FPCP IAC Meeting
    Time: May 28, 2024 12:30 PM Bangkok

    Join Zoom Meeting
    https://cern.zoom.us/j/65325537999?pwd=LzdXakNXRmphdkJuUVVETlpCbythZz09

    Meeting ID: 653 2553 7999
    Passcode: 544134

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  35. Hsiang-nan Li
    28/05/2024, 14:00
    Neutrino physics
    Parallel session

    We propose theoretical constraints that fermion masses and mixing angles should respect. These constraints are derived from the dispersion relation obeyed by the box diagrams, which are responsible for the mixing of neutral states, such as the $\mu^-e^+$ and $\mu^+e^-$ mixing . The only assumption is that the electroweak symmetry of the Standard Model is restored at a high energy scale, which...

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  36. Ms Lipika Kolay (IIT Guwahati)
    28/05/2024, 14:00
    Flavor and Dark Sector
    Parallel session

    We have considered a simplified dark matter model featuring a spin-0 mediator that contributes to Flavor Changing Charge Current (FCCC) and Neutral Current (FCNC) processes, as well as electroweak observables at the one-loop level. Through a combined fit incorporating all flavor observables of FCNC, FCCC, and EW observables, we constrain the parameter space. This model adequately describes...

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  37. Qipeng Hu (University of Science and Technology of China (CN))
    28/05/2024, 14:00
    Heavy quark decays and CKM
    Parallel session

    Recent results on open heavy flavour and charmonium production from ATLAS experiment with Run-2 data are presented. This covers the double differential measurements of J/ψ and ψ(2S) production, D mesons and B+ production at √s=13 TeV

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  38. Manas Mohapatra (University of Hyderabad)
    28/05/2024, 14:15
    Flavor and Dark Sector
    Parallel session

    We explore $U(1)_{L_e-L_\mu}$ gauge extension of the Standard model with particle content enlarged by three neutral fermions, of which the lightest one contributes to dark matter content of the Universe. The scalar sector is enriched with a $\tilde{R}_2$ scalar leptoquark doublet to investigate flavor anomalies in $B$-meson sector, an additional inert scalar doublet to realize neutrino mass at...

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  39. Sudeshna Ganguly (Fermilab)
    28/05/2024, 14:15
    Neutrino physics
    Parallel session

    The upcoming long baseline neutrino experiments aim to enhance proton beam power to multi-MW scale and utilize large-scale detectors to address the challenge of limited event statistics. The DUNE experiment at LBNF will test the three neutrino flavor paradigm and directly search for CP violation by studying oscillation signatures in the high intensity $\nu_{\mu}$ (anti-$\nu_{\mu}$) beam to...

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  40. Marek Biros (Charles University (CZ))
    28/05/2024, 14:15
    Heavy quark decays and CKM
    Parallel session

    Various precision measurements with B mesons from ATLAS are presented. They include studies of CP violation in $B^0_s\to J/\psi\phi$ decay, $B_c^+$ meson decay properties and measurement of B0 meson lifetime, along with average decay width $\Gamma_d$ and $\Gamma_d/\Gamma_s$ ratio.

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  41. Dr Manoranjan Dutta (North Lakhimpur University)
    28/05/2024, 14:30
    Flavor and Dark Sector
    Parallel session

    The nature of neutrinos, whether Dirac or Majorana, is hitherto not known. Assuming that the neutrinos are Dirac, which needs $B-L$ to be an exact symmetry, we attempt to explain the observed proportionality between the relic densities of dark matter (DM) and baryonic matter in the present Universe ${\it i.e.,}\,\, \Omega_{\rm DM} \approx 5\, \Omega_{\rm B}$. We extend the Standard Model (SM)...

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  42. Anjan Giri
    28/05/2024, 14:30
    Neutrino physics
    Parallel session

    Neutrino oscillation in the matter could be affected by the sub-dominant, yet unknown, non-standard interactions (NSI). The upcoming long-baseline (LBL) neutrino experiments will be sensitive to these effects and can provide information on the unknown oscillation parameter values. The observed shift in $\delta_{CP}$ value observed for NOvA in case of standard model (SM) and NSIs arising...

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  43. Marcello Rotondo (INFN e Laboratori Nazionali di Frascati (IT))
    28/05/2024, 14:30
    Heavy quark decays and CKM
    Parallel session

    Lepton Flavor Universality (LFU) is a fundamental principle in the Standard Model (SM) of particle physics, stating that the interactions of different generations of leptons with the weak force should be identical. However, experimental observations in the last decade have hinted at potential violations of LFU by comparing the ratios of branching fractions of semileptonic $b \to c \ell \nu$...

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  44. Michele Mantovano (University and INFN Trieste)
    28/05/2024, 14:45
    Heavy quark decays and CKM
    Parallel session

    The Belle and Belle$~$II experiments have collected a 1.1$~$ab$^{-1}$ sample of $e^+ e^-\to B\bar{B}$ collisions at the $\Upsilon(4S)$ resonance. These data, with low particle multiplicity, constrained initial state kinematics and excellent lepton identification, are an ideal environment to study lepton-flavour universality in semileptonic decays of the $B$ meson. We present results on the...

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  45. Chinmay Bera (Mahindra University, Hyderabad-500043, India)
    28/05/2024, 14:45
    Neutrino physics
    Parallel session

    In this work, we study the impact of the environmental decoherence at Protvino to ORCA (P2O) experiment which has a substantial baseline of 2595 kilometres. We simulate this experiment assuming different phenomenological models and by considering energy dependency of decoherence parameter, $\Gamma \propto E_{\nu}^n$ ( $n = 0, \pm 1, \pm 2$). We estimate the sensitivity of P2O experiment to...

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  46. Ms Priyanka Boora (Malaviya National Institute of Technology Jaipur)
    28/05/2024, 14:45
    Flavor and Dark Sector
    Parallel session

    We perform a model-independent study of $c \to s \mu \nu$ mediated transitions to analyze the new physics effects in the presence of right-handed neutrinos. We have adopted the effective field theory approach and write the low-energy effective Hamiltonian including all possible dimension-six operators. The Wilson coefficients introduced through low energy effective Hamiltonian encode all NP...

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  47. Matthew Gar Jun Man (University of Toronto (CA))
    28/05/2024, 15:00
    Neutrino physics
    Parallel session

    The Deep Underground Neutrino Experiment (DUNE) is a next-generation long-baseline neutrino experiment currently under construction in the US. The experiment consists of a broadband neutrino beam from Fermilab to the Sanford Underground Research Facility (SURF) in Lead, South Dakota, a high-precision near detector, and a large liquid argon time-projection chamber (LArTPC) far detector. Two...

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  48. Ms Swagata Biswas (National Institute of Technology Durgapur)
    28/05/2024, 15:00
    Flavor and Dark Sector
    Parallel session

    Inspired by the various LHCb results of lepton flavour violation on b→s transition we will study the lepton flavour violating b→l1l2 decays in terms of transversity amplitudes in non-universal Z’ model. These LFV
    processes are extremely suppressed in the Standard Model (SM) because the expected levels at the SM lie far below current experimental sensitivities. In particular the branching...

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  49. Sebastiano Raiz
    28/05/2024, 15:00
    Heavy quark decays and CKM
    Parallel session

    The Belle and Belle$~$II experiments have collected a 1.1$~$ab$^{-1}$ sample of $e^+ e^-\to B\bar{B}$ collisions at the $\Upsilon(4S)$ resonance. The study of hadronic $B$ decays in these data allows the precise measurement of absolute branching fractions and angular distributions of the decay products. These measurements provide tests of QCD and allow the generation of more realistic...

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  50. Dhiren Panda (UNIVERSITY OF HYDERABAD)
    28/05/2024, 15:15
    Heavy quark decays and CKM
    Parallel session

    Motivated by the interplay between the LEFT and SMEFT operators at the electroweak scale, we study the interrelation among the transitions $b \to c \ell \nu_{\ell}$, $b \to s \nu _\ell \nu _\ell$ and $b \to s\ell \ell$ ($\ell = e, \mu, \tau$). We explore this correlation within the context of six - SMEFT operators: $\mathcal{Q}_{\ell q}^{(3)}$, $\mathcal{Q}_{\ell ed q}$, $\mathcal{Q}_{\ell e...

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  51. Matthew Gar Jun Man (University of Toronto (CA))
    28/05/2024, 15:15
    Neutrino physics
    Parallel session

    The Deep Underground Neutrino Experiment (DUNE) is the next generation neutrino experiment currently under construction. It consists of a broadband neutrino beam at Fermilab, a high precision near detector, and the largest liquid argon time projection chamber far detector ever designed at the Sanford Underground Research Facility (SURF).

    The Region of Interest (ROI) filter is designed for...

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  52. Ms Mansi Mandal (National Institute of Technology Durgapur)
    28/05/2024, 15:15
    Rare decays of hadrons and leptons
    Parallel session

    Charm decays have immense potential to probe physics beyond the standard model [1, 2]. The charm sector has shown some interesting phenomena, for instance, $D^0-\bar{D^0}$ mixing and CP violation [3, 4]. The experimental upper bounds for the branching fractions are constrained at $7.9×10^{-8}$ for $D^0→e^+ e^-$[5] and $6.2×10^{-9}$ for $D^0→μ^+ μ^-$[6]. Recent results from the LHCb have...

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  53. Huijing Li
    28/05/2024, 16:00
    Heavy quark decays and CKM
    Plenary session
  54. Oliver Witzel (Universität Siegen)
    28/05/2024, 16:25
    Heavy quark decays and CKM
    Plenary session
  55. Dr Umut Kose (ETH-Zurich), Umut Kose
    28/05/2024, 16:55
    Neutrino physics
    Plenary session
  56. Dr Veera Matilda Mikola (University of Glasgow)
    28/05/2024, 17:20
    Neutrino physics
    Plenary session

    T2K and NOvA experiments are the two long-baseline experiments currently collecting data to study neutrino oscillations, a quantum mechanical interference phenomenon where the observed neutrino flavor differs from that measured earlier, stemming from neutrino mass and flavor states mixing. The T2K experiment is based in Japan with a peak neutrino energy of ~0.6GeV and a baseline length of...

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  57. Adi Ashkenazi, Adi Ashkenazi (Tel Aviv University (IL))
    28/05/2024, 17:45
    Neutrino physics
    Plenary session
  58. Dr César Jesús-Valls (Kavli IPMU)
    28/05/2024, 18:15
    Neutrino physics
    Plenary session

    Hyper-Kamiokande, the next-generation neutrino observatory in Japan, evolves from its predecessors, Kamiokande and Super-Kamiokande, with a significant upgrade to a 260-kton water Cherenkov detector equipped with 20,000 PMTs. Hyper-Kamiokande will host an extremely rich and broad physics program, covering areas from neutrino astrophysics to nucleon decay searches and precision neutrino...

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  59. Xu Feng (Peking University), Xu Feng
    29/05/2024, 09:00
    Kaon physics
    Plenary session
  60. Zach Polonsky (University of Zurich)
    29/05/2024, 09:30
    Kaon physics
    Plenary session
  61. Silvia Martellotti (INFN Laboratori Nazionali di Frascati (IT))
    29/05/2024, 10:00
    Kaon physics
    Plenary session
  62. YU-CHEN TUNG (National Taiwan University)
    29/05/2024, 11:10
    Kaon physics
    Plenary session
  63. Rainer Wanke (Universität Mainz)
    29/05/2024, 11:35
    Kaon physics
    Plenary session
  64. 29/05/2024, 12:00
  65. Prof. Cheng-Wei Chiang (National Taiwan University)
    30/05/2024, 09:00
    CP violation in hadrons and leptons, EDMs
    Plenary session
  66. Kaori Fuyuto (Los Alamos National Laboratory), Kaori Fuyuto (Japan)
    30/05/2024, 09:30
    CP violation in hadrons and leptons, EDMs
    Plenary session
  67. Prof. Jacek Zejma (Jagiellonian University in Kraków, Poland)
    30/05/2024, 10:00
    CP violation in hadrons and leptons, EDMs
    Plenary session
  68. Sergey Barsuk (Université Paris-Saclay (FR))
    30/05/2024, 10:55
    CP violation in hadrons and leptons, EDMs
    Plenary session

    Studies of CP-parity violation (CPV) in heavy flavours allow measurements of important theory parameters and searches for effects deviating from the Standard Model predictions. The talk features new results of CPV studies at the LHC. Following the observation of CPV in a charm decay by the LHCb experiment, new studies of CPV in charm decays are reported. In B sector, new measurements of the...

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  69. Stefano Lacaprara (INFN sezione di Padova)
    30/05/2024, 11:20
    CP violation in hadrons and leptons, EDMs
    Plenary session
  70. Claudia Cecchi (Universita e INFN, Perugia (IT))
    30/05/2024, 11:45
    Future facility
    Plenary session
  71. Mark Tobin (Chinese Academy of Sciences (CN))
    30/05/2024, 12:05
    Future facility
    Plenary session

    The LHCb experiment was designed to measure CP-violation in the b-sector and to study rare decays of b- and c-hadrons at the LHC. The excellent performance of the detector during Run 1 and 2 of the LHC enabled LHCb to produce many interesting results. However, the maximum data rate was limited to by a Level-0 hardware trigger to 1.1 MHz and the trigger yield saturated at higher luminosities...

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  72. Ria sain
    30/05/2024, 14:00
    Heavy quark decays and CKM
    Parallel session

    We have conducted an investigation and prediction of the angular observables in the complete 4-body angular distribution for the decay of $\Lambda_b^0 \to \Lambda_c^{+}(\to \Lambda \pi^{+})\tau \bar{\nu_{\tau}}$. This analysis takes into account all New Physics (NP) operators in a model-independent manner while analyzing the NP sensitivity of each angular observable with the associated NP...

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  73. Gemma Tinti (INFN e Laboratori Nazionali di Frascati (IT))
    30/05/2024, 14:00
    Kaon physics
    Parallel session

    The NA62 experiment at CERN, designed to measure the highly-suppressed decay $K^{+} \rightarrow \pi^{+}\nu\bar{\nu}$, has the capability to collect data in a beam-dump mode, where 400~GeV protons are dumped on an absorber. In this configuration, New Physics (NP) particles, including dark photons, dark scalars and axion-like particles, may be produced and reach a decay volume beginning 80~m...

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  74. Chayanit Asawatangtrakuldee (Chulalongkorn University (TH))
    30/05/2024, 14:00
    Flavor and Dark Sector
    Parallel session

    SND@LHC is a compact and stand-alone experiment to perform measurements with neutrinos produced at the LHC in a hitherto unexplored pseudo-rapidity region of 7.2 < 𝜂 < 8.6, complementary to all the other experiments at the LHC. The experiment is located 480 m downstream of IP1 in the unused TI18 tunnel. The detector is composed of a hybrid system based on an 800 kg target mass of tungsten...

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  75. Alessio Giarnetti (Roma Tre University & INFN)
    30/05/2024, 14:15
    Neutrino physics
    Parallel session

    The ESSnuSB project aims to measure the leptonic CP violation at the second neutrino oscillation maximum using an intense neutrino beam produced by the powerful ESS proton linear accelerator in Sweden. This next-to-next generation long baseline neutrino oscillation experiment has a potential to start the precision era in the field of the leptonic CP violation measurement. Indeed, the reduced...

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  76. Kai Yi (Tsinghua University (CN))
    30/05/2024, 14:15
    Exotic quarkonium-like states
    Parallel session

    The speaker will discuss the new structures reported by the CMS collaboration recently. Three structures are found in the J/ψJ/ψ mass spectrum in proton-proton collisions at 13 TeV, and a model with quantum interference among these structures provides a good description of the data. Among them, a new structure with mass around 6.6 GeV is observed with a local significance > 5 sigma. Another...

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  77. Supravat Mahata (National Institute of Technology Durgapur)
    30/05/2024, 14:15
    Rare decays of hadrons and leptons
    Parallel session

    Recent measurements in flavour changing charged current (FCCC) $b→c\bar l \nu_l$ transitions hint existence of new physics (NP) beyond the standard model (SM). The lepton flavour universality (LFU) ratios $R_{D^{(*)}}$ measured by BaBar, Belle and LHCb have shown around $3.3\sigma$ deviation between theory and experiment [1]. These anomalous results connected to the $b$ hadron decays indicate...

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  78. Zhen Hu (Tsinghua University (CN))
    30/05/2024, 14:30
    Exotic quarkonium-like states
    Parallel session

    The first observation of the concurrent production of two $\rm{J}/\psi$ mesons in proton-nucleus collisions will be presented. The analysis is based on a data sample recorded at a nucleon-nucleon center-of-mass energy of 8.16 TeV by the CMS experiment at the CERN LHC corresponding to an integrated luminosity of 174.6 $\rm{nb}^{-1}$. The $\rm{J}/\psi$ mesons are reconstructed in their...

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  79. Yingrui Hou (Centre National de la Recherche Scientifique (FR))
    30/05/2024, 14:30
    Rare decays of hadrons and leptons
    Parallel session

    Radiative b-hadron decays are sensitive probes to new physics through the study of branching fractions, angular observables, CP violation parameters, and photon polarization. The LHCb experiment is ideally suited for the analysis of these decays due to the high luminosity of B production, its high trigger efficiency, as well as excellent tracking and particle identification performance. Recent...

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  80. Savino Longo (University of Manitoba)
    30/05/2024, 14:30
    Flavor and Dark Sector
    Parallel session

    The Belle and Belle$~$II experiment have collected samples of $e^+e^-$ collision data at centre-of-mass energies near the $\Upsilon(nS)$ resonances. These data have constrained kinematics and low multiplicity, which allow searches for dark sector particles in the mass range from a few MeV to 10$~$GeV. Latest results are presented.

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  81. Mr AJAY KUMAR YADAV (Central University of Karnataka, Kalaburgi, India)
    30/05/2024, 14:45
    Rare decays of hadrons and leptons
    Parallel session

    We study the exclusive semileptonic $B_c\to D_s^{(*)} (\mu^+ \mu^-, \nu \bar{\nu})$ decay modes mediated by $b \to s$ quark level transitions in the Effective field theory formalism. There are discrepancies between the experimental measurements and the Standard Model predictions in various observables associated with the $B \to (K, K^*, \phi)\ell \ell$ processes. On the other hand, a very...

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  82. Kirill Ivanov (Moscow Institute of Physics and Technology State University (RU))
    30/05/2024, 14:45
    Flavor and Dark Sector
    Parallel session

    Recent CMS Experiment results on conventional spectroscopy and production of heavy flavour states in pp collisions at 13 TeV are reported, including the first observation of the Xi_b- —> psi(2S) Xi- decay. We discuss the measured properties of the ground and excited hadron states.

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  83. Qipeng Hu (University of Science and Technology of China (CN))
    30/05/2024, 15:10
    Future facility
    Plenary session

    The Super Tau Charm Facility (STCF), a planned symmetric electron-positron collider in China, aims to facilitate $e^+e^−$ collisions across a center-of-mass energy range of 2 to 7 GeV, targeting a peak luminosity of $0.5×10^{35}\mathrm{cm}^{−2}\mathrm{s}^{−1}$. With an anticipated annual integrated luminosity exceeding $1~ab^{−1}$, the STCF is poised to generate vast datasets. These will...

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  84. Kai Xu (Suranaree University of Technology)
    30/05/2024, 16:00
    Exotic quarkonium-like states
    Plenary session

    In the naive quark model, baryons and mesons are bound states of three quarks and quark-antiquark pair, respectively. However, Exotic hadrons such as tetraquark ($q^2{\overline q}^2$), pentaquark ($q^4{\overline q}$), hexaquark ($q^3{\overline q}^3$), and even quark-gluon hydrid ($q^3G$) and glueball are not forbidden in the framework of QCD. Some exotic hadron states may possess quantum...

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  85. Liang Yan (Universita e INFN Torino (IT))
    30/05/2024, 16:30
    Exotic quarkonium-like states
    Plenary session
  86. Renu Garg
    30/05/2024, 16:55
    Exotic quarkonium-like states
    Plenary session
  87. Xiaoming Zhang (Central China Normal University CCNU (CN))
    30/05/2024, 17:20
    Exotic quarkonium-like states
    Plenary session
  88. 30/05/2024, 19:30
  89. Thomas Teubner (U), Thomas Teubner
    31/05/2024, 09:00
    Muon g-2
    Plenary session
  90. Fabio Anulli (Sapienza Universita e INFN, Roma I (IT))
    31/05/2024, 09:30
    Muon g-2
    Plenary session

    After more than 60 years since the first measurements, the study of $e^+e^-$ annihilation processes at low energies are still
    a great source of information in an energy region where perturbative Quantum Chromodinamyc cannot be used.
    The hadronic cross section is also the experimental input for the theoretical
    calculation of the hadronic contribution to the anomalous magnetic moment of...

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  91. Liang Li (Shanghai Jiao Tong University (CN))
    31/05/2024, 09:55
    Muon g-2
    Plenary session
  92. Tamaki Yoshioka, Tamaki Yoshioka (ICEPP, Univ. of Tokyo)
    31/05/2024, 10:20
    Muon g-2
    Plenary session
  93. Jure Zupan (University of Cincinnati)
    31/05/2024, 11:10
    Flavor and Dark Sector
    Plenary session
  94. Michael Roney, Michael Roney (BABAR Collaboration/University of Victoria)
    31/05/2024, 11:40
    Flavor and Dark Sector
    Plenary session
  95. Fabrizio Bianchi, Fabrizio Bianchi (Universita degli Studi di Torino)
    31/05/2024, 12:05
    Flavor and Dark Sector
    Plenary session
  96. Joachim Brod (University of Cincinnati)
    31/05/2024, 12:30
    Plenary session
  97. Phat Srimanobhas (Chulalongkorn University (TH))
    31/05/2024, 12:35
  98. Dr Patipan Uttayarat
    31/05/2024, 15:00
    Flavor and Dark Sector

    The P in FPCP has a long and interesting history. Here, I argue that P does not stand for Patipan

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  99. Phat Srimanobhas (Chulalongkorn University (TH))
    31/05/2024, 15:20
    Neutrino physics
  100. Frederic Deliot (Université Paris-Saclay (FR))
    Rare decays of hadrons and leptons
    Parallel session

    ATLAS measurement of B0s → μ+ μ- effective lifetime with 2015-2016 data is presented. This observable, along with the branching fraction of the decay, is sensitive to New physics contributions to the decay amplitude. The measurement result is consistent with the SM.

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  101. Frederic Deliot (Université Paris-Saclay (FR))
    Exotic quarkonium-like states
    Parallel session

    Recent results on spectroscopy of exotic hadrons in ATLAS with Run-2 data are presented. Four-muon mass spectrum is studied investigating the structures earlier observed by LHCb experiment, using di-J/ψ and J/ψ+ψ(2S) channels. The latter is also investigated using ψ(2S)→ J/ψ(μ+μ−)π+π− decay mode.

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