Celata, C.M., Abbott, S., Bennett, M., Bordua, M., Calvert, J., Dwinell, R., Howard, D., Hunt, D., Feinberg, B., Force, R., Frias, R., Kalnins, J., Lewis, S., Nyman, M., Shalz, L., Solomons, S.R., and Tekawa, M.. The Bevalac long flattop. United States: N. p., 1992.
Web. doi:10.2172/10160374.
Celata, C.M., Abbott, S., Bennett, M., Bordua, M., Calvert, J., Dwinell, R., Howard, D., Hunt, D., Feinberg, B., Force, R., Frias, R., Kalnins, J., Lewis, S., Nyman, M., Shalz, L., Solomons, S.R., & Tekawa, M.. The Bevalac long flattop. United States. doi:10.2172/10160374.
Celata, C.M., Abbott, S., Bennett, M., Bordua, M., Calvert, J., Dwinell, R., Howard, D., Hunt, D., Feinberg, B., Force, R., Frias, R., Kalnins, J., Lewis, S., Nyman, M., Shalz, L., Solomons, S.R., and Tekawa, M.. Thu .
"The Bevalac long flattop". United States.
doi:10.2172/10160374. https://www.osti.gov/servlets/purl/10160374.
@article{osti_10160374,
title = {The Bevalac long flattop},
author = {Celata, C.M. and Abbott, S. and Bennett, M. and Bordua, M. and Calvert, J. and Dwinell, R. and Howard, D. and Hunt, D. and Feinberg, B. and Force, R. and Frias, R. and Kalnins, J. and Lewis, S. and Nyman, M. and Shalz, L. and Solomons, S.R. and Tekawa, M.},
abstractNote = {Until July of 1992, the maximum length of the Bevalac flattop was 2 seconds, limiting the beam spill to 1.5 seconds. The normal running condition was a 1.5 second flattop, with a 1.0 second beam spill. If we define the duty factor as the spill length (in time) divided by the synchrotron pulse length, that is, the percentage of time the Bevalac can deliver beam to experiments, the duty factor for the 1.5 second flattop ranged from 17% (at full field, i.e., 12575 G) to 25% (low field). The purpose of the Long Flattop Project was to increase the length of the flattop, thus increasing the duty factor of the machine, and its efficiency for experiments. This has been done, with resultant increase in the duty factor and experimental data rate. It is now possible to run with duty factor of about 80% for low fields, falling to about 60% at 10 kG, and 34% at full field. This report documents what was done, and its limitations. It should be noted that increasing the length of the beam spill is only possible if the source can produce more beam per pulse than is usable by the experimenter. Experimenters running at full intensity with a short flattop (1.5 seconds) cannot benefit from a longer flattop. This paper describe the changes that have been made to Bevalac systems to make the long flattop possible, the limits put on the length of the flattop by existing hardware, and the procedure for tuning for the long flattop.},
doi = {10.2172/10160374},
journal = {},
number = ,
volume = ,
place = {United States},
year = {Thu Oct 01 00:00:00 EDT 1992},
month = {Thu Oct 01 00:00:00 EDT 1992}
}
