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13/11/2024, 13:45
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Ana Margarida TEIXEIRA (LPC Clermont), Dr Cyril Hugonie (LUPM), Jean Orloff (LPC Clermont, Univ. Blaise Pascal)13/11/2024, 13:50
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Laurent Vacavant (IN2P3)13/11/2024, 14:30
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Fabrice Balli (CEA Saclay), Fabrice Balli (CEA Saclay)13/11/2024, 14:35
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Dirk ZERWAS (DMLab and IJCLab)13/11/2024, 14:55
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Margarete Muehlleitner (ITP Karlsruhe)13/11/2024, 15:20
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Sabine Crépé-Renaudin (IN2P3)13/11/2024, 15:45
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Samuel Calvet (LPC)13/11/2024, 16:05
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Louis D'Eramo (LPCA - Clermont)13/11/2024, 16:25
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13/11/2024, 17:00
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Andreas Goudelis (LPC - Clermont Ferrand)14/11/2024, 09:00Methods and Tools
MicrOMEGAs is a computer program to compute different dark matter observables. In this talk we will present some new features of its latest release, version 6, and discuss some of their physics applications.
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Mohammad Mahdi Altakach14/11/2024, 09:25Methods and Tools
SModelS is a public tool for fast reinterpretation of LHC searches for new physics based on a large database of simplified model results. While previous versions were limited to models with a Z2-type symmetry, version 3 can now handle arbitrary signal topologies. To this end, the tool was fully restructured and now relies on a graph-based description of simplified model topologies. In this...
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Niels FARDEAU, Théo REYMERMIER (IP2I Lyon + LPSC)14/11/2024, 09:50Methods and Tools
Hyperiso is a refactored and expanded version of the flavour code SuperIso allowing for efficient calculations of flavour observables. While SuperIso was dedicated to SM, THDM and several SUSY models, Hyperiso now implements a transparent interface with MARTY (a public tool to perform analytical QFT calculations) to extend SuperIso's observable calculation routines to generic BSM scenarii. In...
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Rafal MASELEK (LPSC (Grenoble))14/11/2024, 10:10Methods and Tools
In recent years, the ATLAS collaboration has released full statistical models for some of their analyses, allowing for precise reinterpretation of experimental limits. These models incorporate numerous nuisance parameters and correlations between signal bins, but their complexity often results in prolonged computation times. This project seeks to develop a method for efficient yet accurate...
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Abdelhamid Haddad (LPCA)14/11/2024, 11:00
I will present the reinterpretation of the CalRatio + X ATLAS analysis (arXiv:2407.09183), focusing on neutral long-lived particles decaying within the ATLAS hadronic calorimeter. The reinterpretation involves a Boosted Decision Tree (BDT) trained on truth-level variables to estimate the probability of events within the ABCD plane and assess the sensitivity of the analysis. The BDT weights,...
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Theo Heimel (Heidelberg)14/11/2024, 11:25
Theory predictions for the LHC require precise numerical phase-space integration and generation of unweighted events. We combine machine-learned multi-channel weights with a normalizing flow for importance sampling to improve classical methods for numerical integration. By integrating buffered training for potentially expensive integrands, VEGAS initialization, symmetry-aware channels, and...
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Quentin BONNEFOY (Université de Strasbourg & IPHC, CNRS)14/11/2024, 11:50
While axions (which are very well-motivated) heavily dominate the amount of work currently done regarding the strong CP problem, alternatives ought to be systematically investigated, in order to assess what the strong CP problem really entails (and potentially update our theoretical biases). In this context, I will talk about solutions that rely on spontaneously broken spacetime symmetries,...
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Baibhab Pattnaik (IFIC (CSIC-University of Valencia) and LPC)14/11/2024, 12:10BSM
We present the detection prospects of new Standard Model (SM)-neutral vector bosons ($Z_{\prime}$) that couple exclusively to leptons at the Future Circular Collider in the electron-positron stage (FCC-ee). We focus our search on $Z’$ production with a radiated photon, and show that FCC-ee can significantly extend the unprobed parameter space for this class of models in the kinematically...
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Yoav Afik (Enrico Fermi Institute, University of Chicago)14/11/2024, 14:00
The Standard Model of particle physics is a quantum field theory, based on quantum mechanics and special relativity. Therefore, it allows us to test fundamental properties of quantum mechanics. Top-quark pairs, which are generated at the LHC, are a unique high-energy system since their spin correlations can be measured. Thus, it is possible to study fundamental aspects of quantum mechanics...
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Caroline COLLARD (IPHC (Strasbourg))14/11/2024, 14:25BSM
Depending on the length of the talk and the preference of the session conveners, the presentation could either focus on the search for heavy stable charged particles at CMS (work performed at IPHC) or cover a broader panel of LLP searches at CMS, associated to different experimental signatures in the detector.
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Yann Monceaux (IP2I (Lyon))14/11/2024, 14:50BSM
Deviations from the Standard Model have long been observed in semileptonic B-meson decays, notably $b→ s \ell \ell$ transitions, triggering speculations on potential New Physics effects in this sector. Following recent updates of $R_{K^{(*)}}$ and $BR(B_{(s)} → μμ)$, and the first measurement of $R_\phi$ by the LHCb collaboration, the sole remaining significant deviations from the SM in...
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Anna CHRYSOSTOMOU (LPTHE)14/11/2024, 15:10BSM
Under certain conditions, a first-order phase transition during early-universe symmetry breaking can generate observable signals in the stochastic gravitational-wave (GW) background. Since the Standard Model (SM) predicts a cross-over phase transition, detectable signals are expected to arise from beyond the SM frameworks, traditionally testable only at colliders. Motivated by this...
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14/11/2024, 15:30
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Ananthakrishnan RAVINDRAN14/11/2024, 16:15
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Vijay Dabhi (CPPM, Marseille)14/11/2024, 16:45
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Pascal PRALAVORIO (CPPM, Aix-Marseille Université, CNRS/IN2P3)14/11/2024, 17:15
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14/11/2024, 17:45
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14/11/2024, 20:00
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Christophe Ochando (LLR), Iro Koletsou (LAPP), Louis D'Eramo (LPCA - Clermont), Pietro Slavich (LPTHE Paris)15/11/2024, 09:30
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Joany Manjarres Ramos (L2I Toulouse, UT3, CNRS/IN2P3)15/11/2024, 09:35
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Mr Geliang Liu (Ecole polytechnique)15/11/2024, 09:55
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Minori FUJIMOTO (CPPM, Aix-Marseille Université, CNRS/IN2P3), Minori Fujimoto15/11/2024, 10:45Higgs
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Giovanni Marchiori (APC Paris)15/11/2024, 11:05Higgs
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Imad Laktineh ({UNIV CLAUDE BERNARD}UMR5822)15/11/2024, 11:35Higgs
The physics programme of linear e+e- colliders spans from the Z-Pole deep into the TeV range. Therefore, all Standard Model particles and their interactions are covered by the scientific programme of linear colliders. Beam polarisation allows for testing all aspects of the electroweak and the Higgs sector. New physics would lead to unique patterns of deviations from the Standard Model...
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Roman Poeschl (LAL Orsay)15/11/2024, 11:55Higgs
At energies above 500 GeV processes such as di-Higgs production or associated top-Higgs production open up. Both processes will profit from the clean environment of e+e- collisions that will allow for a direct measurement of the Higgs self-coupling and an unambiguous determination of the CP properties of the Higgs boson.
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The Higgs particle is intimately coupled to the top quark. Therefore,... -
15/11/2024, 12:15
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Pascal PRALAVORIO (CPPM, Aix-Marseille Université, CNRS/IN2P3)Dark Universe
The MAgnetized Disk and Mirror Axion eXperiment (MADMAX) is a future experiment aiming to detect dark matter axions from the galactic halo by resonant conversion to photons in a strong magnetic field. It uses a novel concept based on a stack of dielectric disks, called booster,to enhance the axion-photon conversion probability over a significant mass range. In its final version MADMAX can scan...
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Mr Ananthakrishnan RAVINDRAN (SUBATECH, IMT Atlantique & The University of Melbourne)Dark Universe
The XENONnT project is located in the Gran Sasso laboratory in Italy.
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Its main goal is the direct detection of dark matter, particularly
Weakly Interacting Massive Particles (WIMPs). It uses a dual-phase
liquid xenon time projection chamber (TPC) to identify particle
interactions. When a particle interacts with the target mass, light (S1
signal) and charge (S2 signal) are produced. The...
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