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Related papers: Integrated luminosity measurement at CEPC

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The Mu2e experiment at Fermilab will search for the charged lepton flavor violating process of neutrino-less $\mu \to e$ coherent conversion in the field of an aluminum nucleus. Mu2e will reach a single event sensitivity of about $2.5\cdot…

The physics program accessible in $e^+e^-$ collisions at the Future Circular Collider (FCC-ee) is summarized. The FCC-ee aims at collecting multi-ab$^{-1}$ integrated luminosities in $e^+e^-$ at $\sqrt{s}$ = 90, 160, 240, and 350 GeV,…

High Energy Physics - Experiment · Physics 2016-03-11 David d'Enterria

The absolute machine luminosity is a key quantity to achieve the high-precision physics program of future $e^+e^-$ collider. It is determined by measuring a theoretically well-known process, which, ideally, can be computed with arbitrary…

High Energy Physics - Phenomenology · Physics 2025-12-23 Clara L. Del Pio , Francesco P. Ucci

The High Luminosity LHC (HL-LHC) will integrate 10 times more luminosity than the LHC, posing significant challenges for radiation tolerance and event pileup on detectors, especially for forward calorimetry, and hallmarks the issue for…

Instrumentation and Detectors · Physics 2018-02-18 Arabella Martelli

This paper studies the possibility to measure the centre of mass energy using e+e- -> Z,gamma -> mu+mu-,gamma events at the ILC. With L = 100 fb^-1 at sqrt(s) = 350 GeV a relative error of around 10^{-4} is possible. The potentially largest…

Instrumentation and Detectors · Physics 2007-05-23 A. Hinze , K. Moenig

This note discusses methods of particle reconstruction in the forward region detectors of future e+e- linear colliders such as ILC or CLIC. At the nominal luminosity the innermost electromagnetic calorimeters undergo high particle fluxes…

Instrumentation and Detectors · Physics 2017-02-24 Andre Sailer , Andrey Sapronov

The proposed high-luminosity, circular electron-positron collider, FCC-ee, provides unparalleled opportunities for precise exploration of Higgs, electroweak, top, flavour, and beyond standard model physics. Very advanced detector systems…

High Energy Physics - Experiment · Physics 2025-08-06 Mogens Dam

CLIC is a proposed linear $e^{+}e^{-}$ collider with center-of-mass energies of up to $3\,\textrm{TeV}$. Its main objectives are precise top quark and Higgs boson measurements, as well as searches for Beyond Standard Model physics. To meet…

Instrumentation and Detectors · Physics 2018-12-07 Simon Spannagel

Beam polarisation is an integral part of the physics case of future Linear Colliders. In this contribution, important examples from Higgs coupling measurements, top and electroweak physics at high energies, the Z pole program as well as…

High Energy Physics - Experiment · Physics 2021-02-10 Jenny List

We report on the design and performance of the electromagnetic calorimeter timing readout system (EMTiming) for the Collider Detector at Fermilab (CDF). The system will be used in searches for rare events with high energy photons to verify…

Instrumentation and Detectors · Physics 2008-11-26 M. Goncharov , T. Kamon , V. Khotilovich , V. Krutelyov , S. W. Lee , D. Toback , P. Wagner , H. Frisch , H. Sanders , M. Cordelli , F. Happacher , S. Miscetti , R. Wagner

Chromatic calorimetry (CCAL) analyses particle detection by utilizing scintillators with distinct emission wavelengths to measure the longitudinal energy deposition of particle showers in high-energy physics, improving particle…

High Energy Physics - Experiment · Physics 2025-09-12 Devanshi Arora

The CMS experiment at the CERN LHC will be upgraded to accommodate the 5-fold increase in the instantaneous luminosity expected at the High-Luminosity LHC (HL-LHC). Concomitant with this increase will be an increase in the number of…

Instrumentation and Detectors · Physics 2021-04-28 B. Acar , G. Adamov , C. Adloff , S. Afanasiev , N. Akchurin , B. Akgün , M. Alhusseini , J. Alison , G. Altopp , M. Alyari , S. An , S. Anagul , I. Andreev , M. Andrews , P. Aspell , I. A. Atakisi , O. Bach , A. Baden , G. Bakas , A. Bakshi , P. Bargassa , D. Barney , E. Becheva , P. Behera , A. Belloni , T. Bergauer , M. Besancon , S. Bhattacharya , S. Bhattacharya , D. Bhowmik , P. Bloch , A. Bodek , M. Bonanomi , A. Bonnemaison , S. Bonomally , J. Borg , F. Bouyjou , D. Braga , J. Brashear , E. Brondolin , P. Bryant , J. Bueghly , B. Bilki , B. Burkle , A. Butler-Nalin , S. Callier , D. Calvet , X. Cao , B. Caraway , S. Caregari , L. Ceard , Y. C. Cekmecelioglu , G. Cerminara , N. Charitonidis , R. Chatterjee , Y. M. Chen , Z. Chen , K. y. Cheng , S. Chernichenko , H. Cheung , C. H. Chien , S. Choudhury , D. Čoko , G. Collura , F. Couderc , I. Dumanoglu , D. Dannheim , P. Dauncey , A. David , G. Davies , E. Day , P. DeBarbaro , F. De Guio , C. de La Taille , M. De Silva , P. Debbins , E. Delagnes , J. M. Deltoro , G. Derylo , P. G. Dias de Almeida , D. Diaz , P. Dinaucourt , J. Dittmann , M. Dragicevic , S. Dugad , V. Dutta , S. Dutta , J. Eckdahl , T. K. Edberg , M. El Berni , S. C. Eno , Yu. Ershov , P. Everaerts , S. Extier , F. Fahim , C. Fallon , B. A. Fontana Santos Alves , E. Frahm , G. Franzoni , J. Freeman , T. French , E. Gurpinar Guler , Y. Guler , M. Gagnan , P. Gandhi , S. Ganjour , A. Garcia-Bellido , Z. Gecse , Y. Geerebaert , H. Gerwig , O. Gevin , W. Gilbert , A. Gilbert , K. Gill , C. Gingu , S. Gninenko , A. Golunov , I. Golutvin , T. Gonzalez , N. Gorbounov , L. Gouskos , Y. Gu , F. Guilloux , E. Gülmez , M. Hammer , A. Harilal , K. Hatakeyama , A. Heering , V. Hegde , U. Heintz , V. Hinger , N. Hinton , J. Hirschauer , J. Hoff , W. S. Hou , C. Isik , J. Incandela , S. Jain , H. R. Jheng , U. Joshi , O. Kara , V. Kachanov , A. Kalinin , R. Kameshwar , A. Kaminskiy , A. Karneyeu , O. Kaya , M. Kaya , A. Khukhunaishvili , S. Kim , K. Koetz , T. Kolberg , A. Kristić , M. Krohn , K. Krüger , N. Kulagin , S. Kulis , S. Kunori , C. M. Kuo , V. Kuryatkov , S. Kyre , O. K. Köseyan , Y. Lai , K. Lamichhane , G. Landsberg , J. Langford , M. Y. Lee , A. Levin , A. Li , B. Li , J. -H. Li , H. Liao , D. Lincoln , L. Linssen , R. Lipton , Y. Liu , A. Lobanov , R. S. Lu , I. Lysova , A. M. Magnan , F. Magniette , A. A. Maier , A. Malakhov , I. Mandjavize , M. Mannelli , J. Mans , A. Marchioro , A. Martelli , P. Masterson , B. Meng , T. Mengke , A. Mestvirishvili , I. Mirza , S. Moccia , I. Morrissey , T. Mudholkar , J. Musić , I. Musienko , S. Nabili , A. Nagar , A. Nikitenko , D. Noonan , M. Noy , K. Nurdan , C. Ochando , B. Odegard , N. Odell , Y. Onel , W. Ortez , J. Ozegović , L. Pacheco Rodriguez , E. Paganis , D. Pagenkopf , V. Palladino , S. Pandey , F. Pantaleo , C. Papageorgakis , I. Papakrivopoulos , J. Parshook , N. Pastika , M. Paulini , P. Paulitsch , T. Peltola , R. Pereira Gomes , H. Perkins , P. Petiot , F. Pitters , F. Pitters , H. Prosper , M. Prvan , I. Puljak , T. Quast , R. Quinn , M. Quinnan , K. Rapacz , L. Raux , G. Reichenbach , M. Reinecke , M. Revering , A. Rodriguez , T. Romanteau , A. Rose , M. Rovere , A. Roy , P. Rubinov , R. Rusack , A. E. Simsek , U. Sozbilir , O. M. Sahin , A. Sanchez , R. Saradhy , T. Sarkar , M. A. Sarkisla , J. B. Sauvan , I. Schmidt , M. Schmitt , E. Scott , C. Seez , F. Sefkow , S. Sharma , I. Shein , A. Shenai , R. Shukla , E. Sicking , P. Sieberer , Y. Sirois , V. Smirnov , E. Spencer , A. Steen , J. Strait , T. Strebler , N. Strobbe , J. W. Su , E. Sukhov , L. Sun , M. Sun , C. Syal , B. Tali , U. G. Tok , A. Kayis Topaksu , C. L. Tan , I. Tastan , T. Tatli , R. Thaus , S. Tekten , D. Thienpont , T. Pierre-Emile , E. Tiras , M. Titov , D. Tlisov , J. Troska , Z. Tsamalaidze , G. Tsipolitis , A. Tsirou , N. Tyurin , S. Undleeb , D. Urbanski , V. Ustinov , A. Uzunian , M. van de Klundert , J. Varela , M. Velasco , M. Vicente Barreto Pinto , P. M. da Silva , T. Virdee , R. Vizinho de Oliveira , J. Voelker , E. Voirin , Z. Wang , X. Wang , F. Wang , M. Wayne , S. N. Webb , M. Weinberg , A. Whitbeck , D. White , R. Wickwire , J. S. Wilson , H. Y. Wu , L. Wu , C. H Yeh , R. Yohay , G. B. Yu , S. S. Yu , D. Yu , F. Yumiceva , A. Zacharopoulou , N. Zamiatin , A. Zarubin , S. Zenz , H. Zhang , J. Zhang

The precision physics program of the ILC requires precise knowledge of the state of beam polarisation. In fact the Compton polarimeters intended for the ILC will have to measure the polarisation with error a factor of 2 smaller than the…

Instrumentation and Detectors · Physics 2014-11-20 Christoph Bartels , Anthony Hartin , Christian Helebrant , Daniela Kaefer , Jenny List

The Particle Flow Algorithms adopted for future $e^{+}e^{-}$ colliders detectors and phase-II CMS upgrade require very high granularity calorimeters to deconvolve the individual contributions of particles in jets. This is especially true…

Instrumentation and Detectors · Physics 2017-11-27 Kostiantyn Shpak

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…

CLIC is a proposed linear e+e- collider designed to provide particle collisions at center-of-mass energies of up to 3 TeV. Precise measurements of the properties of the top quark and the Higgs boson, as well as searches for Beyond the…

Instrumentation and Detectors · Physics 2017-06-21 Simon Spannagel

Selectrons may be studied in both e-e- and e+e- collisions at future linear colliders. Relative to e+e-, the e-e- mode benefits from negligible backgrounds and \beta threshold behavior for identical selectron pair production, but suffers…

High Energy Physics - Phenomenology · Physics 2009-11-07 Jonathan L. Feng , Michael E. Peskin

We present a study of the capability of a 500 GeV e+e- collider based on CLIC technology for precision measurements of top quark properties. The analysis is based on full detector simulations of the CLIC_ILD detector concept using Geant4,…

High Energy Physics - Experiment · Physics 2012-02-16 Frank Simon , Katja Seidel , Stephane Poss

The production of a dark photon $A^{\prime}$ at the proposed CERN FCC-ee collider is investigated. The study addresses the associated production $e^+e^-\rightarrow\gamma A^{\prime}$ followed by the decay $A^{\prime}\rightarrow\mu^+\mu^-$.…

High Energy Physics - Phenomenology · Physics 2025-12-01 Giacomo Polesello

A silicon-based fine granularity calorimeter is a potential technology for the future International Linear Collider ILC, the future circular collider CEPC, and is also the chosen technology for the upgraded CMS experiment of the Large…

Instrumentation and Detectors · Physics 2017-08-02 Stathes Paganis , Andreas Psallidas , Arnaud Steen
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