ILC CRYOGENIC SYSTEMS REFERENCE DESIGN | Zendy

T. Peterson | Zendy; M. Geynisman | Zendy; Arkadiy Klebaner | Zendy; V. Parma | Zendy; L. Tavian | Zendy; J. Theilacker | Zendy; J. G. Weisend | Zendy; John Barclay | Zendy; Susan Breon | Zendy; Jonathan Demko | Zendy; Michael DiPirro | Zendy; J. Patrick Kelley | Zendy; Peter Kittel | Zendy; Al Zeller | Zendy; Mark Zagarola | Zendy; Steven Van Sciver | Zendy; Andrew Rowe | Zendy; John Pfotenhauer | Zendy; Tom Peterson | Zendy; Jennifer Lock | Zendy

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ILC CRYOGENIC SYSTEMS REFERENCE DESIGN

Author(s) -

T. Peterson,

M. Geynisman,

Arkadiy Klebaner,

V. Parma,

L. Tavian,

J. Theilacker,

J. G. Weisend,

John Barclay,

Susan Breon,

Jonathan Demko,

Michael DiPirro,

J. Patrick Kelley,

Peter Kittel,

Al Zeller,

Mark Zagarola,

Steven Van Sciver,

Andrew Rowe,

John Pfotenhauer,

Tom Peterson,

Jennifer Lock

Publication year - 2008

Publication title -

aip conference proceedings

Language(s) - English

Resource type - Conference proceedings

SCImago Journal Rank - 0.177

H-Index - 75

eISSN - 1551-7616

pISSN - 0094-243X

DOI - 10.1063/1.2908522

Subject(s) - international linear collider , linear particle accelerator , superconducting radio frequency , physics , superconducting magnet , electron cooling , nuclear physics , cryogenics , collider , particle accelerator , positron , electron , nuclear engineering , beam (structure) , magnet , engineering , optics , quantum mechanics , detector

A Global Design Effort (GDE) began in 2005 to study a TeV scale electron-positron linear accelerator based on superconducting radio-frequency (RF) technology, called the International Linear Collider (ILC). In early 2007, the design effort culminated in a reference design for the ILC, closely based on the earlier TESLA design. The ILC will consist of two 250 GeV linacs, which provide positron-electron collisions for high energy physics research. The particle beams will be accelerated to their final energy in superconducting niobium RF cavities operating at 2 kelvin. At a length of about 12 km each, the main linacs will be the largest cryogenic systems in the ILC. Positron and electron sources, damping rings, and beam delivery systems will also have a large number and variety of other superconducting RF cavities and magnets, which require cooling at liquid helium temperatures. Ten large cryogenic plants with 2 kelvin refrigeration are envisioned to cool the main linacs and the electron and positron sources. Three smaller cryogenic plants will cool the damping rings and beam delivery system components predominately at 4.5 K. This paper describes the cryogenic systems concepts for the ILC

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