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Related papers: The TESLA Detector

200 papers

The status of the design of a detector for the TESLA collider is presented.

High Energy Physics - Experiment · Physics 2007-05-23 P. N. Burrows

As next generation e+e- linear collider the superconducting accelerator project TESLA has been proposed. In this note the physics potential goals of this project, which is highly complementary to LHC, are described.

High Energy Physics - Experiment · Physics 2015-06-25 Klaus Moenig

The physics at a 500-800 GeV electron positron linear collider, TESLA, is reviewed. The machine parameters that impact directly on the physics are discussed and a few key performance goals for a detector at TESLA are given. Emphasis is…

High Energy Physics - Experiment · Physics 2017-08-23 Grahame A. Blair

TESLA is designed as an electron-positron linear collider (LC) based on super-conducting technology. A second interaction region is forseen to be incorporated in the design allowing its possible operation as a photon collider. In this paper…

High Energy Physics - Experiment · Physics 2011-09-13 Aura Rosca

Extending the sensitivity to New Physics beyond the anticipated reach of the LHC is a prime aim of future colliders. This paper summarises the potential of an e+e- linear collider, at and beyond 1 TeV, using a realistic simulation of the…

High Energy Physics - Phenomenology · Physics 2009-09-25 M. Battaglia , S. De Curtis , D. Dominici , S. Riemann

A large Time Projection Chamber is proposed as part of the tracking system for a detector at the TESLA electron positron linear collider. Different ongoing R&D studies are reviewed, stressing progress made on a new type readout technique…

High Energy Physics - Experiment · Physics 2009-11-07 Nabil Ghodbane

The proposed linear electron-positron collider TESLA is based on 1.3 GHz superconducting niobium cavities for particle acceleration. For a centre-of-mass energy of 500 GeV, an accelerating field of 23.4 MV/m is required which is reliably…

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

In order to fully exploit the physics potential of a e+e- linear collider, such as TESLA, a Vertex Tracker providing high resolution track reconstruction is required. Hybrid Silicon pixel sensors are an attractive sensor technology option…

High Energy Physics - Experiment · Physics 2007-05-23 M. Battaglia , M. Caccia , S. Borghi , R. Campagnolo , K. Domanski , P. Grabiec , B. Jaroszewicz , J. Marczewski , D. Tomaszewski , W. Kucewicz , A. Zalewska , K. Tammi

We describe a study of high-energy Compton beam polarimeters for the future e+e- linear collider machine TESLA. A segment of the beam delivery system has been identified, which is aligned with the e+e- collision axis and which has a…

High Energy Physics - Experiment · Physics 2007-05-23 V. Gharibyan , N. Meyners , K. P. Schuler

We discuss the physics motivations for building a 500 - 1 TeV electron-positron linear collider. The state of the art collider technologies and the physics-driven machine parameters are discussed. A survey of some of the phenomena well…

High Energy Physics - Phenomenology · Physics 2009-11-10 Sally Dawson , Mark Oreglia

We discuss the new layout of a cavity chain (superstructure) allowing, we hope, significant cost reduction of the RF system of both linacs of the TESLA linear collider. The proposed scheme increases the fill factor and thus makes an…

Accelerator Physics · Physics 2009-10-31 J. Sekutowicz , M. Ferrario , C. Tang

This article summarises the physics at future linear colliders. It will be shown that in all studied physics scenarios a 1 TeV linear collider in addition to the LHC will enhance our knowledge significantly and helps to reconstruct the…

High Energy Physics - Phenomenology · Physics 2011-02-09 Klaus Moenig

In order to fully exploit the physics potential of a future high energy e+e- linear collider, a Vertex Tracker, providing high resolution track reconstruction, is required. Hybrid Silicon pixel sensors are an attractive option, for the…

High Energy Physics - Experiment · Physics 2009-10-31 M. Battaglia , R. Orava , K. Tammi , K. Osterberg , W. Kucewicz , A. Zalewska , M. Caccia , R. Campagnolo , C. Meroni , P. Grabiec , B. Jaroszewicz , J. Marczewski

The Large Hadron Electron Collider (LHeC) is a proposed upgrade to the LHC, to provide high energy, high luminosity electron-proton collisions to run concurrently with Phase 2 of the LHC. The baseline design of a detector for the LHeC is…

Accelerator Physics · Physics 2013-10-10 Peter Kostka , Alessandro Polini , David M. South

DEPFET pixel detectors are unique devices in terms of energy and spatial resolution because very low noise (ENC = 2.2e at room temperature) operation can be obtained by implementing the amplifying transistor in the pixel cell itself. Full…

A new cavity-chain layout has been proposed for the main linac of the TESLA linear collider. This superstructure-layout is based upon four 7-cell superconducting standing-wave cavities, coupled by short beam pipes. The main advantages of…

Accelerator Physics · Physics 2007-05-23 N. Baboi , M. Ferrario , M. Liepe , J. Sekutowicz

New facilities for particle and nuclear physics research, which will be available due to constructing the TESLA linear electron-positron collider tangentially to the HERA proton ring, are discussed.

High Energy Physics - Experiment · Physics 2007-05-23 O. Yavas , A. K. Ciftci , S. Sultansoy

The general features of the Moller scattering and its use as an electron polarimeter are described and studied in view of the planned future high energy e^+e^- linear colliders. In particular the study concentrates on the TESLA collider…

High Energy Physics - Experiment · Physics 2015-06-25 Gideon Alexander , Iuliana Cohen

The relative merits and disadvantages of various alternatives for vertexing and central tracking detectors for the Linear Collider detector are presented. Research and development prospects for the various alternatives are also discussed,…

High Energy Physics - Experiment · Physics 2007-05-23 B. A. Schumm
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