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In view of the LHC upgrade phases towards the High Luminosity LHC (HL-LHC), the ATLAS experiment plans to upgrade the Inner Detector with an all-silicon system. Because of its radiation hardness and cost effectiveness, the n-on-p silicon…

Instrumentation and Detectors · Physics 2015-06-17 M. Bomben , A. Bagolini , M. Boscardin , L. Bosisio , G. Calderini , J. Chauveau , G. Giacomini , A. La Rosa , G. Marchori , N. Zorzi

In view of the LHC upgrade phases towards HL-LHC, the ATLAS experiment plans to upgrade the Inner Detector with an all-silicon system. The n-on-p silicon technology is a promising candidate for the pixel upgrade thanks to its radiation…

Instrumentation and Detectors · Physics 2015-06-12 M. Bomben , A. Bagolini , M. Boscardin , L. Bosisio , G. Calderini , J. Chauveau , G. Giacomini , A. La Rosa , G. Marchori , N. Zorzi

The ATLAS experiment will undergo around the year 2025 a replacement of the tracker system in view of the high luminosity phase of the LHC (HL-LHC) with a new 5-layer pixel system. Thin planar pixel sensors are promising candidates to…

Instrumentation and Detectors · Physics 2017-02-01 Anna Macchiolo , Julien Beyer , Alessandro La Rosa , Richard Nisius , Natascha Savic

The ATLAS Inner Detector is a composite tracking system consisting of silicon pixels, silicon strips and straw tubes in a 2 T magnetic field. Its installation was completed in August 2008 and the detector took part in data- taking with…

Instrumentation and Detectors · Physics 2012-08-27 The ATLAS Collaboration

The LHC accelerator complex will be upgraded between 2020-2022, to the High-Luminosity-LHC, to considerably increase statistics for the various physics analyses. To operate under these challenging new conditions, and maintain excellent…

Instrumentation and Detectors · Physics 2015-04-09 C. Nellist , N. Dinu , E. Gkougkousis , A. Lounis

The ALICE ITS3 is a novel vertex detector replacing the innermost layers of ITS2 during LS3. Composed of three truly cylindrical layers of wafer-sized 65 nm stitched Monolithic Active Pixel Sensors, ITS3 provides high-resolution tracking of…

Instrumentation and Detectors · Physics 2024-02-27 Ola Groettvik

During the shutdown of the CERN Large Hadron Collider in 2013-2014, an additional pixel layer was installed between the existing Pixel detector of the ATLAS experiment and a new, smaller radius beam pipe. The motivation for this new pixel…

Instrumentation and Detectors · Physics 2018-06-07 B. Abbott , J. Albert , F. Alberti , M. Alex , G. Alimonti , S. Alkire , P. Allport , S. Altenheiner , L. Ancu , E. Anderssen , A. Andreani , A. Andreazza , B. Axen , J. Arguin , M. Backhaus , G. Balbi , J. Ballansat , M. Barbero , G. Barbier , A. Bassalat , R. Bates , P. Baudin , M. Battaglia , T. Beau , R. Beccherle , A. Bell , M. Benoit , A. Bermgan , C. Bertsche , D. Bertsche , J. Bilbao de Mendizabal , F. Bindi , M. Bomben , M. Borri , C. Bortolin , N. Bousson , R. Boyd , P. Breugnon , G. Bruni , J. Brossamer , M. Bruschi , P. Buchholz , E. Budun , C. Buttar , F. Cadoux , G. Calderini , L. Caminada , M. Capeans , R. Carney , G. Casse , A. Catinaccio , M. Cavalli-Sforza , M. Červ , A. Cervelli , C. Chau , J. Chauveau , S. Chen , M. Chu , M. Ciapetti , V. Cindro , M. Citterio , A. Clark , M. Cobal , S. Coelli , J. Collot , O. Crespo-Lopez , G. Dalla Betta , C. Daly , G. D'Amen , N. Dann , V. Dao , G. Darbo , C. DaVia , P. David , S. Debieux , P. Delebecque , F. De Lorenzi , R. de Oliveira , K. Dette , W. Dietsche , B. Di Girolamo , N. Dinu , F. Dittus , D. Diyakov , F. Djama , D. Dobos , P. Dondero , K. Doonan , J. Dopke , O. Dorholt , S. Dube , D. Dzahini , K. Egorov , O. Ehrmann , K. Einsweiler , S. Elles , M. Elsing , L. Eraud , A. Ereditato , A. Eyring , D. Falchieri , A. Falou , C. Fausten , A. Favareto , Y. Favre , S. Feigl , S. Fernandez Perez , D. Ferrere , J. Fleury , T. Flick , D. Forshaw , D. Fougeron , L. Franconi , A. Gabrielli , R. Gaglione , C. Gallrapp , K. Gan , M. Garcia-Sciveres , G. Gariano , T. Gastaldi , I. Gavrilenko , A. Gaudiello , N. Geffroy , C. Gemme , F. Gensolen , M. George , P. Ghislain , N. Giangiacomi , S. Gibson , M. Giordani , D. Giugni , H. Gjersdal , K. Glitza , D. Gnani , J. Godlewski , L. Gonella , S. Gonzalez-Sevilla , I. Gorelov , A. Gorišek , C. Gössling , S. Grancagnolo , H. Gray , I. Gregor , P. Grenier , S. Grinstein , A. Gris , V. Gromov , D. Grondin , J. Grosse-Knetter , F. Guescini , E. Guido , P. Gutierrez , G. Hallewell , N. Hartman , S. Hauck , J. Hasi , A. Hasib , F. Hegner , S. Heidbrink , T. Heim , B. Heinemann , T. Hemperek , N. Hessey , M. Hetmánek , R. Hinman , M. Hoeferkamp , T. Holmes , J. Hostachy , S. Hsu , F. Hügging , C. Husi , G. Iacobucci , I. Ibragimov , J. Idarraga , Y. Ikegami , T. Ince , R. Ishmukhametov , J. M. Izen , Z. Janoška , J. Janssen , L. Jansen , L. Jeanty , F. Jensen , J. Jentzsch , S. Jezequel , J. Joseph , H. Kagan , M. Kagan , M. Karagounis , R. Kass , A. Kastanas , C. Kenney , S. Kersten , P. Kind , M. Klein , R. Klingenberg , R. Kluit , M. Kocian , E. Koffeman , O. Korchak , I. Korolkov , I. Kostyukhina-Visoven , S. Kovalenko , M. Kretz , N. Krieger , H. Krüger , A. Kruth , A. Kugel , W. Kuykendall , A. La Rosa , C. Lai , K. Lantzsch , C. Lapoire , D. Laporte , T. Lari , S. Latorre , M. Leyton , B. Lindquist , K. Looper , I. Lopez , A. Lounis , Y. Lu , H. Lubatti , S. Maeland , A. Maier , U. Mallik , F. Manca , B. Mandelli , I. Mandić , D. Marchand , G. Marchiori , M. Marx , N. Massol , P. Mättig , J. Mayer , G. Mc Goldrick , A. Mekkaoui , M. Menouni , J. Menu , C. Meroni , J. Mesa , S. Michal , S. Miglioranzi , M. Mikuž , A. Miucci , K. Mochizuki , M. Monti , J. Moore , P. Morettini , A. Morley , J. Moss , D. Muenstermann , P. Murray , K. Nakamura , C. Nellist , D. Nelson , M. Nessi , R. Nisius , M. Nordberg , F. Nuiry , T. Obermann , W. Ockenfels , H. Oide , M. Oriunno , F. Ould-Saada , C. Padilla , P. Pangaud , S. Parker , G. Pelleriti , H. Pernegger , G. Piacquadio , A. Picazio , D. Pohl , A. Polini , X. Pons , J. Popule , X. Portell Bueso , K. Potamianos , M. Povoli , D. Puldon , Y. Pylypchenko , A. Quadt , B. Quayle , F. Rarbi , F. Ragusa , T. Rambure , E. Richards , C. Riegel , B. Ristic , F. Rivière , F. Rizatdinova , O. Røhne , C. Rossi , L. Rossi , A. Rovani , A. Rozanov , I. Rubinskiy , M. Rudolph , A. Rummler , E. Ruscino , F. Sabatini , D. Salek , A. Salzburger , H. Sandaker , M. Sannino , B. Sanny , T. Scanlon , J. Schipper , U. Schmidt , B. Schneider , A. Schorlemmer , N. Schroer , P. Schwemling , A. Sciuccati , S. Seidel , A. Seiden , P. Šícho , P. Skubic , M. Sloboda , D. Smith , M. Smith , A. Sood , E. Spencer , M. Stramaglia , M. Strauss , S. Stucci , B. Stugu , J. Stupak , N. Styles , D. Su , Y. Takubo , J. Tassan , P. Teng , A. Teixeira , S. Terzo , X. Therry , T. Todorov , M. Tomášek , K. Toms , R. Travaglini , W. Trischuk , C. Troncon , G. Troska , S. Tsiskaridze , I. Tsurin , D. Tsybychev , Y. Unno , L. Vacavant , B. Verlaat , E. Vigeolas , M. Vogt , V. Vrba , R. Vuillermet , W. Wagner , W. Walkowiak , R. Wang , S. Watts , M. Weber , M. Weber , J. Weingarten , S. Welch , S. Wenig , M. Wensing , N. Wermes , T. Wittig , M. Wittgen , T. Yildizkaya , Y. Yang , W. Yao , Y. Yi , A. Zaman , R. Zaidan , C. Zeitnitz , M. Ziolkowski , V. Zivkovic , A. Zoccoli , L. Zwalinski

Collider detectors have taken advantage of the resolution and accuracy of silicon detectors for at least four decades. Future colliders will need large areas of silicon sensors for low mass trackers and sampling calorimetry. Monolithic…

We have developed a new detector of photons and charged particles- a hole-type structure with electrodes made of a double layered resistive material: a thin low resistive layer coated with a layer having a much higher resistivity. One of…

Instrumentation and Detectors · Physics 2008-11-26 G. Charpak , P. Benaben , P. Breuil , A. Di Mauro , P. Martinengo , V. Peskov

Results of beam tests with planar silicon pixel sensors aimed towards the ATLAS Insertable B-Layer and High Luminosity LHC (HL-LHC) upgrades are presented. Measurements include spatial resolution, charge collection performance and charge…

Within the ATTRACT FASTPIX project, a monolithic pixel sensor demonstrator chip has been developed in a modified 180 nm CMOS imaging process technology, targeting sub-nanosecond timing precision for single ionising particles. It features a…

Deep sub micron HV-CMOS processes offer the opportunity for sensors built by industry standard techniques while being HV tolerant, making them good candidates for drift-based, fast collecting, thus radiation-hard pixel detectors. For the…

Instrumentation and Detectors · Physics 2016-09-21 Branislav Ristic

In view of the LHC upgrade for the High Luminosity Phase (HL-LHC), the ATLAS experiment is planning to replace the Inner Detector with an all-Silicon system. The n-on-p technology represents a valid solution for the modules of most of the…

Organic light-emitting diodes (OLEDs) are the leading self-emitting pixel technology in current and future small and large area displays. Once integrated with a certain layer architecture into the backplane layout, their emission colour and…

Applied Physics · Physics 2019-06-07 Felix Fries , Markus Fröbel , Pen Yiao Ang , Simone Lenk , Sebastian Reineke

The phase 1 upgrade of the CMS pixel detector has been designed to maintain the tracking performance at instantaneous luminosities of $2 \times 10^{34} \mathrm{~cm}^{-2} \mathrm{~s}^{-1}$. Both barrel and endcap disk systems now feature one…

Instrumentation and Detectors · Physics 2018-07-25 Jory Sonneveld

In order to increase its discovery potential, the Large Hadron Collider (LHC) accelerator will be upgraded in the next decade. The high luminosity LHC (HL-LHC) period demands new sensor technologies to cope with increasing radiation…

Instrumentation and Detectors · Physics 2017-02-01 D. Vázquez Furelos , M. Carulla , E. Cavallaro , F. Förster , S. Grinstein , J. Lange , I. López Paz , M. Manna , G. Pellegrini , D. Quirion , S. Terzo

Plasma Display Panels (PDP), the underlying engine of panel plasma television displays, are being investigated for their utility as radiation detectors called Plasma Panel Sensors (PPS). The PPS a novel variant of a micropattern radiation…

In view of the LHC upgrade for the High Luminosity Phase (HL-LHC), the ATLAS experiment is planning to replace the Inner Detector with an all-Silicon system. The n-in-p bulk technology represents a valid solution for the modules of most of…

Instrumentation and Detectors · Physics 2015-06-17 G. Calderini , A. Bagolini , M. Bomben , M. Boscardin , L. Bosisio , J. Chauveau , G. Giacomini , A. La Rosa , G. Marchiori , N. Zorzi

The two innermost layers of the ALICE inner tracking system are instrumented with silicon pixel detectors. Single chip assembly prototypes of the ALICE pixels have been tested in high energy particle beams at the CERN SPS. Detection…

Nuclear Experiment · Physics 2009-11-11 D. Elia

The advanced imaging and delivery techniques in proton therapy allow conformal high-dose irradiation of the target volume with high accuracy using pencil beam scanning or beam shaping apertures. These irradiation methods increasingly…