Integration of the full-acceptance detector into JLEIC

G. H. Wei, V. S. Morozov, F. Lin, F. Pilat, Y. Zhang, Y. M. Nosochkov, M. H. Wang

Research output: Chapter in Book/Report/Conference proceedingConference contributionpeer-review

1 Scopus citations

Abstract

Fully meeting the nuclear physics goals of JLEIC (Jefferson Lab Electron Ion Collider) requires a full-acceptance detector. Integration of such a detector into the collider presents many challenges for design of the beam dynamics. Small β* values at the Interaction Point (IP) needed to reach a luminosity level of a few 1033 cm-2sec-1 cause large natural chromaticities. Their compensation involves installation of dedicated chromaticity correction sections in the collider rings. Small β* values and a large space occupied by the full-acceptance detector also mean large β in the final focus area. This sets a constraint on the field quality of the magnets in the large beta areas, in order to ensure a large enough dynamic aperture. Additional complications include asymmetric lattice and beam envelopes in the Interaction Region (IR), forward detection requirements, large crossing angle with associated crab dynamics, coupling and coherent orbit distortion from the detector solenoid, etc. This paper briefly describes how we address these issues.

Original languageEnglish
Title of host publicationIPAC 2017 - Proceedings of the 8th International Particle Accelerator Conference
PublisherJoint Accelerator Conferences Website - JACoW
Pages3912-3914
Number of pages3
ISBN (Electronic)9783954501823
StatePublished - Jul 2017
Externally publishedYes
Event8th International Particle Accelerator Conference, IPAC 2017 - Bella Conference Center, Denmark
Duration: May 14 2017May 19 2017

Publication series

NameIPAC 2017 - Proceedings of the 8th International Particle Accelerator Conference

Conference

Conference8th International Particle Accelerator Conference, IPAC 2017
Country/TerritoryDenmark
CityBella Conference Center
Period05/14/1705/19/17

Funding

This material is based upon work supported by the U.S. DOE, Office of Science, Office of Nuclear Physics under contracts DE-AC05-06OR23177 and DE-AC02-06CH11357. Work is supported in part by the U.S. DOE Contract DE-AC02-76SF00515.

FundersFunder number
U.S. Department of Energy
Office of Science
Nuclear PhysicsDE-AC02-06CH11357, DE-AC05-06OR23177, DE-AC02-76SF00515

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