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Related papers: DSiD: a Delphes Detector for ILC Physics Studies

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The SiD Detector is one of two detector designs for the future International Linear Collider (ILC) that were validated in 2012 SiD features a compact, cost-constrained design for precision Higgs and other measurements, and sensitivity to a…

Instrumentation and Detectors · Physics 2025-05-20 M. Breidenbach , J. E. Brau , P. Burrows , T. Markiewicz , M. Stanitzki , J. Strube , A. P. White

The SiD Detector is one of two validated detector designs for the future International Linear Collider. SiD features a compact, cost-constrained design for precision Higgs couplings determination, and other measurements, and sensitivity to…

Instrumentation and Detectors · Physics 2015-11-03 Andrew P. White

The Compact Linear Collider, CLIC, is a multi-TeV electron-positron collider proposed for construction at CERN. A detector model, CLICdet, that is suited for the experimental conditions at CLIC and is based on realistic performance, has…

High Energy Physics - Experiment · Physics 2019-09-30 Emilia Leogrande , Philipp Roloff , Ulrike Schnoor , Matthias Weber

Letter of intent describing SiD (Silicon Detector) for consideration by the International Linear Collider IDAG panel. This detector concept is founded on the use of silicon detectors for vertexing, tracking, and electromagnetic calorimetry.…

Instrumentation and Detectors · Physics 2009-11-03 H. Aihara , P. Burrows , M. Oreglia

Various proposals for a new $e^+ e^-$ collider operating below 1 TeV are now under consideration by the worlwide High Energy Physics community. Among these are the International Linear Collider and the Circular Electron Positron Collider.…

High Energy Physics - Phenomenology · Physics 2017-06-30 C. T. Potter

In the past 10 years, two design innovations, the introduction of low internal gain (LGAD) and of resistive read-out (RSD), have radically changed the performance of silicon detectors. The LGAD mechanism, increasing the signal-to-noise…

We first outline the Standard Model (SM) of particle physics, particle production and decay, and the expected signal and background at a Higgs factory like the International Linear Collider (ILC). We then introduce high energy colliders and…

High Energy Physics - Phenomenology · Physics 2020-05-12 C. T. Potter

In this work, we introduce a new design concept: the DC-Coupled Resistive Silicon Detectors, based on the LGAD technology. This new approach intends to address a few known features of the first generation of AC-Coupled Resistive Silicon…

SiD is a robust, silicon-based detector proposed for the International Linear Collider (ILC). SiD employs a sampling silicon-tungsten electromagnetic calorimeter (ECal) to accurately measure the energies of electrons, positrons, and photons…

Instrumentation and Detectors · Physics 2020-02-17 Lucas Braun , Jason T. Barkeloo , James E. Brau , Christopher T. Potter

For the International Large Detector (ILD) at the planned International Linear Collider (ILC) a Time Projection Chamber (TPC) is foreseen as the main tracking detector. To achieve the required point resolution, Micro Pattern Gaseous…

Instrumentation and Detectors · Physics 2019-02-15 Uli Einhaus , Uwe Krämer , Paul Malek

The long slab is a new prototype for the SiW-Ecal, a silicon tungsten electromagnetic calorimeter for the ILD detector of the future International Linear Collider. This new prototype has been designed to demonstrate the ability to build a…

The International Large Detector (ILD) is a concept for a detector at the International Linear Collider, ILC. The ILC will collide electrons and positrons at energies of initially 500 GeV, upgradeable to 1 TeV. The ILC has an ambitious…

High Energy Physics - Experiment · Physics 2012-08-27 The ILD Concept Group

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 correct modeling of $e^+e^-$ collision events at the International Linear Collider (ILC), as well as the response of a collider detector like the Silicon Detector (SiD), is crucial to evaluating the expected sensitivity to key…

High Energy Physics - Phenomenology · Physics 2021-08-23 Chris Potter

The performance of a double sided silicon strip detector (DSSSD), used for position and energy detection of heavy ions, is reported. The analysis shows that the incomplete charge collection (ICC) and charge sharing (CS) effects of the DSSSD…

Instrumentation and Detectors · Physics 2015-06-16 J L Han , J B Ma , X G Cao , Q Wang , J S Wang , Y Y Yang , P Ma , M R Huang , S L Jin , X J Rong , Z Bai , F Fu , Q Hu , R F Chen , S W Xu , J B Chen , L Jin , Y Li , M H Zhao , H S Xu

The SiD concept is one of two proposed detectors to be mounted at the interaction region of the International Linear Collider (ILC). A substantial ILC background arises from low transverse momentum $\mathrm{e}^{+}\mathrm{e}^{-}$ pairs…

Instrumentation and Detectors · Physics 2016-09-27 Timothy Barklow , Luc d`Hautuille , Christopher Milke , Bruce Schumm , Anne Schütz , Marcel Stanitzki , Jan Strube

The R&D Collaboration SiLC (Silicon tracking for Linear Colliders) is based on generic R&D aiming to develop the next generation of large Silicon tracking systems for the Linear collider experiments; it serves all three ILC detector…

Instrumentation and Detectors · Physics 2009-03-26 Aurore Savoy-Navarro

The ILD detector is proposed for an electron-positron collider with collision centre-of-mass energies from 90~\GeV~to about 1~\TeV. It has been developed over the last 10 years by an international team of scientists with the goal to design…

Instrumentation and Detectors · Physics 2020-03-04 The ILD Collaboration

The SiD detector concept is one of two currently accepted approaches to providing a detector for the future International Linear Collider. The SiD design philosophy is described and an overview of the concept given. Each major component of…

Instrumentation and Detectors · Physics 2010-06-18 Andrew P. White

The International Large Detector, ILD, is a detector concept which has been developed for the electron-positron collider ILC. The detector has been optimized for precision physics in a range of energies between 90 GeV and 1 TeV. ILD…

Instrumentation and Detectors · Physics 2019-12-11 The ILD Collaboration , contact Ties Behnke
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