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Insertion of STC into TRT at the Department of Physics, Oxford
Credit: CERN

Philip Burrows

Professor of Physics

Sub department

  • Particle Physics
Philip.Burrows@physics.ox.ac.uk
Telephone: 01865 (2)73451
Denys Wilkinson Building, room 615a
  • About
  • Publications

The International Linear Collider Technical Design Report - Volume 3.II: Accelerator Baseline Design

(2013)

Authors:

Chris Adolphsen, Maura Barone, Barry Barish, Karsten Buesser, Philip Burrows, John Carwardine, Jeffrey Clark, Hélène Mainaud Durand, Gerry Dugan, Eckhard Elsen, Atsushi Enomoto, Brian Foster, Shigeki Fukuda, Wei Gai, Martin Gastal, Rongli Geng, Camille Ginsburg, Susanna Guiducci, Mike Harrison, Hitoshi Hayano, Keith Kershaw, Kiyoshi Kubo, Victor Kuchler, Benno List, Wanming Liu, Shinichiro Michizono, Christopher Nantista, John Osborne, Mark Palmer, James McEwan Paterson, Thomas Peterson, Nan Phinney, Paolo Pierini, Marc Ross, David Rubin, Andrei Seryi, John Sheppard, Nikolay Solyak, Steinar Stapnes, Toshiaki Tauchi, Nobu Toge, Nicholas Walker, Akira Yamamoto, Kaoru Yokoya
More details from the publisher
Details from ArXiV

The International Linear Collider Technical Design Report - Volume 4: Detectors

(2013)

Authors:

Ties Behnke, James E Brau, Philip N Burrows, Juan Fuster, Michael Peskin, Marcel Stanitzki, Yasuhiro Sugimoto, Sakue Yamada, Hitoshi Yamamoto
More details from the publisher

ILC Technical Design Report: Volume 3 - Accelerator

International Linear Collider, 2013

ILC Technical Design Report: Volume 4 - Detectors

, 2013

CLIC recombination scheme for the low energy operation mode

IPAC 2012 - International Particle Accelerator Conference 2012 (2012) 1864-1866

Authors:

A Gerbershagen, D Schulte, PN Burrows

Abstract:

The CLIC recombination scheme is a concept of multiplication of the drive beamfrequency in order to generate a 12 GHz RF wave for the main beam acceleration. CLIC isdesigned to be operated at nominal energy and in low energy modes. The low energy operationmodes require the train length to be increased by different factors in order to maintainthe same level of luminosity. Also the number of initial trains that are merged to formeach final train is changed. The combination scheme must be able to accommodate andrecombine both long and short trains for nominal and low energy CLIC operation modes. Therecombination hence becomes a non-trivial process and makes the correction of the errors inthe drive beam more challenging. The present paper describes in detail the recombinationprocess and its consequences. Copyright © 2012 by IEEE.

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