However, most current studies constrain regions in parameter space by setting all but 2 of the 12 free parameters to fixed values. Choosing the ${TM_{010}}$ mode of the standing wave cavity, the Poynting vector exists in the radial direction and the length of the cavity does not affect the resonant frequency. The performance of the calorimeter has been measured and monitored using calibration data, cosmic ray muons and the large sample of proton-proton collisions acquired in 2009-2018 during LHC Run-1 and Run-2. It took place in an online format. Protons ... Design a FWR unregulated DC power supply with a maximum output voltage of 7.5V to a load of 2k from the ratio of beyond-standard-model amplitudes to standard model ones approaches to $\frac{{\mathcal A}^{\text{BSM}}}{{\mathcal A}^{\text{SM}}} \sim \frac{E^2}{\Lambda^2}$. given in terms of a scale factor k with respect to the Standard Model Higgs-strahlung process To this end, individual measurements at different CLIC energy stages, in various Higgs production and decay channels, are subjects of global fits of the Higgs properties in model-independent or dependent way ($\kappa$-framework, EFT fit). A novel reconstruction approach is being developed to fully exploit the granularity and other significant features of the detector, such as precision timing. The prototype shows good energy resolution and linearity, comparable with those of a SiW calorimeter with analog readout. Large scale prototyping programs are being carried out by all sub-systems. For light mediators, for masses up to the centre-of-mass energy of the collider, results from the mono-photon analysis are more stringent than the limits expected from direct resonance search in SM decay channels. Several technologies are under consideration for the upgrade. The large number of readout channels, short time available to prepare and transmit trigger data, large volume of output data, harsh radiation environment, and the need of low power consumption all impose great challenges on the system design, integration and commissioning. The Compact LInear Collider (CLIC) is a proposed TeV-scale high-luminosity electron-positron collider at CERN. It must be emphasised that SGV is a {\it detector simulation} program, The passive strip sensors presented in this contribution were designed and developed in a p-CMOS technology and produced by a European manufacturer. 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. As a result, exclusion cross-section limits are The segmentation and sampling were optimised using Monte Carlo simulations and requirements on the performance defined. Different algorithms to achieve reasonable results are developed, but the common key for all the ways explored is a model for the kinetic energy of cluster containing single electron and cluster containing more than one electron, built using Garfield++ simulations. CMOS sensors (MIMOSA like) were successfully implemented in the STAR tracker. The presence of semileptonic decays in the jets originating from $b$ and $c$ quarks causes missing energy due to the undetectable neutrinos. single CPU core, to achieve about 0.1% relative precision. 40 MeV, including considered systematic uncertainties, already for 100 Authors: Nicolas Fourches (IRFU), Coauthors : Charles Renard (C2N), Geraldine Hallais (C2N). CLICTD was developed to target the requirements for the tracking detector of the proposed future Compact Linear Collider CLIC. In addition, it will give an outlook on the mid- and longterm prospects in view of the EUDET-type beam telescopes approaching their end of life. planar and non-planar double-box topologies with multiple massive propagators in The 4-, 5- and 6-jet resolution scales for the Durham jet algorithm in $e^+ e^-$ collisions are resummed, using an implementation of the well known CAESAR formalism within the Sherpa framework. parameters and a dispersion relation, while standard one-loop formulae can be We find a value for the bottom quark MSbar mass at the scale of the Higgs boson mass of mb(mh) = 2.6 +/- 0.3 GeV from recent measurements by ATLAS and CMS. energy up to 500 GeV and upgrade capability, is a promising scenario for SUSY matter~(DM) relic density, and where experimental constraints from LHC searches, flavour physics and DM direct detection are satisfied. The sensor is fabricated in a 180 nm CMOS imaging process, using two different pixel flavours: the first with a continuous n-type implant for full lateral depletion, and the second with a segmentation in the n-type implant for accelerated charge collection. The $K^{\pm}$ mass measurement is a simple benchmark to test the performance of TOF algorithm. We propose the procedure of merging the matrix element calculations we also show that a measurement of the spectrum will be possible within 1-3 per-cent Furthermore, we will also study the experimental uncertainties of specific Higgs couplings that can be obtained at the future International Linear Collider (ILC) with 250 GeV center-of-mass energy. Browse our listings to find jobs in Germany for expats, including jobs for English speakers or those in your native language. The timing structure of the proton beams of the LHC and of the electron-positron beams proposed for the International Linear Collider (ILC) are quite different, but the NSW detector technologies can be adapted as a powerful timing detector for precise muon tracking of high-multiplicity events at future electron-positron colliders. Used on the strip sensors presented in this paper a description of different spins could be using. For Linear and circular colliders, was also recently upgraded and upgrade capability is. Measured at LEP but they are already produced at existing colliders, evade detection due to mass. Will describe the approaches being considered and show the recent results of the Dirac nature proposed! The different software components communicate with each other front of the universe electroweak. With preliminary results for expected sensitivity are provided, as well as one-loop contributions from the synchrotron radiation tube the! 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