23 August 2021 to 7 October 2021
Venue: OAC conference center, Kolymbari, Crete, Greece. Participation is possible also via internet.
Europe/Athens timezone

Session

Mini-workshop on Machine Learning for Particle Physics

25 Aug 2021, 11:00
Venue: OAC conference center, Kolymbari, Crete, Greece. Participation is possible also via internet.

Venue: OAC conference center, Kolymbari, Crete, Greece. Participation is possible also via internet.

Conveners

Mini-workshop on Machine Learning for Particle Physics

  • Tommaso Dorigo (Universita e INFN, Padova (IT))

Mini-workshop on Machine Learning for Particle Physics

  • There are no conveners in this block

Mini-workshop on Machine Learning for Particle Physics

  • There are no conveners in this block

Mini-workshop on Machine Learning for Particle Physics

  • There are no conveners in this block

Presentation materials

There are no materials yet.

  1. Francisco Matorras (Instituto de Fisica de Cantabria, Santander, IFCA (ES))
    25/08/2021, 11:00
    Talk

    One of the main limitations in particle physics analyses in which the signal selection is based on machine learning is the understanding of the implications of systematic uncertainties. The usual approach consisting in the training with samples ignoring systematic effects and estimating their contribution to the magnitudes measured on modified test samples. We propose here an alternative...

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  2. Mr Rubén López Ruiz (University of Cantabria)
    25/08/2021, 11:30
    Talk

    Many searches at the LHC experiments target topologies with three or more invisible particles in the final state. The reconstruction of the full event kinematics is in general not possible even using the information provided by the missing transverse momentum or by the constraints based on the presence of known-mass resonances in the decay chain process. On the other hand, the space of...

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  3. Kateřina Hladká (Czech Technical University in Prague)
    25/08/2021, 12:00
    Talk

    In heavy-ion collisions at large particle colliders, such as LHC or RHIC, heavy-flavour (charm and beauty) quarks are produced mainly through initial hard scatterings. Therefore, they can serve as probes of the properties of the hot medium created in such collisions. Hadrons, that contain such quarks, could not be directly detected, thus they are measured via reconstruction of their decay...

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  4. Lukas Layer (Universita e INFN, Padova (IT))
    25/08/2021, 12:30
    Talk

    A challenge for future particle-physics experiments at the high-energy frontier is the precise measurement of muon momenta at very high energy. In this work we discuss the feasibility of an entirely new avenue for the measurement of the energy of muons based on their radiative losses in a dense, finely segmented calorimeter. We demonstrate with an idealised calorimeter layout, how spatial and...

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  5. Santiago Rafael Paredes Saenz (Universite Libre de Bruxelles (BE))
    25/08/2021, 13:00
    Talk

    Searches for pairs of Higgs bosons will be, in all likelihood, the best tools to precisely measure the Higgs boson self-coupling $\lambda_{hhh}$ in future colliders. We study various strategies for the $hh\to b \bar{b} b \bar{b}$ search in the HL-LHC era with focus on constraining $\lambda_{hhh}$. We implement a machine-learning-based approach to separate signal and background and apply...

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  6. Mary Touranakou (National and Kapodistrian University of Athens (GR))
    25/08/2021, 17:00
    Poster presentation

    We study how to use Deep Variational Autoencoders for a fast simulation of jets of particles at the LHC. We represent jets as a list of constituents, characterized by their momenta. Starting from a simulation of the jet before detector effects, we train a Deep Variational Autoencoder to return the corresponding list of constituents after detection. Doing so, we bypass both the detector...

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  7. Hang Qi (University of Science and Technology of China)
    26/08/2021, 17:00
    Talk

    PANDA is a hadron physics research detector at the FAIR facility in Darmstadt, using antiproton beams with momenta between 1.5 and 15 GeV/c interacting with fixed proton targets. From the scientific requirements, the high-performance of electromagnetic calorimeters (EMC) is of utmost importance for the success of the PANDA experiment. Excellent identification and reconstruction of...

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  8. Peiyong Jiang (GSI Helmholtzzentrum für Schwerionenforschung GmbH)
    26/08/2021, 17:30
    Talk

    Deep machine learning methods have been studied for the PANDA software trigger with data sets from full Monte Carlo simulation using PandaRoot. Following the first comparison of multiclass and binary classification, the binary classification has been selected because of higher signal efficiencies. In total seven neural network types have been compared and the residual convolutional neural...

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  9. Etienne Marie Fortin (Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France)
    27/08/2021, 11:00
    Talk

    The Phase-II upgrade of the LHC will increase its instantaneous luminosity by a factor of 7 leading to the High Luminosity LHC (HL-LHC). At the HL-LHC, the number of proton-proton collisions in one bunch crossing (called pileup) increases significantly, putting more stringent requirements on the LHC detectors electronics and real-time data processing capabilities.

    The ATLAS Liquid Argon...

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  10. 27/08/2021, 11:30
    Talk

    The talk addresses the use of neural networks in particle tracking applications. Image based approaches (Convolutional neural networks) and pattern based approaches (graph networks) are being discussed that have successfully been used in the TrackML particle tracking challenge.

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  11. Tommaso Dorigo (INFN Padova)
    27/08/2021, 12:00
    Talk
  12. Dr Pietro Vischia (Universite Catholique de Louvain (UCL) (BE))
    27/08/2021, 12:30
    Talk

    In modern neural networks, supervised learning is implemented as minimization of a loss function that typically represents an estimate of the prediction error on the training samples.The gradient of the loss function is traversed in steps towards the minimum, and at each step the prediction error is propagated backwards to all the network weights.The gradient steps are computed using the loss...

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  13. Aleksandr Petukhov (National Research Nuclear University MEPhI (RU))
    27/08/2021, 13:00
    Talk

    In the collider physics searches, missing values can occur if some of the final state particles are not present in all the events. The electroweak production of the $Z\gamma jj$ – a good probe for the electroweak symmetry breaking – is an example of a process with such final state. Third jet parameters are known to be good at distinguishing it from its’ main background – QCD $Z\gamma jj$...

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  14. Hevjin Yarar (Universita e INFN, Padova (IT))
    Talk

    Searches for new physics at the LHC typically focus on well-specified new physics models. However, this may leave interesting potential signals untested. In this presentation, we describe a search method that does not assume a specific form for the searched distributions. The method is based on a scan of the copula space of multidimensional features of collider events. The performances are...

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