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Monolithic active pixel sensors (MAPS) produced in a 65 nm CMOS imaging technology are being investigated for applications in particle physics. The MAPS design has a small collection electrode characterized by an input capacitance of ~fF,…

In order to achieve the challenging requirements on the CLIC vertex detector, a range of technology options have been considered in recent years. One prominent idea is the use of active sensors implemented in a commercial high-voltage CMOS…

Detectors at future e+e- collider need special calorimeters in the very forward region for a fast estimate and precise measurement of the luminosity, to improve the hermeticity and mask the central tracking detectors from backscattered…

Instrumentation and Detectors · Physics 2012-02-01 Ivanka Bozovic-Jelisavcic

The first Resistive Plate Chambers detectors were developed for cosmic ray experiments, where low rate capability, good time resolution and low cost per unit of area were needed. These same features, except for the low rate capability, were…

Instrumentation and Detectors · Physics 2020-01-29 R. Cardarelli , G. Aielli , E. Alunno Camelia , S. Bruno , A. Caltabiano , P. Camarri , A. Di Ciaccio , B. Liberti , L. Massa , L. Pizzimento , A. Rocchi

To detect tracks of charged particles close to the interaction point in high energy physics experiments of the next generation colliders, hybrid pixel detectors, in which sensor and read-out IC are separate entities, constitute the present…

Instrumentation and Detectors · Physics 2010-01-22 N. Wermes

Hybrid pixel detectors have been invented for the LHC to make tracking and vertexing possible at all in LHC's radiation intense environment. The LHC pixel detectors have meanwhile very successfully fulfilled their promises and R\&D for the…

Instrumentation and Detectors · Physics 2016-01-06 Norbert Wermes

Owing to their intrinsic (geometry dependent) radiation hardness, 3D pixel sensors are promising candidates for the innermost tracking layers of the forthcoming experiment upgrades at the Phase 2 High-Luminosity LHC (HL-LHC). To this…

Instrumentation and Detectors · Physics 2017-02-01 DMS Sultan , Gian-Franco Dalla Betta , Roberto Mendicino , Maurizio Boscardin , Sabina Ronchin , Nicola Zorzi

A new pixel detector for the CMS experiment is being built, owing to the instantaneous luminosities anticipated for the Phase I Upgrade of the LHC. The new CMS pixel detector provides four-hit tracking while featuring a significantly…

Instrumentation and Detectors · Physics 2016-12-23 Simon Spannagel

An R&D program on monolithic CMOS pixel sensors for application at the ILC has been started at LBNL. This program profits of significant synergies with other R&D activities on CMOS pixel sensors. The project activities after the first…

Instrumentation and Detectors · Physics 2010-01-05 M. Battaglia , G. Abrams , P. Denes , L. C. Greiner , B. Hooberman , L. Tompkins , H. H. Wieman

Pixelated silicon detectors are state-of-the-art technology to achieve precise tracking and vertexing at collider experiments, designed to accurately measure the hit position of incoming particles in high rate and radiation environments.…

Instrumentation and Detectors · Physics 2021-12-08 I. Zoi , A. Ebrahimi , F. Feindt , E. Garutti , P. Gunnellini , A. Hinzmann , C. Niemeyer , D. Pitzl , J. Schwandt , G. Steinbrück

The International Linear Collider (ILC) is a project of an electron-positron (e+e-) linear collider with the centre-of-mass energy of 200-500 GeV. Monolithic Active Pixel Sensors (MAPS) are one of the proposed silicon pixel detector…

Instrumentation and Detectors · Physics 2010-05-21 Lukasz Maczewski

Following in the footsteps of the LHC, the Future Circular Collider (FCC) plans to be the next multi-generational collider project. In the first stage, FCC-ee will collide intense beams of electrons and positrons at centre of mass energies…

High Energy Physics - Experiment · Physics 2025-07-03 Armin Ilg , Anna Macchiolo , Fabrizio Palla

Visible light communication (VLC) could provide short-range optical wireless communication together with illumination using LED lighting. However, conventional forward error correction (FEC) codes for reliable communication do not have the…

Information Theory · Computer Science 2018-10-18 Junbin Fang , Zhen Che , Xiaolong Yu , Zhe Chen , Zoe L. Jiang , Siu-Ming Yiu , Kui Ren , Xiaoqing Tan

The Large Hadron Collider (LHC) experiments ATLAS and CMS have established hybrid pixel detectors as the instrument of choice for particle tracking and vertexing in high rate and radiation environments, as they operate close to the LHC…

Instrumentation and Detectors · Physics 2018-06-27 Maurice Garcia-Sciveres , Norbert Wermes

A detector concept, named IDEA, optimized for the physics and running conditions at the FCC-ee is presented. After discussing the expected running conditions and the main physics drivers, a detailed description of the individual…

Instrumentation and Detectors · Physics 2025-03-31 The IDEA Study Group

The development of an innovative position sensitive pixelated sensor to detect and measure with high precision the coordinates of the ionizing particles is proposed. The silicon avalanche pixel sensors (APiX) is based on the vertical…

Instrumentation and Detectors · Physics 2015-06-18 N. D'Ascenzo , P. S. Marrocchesi , C. S. Moon , F. Morsani , L. Ratti , V. Saveliev , A. Savoy Navarro , Q. Xie

Modern precise radial velocity spectrometers are designed to infer the existence of planets orbiting other stars by measuring few-nm shifts in the positions of stellar spectral lines recorded at high spectral resolution on a large-area…

Instrumentation and Methods for Astrophysics · Physics 2019-09-24 Cullen H. Blake , Dan Li , Joseph R. Tufts , Joe Ninan , Suvrath Mahadevan , Chad Bender , Fred R. Hearty , Andy Monson , Mark Giovinazzi

Swift, high resolution CMOS pixel sensors are being developed for the ILC vertex detector, aiming to allow approaching the interaction point very closely. A major issue is the time resolution of the sensors needed to deal with the high…

This document illustrates the technical layout and the expected performance of the Micro Vertex Detector (MVD) of the PANDA experiment. The MVD will detect charged particles as close as possible to the interaction zone. Design criteria and…

Instrumentation and Detectors · Physics 2012-08-13 PANDA Collaboration , W. Erni , I. Keshelashvili , B. Krusche , M. Steinacher , Y. Heng , Z. Liu , H. Liu , X. Shen , Q. Wang , H. Xu , M. Albrecht , J. Becker , K. Eickel , F. Feldbauer , M. Fink , P. Friedel , F. H. Heinsius , T. Held , H. Koch , B. Kopf , M. Leyhe , C. Motzko , M. Pelizäus , J. Pychy , B. Roth , T. Schröder , J. Schulze , M. Steinke , T. Trifterer , U. Wiedner , J. Zhong , R. Beck , M. Becker , S. Bianco , K. -Th. Brinkmann , C. Hammann , F. Hinterberger , R. Jäkel , D. Kaiser , R. Kliemt , K. Koop , C. Schmidt , R. Schnell , U. Thoma , P. Vlasov , C. Wendel , A. Winnebeck , Th. Würschig , H. -G. Zaunick , A. Bianconi , M. Bragadireanu , M. Caprini , M. Ciubancan , D. Pantea , P. -D Tarta , M. De Napoli , F. Giacoppo , E. Rapisarda , C. Sfienti , T. Fiutowski , N. Idzik , B. Mindur , D. Przyborowski , K. Swientek , E. Bialkowski , A. Budzanowski , B. Czech , S. Kliczewski , A. Kozela , P. Kulessa , P. Lebiedowicz , K. Malgorzata , K. Pysz , W. Schäfer , R. Siudak , A. Szczurek , P. Brandys , T. Czyzewski , W. Czyzycki , M. Domagala , M. Hawryluk , G. Filo , D. Kwiatkowski , E. Lisowski , F. Lisowski , W. Bardan , D. Gil , B. Kamys , St. Kistryn , K. Korcyl , W. Krzemieñ , A. Magiera , P. Moskal , Z. Rudy , P. Salabura , J. Smyrski , A. Wroñska , M. Al-Turany , R. Arora , I. Augustin , H. Deppe , D. Dutta , H. Flemming , K. Götzen , G. Hohler , R. Karabowicz , D. Lehmann , B. Lewandowski , J. Lühning , F. Maas , H. Orth , K. Peters , T. Saito , G. Schepers , C. J. Schmidt , L. Schmitt , C. Schwarz , J. Schwiening , B. Voss , P. Wieczorek , A. Wilms , V. M. Abazov , G. D. Alexeev , V. A. Arefiev , V. I. Astakhov , M. Yu. Barabanov , B. V. Batyunya , Yu. I. Davydov , V. Kh. Dodokhov , A. A. Efremov , A. G. Fedunov , A. A. Feshchenko , A. S. Galoyan , S. Grigoryan , A. Karmokov , E. K. Koshurnikov , V. I. Lobanov , Yu. Yu. Lobanov , A. F. Makarov , L. V. Malinina , V. L. Malyshev , G. A. Mustafaev , A. G. Olshevski , M. A. Pasyuk , E. A. Perevalova , A. A. Piskun , T. A. Pocheptsov , G. Pontecorvo , V. K. Rodionov , Yu. N. Rogov , R. A. Salmin , A. G. Samartsev , M. G. Sapozhnikov , G. S. Shabratova , A. N. Skachkova , N. B. Skachkov , E. A. Strokovsky , M. K. Suleimanov , R. Sh. Teshev , V. V. Tokmenin , V. V. Uzhinsky , A. S. Vodopyanov , S. A. Zaporozhets , N. I. Zhuravlev , A. G. Zorin , D. Branford , D. Glazier , D. Watts , P. Woods , A. Britting , W. Eyrich , A. Lehmann , F. Uhlig , S. Dobbs , Z. Metreveli , K. Seth , B. Tann , A. Tomaradze , D. Bettoni , V. Carassiti , P. Dalpiaz , A. Drago , E. Fioravanti , I. Garzia , M. Negrini , M. Savriè , G. Stancari , B. Dulach , P. Gianotti , C. Guaraldo , V. Lucherini , E. Pace , A. Bersani , M. Macri , M. Marinelli , R. F. Parodi , V. Dormenev , P. Drexler , M. Düren , T. Eisner , K. Foehl , A. Hayrapetyan , P. Koch , B. Krïoch , W. Kühn , S. Lange , Y. Liang , M. Liu , O. Merle , V. Metag , M. Moritz , M. Nanova , R. Novotny , B. Spruck , H. Stenzel , C. Strackbein , M. Thiel , Q. Wang , T. Clarkson , C. Euan , G. Hill , M. Hoek , D. Ireland , R. Kaiser , T. Keri , I. Lehmann , K. Livingston , P. Lumsden , D. MacGregor , B. McKinnon , R. Montgomery , M. Murray , D. Protopopescu , G. Rosner , B. Seitz , G. Yang , M. Babai , A. K. Biegun , A. Glazenborg-Kluttig , E. Guliyev , V. S. Jothi , M. Kavatsyuk , P. Lemmens , H. Löhner , J. Messchendorp , T. Poelman , H. Smit , J. C. van der Weele , H. Sohlbach , M. Büscher , R. Dosdall , R. Dzhygadlo , S. Esch , A. Gillitzer , F. Goldenbaum , D. Grunwald , V. Jha , G. Kemmerling , H. Kleines , A. Lehrach , R. Maier , M. Mertens , H. Ohm , D. L. Pohl , D. Prasuhn , T. Randriamalala , J. Ritman , M. Roeder , G. Sterzenbach , T. Stockmanns , P. Wintz , P. Wüstner , H. Xu , J. Kisiel , S. Li , Z. Li , Z. Sun , H. Xu , K. Fissum , K. Hansen , L. Isaksson , M. Lundin , B. Schröder , P. Achenbach , A. Denig , M. Distler , M. Fritsch , D. Kangh , A. Karavdina , W. Lauth , M. Michel , M. C. Mora Espi , J. Pochodzalla , S. Sanchez , A. Sanchez-Lorente , C. Sfienti , T. Weber , V. I. Dormenev , A. A. Fedorov , M. V. Korzhik , O. V. Missevitch , V. Balanutsa , V. Chernetsky , A. Demekhin , A. Dolgolenko , P. Fedorets , A. Gerasimov , V. Goryachev , A. Boukharov , O. Malyshev , I. Marishev , A. Semenov , R. Varma , B. Ketzer , I. Konorov , A. Mann , S. Neubert , S. Paul , M. Vandenbroucke , Q. Zhang , A. Khoukaz , T. Rausmann , A. Täschner , J. Wessels , E. Baldin , K. Kotov , S. Peleganchuk , Yu. Tikhonov , T. Hennino , M. Imre , R. Kunne , C. Le Galliard , J. P. Le Normand , D. Marchand , A. Maroni , S. Ong , J. Pouthas , B. Ramstein , P. Rosier , M. Sudol , C. Theneau , E. Tomasi-Gustafsson , J. Van de Wiele , T. Zerguerras , G. Boca , A. Braghieri , S. Costanza , A. Fontana , P. Genova , L. Lavezzi , P. Montagna , A. Rotondi , V. Buda , V. V. Abramov , A. M. Davidenko , A. A. Derevschikov , Y. M. Goncharenko , V. N. Grishin , V. A. Kachanov , D. A. Konstantinov , V. A. Kormilitsin , Y. A. Matulenko , Y. M. Melnik , A. P. Meschanin , N. G. Minaev , V. V. Mochalov , D. A. Morozov , L. V. Nogach , S. B. Nurushev , A. V. Ryazantsev , P. A. Semenov , L. F. Soloviev , A. V. Uzunian , A. N. Vasiliev , A. E. Yakutin , S. Belostotski , G. Gavrilov , A. Itzotov , A. Kisselev , P. Kravchenko , S. Manaenkov , O. Miklukho , Y. Naryshkin , D. Veretennikov , V. Vikhrov , A. Zhadanov , T. Bäck , B. Cederwall , C. Bargholtz , L. Gerén , P. E. Tegnér , P. Thørngren , K. M. von Würtemberg , L. Fava , D. Alberto , A. Amoroso , M. P. Bussa , L. Busso , F. De Mori , M. Destefanis , L. Ferrero , M. Greco , T. Kugathasan , M. Maggiora , S. Marcello , S. Sosio , S. Spataro , D. Calvo , S. Coli , P. De Remigis , A. Filippi , G. Giraudo , S. Lusso , G. Mazza , M. Mignone , A. Rivetti , R. Wheadon , L. Zotti , O. Morra , F. Iazzi , A. Lavagno , P. Quarati , K. Szymanska , R. Birsa , F. Bradamante , A. Bressan , A. Martin , H. Clement , B. Galnander , H. Calén , K. Fransson , T. Johansson , A. Kupsc , P. Marciniewski , E. Thomé , M. Wolke , J. Zlomanczuk , J. Díaz , A. Ortiz , P. Buda , K. Dmowski , R. Korzeniewski , D. Przemyslaw , B. Slowinski , S. Borsuk , A. Chlopik , Z. Guzik , J. Kopec , T. Kozlowski , D. Melnychuk , M. Plominski , J. Szewinski , K. Traczyk , B. Zwieglinski , P. Bühler , A. Gruber , P. Kienle , J. Marton , E. Widmann , J. Zmeskal

The electron-positron stage of the Future Circular Collider (FCC-ee) provides exciting opportunities that are enabled by next generation particle physics detectors. This contribution presents IDEA, a detector concept optimised for FCC-ee…

Instrumentation and Detectors · Physics 2026-04-30 Armin Ilg
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