Design of the ILC Crab Cavity System | Zendy

C. Adolphsen | Zendy; C. Beard | Zendy; L. Bellantoni | Zendy; Graeme Burt | Zendy; Richard G. Carter | Zendy; Brian Chase | Zendy; M. Church | Zendy; A. Dexter | Zendy; M. Dykes | Zendy; H. Edwards | Zendy; P. Goudket | Zendy; Richard O. Jenkins | Zendy; R.M. Jones | Zendy; A. Kalinin | Zendy; T. Khabiboulline | Zendy; Kyung-Ja Ko | Zendy; A. Latina | Zendy; Z. Li | Zendy; Lingwei Ma | Zendy; Peter McIntosh | Zendy; C. Ng | Zendy

AI Assistant Blog Pricing

Home ZAIA Blog

Open Access

Design of the ILC Crab Cavity System

Author(s) -

C. Adolphsen,

C. Beard,

L. Bellantoni,

Graeme Burt,

Richard G. Carter,

Brian Chase,

M. Church,

A. Dexter,

M. Dykes,

H. Edwards,

P. Goudket,

Richard O. Jenkins,

R.M. Jones,

A. Kalinin,

T. Khabiboulline,

Kyung-Ja Ko,

A. Latina,

Z. Li,

Lingwei Ma,

Peter McIntosh,

C. Ng

Publication year - 2007

Publication title -

osti oai (u.s. department of energy office of scientific and technical information)

Language(s) - English

Resource type - Reports

DOI - 10.2172/915387

Subject(s) - international linear collider , bunches , luminosity , physics , collision , dipole , optics , beam (structure) , astrophysics , computer science , detector , computer security , quantum mechanics , galaxy

The International Linear Collider (ILC) has a 14 mrad crossing angle in order to aid extraction of spent bunches. As a result of the bunch shape at the interaction point, this crossing angle at the collision causes a large luminosity loss which can be recovered by rotating the bunches prior to collision using a crab cavity. The ILC baseline crab cavity is a 9-cell superconducting dipole cavity operating at a frequency of 3.9 GHz. In this paper the design of the ILC crab cavity and its phase control system, as selected for the RDR in February 2007 is described in fuller detail

The content you want is available to Zendy users.

Already have an account? Click here to sign in.

Having issues? You can contact us here

Accelerating Research