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    Physical Properties of Materials and Testing Methods

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    The use of materials in particle accelerator applications implies the consideration of physical properties in different environments than usual industrial applications. Cryogenic temperatures, high radiation, medium to high vacuum and high magnetic fields are requirements for which the behavior of materials has to be evaluated. In this lecture, Thermal, Electrical and Magnetic properties are briefly introduced, highlighting the mechanisms governing variation with temperature and magnetic field. Standards and testing methods for different properties are described, illustrated with practical examples. With regard to the characterization of thermal properties of a material, testing methods of heat capacity and thermal conductivity are described, with details of the main working principle and measurement examples. Determination of electrical resistivity and the residual resistivity ratio (RRR) are the main characteristics of electrical properties, together with specific characterization of superconducting materials. Testing magnetic properties deserve special attention; different methods are commonly employed to characterize non-magnetic and magnetic materials. In magnetic metals and ferrites non-linear behavior and hysteresis effects need to be considered in order to assess their suitability for applications or to model material performance

    ATLAS and CMS HH/SH resonant searches in the 2b2τ final state

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    This talk is an overview of the latest ATLAS results in the search for resonant di-Higgs to bbtautau, together with the latest public CMS result, which involves an additional scalar

    CMS track reconstruction performance during Run 3

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    The precise reconstruction of charged particle tracks is crucial for the overall performance of the CMS experiment. In this contribution, performance measurements of the track reconstruction both in simulation and data are presented, from the collisions that occurred during the last periods of the Run 3 of data taking at the LHC. A particular focus is given to the role and performance of the Silicon Pixel detector. Together with comparisons between data and simulation on important track quantities, the efficiencies measured at high level trigger and with the tag-and-probe techniques are discussed

    HL-LHC Cost & Schedule Review 2025 - visits

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    Photos from the visits as part of the HL-LHC CSR25 to the HL-LHC underground galleries at Point 1, IT String and beam screen facility

    BDF/SHiP Annual Report 2025

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    The report covers the progress of the SHiP collaboration and the HI-ECN3 Project Team since the start of the TDR phase mid-2024

    Upgrade of ATLAS Hadronic Tile Calorimeter for the High Luminosity LHC

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    The Tile Calorimeter (TileCal) is a sampling hadronic calorimeter covering the central region of the ATLAS experiment, with steel as absorber and plastic scintillators as active medium. The High-Luminosity phase of LHC, delivering five times the LHC nominal instantaneous luminosity, is expected to begin in 2029. TileCal will require new electronics to meet the requirements of a 1 MHz trigger, higher ambient radiation, and to ensure better performance under high pile-up conditions. Both the on- and off-detector TileCal electronics will be replaced during the shutdown of 2026-2028. PMT signals from every TileCal cell will be digitized and sent directly to the back-end electronics, where the signals are reconstructed, stored, and sent to the first level of trigger at a rate of 40 MHz. This will provide better precision of the calorimeter signals used by the trigger system and will allow the development of more complex trigger algorithms. The modular front-end electronics feature radiation-tolerant commercial off-the-shelf components and redundant design to minimise single points of failure. The timing, control and communication interface with the off-detector electronics is implemented with modern Field Programmable Gate Arrays (FPGAs) and high speed fibre optic links running up to 9.6 Gb/s. The TileCal upgrade program has included extensive R&D and test beam studies

    QCD String Axions and MM-theory

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    In SU(N)SU(N) Yang-Mills theory without matter, there exist stable long electric fluxtube strings which carry a 1-form symmetry charge. Over the past decade or so, there has been increasing evidence from lattice calculations that the worldsheet theories of such QCD strings contain a massive pseudoscalar (axion), at least when N3N\geq 3. This has so far been puzzling from the perspective of holographic realizations of strings in confining gauge theories. In this note, we will show how such axions appear naturally in the realization of 4D N=1\mathcal{N}=1 Super-Yang-Mills (SYM) from MM-theory spacetimes in which the extra dimensions are modeled by certain complete metrics of G2G_2-holonomy. This picture predicts that QCD string axions exist only if the gauge group is SU(N3)SU(N\geq 3), SO(4N+2)SO(4N+2), or E6E_6 (or a quotient/double-cover thereof), and is absent from the spectrum of stable QCD strings if the gauge group is SU(2)SU(2), SO(2N+1)SO(2N+1), SO(4N)SO(4N), Sp(N)Sp(N), or E7E_7. We argue why we expect this pattern to persist for non-supersymmetric Yang-Mills strings, at least for large NN, something which could be tested in future lattice studies of QCD strings for gauge algebras of B, C, D, and E-type

    4th International Symposium on the History of Particle Physics

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    Recent top-quark mass measurements from cross section from ATLAS

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    HIghlights of recent top-quark mass extractions from ATLAS measurements of ttbar cross sections

    4th International Symposium on the History of Particle Physics

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