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Andrzej Kupsc, Bastian Kubis (University of Bonn (DE)), Johan Bijnens (Lund University), Sean Tulin (York University)13/05/2025, 08:30
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Andreas Crivellin (University Bern)13/05/2025, 09:00
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Emilie Passemar13/05/2025, 10:00
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Dr Jun Shi (South China Normal University), Susan Gardner (University of Kentucky)13/05/2025, 11:00
The decay $\eta\to\pi^+\pi^- \pi^0$ is an ideal channel in which to study flavor-conserving $C$ and $CP$ violation beyond the Standard Model. We use Standard Model Effective Field Theory (SMEFT) to deduce the mass-dimension-six operators that can contribute to its signature, i.e., an observed breaking of mirror symmetry in its Dalitz plot. Using chiral-effective theory, we present the leading...
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Dr PABLO SÁNCHEZ PUERTAS (University of Granada)13/05/2025, 11:30
Currently and in the near future, a variety of $\eta$ factories are exploring the potential to search for new physics through different $\eta$ decays. One possibility being considered is to search for signs of CP-violation in eta decays. Since the Standard Model predicts an extremely suppressed rate for CP-violation in the $\eta$ sector, any positive signal would be a clear sign of new...
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Konstantin Ottnad (University of Mainz)13/05/2025, 13:30
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Prof. Liping Gan (University of North Carolina Wilmington)13/05/2025, 14:00
The system of η and η′ offers a flavor-conserving laboratory to test the low-energy QCD and to search for new physics Beyond the Standard Model. The symmetry properties of QCD at low-energy, such as the chiral symmetry or the axial anomalies, are manifested in the decays of η and η′. Thus, a study of η/η′ will yield light on our understanding of the origin and the dynamics of QCD...
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xiaolin Kang13/05/2025, 14:30
The talk will include recent progress and insights on eta/eta' decays at KLOE/KLOE2 and the propest in this field that could be achieved with the future e+e- collider proposed like STCF.
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PABLO SÁNCHEZ PUERTAS (University of Granada)13/05/2025, 15:30
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Frederic Noël13/05/2025, 16:00
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David McKeen (TRIUMF)14/05/2025, 08:30
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Felix Kahlhoefer (Karlsruhe Institute of Technology)14/05/2025, 09:30
Dark photons arising at or below the GeV scale from a spontaneously broken gauge symmetry are one of the simplest and most exciting extensions of the Standard Model. They couple to known particles via kinetic mixing with the Standard Model gauge bosons and can act as mediators between visible matter and new hidden states, such as sub-GeV dark matter particles. I will show that these models can...
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Frank Simon (KIT - Karlsruhe Institute of Technology (DE))14/05/2025, 10:00
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Hao Qiu14/05/2025, 11:00
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Johan Bijnens (Lund University), Valentina Santoro (ESS)14/05/2025, 11:30
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Dr Alexander Somov (Jefferson Lab)14/05/2025, 13:30
The goal of the new JLab Eta Factory (JEF) experiment, conducted with the GlueX detector in Hall D at Jefferson Lab, is to perform measurements of various $\eta^{(\prime)}$ decays with a primary focus on rare neutral modes. The experiment's physics program ranges from precision tests of low-energy QCD to searches for gauge bosons with masses below 1 GeV that could couple the Standard Model...
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HE ZHAO (Institute of Modern Physics)14/05/2025, 14:00
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Szymon Treliński14/05/2025, 14:30
Proton-proton collisions at 4.5 GeV beam kinetic energy, measured with
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the High Acceptance Di-Electron Spectrometer (HADES) operating at GSI
Helmholtzzentrum have been used to study exclusive η meson production.
This energy range is particularly interesting as it lies in an
intermediate regime — between near-threshold energies, where effective
Lagrangian models are typically applied, and... -
Marco Ayala (SAPHIR - UNAB)14/05/2025, 15:30
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Khépani Raya Montaño14/05/2025, 16:00
The structural properties of pseudoscalar mesons are closely linked with QCD's emergent phenomena, confinement and emergent hadronic mass, as well as to fundamental symmetries of the Standard Model. Two-photon transition form factors (TFFs) offer an efficient way to explore these phenomena, while tracing the transition between soft and hard energy scales. Moreover, these form factors are...
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Maxim Pospelov15/05/2025, 08:30
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Shuangshi Fang15/05/2025, 09:30
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Dr Marcin Zielinski (Jagiellonian University (PL))15/05/2025, 10:00
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Antoine Gérardin (CPT Marseille)15/05/2025, 11:00
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Simon Holz (Universität Bern)15/05/2025, 11:30
The uncertainty of the Standard Model prediction of the anomalous magnetic moment of the muon $(g-2)_\mu$ is dominated by hadronic contributions. As part of these hadronic inputs, the pseudoscalar-pole contribution in hadronic-light-by-light scattering plays a vital role. The currently sought precision of the Standard Model prediction of $(g-2)_\mu$ requires a careful evaluation not only of...
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Bai-Long Hoid15/05/2025, 13:30
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Federica Maria Simone (Universita e INFN, Bari (IT))15/05/2025, 14:00
Novel trigger strategies, combined with the large proton-proton collision datasets collected by the CMS experiment, have extended its sensitivity to rare flavor decay processes. Leveraging CMS’s ability to efficiently trigger on and reconstruct low-momentum muons, the experiment offers complementary sensitivity to rare meson decays.
This contribution presents recent results on η meson...
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Dr Michele Lucente (University of Bologna)15/05/2025, 14:30
The recently reported evidence of a Stochastic Gravitational Wave Background (SGWB) in the nHz frequency range is in tension with standard astrophysical expectations, motivating the study of new physics beyond the Standard Model. A preferred explanation relies on a supercooled first order phase transition at the 100 MeV - GeV scale. I will present a minimal model that can account for the SGWB,...
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Karol Kampf (Charles University (CZ))15/05/2025, 15:30
This talk will provide an overview of the precise higher-order calculation in the anomalous sector. The focus will be on the two-photon decays for pion and eta and on the corresponding Dalitz decays.
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Dr Emilio Royo (Universidad Cardenal Herrera CEU and IFAE)16/05/2025, 09:00
We analyse vector, scalar and tensor meson-exchange contributions to the doubly radiative decays $\eta^{(\prime)}\to\pi^0\gamma\gamma$ and $\eta^{\prime}\to\eta\gamma\gamma$, and investigate the sensitivity of these processes to a leptophobic $B$ boson in the sub-GeV mass range. Our results are relevant for measurements of these decays at existing (A2, BESIII, KLOE-2) and forthcoming...
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Alejandro Miranda (IFAE)16/05/2025, 09:30
The sensitivity of the rare decay process $\phi\rightarrow\pi^0\eta\gamma$ to signatures of a leptophobic boson in the MeV-GeV mass range is analyzed in this talk. First, we improve the description of the dominant scalar contribution. Next, we incorporate an explicit B-boson resonance exchange alongside the Standard Model (SM) contributions from vector and scalar meson exchanges. By utilizing...
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Sergi Gonzalez-Solis (University of Barcelona)16/05/2025, 10:00
With upcoming $\eta/\eta^{\prime}$ factories in the horizon, dedicated searches for hadronic ALPs would open a new window into the exploration of strong CP solutions and low scale dark sectors. In this talk, we present branching ratio sensitivities of the axio-hadronic $\eta/\eta^{\prime}\to\pi\pi a$ decays, where $a$ is an axion or axion-like particle (ALP), using the leading order ALP-ChPT...
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Susan Gardner (University of Kentucky)16/05/2025, 11:00
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Krzysztof Prościński (Jagiellonian University)16/05/2025, 11:30
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Maksym Ovchynnikov (CERN)
In this talk, I present a comprehensive discussion on how to search for generic axion-like particles (ALPs) coupled to quarks and gluons at Eta-Factories. First, I will review the phenomenology of the ALPs in the GeV mass range, and highlight existing open questions and complications in the field. Then, I will proceed with calculating the yields of ALPs from decays of pi0, eta, eta' mesons,...
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Susan Gardner (University of Kentucky)
The decay rate for $\eta\to \pi\pi$ is known to be vanishingly small in the SM, and it is similarly so in the presence of strong CP violation. Here we consider whether new sources of CP violation, as encoded in SMEFT, or the emission of a dark-sector particle, such as the axion, can give rise to potentially observable effects $-$ and how the two mechanisms might be distinguished.
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