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Related papers: Overview of the SiLC R&D Activities

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A high-energy $e^+e^-$ Linear Collider has been considered since a long time as an important complement to the LHC. Unprecedented precision measurements as well as the exploration of so far untouched phase space for direct production of new…

High Energy Physics - Phenomenology · Physics 2018-09-26 Jenny List , Gudrid Moortgat-Pick , Jürgen Reuter

In order to fully exploit the physics potential of the future high energy e+e- linear collider, a Vertex Tracker able to provide particle track extrapolation with very high resolution is needed. Hybrid Si pixel sensors are an attractive…

High Energy Physics - Experiment · Physics 2010-01-26 M. Battaglia , S. Borghi , R. Campagnolo , M. Caccia , W. Kucewicz , P. Jalocha , J. Palka , A. Zalewska

The JLC is a linear collider project pursued in Japan by researchers centered around KEK. The R&D status for the JLC project is presented, with emphasis on recent results from ATF concerning studies of production of ultra-low emittance…

Accelerator Physics · Physics 2007-05-23 N. Toge

We present recent improvements in the performance of the reconstruction of non-prompt track in the SiD Detector Concept Design, including initial results on the effect of longitudinal segmentation in the SiD tracker. We also describe a…

Instrumentation and Detectors · Physics 2009-02-16 Chris Meyer , Tyler Rice , Lori Stevens , Bruce A. Schumm

The "LiC Detector Toy" is a fast single-track simulation and reconstruction tool, aiming at the optimization of tracking detector design, i.e. geometric layout and material budgets. Its implementation is based on the MATLAB system.…

Instrumentation and Detectors · Physics 2009-01-28 Manfred Valentan , Meinhard Regler , Winfried Mitaroff , Rudolf Fruhwirth

The goal of the EUDET project is the development and construction of infrastructure to permit detector R&D for the International Linear Collider (ILC) with larger scale prototypes. It encompasses major detector components: the vertex…

Instrumentation and Detectors · Physics 2008-11-07 J. Mnich , M. Wing

The International Linear Collider (ILC) is now under consideration as the next global project in particle physics. In this report, we review of all aspects of the ILC program: the physics motivation, the accelerator design, the run plan,…

The planned upgrade of the LHC accelerator at CERN, namely the high luminosity (HL) phase of the LHC (HL-LHC foreseen for 2023), will result in a more intense radiation environment than the present tracking system was designed for. The…

Instrumentation and Detectors · Physics 2015-12-09 Timo Peltola

While the tracking detectors of the ATLAS and CMS experiments have shown excellent performance in Run 1 of LHC data taking, and are expected to continue to do so during LHC operation at design luminosity, both experiments will have to…

Silicon pad sensors with novel functions of higher timing resolution (LGAD: Low Gain Avalanche Detector) and higher position resolution (PSD: Position Sensitive Detector) are studied for an application to Silicon-Tungsten electromagnetic…

Instrumentation and Detectors · Physics 2021-01-07 Taikan Suehara , Yuto Deguchi , Yuto Uesugi , Yu Kato , Ryo Yonamine

In this article, we describe the key features of the recently completed technical design for the International Linear Collider (ILC), a 200-500 GeV linear electron-positron collider (expandable to 1 TeV) that is based on 1.3 GHz…

Accelerator Physics · Physics 2013-11-15 Barry Barish , James E. Brau

The International Linear Collider (ILC) is the next large project in accelerator based particle physics. It is complementary to the LHC in many aspects. Measurements from both machines together will finally shed light onto the known…

High Energy Physics - Experiment · Physics 2007-05-23 J. List

The International Large Detector, ILD, is a detector concept for an experiment at a future high energy lepton collider. The detector has been optimised for precision physics in a range of energies from 90~GeV to about 1~TeV. ILD features a…

High Energy Physics - Experiment · Physics 2025-06-09 H. Abramowicz , D. Ahmadi , J. Alcaraz , O. Alonso , L. Andricek , J. Anguiano , O. Arquero , F. Arteche , D. Attie , O. Bach , M. Basso , J. Baudot , A. Bean , T. Behnke , A. Bellerive , Y. Benhammou , M. Berggren , G. Bertolone , M. Besancon , A. Besson , O. Bezshyyko , G. Blazey , B. Bliewert , J. Bonis , R. Bosley , V. Boudry , C. Bourgeois , I. Bozovic Jelisavcic , D. Breton , J. -C. Brient , B. Brudnowski , V. Buescher , K. Buesser , P. Buhmann , M. Böhler , S. Callier , E. Calvo Alamillo , M. Cepeda , S. Chen , G. Claus , P. Colas , C. Colledani , C. Combaret , R. Cornat , F. Corriveau , J. Cvach , C. De La Taille , K. Desch , H. Diao , A. Dieguez , R. Diener , A. Dorokhov , A. Drutskoy , B. Dudar , A. Dyshkant , I. Echeverria , U. Einhaus , Z. El Bitar , A. Escalante del Valle , M. Fernandez , M. Firlej , T. Fiutowski , I. Fleck , N. Fourches , M. C. Fouz , K. Francis , C. Fu , K. Fujii , T. Fusayasu , J. Fuster , K. Gadow , F. Gaede , J. Galindo , A. Gallas , S. Ganjour , E. Garutti , I. Giomataris , M. Goffe , A. Gonnin , F. González , O. Gonzalez Lopez , I. Gregor , G. Grenier , P. Göttlicher , F. Hartjes , J. Heilman , C. Hensel , S. Hidalgo , A. Himmi , Y. Horii , R. Hosokawa , C. Huo-Guo , M. Idzik , M. Iglesias , F. Ikeda , A. Irles , A. Ishikawa , M. Iwasaki , K. Jaaskelainen , R. Jaramillo , D. Jeans , J. Jeglot , L. Jönsson , G. Kacarevic , M. Kachel , J. Kalinowski , J. Kaminski , Y. Kamiya , T. Kamiyama , Y. Kato , K. Kawagoe , S. A. Khan , J. Klamka , P. Kluit , M. Kobayashi , K. Kong , A. Korol , P. Koppenburg , K. Krüger , M. Kuriki , J. Kvasnicka , D. Lacour , I. Laktineh , A. Laudrain , F. LeDiberder , A. Levy , I. Levy , W. Li , B. List , J. List , J. Liu , A. Lopez Virto , M. Lopez , Y. Lu , B. Lundberg , J. Maalmi , B. Madison , T. Madlener , A. Martens , S. Martens , I. Masamune , L. Masetti , H. Mathez , A. Matsushita , K. McDonald , K. Mekala , G. Milutinovic Dumbelovic , W. Minori , L. Mirabito , W. Mitaroff , V. Mitsou , U. Mjörnmark , T. Mogi , G. Moortgat-Pick , F. Morel , T. Mori , S. Morimasa , J. Moron , D. Moya , T. Murata , E. Musumeci , J. Márquez Hernández , J. Nakajima , E. Nakano , J. Nanni , S. Narita , J. Nilsson , J. Ninkovic , D. Ntounis , T. Nunez , H. Ogawa , K. Oikawa , Y. Okugawa , T. Omori , H. Ono , W. Ootani , C. Orero , A. Oskarsson , L. Osterman , Q. Ouyang , T. Pasquier , G. Pellegrini , H. Pham , J. Piedrafita , I. Polak , A. Pradas , V. Prahl , T. Price , J. Puerta Pelayo , R. Pöschl , H. Qi , Y. Radkhorrami , G. Raven , L. Reichenbach , M. Reinecke , E. Reynolds , F. Richard , R. Richter , S. Ritter , C. Rogan , J. Rolph , A. Rosmanitz , C. Royon , M. Ruan , S. Rudrabhatla , A. Ruiz-Jimeno , A. Sajbel , R. Sakakibara , I. Salehinia , T. Sanuki , H. Sato , C. Schmitt , T. Schoerner-Sadenius , M. Schumacher , V. Schwan , O. Schäfer , F. Sefkow , T. Seino , S. Senyukov , R. Settles , Z. Shen , A. Shoji , F. Simon , I. Smiljanic , M. Specht , T. Suehara , R. Sugawara , A. Sugiyama , Z. Sun , P. Svihra , K. Swientek , T. Takahashi , T. Takatsu , T. Takeshita , S. Tapprogge , P. Terlecki , A. Thiebault , J. Tian , J. Timmermans , M. Titov , L. Tomasek , J. Torndal , B. Tuchming , M. Tytgat , W. Vaginay , I. Valin , C. Vallee , R. van Kooten , H. van der Graaf , C. Vernieri , I. Vidakovic , H. Videau , I. Vila , A. Vilà , M. Vos , N. Vukasinovic , J. Wang , R. Wanke , K. Watanabe , T. Watanabe , N. Watson , J. Wellhausen , U. Werthenbach , G. Wilson , M. Wing , A. Winter , M. Winter , H. Yamamoto , K. Yamamoto , R. Yonamine , T. Yonemoto , J. Zalesak , A. F. Zarnecki , C. Zeitnitz , K. Zembaczynski , D. Zerwas , Y. Zhang , F. Zomer , V. Zutshi

The International Linear Collider (ILC) is the next large scale project in accelerator particle physics. Colliding electrons with positrons at energies from 0.3 TeV up to about 1 TeV, the ILC is expected to provide the accuracy needed to…

High Energy Physics - Experiment · Physics 2016-11-23 Marco Battaglia

Resistive AC-coupled Silicon Detectors (RSDs) are silicon sensors which provide high temporal and spatial resolution. The RSD is a candidate sensor to be used in future tracking detectors with the objective of obtaining '4D' tracking, where…

With an active silicon area of more than 200 squaremetres, the silicon strip tracker of the CMS experiment, one of the experiments currently under construction for the future Large Hadron Collider at CERN, will be by far the largest silicon…

Instrumentation and Detectors · Physics 2008-11-26 Katja Klein

In order to achieve the physics goals of future Linear Colliders, it is important that electron and positron beams are polarized. The baseline design at the International Linear Collider (ILC) foresees an e+ source based on helical…

Accelerator Physics · Physics 2012-02-06 V. Kovalenko , O. S. Adeyemi , A. Hartin , G. Moortgat-Pick , L. Malysheva , S. Riemann , F. Staufenbiel , A. Ushakov

CLIC is a proposed linear e+e- collider designed to provide particle collisions at center-of-mass energies of up to 3 TeV. Precise measurements of the properties of the top quark and the Higgs boson, as well as searches for Beyond the…

Instrumentation and Detectors · Physics 2017-06-21 Simon Spannagel

Basic scaling laws are used to compare the relative capabilities of gaseous and solid-state tracking. Conclusions are drawn in the context of physics processes expected to be at the focus of studies at the International Linear Collider.

Instrumentation and Detectors · Physics 2007-05-23 Bruce A. Schumm

The Compact Linear Collider CLIC is designed to deliver e+e- collisions at a center of mass energy of up to 3 TeV. The detector systems at this collider have to provide highly efficient tracking and excellent jet energy resolution and…

Instrumentation and Detectors · Physics 2011-09-16 Frank Simon