4.5 Article

Independent normalization for γ-ray strength functions: The shape method

Journal

PHYSICAL REVIEW C
Volume 104, Issue 1, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevC.104.014311

Keywords

-

Funding

  1. National Research Foundation of South Africa [118846]
  2. Research Council of Norway [263030]
  3. National Science Foundation [PHY 1913554]
  4. DOE National Nuclear Security Administration [DOE-DE-NA0003906]
  5. Nuclear Science and Security Consortium [DE-NA0003180]
  6. Department of Energy, Office of Nuclear Physics [DE-SC0020451]
  7. European Research Council [637686]
  8. ChETEC COST Action [CA16117]
  9. COST (European Cooperation in Science and Technology)
  10. JINA-CEE through the National Science Foundation (JINA Center for the Evolution of the Elements) [PHY-1430152]
  11. U.S. Department of Energy (DOE) [DE-SC0020451] Funding Source: U.S. Department of Energy (DOE)

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The shape method is a novel approach to obtain the functional form of the gamma-ray strength function, and to simultaneously determine the slope of the nuclear level density. Utilizing primary gamma-ray transitions, the shape method has been successfully applied to representative cases demonstrating the retention of the functional form of the gamma SF.
The shape method, a novel approach to obtain the functional form of the gamma-ray strength function (gamma SF), is introduced. In connection with the Oslo method the slope of the nuclear level density (NLD) and gamma SF can be obtained simultaneously even in the absence of neutron resonance spacing data. The foundation of the shape method lies in the primary gamma-ray transitions which preserve information on the functional form of the gamma SF. The shape method has been applied to Fe-56, Zr-92, and Dy-164, which are representative cases for the variety of situations encountered in typical NLD and gamma SF studies. The comparisons of results from the shape method to those from the Oslo method demonstrate that the functional form of the gamma SF is retained regardless of nuclear structure details or J(pi) values of the states fed by the primary transitions.

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