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Related papers: BDS tuning and Luminosity Monitoring in CLIC

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The CMS beam and radiation monitoring subsystem BCM1F (Fast Beam Condition Monitor) consists of 8 individual diamond sensors situated around the beam pipe within the pixel detector volume, for the purpose of fast bunch-by-bunch monitoring…

The physics aims at the proposed future high-energy linear $e^+e^-$ collider CLIC pose challenging demands on the performance of the detector system. In particular, the vertex and tracking detectors have to combine a spatial resolution of a…

Instrumentation and Detectors · Physics 2020-10-22 Katharina Dort

The high-luminosity upgrade of the LHC (HL-LHC) brings unprecedented requirements for precision bunch-by-bunch luminosity measurement and beam-induced background monitoring in real time. A key component of the CMS Beam Radiation…

The CMS Beam Conditions and Radiation Monitoring System, BRM, will support beam tuning, protect the CMS detector from adverse beam conditions, and measure the accumulated dose close to or inside all sub-detectors. It is composed of…

Instrumentation and Detectors · Physics 2014-11-20 A. Bell , E. Castro , R. Hall-Wilton , W. Lange , W. Lohmann , A. Macpherson , M. Ohlerich , N. Rodriguez , V. Ryjov , R. S. Schmidt , R. L. Stone

Visible light communication (VLC) systems can provide illumination and communication simultaneously via light emitting diodes (LEDs). Orthogonal frequency division multiplexing (OFDM) waveforms transmitted in a VLC system will have high…

Information Theory · Computer Science 2014-06-25 Z. Yu , R. J. Baxley , G. T. Zhou

The high-luminosity upgrade of the LHC brings unprecedented requirements for real-time and precision bunch-by-bunch online luminosity measurement and beam-induced background monitoring. A key component of the CMS Beam Radiation,…

The CLIC study of a high-energy (0.5 - 5 TeV), high-luminosity (1034 - 1035 cm-2 sec-1) e+e- linear collider is presented. Beam acceleration using high frequency (30 GHz) normal-conducting structures operating at high accelerating fields…

Accelerator Physics · Physics 2008-11-26 Jean-Pierre Delahaye , Ian Wilson

The CLIC linear collider aims at accelerating multiple bunches of electrons and positrons and colliding them at a centre of mass energy of 3 TeV. These bunches will be accelerated through X-band linacs, operating at an accelerating…

Accelerator Physics · Physics 2014-11-18 V. Khan , R. M. Jones

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

Luminosity spectrum and accelerator background levels strongly influence the experimental conditions and have an important impact on detector design. The expected rates of the main beam-beam products at CLIC 3 TeV CM energy, taking into…

Accelerator Physics · Physics 2012-02-06 B. Dalena , J. Esberg , D. Schulte

As part of the Snowmass'21 community planning excercise, the Advanced Accelerator Concepts (AAC) community proposed future linear colliders with center-of-mass energies up to 15 TeV and luminosities up to 50$\times10^{34}$ cm$^{-2}$s$^{-1}$…

The dense beams used at CLIC to achieve a high luminosity will cause a large amount of background particles through beam-beam interactions. Generator level studies with GuineaPig and full detector simulation studies with an ILD based CLIC…

Instrumentation and Detectors · Physics 2010-06-18 André Sailer

The design luminosity for the future linear colliders is very demanding and challenging. Beam-based feedback systems will be required to achieve the necessary beam-beam stability and steer the two beams into collision. In particular we have…

Accelerator Physics · Physics 2009-02-18 J. Resta-Lopez , P. N. Burrows , A. Latina , D. Schulte

The implications of long-range wakefields on the beam quality are investigated through a detailed beam dynamics study. Injection offsets are considered and the resulting emittance dilution recorded, including systematic sources of error.…

Accelerator Physics · Physics 2012-06-04 I. Nesmiyan , R. M. Jones , A. Latina , D. Schulte

The Compact Linear Collider CLIC is designed to deliver e+e- collisions at a center of mass energy of up to 3 TeV. The detector systems at this collider have to provide highly efficient tracking and excellent jet energy resolution and…

Instrumentation and Detectors · Physics 2011-09-16 Frank Simon

The Compact Linear Collider (CLIC) is a high-energy high-luminosity linear electron-positron collider under development. It is foreseen to be built and operated in three stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV,…

Instrumentation and Detectors · Physics 2019-05-08 A. C. Abusleme Hoffman , G. Parès , T. Fritzsch , M. Rothermund , H. Jansen , K. Krüger , F. Sefkow , A. Velyka , J. Schwandt , I. Perić , L. Emberger , C. Graf , A. Macchiolo , F. Simon , M. Szalay , N. van der Kolk , H. Abramowicz , Y. Benhammou , O. Borysov , M. Borysova , A. Joffe , S. Kananov , A. Levy , I. Levy , G. Eigen , R. Bugiel , S. Bugiel , M. Firlej , T. A. Fiutowski , M. Idzik , J. Moroń , K. P. Świentek , P. Terlecki , P. Brückman de Renstrom , B. Turbiarz , T. Wojtoń , L. K. Zawiejski , E. Firu , V. Ghenescu , A. T. Neagu , T. Preda , I. Boyko , Yu. Nefedov , A. Rymbekova , A. Sapronov , G. Shelkov , A. Zhemchugov , A. Ruiz-Jimeno , I. Vila , E. Fullana , J. Fuster , P. Gomis Lopez , M. Perelló , M. A. Villarejo , M. Vos , J. Alozy , N. Alipour Tehrani , D. Arominski , R. Ballabriga Sune , F. Boyer , E. Brondolin , M. Buckland , M. Campbell , D. Dannheim , K. Dette , F. Duarte Ramos , N. Egidos Plaja , K. Elsener , A. Fiergolski , C. Fuentes Rojas , C. Grefe , D. Hynds , W. Klempt , I. Kremastiotis , J. Kröger , S. Kulis , E. Leogrande , L. Linssen , X. Llopart Cudie , A. Lucaci-Timoce , M. Munker , L. Musa , A. Nürnberg , F. -X. Nuiry , E. Perez Codina , H. Pernegger , M. Petrič , F. Pitters , T. Quast , S. Redford , P. Riedler , P. Roloff , A. Sailer , E. Santin , U. Schnoor , E. Sicking , K. Sielewicz , R. Simoniello , W. Snoeys , S. Spannagel , S. Sroka , R. Ström , P. Valerio , S. van Dam , E. van der Kraaij , T. Vǎnát , O. Viazlo , M. Vicente Barreto Pinto , M. A. Weber , M. Williams , K. Wolters , M. Benoit , G. Iacobucci , D M S Sultan , R. R. Bosley , T. Price , M. F. Watson , N. K. Watson , A. G. Winter , J. Goldstein , S. Green , J. S. Marshall , M. A. Thomson , B. Xu , G. Casse , J. Vossebeld , T. Coates , F. Salvatore , J. Repond , L. Xia , C. Kenney , A. Tomada

The requirements on the Final Focusing System (FFS) for a new linear collider has lead to lattice designs where chromaticity is corrected either locally or non-locally. Here, we present the status of an alternative lattice design developed…

Accelerator Physics · Physics 2015-04-02 Oscar Blanco , Rogelio Tomas , Philip Bambade

For the CLIC two-beam scheme, a high-current, long-pulse drive beam is required for RF power generation. Taking advantage of the 3 GHz klystrons available at the LEP injector once LEP stops, a 180 MeV electron accelerator is being…

Accelerator Physics · Physics 2007-05-23 G. Carron , E. Jensen , M. Luong , A. Millich , E. Rugo , I. Syratchev , L. Thorndahl

The role of the ILC final focus system (FFS) is to demagnify the beam to the sizes at the IP required to meet the ILC luminosity goals. The current design of final focus performs perfect chromaticity correction in both horizontal and…

Accelerator Physics · Physics 2015-12-09 Dou Wang , Yiwei Wang , Philip Bambade , Jie Gao

The Fast Beam Condition Monitor (FBCM) is a standalone luminometer for the High Luminosity LHC (HL-LHC) program of the CMS Experiment at CERN. The detector is under development and features a new, radiation-hard, front-end…

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