Name: Séminaires doctorants 2ème année - Session 3
Start: 2022-06-07T14:00:00+02:00
End: 2022-06-07T17:20:00+02:00
Location: IJCLab

- 1
  
  Background studies for the CROSS, CUPID-Mo and CUPID neutrinoless double beta decay experiments¶
  
  Orateur: Léonard Imbert
  
  presentation_CAT.pdf
- 2
  
  Contribution to the construction of the pixel detector of the ATLAS experiment for the HL-LHC¶
  
  Orateur: Yahya Khwaira (IJC LAB - Laboratoire de Physique des 2 Infinis Irène Joliot Curie)
  
  Khwaira_Yahya PhD Seminar - IJC Lab 2022.pdf
- 3
  
  Measurement of the Higgs couplings using diphoton channel with ATLAS full Run 2 data¶
  
  Orateur: Oleksii Lukianchuk (IJCLab)
  
  CAT_07Jun2022_Lukianchuk.pdf
- 4
  
  Off-shell Higgs into 4 leptons using EFTs and Simulation-Based Inference & electron tracking in ATLAS (ITk)¶
  
  The discovery of the Higgs was first made in the Higgs-to-4-lepton (H4l) decay channel, almost 10
  years ago. Yet, new possibilities of analysis are still available in this channel. They lay beyond
  the on-shell data by studying the off-shell Higgs, defined as having a centre-of-mass energy above
  220 GeV. In particular, we shall use the framework of EFTs (Effective Field Theory) which aims to
  better understand the deviations of data relative to the Standard Model. The goal is to generate
  trustworthy Monte-Carlo samples for the relevant EFT operators in order to fit data and measure the
  Wilson coefficients for those operators. In this work so far, we have focused on the Monte-Carlo
  generation process in order to compare and validate several software versions.
  The process of linking experimental data back to the theory parameters is called inference, using a
  function called the likelihood. The complexity of this problem of HEP is such that the likelihood
  cannot be calculated analytically: this problem is intractable. Simulation-based inference is a
  promising method to extract the most information possible from the available data.
  
  At the future HL-LHC, the ITk (Inner Tracker) is scheduled to replace and upgrade the current Inner
  Detector. The ATLAS tracking software was reworked into an experiment-independent software
  collaboration called ACTS (A Common Tracking Software), with the idea of future implementation of
  multi-threading and Machine Learning. The ACTS is therefore being reintegrated into the Athena,
  ATLAS’ software framework. Tracking is particularly challenging for the electron because of
  increased brehmstrallung, as the particle loses energy as it progresses in the tracker. The Gaussian
  Sum Filter (GSF) fitter, which exists in the ATLAS software, is being implemented and optimized into
  ACTS. The GSF fitter from ACTS must therefore be validated and compared to the reference track
  fitting algorithm in ACTS (called the CKF) and to the existing GSF fitter from ATLAS.
  
  Orateur: Arnaud Maury (IJCLab)
  
  MAURY_2022_CAT_seminar.pdf
- 15:20
  
  Pause café
- 5
  
  Charmonium production as a function of charged- particle multiplicity with the ALICE experiment at the LHC¶
  
  Orateur: Theraa TORK (IJCLab)
  
  TheraaTORK_CAT.pdf
- 6
  
  Vidya Sagar Vobbilisetti - Search for $B^{+} \to K^{+} τ^{+} τ^{-}$ at Belle II¶
  
  Orateur: Vidya Sagar VOBBILISETTI (This is the correct one)
  
  Slides 07 May 2022.pdf
- 7
  
  Felicia Carolin Volle - Angular analysis of $Λ_{b} \to Λ (1520) μ^{+} μ^{-}$ ¶
  
  Orateur: Felicia Volle
  
  CAT_7juin2022.pdf
- 8
  
  Volume de relaxation des défauts cristallins dans le fer¶
  
  Orateur: Mohamed El Bakouri El Haddaji
  
  Seminaire_CAT_2022.pdf
- 9
  
  Sami Habet¶
  
  Orateur: Sami HABET (IJCLab)
  
  CAT 2 Sami's talk.pdf
  
  Polarized and unpolarized positron beams are essential for the future hadronic physics experimental program at the
  Thomas Jefferson National Accelerator Facility (JLab). The main challenge is to produce high duty-cycle, and high intensity polarized positron beams. The JLab positron source uses the Polarized Electrons for Polarized Positrons (PEPPo) technique to create either a low intensity, high polarization positron beam (I > 100 nA, P=60%) or a high-intensity unpolarized positron beam (I > 3 μA ), from an intense highly polarized electron beam (I=1 mA, P=90%). The current design involves a new injector dedicated to positron production, collection, and shaping suitable for acceleration through the Continuous Electron Beam Accelerator Facility (CEBAF). The optimization of the layout and the performance of the positron source will be explored in this presentation.

Séminaires doctorants 2ème année - Session 3

100/-1-A900 - Auditorium Joliot Curie

IJCLab