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Title: A doublet C0 IR solution using existing magnets

Abstract

This note explores, in a very limited way, some of the possibilities and difficulties encountered in creating collisions at C0 solely using magnets looted from the existing IR's at B0 and D0. In the strawman model considered her a standard Collins straight section is installed at D0, while all the useful D0 IR magnets are moved to C0. There is no obvious reason from either an optics or beam-separation viewpoint to prefer the demise of D0 over CDF, or vice-versa, so the model choice is fairly arbitrary. Apart from modifications to the final-focus optics, the magnets appear at C0 locations just as they are currently installed at D0.

Authors:
Publication Date:
Research Org.:
Fermi National Accelerator Lab., Batavia, IL (US)
Sponsoring Org.:
USDOE Office of Energy Research (ER) (US)
OSTI Identifier:
799184
Report Number(s):
FERMILAB-TM-2181
TRN: US0204883
DOE Contract Number:  
AC02-76CH03000
Resource Type:
Technical Report
Resource Relation:
Other Information: PBD: 19 Aug 2002
Country of Publication:
United States
Language:
English
Subject:
43 PARTICLE ACCELERATORS; 71 CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS; FERMILAB COLLIDER DETECTOR; MAGNETS; MODIFICATIONS; OPTICS

Citation Formats

John A Johnstone. A doublet C0 IR solution using existing magnets. United States: N. p., 2002. Web. doi:10.2172/799184.
John A Johnstone. A doublet C0 IR solution using existing magnets. United States. doi:10.2172/799184.
John A Johnstone. Mon . "A doublet C0 IR solution using existing magnets". United States. doi:10.2172/799184. https://www.osti.gov/servlets/purl/799184.
@article{osti_799184,
title = {A doublet C0 IR solution using existing magnets},
author = {John A Johnstone},
abstractNote = {This note explores, in a very limited way, some of the possibilities and difficulties encountered in creating collisions at C0 solely using magnets looted from the existing IR's at B0 and D0. In the strawman model considered her a standard Collins straight section is installed at D0, while all the useful D0 IR magnets are moved to C0. There is no obvious reason from either an optics or beam-separation viewpoint to prefer the demise of D0 over CDF, or vice-versa, so the model choice is fairly arbitrary. Apart from modifications to the final-focus optics, the magnets appear at C0 locations just as they are currently installed at D0.},
doi = {10.2172/799184},
journal = {},
number = ,
volume = ,
place = {United States},
year = {Mon Aug 19 00:00:00 EDT 2002},
month = {Mon Aug 19 00:00:00 EDT 2002}
}

Technical Report:

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