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The Electron-Ion Collider (EIC) will be the next frontier project of nuclear physics in the United States. It is planned to be built in the Brookhaven National Laboratory (BNL) in close collaboration with Jefferson Lab. One of the key…

Instrumentation and Detectors · Physics 2022-02-15 Greg Kalicy

The International Linear Collider (ILC) will collide polarised electrons and positrons at beam energies of 45.6 GeV to 250 GeV and optionally up to 500 GeV. To fully exploit the physics potential of this machine, not only the luminosity and…

Instrumentation and Detectors · Physics 2008-10-13 C. Helebrant , D. Käfer , J. List

The design of the positron source for the International Linear Collider (ILC) is still under discussion. The baseline design plans to use the high-energy electron beam for the positron production before it goes to the IP. The electrons pass…

Accelerator Physics · Physics 2020-02-26 Sabine Riemann , Peter Sievers , Gudrid Moortgat-Pick , Andriy Ushakov

This paper discusses recently proposed Higgs Energy LEptoN (HELEN) $e+e-$ linear collider based on advances in superconducting radio frequency technology. The collider offers cost and AC power savings, smaller footprint (relative to the…

We describe another detectora designed for the International Linear Collider based on several tested instrumentation innovations in order to achieve the necessary experi- mental goal of a detecter that is 2-to-10 times better than the…

The Compact Linear Collider (CLIC) was proposed as the next energy-frontier infrastructure at CERN, to study e$^+$e$^-$ collisions at three centre-of-mass energy stages: 380 GeV, 1.5 TeV and 3 TeV. The main goal of its high-energy stages is…

High Energy Physics - Experiment · Physics 2022-03-11 Jan Klamka

In the baseline design of the International Linear Collider (ILC) an undulator-based source is foreseen for the positron source in order to match the physics requirements. The baseline parameters are optimized for the ILC at sqrt(s)=500…

Accelerator Physics · Physics 2019-02-22 Manuel Formela , Gudrid Moortgat-Pick , Sabine Riemann , Andriy Ushakov

Besides continued work on the parameters of a 3-4 and 0.5 TeV CoM collider, many studies are now concentrating on a machine near 100 GeV that could be a factory for the s-channel production of Higgs particles. We mention the research on the…

Accelerator Physics · Physics 2007-05-23 R. Palmer , A. Sessler , A. Tollestrup , J. Gallardo

This paper begins with a summary of the status of the Large Hadron Collider at CERN, including the lead-ion injector chain and the plans for the first phases of commissioning and operation with colliding proton beams. In a later phase, the…

Nuclear Experiment · Physics 2011-09-02 John M. Jowett

It is widely accepted that the next lepton collider beyond a Higgs factory would require center-of-mass energy of the order of up to 15 TeV. Since, given reasonable space and cost restrictions, conventional accelerator technology reaches…

For the superconducting linear collider TESLA a multi purpose detector has been designed. This detector is optimised for the important physics processes expected at a next generation linear collider up to around 1 TeV and is designed for…

High Energy Physics - Experiment · Physics 2007-05-23 Klaus Moenig

A highly granular silicon-tungsten electromagnetic calorimeter (SiW-ECAL) is the reference design of the ECAL for International Large Detector (ILD) concept, one of the two detector concepts for the detector(s) at the future International…

Instrumentation and Detectors · Physics 2020-04-28 Adrian Irles

This contribution to LCWS2016 presents recent developments within the CLICdp collaboration. An updated scenario for the staged operation of CLIC has been published; the accelerator will operate at 380 GeV, 1.5 TeV and 3 TeV. The lowest…

Instrumentation and Detectors · Physics 2019-08-13 Naomi van der Kolk

In this Technical Design Report (TDR) we describe the SuperB detector that was to be installed on the SuperB e+e- high luminosity collider. The SuperB asymmetric collider, which was to be constructed on the Tor Vergata campus near the INFN…

Instrumentation and Detectors · Physics 2013-06-25 SuperB Collaboration , M. Baszczyk , P. Dorosz , J. Kolodziej , W. Kucewicz , M. Sapor , A. Jeremie , E. Grauges Pous , G. E. Bruno , G. De Robertis , D. Diacono , G. Donvito , P. Fusco , F. Gargano , F. Giordano , F. Loddo , F. Loparco , G. P. Maggi , V. Manzari , M. N. Mazziotta , E. Nappi , A. Palano , B. Santeramo , I. Sgura , L. Silvestris , V. Spinoso , G. Eigen , J. Zalieckas , Z. Zhuo , L. Jenkovszky , G. Balbi , M. Boldini , D. Bonacorsi , V. Cafaro , I. D'Antone , G. M. Dallavalle , R. Di Sipio , F. Fabbri , L. Fabbri , A. Gabrielli , D. Galli , P. Giacomelli , V. Giordano , F. M. Giorgi , C. Grandi , I. Lax , S. Lo Meo , U. Marconi , A. Montanari , G. Pellegrini , M. Piccinini , T. Rovelli , N. Semprini Cesari , G. Torromeo , N. Tosi , R. Travaglini , V. M. Vagnoni , S. Valentinetti , M. Villa , A. Zoccoli , J. -F. Caron , C. Hearty , P. F. -T. Lu , T. S. Mattison , J. A. McKenna , R. Y. -C. So , M. Yu. Barnyakov , V. E. Blinov , A. A. Botov , V. P. Druzhinin , V. B. Golubev , S. A. Kononov , E. A. Kravchenko , E. B. Levichev , A. P. Onuchin , S. I. Serednyakov , D. A. Shtol , Y. I. Skovpen , E. P. Solodov , A. Cardini , M. Carpinelli , D. S. -T. Chao , C. H. Cheng , D. A. Doll , B. Echenard , K. Flood , J. Hanson , D. G. Hitlin , P. Ongmongkolkul , F. C. Porter , R. Y. Zhu , N. Randazzo , E. De La Cruz Burelo , Y. Zheng , P. Campos , M. De Silva , A. Kathirgamaraju , B. Meadows , B. Pushpawela , Y. Shi , M. Sokoloff , G. Lopez Castro , V. Ciaschini , P. Franchini , F. Giacomini , A. Paolini , G. A. Calderon Polania , S. Laczek , P. Romanowicz , B. Szybinski , M. Czuchry , L. Flis , D. Harezlak , J. Kocot , M. Radecki , M. Sterzel , T. Szepieniec , T. Szymocha , P. Wójcik , M. Andreotti , W. Baldini , R. Calabrese , V. Carassiti , G. Cibinetto , A. Cotta Ramusino , F. Evangelisti , A. Gianoli , E. Luppi , R. Malaguti , M. Manzali , M. Melchiorri , M. Munerato , C. Padoan , V. Santoro , L. Tomassetti , M. M. Beretta , M. Biagini , M. Boscolo , E. Capitolo , R. de Sangro , M. Esposito , G. Felici , G. Finocchiaro , M. Gatta , C. Gatti , S. Guiducci , S. Lauciani , P. Patteri , I. Peruzzi , M. Piccolo , P. Raimondi , M. Rama , C. Sanelli , S. Tomassini , P. Fabbricatore , D. Delepine , M. A. Reyes Santos , M. Chrzaszcz , R. Grzymkowski , P. Knap , J. Kotula , T. Lesiak , J. Ludwin , J. Michalowski , B. Pawlik , B. Rachwal , M. Stodulski , J. Wiechczynski , M. Witek , L. Zawiejski , M. Zdybal , V. Y. Aushev , A. Ustynov , N. Arnaud , P. Bambade , C. Beigbeder , F. Bogard , M. Borsato , D. Breton , J. Brossard , L. Burmistrov , D. Charlet , V. Chaumat , O. Dadoun , M. El Berni , J. Maalmi , V. Puill , C. Rimbault , A. Stocchi , V. Tocut , A. Variola , S. Wallon , G. Wormser , F. Grancagnolo , E. Ben-Haim , S. Sitt , M. Baylac , O. Bourrion , J. -M. Deconto , Y. Gomez Martinez , N. Monseu , J. -F. Muraz , J. -S. Real , C. Vescovi , R. Cenci , A. Jawahery , D. Roberts , E. W. Twedt , R. Cheaib , D. Lindemann , S. Nderitu , P. Patel , S. H. Robertson , D. Swersky , A. Warburton , E. Cuautle Flores , G. Toledo Sanchez , P. Biassoni , L. Bombelli , M. Citterio , S. Coelli , C. Fiorini , V. Liberali , M. Monti , B. Nasri , N. Neri , F. Palombo , F. Sabatini , A. Stabile , A. Berra , A. Giachero , C. Gotti , D. Lietti , M. Maino , G. Pessina , M. Prest , J. -P. Martin , M. Simard , N. Starinski , P. Taras , A. Drutskoy , S. Makarychev , A. V. Nefediev , A. Aloisio , S. Cavaliere , G. De Nardo , M. Della Pietra , A. Doria , R. Giordano , A. Ordine , S. Pardi , G. Russo , C. Sciacca , I. I. Bigi , C. P. Jessop , W. Wang , M. Bellato , M. Benettoni , M. Corvo , A. Crescente , F. Dal Corso , U. Dosselli , C. Fanin , A. Gianelle , S. Longo , M. Michelotto , F. Montecassiano , M. Morandin , R. Pengo , M. Posocco , M. Rotondo , G. Simi , R. Stroili , L. Gaioni , A. Manazza , M. Manghisoni , L. Ratti , V. Re , G. Traversi , S. Zucca , S. Bizzaglia , M. Bizzarri , C. Cecchi , S. Germani , M. Lebeau , P. Lubrano , E. Manoni , A. Papi , A. Rossi , G. Scolieri , G. Batignani , S. Bettarini , G. Casarosa , A. Cervelli , A. Fella , F. Forti , M. Giorgi , L. Lilli , A. Lusiani , B. Oberhof , A. Paladino , F. Pantaleo , E. Paoloni , A. L. Perez Perez , G. Rizzo , J. Walsh , A. Fernández Téllez , G. Beck , M. Berman , A. Bevan , F. Gannaway , G. Inguglia , A. J. Martin , J. Morris , V. Bocci , M. Capodiferro , G. Chiodi , I. Dafinei , N. V. Drenska , R. Faccini , F. Ferroni , C. Gargiulo , P. Gauzzi , C. Luci , R. Lunadei , G. Martellotti , F. Pellegrino , V. Pettinacci , D. Pinci , L. Recchia , D. Ruggeri , A. Zullo , P. Camarri , R. Cardarelli , C. De Santis , A. Di Ciaccio , V. Di Felice , F. Di Palma , A. Di Simone , L. Marcelli , R. Messi , D. Moricciani , R. Sparvoli , S. Tammaro , P. Branchini , A. Budano , S. Bussino , M. Ciuchini , F. Nguyen , A. Passeri , F. Ruggieri , E. Spiriti , F. Wilson , I. Leon Monzon , J. R. Millan-Almaraz , P. L. M. Podesta-Lerma , D. Aston , B. Dey , A. Fisher , P. D. Jackson , D. W. G. S. Leith , S. Luitz , D. MacFarlane , M. McCulloch , S. Metcalfe , A. Novokhatski , S. Osier , R. Prepost , B. Ratcliff , J. Seeman , M. Sullivan , J. Va'vra , U. Wienands , W. Wisniewski , B. D. Altschul , M. V. Purohit , J. Baudot , I. Ripp-Baudot , G. A. P. Cirrone , G. Cuttone , O. Bezshyyko , G. Dolinska , A. Soffer , F. Bianchi , F. De Mori , A. Filippi , D. Gamba , S. Marcello , M. Bomben , L. Bosisio , P. Cristaudo , L. Lanceri , B. Liberti , I. Rashevskaya , C. Stella , E. S. Vallazza , L. Vitale , G. Auriemma , C. Satriano , F. Martinez Vidal , J. Mazorra de Cos , A. Oyanguren , P. Ruiz Valls , A. Beaulieu , S. Dejong , J. Franta , M. J. Lewczuk , M. Roney , R. Sobie

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

A possible solution to realize a conventional positron source driven by a several-GeV electron beam for the International Linear Collider is proposed. A 300 Hz electron linac is employed to create positrons with stretching pulse length in…

The Compact Linear Collider (CLIC) is a concept for a future linear collider that would provide e$^+$e$^-$ collisions at up to 3 TeV. The physics aims require a detector system with excellent jet energy and track momentum resolution, highly…

Instrumentation and Detectors · Physics 2018-03-05 Florian Pitters

The physics potential of the Circular Electron Positron Collider (CEPC) can be significantly strengthened by two detectors with complementary designs. A promising detector approach based on the Silicon Detector (SiD) designed for the…

Instrumentation and Detectors · Physics 2016-12-21 S. V. Chekanov , M. Demarteau

The proposed high-luminosity high-energy Electron-Ion Collider (EIC) will provide a clean environment to precisely study several fundamental questions in the fields of high-energy and nuclear physics . A low material budget and high…

We describe the physics potential of $e^+e^-$ linear colliders in this report. These machines are planned to operate in the first phase at a center-of --mass energy of 500 GeV, before being scaled up to about 1 TeV. In the second phase of…

High Energy Physics - Phenomenology · Physics 2009-09-25 E. Accomando