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Journées de Rencontre Jeunes Chercheurs 2023

22–28 oct. 2023
Fuseau horaire Europe/Paris

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Liste des Contributions

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  1. 2. Introduction
    23/10/2023 09:15
  2. 5. Session Overview
    Olivier Davignon (Laboratoire Leprince-Ringuet)
    23/10/2023 09:30
  3. 64. Combined fit of the hadronic tau energy scale and the identification scale factor
    Océane Poncet
    23/10/2023 10:00
    Standard Model
    Standard Model

    A new method is presented for calibrating hadronic tau leptons ($\tau_h$) using $Z \rightarrow \mu \tau_h$ events, recorded by CMS experiment during 2018 at $\sqrt{s}$ = 13 TeV. The calibration is performed using data samples that reconstruct the decay of a Z boson into $\tau_{\mu}\tau_h$. By reconstructing the invariant visible mass from the visible decay products, a distribution is obtained...

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  4. 78. $B^0_{d(s)}\to K^0_Shh’$ branching fraction measurement at LHCb, first time integrated amplitude analysis of $B^0_s\to K^0_S\pi^+\pi^-$ and feasibility study of $B^0_d\to K^{*0}\tau^+\tau^-$ at FCC-$ee$.
    Tristan Miralles
    23/10/2023 11:00
    Standard Model
    Standard Model

    The first part of the presentation is focused on a current LHCb analysis about the measurement of the branching fraction of the $B^0_{d(s)}\to K^0_Shh’$ modes, where $h$ and $h’$ could denotes a pion or a kaon, by using the LHCb Run1 and Run2 data. The first goal of the analysis is to measure the $B^0_d\to K^0_S K^+K^-$ decay mode unobserved to date. The second goal of the study is to update...

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  5. 53. Measurement of the CKM angle $\gamma$ in $B^\pm\rightarrow D^0(\rightarrow K_s^0\pi^+\pi^-\pi^0)K^\pm$ decays at LHCb
    jessy daniel
    23/10/2023 11:30
    Standard Model
    Standard Model

    The observable Universe is mainly made up of matter, while almost all the antimatter disappeared in the very early times. One explanation is that the Universe obeys the Sakharov conditions, which mean the existence of a C (charge) and CP (charge - parity) symmetry violation. An area of Particle Physics deals with the comprehension and measurement of this symmetry breaking and the potential...

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  6. 58. Jet Calibration with the ATLAS detector
    Line Delagrange (LPNHE, Paris, France)
    23/10/2023 12:00
    Standard Model
    Standard Model

    Jets are collimated sprays of particles that stem from the emission of a quark or a gluon. They are crucial for many Standard Model measurements and search for new physics and they are ubiquitous in high energy proton-proton collisions environments, such as at LHC. The goal of jet calibration is to get the true 4-momentum of the jet, which is that of the particle initiating it, from the...

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  7. 74. Simultaneous jet calibration with ML including in situ JER measurement
    Laura Sara Boggia (CNRS)
    23/10/2023 14:00
    Standard Model
    Standard Model

    In the current ATLAS jet calibration procedure, the GSC/GNNC methods are applied to improve the Jet Energy Resolution (JER) followed by various methods measuring the JER in situ and correcting it.
    This project focuses on merging several aspects of the jet calibration chain, combining a NN-based calibration procedure with a loss function that minimises the JER directly in data. As a first...

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  8. 61. Combined angular analysis of $ B \to D^{*} e \nu_{e}$ and $ B \to D^{*} \mu \nu_{\mu}$ with the LHCb detector
    Bogdan Kutsenko (Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France)
    23/10/2023 14:30
    Standard Model
    Standard Model

    Several intriguing hints on deviations from the SM predictions have appeared in the studies of decays of B hadrons (hadrons containing the beauty (b) quark) involving leptons. The standard model contains three lepton families: electrons, muons, and tau-leptons, each accompanied by the corresponding type of neutrino. The most striking deviation is the hint on violation of lepton flavor...

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  9. 66. High-throughput GNN track reconstruction at LHCb
    Fotis Giasemis
    23/10/2023 15:00
    Standard Model
    Standard Model

    Over the next decade, increases in instantaneous luminosity and detector granularity will increase the amount of data that has to be analyzed by high-energy physics experiments, whether in real time or offline, by an order of magnitude. The reconstruction of charged
    particles, which has always been a crucial element of offline data processing pipelines, must increasingly be deployed from the...

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  10. 81. Improving Tracking Algorithms for ITk Detector at the HL-LHC
    Jeremy Couthures (ATLAS LAPP)
    23/10/2023 15:30
    Standard Model
    Standard Model

    In anticipation of the High-Luminosity phase of the Large Hadron Collider at CERN (HL-LHC), the ATLAS experiment is upgrading its innermost detector to the new Inner Tracker (ITk), characterized by its wider coverage and increased granularity. While this new detector promises enhanced spatial resolution for track measurements, its combination with the increased luminosity of the HL-LHC poses a...

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  11. 80. 3D Clustering in the CMS High Granularity Calorimeter
    Isaac EHLE (Laboratoire Leprince-Ringuet, Institut Polytechnique Paris)
    23/10/2023 16:30
    Standard Model
    Standard Model

    In 2029, the High Luminosity phase of the LHC (HL-LHC) is planned to begin taking data, bringing an unprecedented level of radiation and average particle interactions per brunch-crossing (pileup/PU). In order to preserve the same physics performance that the CMS detector achieves now, the collaboration has decided to replace the endcaps of the current electromagnetic and hadronic calorimeters...

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  12. 9. Session overview
    Aurélie Bonhomme (IPHC/DRS/DNE)
    23/10/2023 17:00
  13. 72. Comparison of (p,n) and (n,gamma) reactions for ADS decommissioning
    M. Jonathan COLLIN (Institut Pluridisciplinaire Hubert Curien (IPHC))
    23/10/2023 17:30
    Nuclear Physics
    Nuclear Physics

    Nuclear activation is the process of production of radionuclides by irradiation. This phenomenon concerns all operating or soon-to-be dismantled particle accelerators used in various fields, from medical applications with the production of radioisotopes or radiotherapy cancer treatments to industrial applications with the sterilization of materials and food preservation [1]. For more than...

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  14. 11. Session overview
    Dr Michel Aguena (APC)
    24/10/2023 10:00
  15. 52. Cosmology with Type Ia Supernovae and the ZTF survey
    Madeleine Ginolin (IP2I/IN2P3/CNRS)
    24/10/2023 11:00
    Cosmology
    Cosmology

    I will present the construction of a Hubble diagram, especially the standardisation of Type Ia Supernovae luminosity. I will then talk about the ongoing ZTF survey, which is the current state of the art low redshift survey. I will then talk about one of the challenge faced by Supernovae cosmology now: the astrophysics dependency of Type Ia Supernovae.

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  16. 54. Development of an ultra-fast, likelihood-based, distance inference, for the next generation of type-Ia supernovae surveys
    Dylan KUHN
    24/10/2023 11:30
    Cosmology
    Cosmology

    As of today, the Hubble diagram, which maps the luminosity distance-redshift relation for type-Ia supernovae (SNe Ia), allows us to infer cosmological parameters such as the Dark Energy equation of state (w) with an accuracy reaching a few per cent. Upcoming SNIa samples with O(30,000) SNe (30 times the current worldwide statistics), will allow us to reach the per cent level and start probing...

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  17. 57. 21cm emission in primordial clouds with full chemical computation
    Hugo Plombat (Laboratoire Univers et Particules de Montpellier)
    24/10/2023 12:00
    Cosmology
    Cosmology

    The 21cm hydrogen line is present during all the eras following the cosmological recombination, containing information about both the cosmology and the astrophysical processes at work in the universe.
    During this presentation, I will discuss the 21cm emission from collapsing gas clouds. I will particularly take into account the gas cooling due to thermal molecular functions. To do so, one...

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  18. 70. Invited talk - Nuclear, renewable energy & economy
    Nicolas Thiollière (IMTA - CNRS)
    24/10/2023 14:00
  19. 8. Session overview
    Alexis VALLIER (L2I Toulouse, CNRS/IN2P3, UT3)
    24/10/2023 16:30
  20. 67. Search for a new resonance decaying to a scalar and a Higgs boson in the final state with two bottom quarks and two photons in proton-proton collisions at $\sqrt{s} = 13$ TeV
    Maxime FERNOUX (Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France)
    24/10/2023 17:00
    Beyond Standard Model
    Beyond Standard Model

    A search for the resonant production of a heavy scalar X decaying into a Higgs boson and
    a new lighter scalar S, through the process X$\rightarrow$ S ($b\bar{b}$) H($\gamma \gamma$), where the two photons are consistent with the Higgs boson decay, is performed. The search is conducted using 140 fb$^{-1}$ of LHC Run 2 data recorded by ATLAS. The mass space investigated in the analysis is 170...

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  21. 79. B-anomalies
    Yann Monceaux (IP2I (Lyon))
    24/10/2023 17:30
    Standard Model
    Beyond Standard Model

    Deviations from the Standard Model have long been observed in semileptonic B-meson decays, notably b→ sll transitions, triggering speculations on potential New Physics effects in this sector. After the recent update of RK(*) and BR(B(s) → μμ) by the LHCb collaboration, the remaining significant deviations from the SM in FCNC B decays are found in the branching ratios of mesonic decays...

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  22. 91. Test of global symetries of the SM in the top quark sector
    David Amram (IP2I)
    24/10/2023 18:00
    Beyond Standard Model
    Beyond Standard Model

    The pursuit of deviations from the Standard Model (SM) is prompted by the recognition of the model's known limitations. Some findings suggest possible violations of lepton universality. The identification of such deviations could potentially lead to a SM extension, adding Z' boson that interacts with leptons in a different manner.

    The SM is also firmly grounded by the principle of Lorentz...

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  23. 77. Vector boson scattering in the ATLAS detector
    Mathieu Markovitch (IJCLab)
    25/10/2023 09:30
    Standard Model
    Standard Model

    Vector boson scattering (VBS) processes probe the fundamental structure of electroweak interactions and provide a high sensitivity to new physics (NP) phenomena affecting gauge and Higgs couplings. These processes are among the rarest ones in the Standard Model (SM) and were observed during last years in the Large Hadron Collider (LHC). The semileptonic final state, where one of the scattered...

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  24. 87. X->HH searches in CMS
    ELISE JOURD'HUY (IP2I/UCBL)
    25/10/2023 10:00
    Beyond Standard Model
    Beyond Standard Model

    Since the existence of the Higgs boson has been experimentally confirmed by the ATLAS and CMS Collaborations, many of its properties have been measured with high precision. However, one of its main property, the shape of the Higgs potential, remains unknown. The Higgs pair production represents the most direct way of measuring this potential, and any excess observed could be a sign of new...

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  25. 51. Recherche d'un nouveau boson vecteur neutre se désintégrant de manière leptonique en association avec de l'énergie transverse manquante dans des collisions de protons-protons à √s=13 TeV avec le détecteur ATLAS.
    TOM CAVALIERE (LAPP)
    25/10/2023 11:00
    Beyond Standard Model
    Beyond Standard Model

    Une recherche de particules de matière noire produites en association avec un nouveau boson vecteur neutre est effectuée en utilisant des collisions de protons-protons à √s=13 TeV, correspondant à une luminosité intégrée de 140 fb−1 enregistrée par le détecteur ATLAS au Grand Collisionneur de Hadrons. Les désintégrations du boson Z′ en leptons légers de même saveur (e+e−/μ+μ−) sont étudiées...

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  26. 63. Search for displaced top quark in the CMS tracker
    Paul Vaucelle (IPHC)
    25/10/2023 11:30
    Beyond Standard Model
    Beyond Standard Model

    My thesis subject aims to search for long-lived decays
    of new massive particles in the Compact Muon Solenoid
    (CMS) experiment at the Large Hadron Collider (LHC).
    CMS is one of the four main experiments at the LHC,
    where high energy proton-proton collisions are pro-
    duced. New long-lived particles are predicted in several
    extensions of the Standard Model (SM). In the model
    considered,...

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  27. 65. Search for Emerging jets in the ATLAS detector and reinterpretation of the LHC results
    Thomas Wojtkowski
    25/10/2023 12:00
    Beyond Standard Model
    Beyond Standard Model

    The Standard Model (SM) cannot explain the composition of Dark Matter in the Universe. Some Beyond Standard Model theories predict the existence of a dark hidden sector which contain new hypothetical particles : stable particles in this sector are Dark Matter candidates. The new particles could weakly interact with Standard Model ones through a new interaction, and thus can be produced in...

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  28. 3. Excursion
    25/10/2023 14:00
  29. 6. Session overview
    Sabrina Sacerdoti (APC-Paris,France)
    26/10/2023 10:00
  30. 1. The ATLAS High-Granularity Timing Detector: test beam campaigns and results
    Oleksii KURDYSH (IJCLab)
    26/10/2023 11:00
    Instrumentation & Interdisciplinaire
    Instrumentation & Interdisciplinarity

    The expected increase of the particle flux at the high luminosity phase of the LHC (HL-LHC) with instantaneous luminosities up to L ≃ 7.5×1034 cm−2 s-1 will have a severe impact on the ATLAS detector performance. The pile-up is expected to increase on average to 200 interactions per bunch crossing. The reconstruction and trigger performance for electrons, photons as well as jets and transverse...

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  31. 73. High-energy ion beam analysis: the study of raw materials and manufacturing techniques for cultural heritage objects.
    Alexandre Gillon (Subatech)
    26/10/2023 11:30
    Instrumentation & Interdisciplinaire
    Instrumentation & Interdisciplinarity

    Ion beam analysis has been developed at ARRONAX cyclotron in Nantes [1]. Light ions including $H^{+}$ and $He^{2+}$ are accelerated to reach the required energy for the analyses before being extracted in-air. We use a fixe 68MeV α beam and several proton beams at 17MeV to 70MeV. We will explore the specific interest concerning material analysis by beam irradiation. Interaction between ions...

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  32. 71. Évaluation des performances du scanner Siemens Somatom go.Open Pro avec GATE
    Gaëtan Raymond (LPC Siemens)
    26/10/2023 12:00
    Instrumentation & Interdisciplinaire
    Instrumentation & Interdisciplinarity

    La réduction de la dose délivrée par les scanners est un enjeu majeur de santé publique [1]. L’objectif est d’obtenir des images scanner qui permettent une interprétation médicale avec une dose la plus faible possible.
    La plateforme de simulations Monte Carlo GATE (version 10 béta) est utilisée dans le cadre de la modélisation du scanner Go Open Pro de Siemens Healthineers.
    La version 10...

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  33. 10. Session overview
    Dr Sami Caroff (LAPP)
    26/10/2023 14:00
  34. 59. Direct detection of Axion dark matter with MADMAX
    Vijay Dabhi (CPPM, Marseille)
    26/10/2023 14:30
    Astroparticle
    Astroparticle

    Dark matter is one of the major puzzles in fundamental physics. Axions are among the best-motivated dark matter candidates. MADMAX experiment will search for axions in the mass range around 100 $\mu$eV, which is favored by theory. Traditional axion cavity experiments are unable to access this mass range. Therefore, a novel detector called dielectric haloscope will be utilised for this...

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  35. 62. Investigating AGN Variability with the Cherenkov Telescope Array and nectarCAM
    M. Guillaume Grolleron (LPNHE (CNRS))
    26/10/2023 15:00
    Astroparticle
    Astroparticle

    Active Galactic Nuclei (AGN) stand as enigmatic cosmic powerhouses, harboring supermassive black holes at their centers. Blazars are AGN with a jet oriented toward the observer. Their emission spans from radio to very high-energy gamma rays. Understanding their spectral variability provides crucial insights into the underlying physics governing these astrophysical phenomena. The Cherenkov...

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  36. 55. Lorentz invariance violation search with the Cherenkov Telescope Array Observatory Large-Sized Telescope
    Cyann Plard (LAPP IN2P3 CNRS)
    26/10/2023 15:30
    Astroparticle
    Astroparticle

    The flares of active galactic nuclei (AGNs) can be used to detect or constrain Lorentz invariance violation (LIV) by measuring time lags in detection of high energetic photons. An important source of uncertainty is our lack of knowledge of source intrinsic processes. However, combining flares and sources allows us to increase the precision of these measurements as well as to limit the noise of...

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  37. 48. Calibration and data reconstruction for the Virgo interferometer : how to compute the data reconstruction uncertainty
    Cervane GRIMAUD (LAPP)
    26/10/2023 16:30
    Astroparticle
    Astroparticle

    Virgo is a gravitational wave detector located near Pisa in Italy. It is composed of a Fabry-Perot Michelson Interferometer and allows to detect gravitational wave passing through it using the interference dark fringe signal going out of the interferometer.
    Virgo is an instrument that needs to be controlled and calibrated with great accuracy in order to achieve the precision required to...

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  38. 56. Ionisation of a single nanoparticle by heavy Cosmic Ray
    Thibault NGUYEN TRUNG (IJCLab)
    26/10/2023 17:00
    Astroparticle
    Astroparticle

    The interstellar medium is made up of gas and dust. This medium is traversed by cosmic radiation and irradiated by stellar UV, except in dense clouds where UV is absent. The interaction of these rays with the dust and gas is crucial to the chemical evolution of interstellar and circumstellar environments. Heavy and slow cosmic rays interact with very small dust particles (-100 atoms) and...

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  39. 90. Search for WIMPs and light DM with XENONnT experiment
    Mlle Yongyu PAN
    26/10/2023 17:30
    Astroparticle
    Astroparticle

    The mysterious nature of Dark Matter (DM) has puzzled physicists the world over. One well-motivated class of DM candidates is Weakly Interacting Massive Particles (WIMPs). The XENON Dark Matter Project for direct search for WIMPs currently operates XENONnT experiment, lying a dual-phase (liquid & gas) xenon time projection chamber (TPC), situated in the underground LNGS in Italy.
    This...

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  40. 86. Study of the PeVatron candidate SNR G106.3+2.7 observed at Large Zenith Angle with LST-1 and MAGIC
    Marie-Sophie Carrasco (Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France)
    27/10/2023 10:00
    Astroparticle
    Astroparticle

    The quest for PeVatrons, sources of cosmic rays accelerated up to PeV energies, saw an exciting development in 2021 when LHAASO detected 12 ultra-high energy (UHE) gamma-ray Galactic sources. Among those sources, the supernova remnant G106.3+2.7 (also called the Boomerang SNR) is a promising candidate to both hadronic and leptonic scenarios for the UHE emissions.

    Gamma-ray astronomy...

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  41. 7. Session overview
    Batoul Diab (CEA Saclay IRFU/DPhN)
    27/10/2023 11:00
  42. 75. Quantum vs. semi classical description of in-medium quarkonia
    Aoumeur Daddi Hammou (Subatech)
    27/10/2023 11:30
    Hadronic Physics
    Hadronic Physics

    Heavy quarkonia are considered among the most promising probes of quark
    gluon plasma (QGP) formed in ultra relativistic heavy ion collisions (URHIC).
    For a reliable use of such probe, we need a rigorous formalism which could
    describe the real time and out of equilibrium evolution of in-medium quarkonia
    while it keeps a full track of the quantum nature of our system, as well, being
    derived...

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  43. 31. J/ψ flow measurements in Pb-Pb collisions with the ALICE detector at LHC Run 3
    Victor Valencia (Subatech - Nantes)
    27/10/2023 12:00
  44. 13. Session overview
    Chiara Filomena Lastoria
    27/10/2023 14:00
  45. 60. Deeply Learning from Neutrino Interactions with the KM3NeT neutrino telescope
    Santiago Peña Martinez (APC)
    27/10/2023 14:30
    Neutrinos
    Neutrinos

    KM3NeT/ORCA is a large-volume water-Cherenkov neutrino detector, under construction at the bottom of the Mediterranean Sea at a depth of 2450 meters. The main research goal of ORCA is the measurement of the neutrino mass ordering and the atmospheric neutrino oscillation parameters. Additionally, the detector is also sensitive to a wide variety of phenomena including non-standard neutrino...

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  46. 76. Multi-messenger observations with the KM3NeT telescope: search for high energy neutrinos coinciding with fast radio bursts
    Felix Bretaudeau
    27/10/2023 15:00
    Neutrinos
    Neutrinos

    The KM3NeT experiment is a next-generation neutrino telescope, consisting of two separate detection structures, organised as arrays of light sensors, and immersed in the depths of the Mediterranean Sea. The two detectors are the Oscillation Research with Cosmics in the Abyss (ORCA detector), located off the coast of France and the Astrophysics Research with Cosmics in the Abyss (ARCA...

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  47. 84. Induction signal characterization in the vertical drift TPC for the DUNE project
    Joshua Pinchault (LPSC)
    27/10/2023 16:30
    Neutrinos
    Neutrinos

    Deep Underground Neutrino Experiment (DUNE) is a next generation long-baseline neutrino experiment in the United States.
    Its main goal is to make precise measurements of neutrino oscillation parameters and to discover the neutrino mass ordering and CP violation phase in the leptonic sector.
    The experiment is made of two elements: the near detector close to neutrino beam source and the far...

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  48. 88. Study of the Photon Detection System in DUNE using simulation techniques
    Ariel Cohen (APC)
    27/10/2023 17:00
    Neutrinos
    Neutrinos

    The Deep Underground Neutrino Experiment (DUNE) is a long baseline neutrino experiment under construction that aims to address the main open questions in neutrino physics such as the ordering of the mass hierarchy and the precise measurement of the neutrino oscillation parameters, including the charge-parity violation phase to determine the existence (or not) of the CP-violation in the...

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  49. 89. Search for Coherent Elastic Scattering of Solar Neutrinos in XENONnT
    M. Quentin Pellegrini (LPNHE (SU))
    27/10/2023 17:30
    Neutrinos
    Neutrinos

    The XENON program aims to directly detect dark matter. As dark matter interacts very weakly, the sensitivity of dark matter experiments has greatly increased over the last two decades. XENONnT, the current XENON detector should be able to study solar neutrinos. This detector is designed to be sensitive to low-energy nuclear recoils which is the expected signal from some dark matter candidates....

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  50. 93. SFP presentation & new tools for networking and jobs
    Maxime Guilbaud (SUBATECH), Maxime Guilbaud (SUBATECH)
    27/10/2023 18:00
  51. 92. Conclusion talk
    Laura Zambelli (LAPP), Laure MASSACRIER (Institut de Physique Nucléaire d'Orsay), Maxime Guilbaud (SUBATECH), Maxime Guilbaud (SUBATECH), Romain Gaior (LPNHE), Thomas STREBLER (CPPM, Aix-Marseille Université, CNRS/IN2P3 (FR))
    27/10/2023 22:00
  52. 83. Elucidating φ Meson Production from K+K- Decay Channel in pp@4.5 GeV Using HADES
    Suman DEB (IJCLAB)
    Hadronic Physics
    Hadronic Physics

    The High Acceptance Di-Electron Spectrometer (HADES) at GSI, Darmstadt, Germany, is an experimental setup designed to investigate hadronic matter within the realm of large net baryon densities and moderate temperatures. It achieves this through fixed-target heavy-ion collisions as well as elementary collisions with incident energies in the range of a few GeV/nucleon.
    One of the recent...

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  53. 4. Invited talk
  54. 82. Ion acceleration from optically shaped high density gas jet targets
    Kristal Bontemps (LP2IB)
    Instrumentation & Interdisciplinaire
    Instrumentation & Interdisciplinarity

    Ion acceleration from optically shaped high density gas jet targets

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  55. 94. Post-PhD networking tool
    Maxime Guilbaud (SUBATECH), Maxime Guilbaud (SUBATECH)
  56. 12. Session overview
    Jonathan Kriewald (LPC Clermont)
  57. 14. Talk Astro #1
    Marie-Sophie Carrasco (Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France)
  58. 15. Talk Astro #2
    Vijay Dabhi (CPPM, Marseille)
  59. 16. Talk Astro #3
    Guillaume Grolleron
  60. 17. Talk Astro #4
    Thibault NGUYEN TRUNG (IJCLab)
  61. 18. Talk Astro #5
    Yongyu PAN
  62. 19. Talk Astro #6
    Cyann Plard (LAPP IN2P3 CNRS)
  63. 49. Talk Astro #7
    Lucas Gréaux (IJCLab)
  64. 21. Talk BSM #2
    ELISE JOURD'HUY (IP2I/UCBL)
  65. 22. Talk BSM #3
    Maxime FERNOUX (Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France), Maxime FERNOUX
  66. 23. Talk BSM #4
    Bogdan Kutsenko (Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France)
  67. 24. Talk BSM #5
    Paul Vaucelle (IPHC)
  68. 25. Talk BSM #6
    Thomas Wojtkowski
  69. 26. Talk Cosmo #1
    Thomas Sainrat (CentraleSupélec)
  70. 47. Talk Cosmo #2
    Marie Lynn Abdul Karim (IRFU/DPhP CEA-Saclay)
  71. 27. Talk Flavor #1
    jessy daniel
  72. 28. Talk Flavor #2
    Tristan Miralles
  73. 29. Talk Flavor #3
    Yann Monceaux (IP2I (Lyon))
  74. 30. Talk Hadronic #1
    Aoumeur Daddi Hammou (Subatech)
  75. 50. Talk Hadronic #3
    Suman DEB (IJCLAB)
  76. 32. Talk instru #1
    Isaac EHLE (Laboratoire Leprince-Ringuet, Institut Polytechnique Paris)
  77. 33. Talk instru #2
    Cervane GRIMAUD (LAPP)
  78. 34. Talk instru #3
    Oleksii KURDYSH (IJCLab)
  79. 35. Talk inter #1
    Kristal Bontemps (LP2IB)
  80. 36. Talk inter #2
    Fotios Ioannis Giasemis, Fotis Giasemis
  81. 37. Talk inter #3
    Alexandre GILLON (Subatech laboratory, Nantes France), Alexandre Gillon (Subatech)
  82. 38. Talk neutrino #1
    Felix Bretaudeau
  83. 39. Talk neutrino #2
    Quentin Pellegrini (LPNHE (SU))
  84. 40. Talk neutrino #3
    Ariel Cohen (APC)
  85. 41. Talk neutrino #4
    Joshua Pinchault (LPSC)
  86. 42. Talk nuclear #1
    Jonathan COLLIN (IPHC)
  87. 43. Talk SM #1
    Jeremy Couthures (ATLAS LAPP)
  88. 44. Talk SM #2
    Line Delagrange (LPNHE, Paris, France)
  89. 45. Talk SM #3
    Mathieu Markovitch (IJCLab)
  90. 46. Talk SM #4
    Océane Poncet (IPHC)
  91. 68. Talk theory #1
    Aoumeur Daddi Hammou (Subatech)
  92. 69. Talk theory #2
    Yann Monceaux (IP2I (Lyon))
  93. 20. Test of global symetries of the SM in the top quark sector
    David Amram (IP2I)

    The pursuit of deviations from the Standard Model (SM) is prompted by the recognition of the model's known limitations. Some findings suggest possible violations of lepton universality. The identification of such deviations could potentially lead to a SM extension, adding Z' boson that interacts with leptons in a different manner.

    The SM is also firmly grounded by the principle of Lorentz...

    Go to contribution page