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We study the prospects for discovering an extra scalar boson $S^0$ at the International Linear Collider (ILC) based on a full simulation of the International Large Detector (ILD). In order to provide results in an as model-independent way…

High Energy Physics - Experiment · Physics 2020-05-14 Yan Wang , Mikael Berggren , Jenny List

For the 1994/95 run of the SLD experiment at SLAC, a Compton polarimeter measured the luminosity-weighted electron beam polarization to be (77.2 +- 0.5)%. This excellent accuracy is achieved by measuring the rate asymmetry of…

High Energy Physics - Experiment · Physics 2007-05-23 M. Woods , representing the SLD collaboration

A large number of measurements with polarized beams and/or spin analysis of final state particles has been performed at the e^+e^- colliders LEP and SLC, providing important information on the dynamics of high energy interactions. In this…

High Energy Physics - Experiment · Physics 2009-10-31 W. Bonivento

Circular colliders have the advantage of delivering collisions to multiple interaction points, which allow different detector designs to be studied and optimized - up to four for FCC-ee. On the one hand, the detectors must satisfy the…

High Energy Physics - Experiment · Physics 2021-07-12 Patrizia Azzi , Emmanuel Perez

This document provides a writeup of all contributions to the workshop on "High precision measurements of $\alpha_s$: From LHC to FCC-ee" held at CERN, Oct. 12--13, 2015. The workshop explored in depth the latest developments on the…

The Future Circular Collider in the $\mathrm{e^{+}e^{-}}$ configuration offers the opportunity to significantly improve SM measurements with dedicated runs at the Z-pole, WW threshold, ZH (240 GeV), and $\mathrm{t}\bar{\mathrm{t}}$…

High Energy Physics - Experiment · Physics 2022-08-18 Eduardo Ploerer

The Compact Linear Collider (CLIC) is a high-energy high-luminosity linear electron-positron collider under development. It is foreseen to be built and operated in three stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV,…

Instrumentation and Detectors · Physics 2019-05-08 A. C. Abusleme Hoffman , G. Parès , T. Fritzsch , M. Rothermund , H. Jansen , K. Krüger , F. Sefkow , A. Velyka , J. Schwandt , I. Perić , L. Emberger , C. Graf , A. Macchiolo , F. Simon , M. Szalay , N. van der Kolk , H. Abramowicz , Y. Benhammou , O. Borysov , M. Borysova , A. Joffe , S. Kananov , A. Levy , I. Levy , G. Eigen , R. Bugiel , S. Bugiel , M. Firlej , T. A. Fiutowski , M. Idzik , J. Moroń , K. P. Świentek , P. Terlecki , P. Brückman de Renstrom , B. Turbiarz , T. Wojtoń , L. K. Zawiejski , E. Firu , V. Ghenescu , A. T. Neagu , T. Preda , I. Boyko , Yu. Nefedov , A. Rymbekova , A. Sapronov , G. Shelkov , A. Zhemchugov , A. Ruiz-Jimeno , I. Vila , E. Fullana , J. Fuster , P. Gomis Lopez , M. Perelló , M. A. Villarejo , M. Vos , J. Alozy , N. Alipour Tehrani , D. Arominski , R. Ballabriga Sune , F. Boyer , E. Brondolin , M. Buckland , M. Campbell , D. Dannheim , K. Dette , F. Duarte Ramos , N. Egidos Plaja , K. Elsener , A. Fiergolski , C. Fuentes Rojas , C. Grefe , D. Hynds , W. Klempt , I. Kremastiotis , J. Kröger , S. Kulis , E. Leogrande , L. Linssen , X. Llopart Cudie , A. Lucaci-Timoce , M. Munker , L. Musa , A. Nürnberg , F. -X. Nuiry , E. Perez Codina , H. Pernegger , M. Petrič , F. Pitters , T. Quast , S. Redford , P. Riedler , P. Roloff , A. Sailer , E. Santin , U. Schnoor , E. Sicking , K. Sielewicz , R. Simoniello , W. Snoeys , S. Spannagel , S. Sroka , R. Ström , P. Valerio , S. van Dam , E. van der Kraaij , T. Vǎnát , O. Viazlo , M. Vicente Barreto Pinto , M. A. Weber , M. Williams , K. Wolters , M. Benoit , G. Iacobucci , D M S Sultan , R. R. Bosley , T. Price , M. F. Watson , N. K. Watson , A. G. Winter , J. Goldstein , S. Green , J. S. Marshall , M. A. Thomson , B. Xu , G. Casse , J. Vossebeld , T. Coates , F. Salvatore , J. Repond , L. Xia , C. Kenney , A. Tomada

We describe the anticipated experimental program of an e+e- linear collider in the energy range 500 GeV -- 1.5 TeV. We begin with a description of current collider designs and the expected experimental environment. We then discuss precision…

High Energy Physics - Experiment · Physics 2009-09-29 Hitoshi Murayama , Michael E. Peskin

The experimental potential of e+e- Linear Colliders to explore the properties of supersymmetric particles is reviewed. High precision measurements of masses, spin-parity, gauge quantum numbers, couplings and mixings, production and decay…

High Energy Physics - Phenomenology · Physics 2007-05-23 Hans-Ulrich Martyn

We classify the possible deviations from the Standard Model in the QED-dominated $\mathrm{e^+e^-}\rightarrow\gamma\gamma$ process under the assumption of a preserved $SU(2)_L \times U(1)_Y$ symmetry. We find that the only deviations really…

High Energy Physics - Phenomenology · Physics 2022-06-16 J. Alcaraz Maestre

The FCC integrated programme comprises an $\rm e^+e^-$ high-luminosity circular collider that will produce very large samples of data in an energy range $88 \le \sqrt{s} \le 365$ GeV, followed by a high-energy $\rm pp$ machine that, with…

High Energy Physics - Experiment · Physics 2025-04-18 Alain Blondel , Christophe Grojean , Patrick Janot , Srini Rajagopalan , Guy Wilkinson

We review recent Z^0 physics results from SLD that use the Cherenkov Ring Imaging Detector for charged particle identification. The performance of the detector and likelihood method are described briefly. Several hadronization measurements…

High Energy Physics - Experiment · Physics 2008-11-26 D. Muller , representing the SLD Collaboration

A wealth of physics results have already been obtained from the LHC, due to the excellent performance of the collider and its experiments. Even more results are expected to be achievable in the phase of the high-luminosity LHC (HL-LHC). It…

High Energy Physics - Experiment · Physics 2021-05-26 Susanne Kuehn

The precision physics program of the ILC requires precise knowledge of the state of beam polarisation. In fact the Compton polarimeters intended for the ILC will have to measure the polarisation with error a factor of 2 smaller than the…

Instrumentation and Detectors · Physics 2014-11-20 Christoph Bartels , Anthony Hartin , Christian Helebrant , Daniela Kaefer , Jenny List

At the end of 2010, the CERN Large Hadron Collider started operation with heavy ion beams, colliding lead nuclei at a centre-of-mass energy of 2.76 TeV/nucleon and opening a new era in ultra-relativistic heavy ion physics at energies…

High Energy Physics - Experiment · Physics 2015-06-04 Berndt Muller , Jurgen Schukraft , Bolek Wyslouch

This review describes the current status of precision QCD studies at the LHC. We introduce the main experimental and theoretical methods, discussing also their cross-stimulated developments and recent advances. The different types of QCD…

High Energy Physics - Phenomenology · Physics 2022-10-12 Thomas Gehrmann , Bogdan Malaescu

The first year of LHC data taking provided an integrated luminosity of about 35/pb in proton-proton collisions at sqrt(s)=7 TeV. The accelerator and the experiments have demonstrated an excellent performance. The experiments have obtained…

High Energy Physics - Experiment · Physics 2011-06-21 Gregor Herten

This note presents constraints on Standard Model parameters using published and preliminary precision electroweak results measured at the electron-positron colliders LEP and SLC. The results are compared with precise electroweak…

Physics at the Large Hadron Collider (LHC) and the International e+e- Linear Collider (ILC) will be complementary in many respects, as has been demonstrated at previous generations of hadron and lepton colliders. This report addresses the…

High Energy Physics - Phenomenology · Physics 2012-08-27 LC Study Group , G. Weiglein , T. Barklow , E. Boos , A. De Roeck , K. Desch , F. Gianotti , R. Godbole , J. F. Gunion , H. E. Haber , S. Heinemeyer , J. L. Hewett , K. Kawagoe , K. Monig , M. M. Nojiri , G. Polesello , F. Richard , S. Riemann , W. J. Stirling , A. G. Akeroyd , B. C. Allanach , D. Asner , S. Asztalos , H. Baer , M. Battaglia , U. Baur , P. Bechtle , G. Belanger , A. Belyaev , E. L. Berger , T. Binoth , G. A. Blair , S. Boogert , F. Boudjema , D. Bourilkov , W. Buchmuller , V. Bunichev , G. Cerminara , M. Chiorboli , H. Davoudiasl , S. Dawson , S. De Curtis , F. Deppisch , M. A. Diaz , M. Dittmar , A. Djouadi , D. Dominici , U. Ellwanger , J. L. Feng , I. F. Ginzburg , A. Giolo-Nicollerat , B. K. Gjelsten , S. Godfrey , D. Grellscheid , J. Gronberg , E. Gross , J. Guasch , K. Hamaguchi , T. Han , J. Hisano , W. Hollik , C. Hugonie , T. Hurth , J. Jiang , A. Juste , J. Kalinowski , W. Kilian , R. Kinnunen , S. Kraml , M. Krawczyk , A. Krokhotine , T. Krupovnickas , R. Lafaye , S. Lehti , H. E. Logan , E. Lytken , V. Martin , H. -U. Martyn , D. J. Miller , S. Moretti , F. Moortgat , G. Moortgat-Pick , M. Muhlleitner , P. Niezurawski , A. Nikitenko , L. H. Orr , P. Osland , A. F. Osorio , H. Pas , T. Plehn , W. Porod , A. Pukhov , F. Quevedo , D. Rainwater , M. Ratz , A. Redelbach , L. Reina , T. Rizzo , R. Ruckl , H. J. Schreiber , M. Schumacher , A. Sherstnev , S. Slabospitsky , J. Sola , A. Sopczak , M. Spira , M. Spiropulu , Z. Sullivan , M. Szleper , T. M. P. Tait , X. Tata , D. R. Tovey , A. Tricomi , M. Velasco , D. Wackeroth , C. E. M. Wagner , S. Weinzierl , P. Wienemann , T. Yanagida , A. F. Zarnecki , D. Zerwas , P. M. Zerwas , L. Zivkovic