Skip to main navigation Skip to search Skip to main content

Measuring reaction probability ratios to simulate neutron-induced cross-sections of short-lived nuclei

  • C. Plettner*
  • , H. Ai
  • , C. W. Beausang
  • , L. A. Bernstein
  • , L. Ahle
  • , H. Amro
  • , M. Babilon
  • , J. T. Burke
  • , J. A. Caggiano
  • , R. F. Casten
  • , J. A. Church
  • , J. R. Cooper
  • , B. Crider
  • , G. Gürdal
  • , A. Heinz
  • , E. A. McCutchan
  • , K. Moody
  • , J. A. Punyon
  • , J. Qian
  • , J. J. Ressler
  • A. Schiller, E. Williams, W. Younes
*Corresponding author for this work

Research output: Contribution to journalArticlepeer-review

1 Citation (Scopus)

Abstract

Measuring the neutron-induced fission cross-sections of short-lived nuclei represents an experimental challenge due to target activity and the low intensity of neutron beams. One way to alleviate the problems inherent in the direct measurement is to use the surrogate method, where one measures the decay probability of the same compound nucleus formed using a charged beam and a stable target. The decay probability of the compound nucleus is then used to estimate the neutron-induced cross-section. As an extension to the surrogate method, we introduce a new method of reporting the fission probabilities of two compound nuclei as a ratio, which has the advantage of removing most of the systematic uncertainties. The ratio method was checked in a known case, the 236U(n, f)/238U(n, f) cross-section ratio, which turned out to be the same as the probability ratio of P(236U(d, pf))/P( 238U(d, pf)). As an application, the 237U(n, f)/ 235U(n, f) cross-section ratio was inferred, on the basis of the measured P(238U(d, d′f))/P(236U(d, d′f)) probability ratio.

Original languageEnglish
Pages (from-to)S1573-S1576
JournalJournal of Physics G: Nuclear and Particle Physics
Volume31
Issue number10
DOIs
Publication statusPublished - 1 Oct 2005
Externally publishedYes

Fingerprint

Dive into the research topics of 'Measuring reaction probability ratios to simulate neutron-induced cross-sections of short-lived nuclei'. Together they form a unique fingerprint.

Cite this