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Title: Experimental study of the Main Ring transition crossing

Abstract

A 12 sec long Main Ring cycle was used with an unbunched beam of low intensity to measure the change of the revolution frequency of the beam as a function of the central momentum setting determined by the magnetic field. The transition gamma was determined as the first order term in the change in the revolution frequency versus fractional change in the momentum, but the nonlinear term {alpha}{sub 1} could not be determined because of the limited momentum aperture of the Main Ring and the present measurement resolution.

Authors:
;
Publication Date:
Research Org.:
Fermi National Accelerator Lab., Batavia, IL (United States)
Sponsoring Org.:
USDOE, Washington, DC (United States)
OSTI Identifier:
10179910
Report Number(s):
FNAL/C-92-/211; CONF-920706-29
ON: DE92040828
DOE Contract Number:  
AC02-76CH03000
Resource Type:
Conference
Resource Relation:
Conference: International conference on high energy accelerators,Hamburg (Germany),20-24 Jul 1992; Other Information: PBD: Aug 1992
Country of Publication:
United States
Language:
English
Subject:
43 PARTICLE ACCELERATORS; COLLIDING BEAMS; FREQUENCY MEASUREMENT; BEAM DYNAMICS; MODIFICATIONS; FERMILAB TEVATRON; MAGNETIC FIELDS; NONLINEAR PROBLEMS; APERTURES; LINEAR MOMENTUM; FREQUENCY DEPENDENCE; ORBITS; 430200; BEAM DYNAMICS, FIELD CALCULATIONS, AND ION OPTICS

Citation Formats

Kourbanis, I, and Ng, King-Yuen. Experimental study of the Main Ring transition crossing. United States: N. p., 1992. Web.
Kourbanis, I, & Ng, King-Yuen. Experimental study of the Main Ring transition crossing. United States.
Kourbanis, I, and Ng, King-Yuen. Sat . "Experimental study of the Main Ring transition crossing". United States. https://www.osti.gov/servlets/purl/10179910.
@article{osti_10179910,
title = {Experimental study of the Main Ring transition crossing},
author = {Kourbanis, I and Ng, King-Yuen},
abstractNote = {A 12 sec long Main Ring cycle was used with an unbunched beam of low intensity to measure the change of the revolution frequency of the beam as a function of the central momentum setting determined by the magnetic field. The transition gamma was determined as the first order term in the change in the revolution frequency versus fractional change in the momentum, but the nonlinear term {alpha}{sub 1} could not be determined because of the limited momentum aperture of the Main Ring and the present measurement resolution.},
doi = {},
url = {https://www.osti.gov/biblio/10179910}, journal = {},
number = ,
volume = ,
place = {United States},
year = {1992},
month = {8}
}

Conference:
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