Abstract

A conventional Reich-Moore approximation (RMA) of R -matrix is generalized into a manifestly unitary form by introducing a set of resonant capture channels treated explicitly in a generalized, reduced R -matrix. A dramatic reduction of channel space witnessed in conventional RMA, from N c × N c full R -matrix to N p × N p reduced R -matrix, where N c = N p + N γ , N p and N γ denoting the number of particle and γ-ray channels, respectively, is due to N p γ . A corresponding reduction of channel space in generalized RMA (GRMA) is from N c × N c full R -matrix to N × N , where N = N p + N , and where N is the number of capture channels defined in GRMA. We show that N = N λ where N λ is the number of R -matrix levels. This reduction in channel space, although not as dramatic as in the conventional RMA, could be significant for medium and heavy nuclides where N γ . The resonant capture channels defined by GRMA accommodate level-level interference (via capture channels) neglected in conventional RMA. The expression for total capture cross section in GRMA is formally equal to that of the full N c × N c R -matrix. This suggests that GRMA could yield improved nuclear data evaluations in the resolved resonance range at a cost of introducing N (N − 1)/2 resonant capture width parameters relative to conventional RMA. Manifest unitarity of GRMA justifies a method advocated by Frohner and implemented in the SAMMY nuclear data evaluation code for enforcing unitarity of conventional RMA. Capture widths of GRMA are exactly convertible into alternative R -matrix parameters via Brune tranform. Application of idealized statistical methods to GRMA shows that variance among conventional RMA capture widths in extant RMA evaluations could be used to estimate variance among off-diagonal elements neglected by conventional RMA. Significant departure of capture widths from an idealized distribution may indicate the presence of underlying doorway states.

Highlights

  • Preservation of unitarity in the generalized RMA (GRMA) could be used to justify Frohner’s prescription that has been conventionally used to enforce unitarity of the total cross section in the conventional Reich-Moore approximation (RMA) [3, 6]. For this purpose it is useful to view the conventional RMA as a special case of GRMA in which off-diagonal elements of GRMA capture matrix in Eq (9) are set to 0 while explicitly retaining the NγG RM A(= Nλ) resonant capture channels introduced in Sect

  • The matrices governing conversion between alternative and formal R-matrix partial width amplitudes are to be computed as if γ -ray channels were absent. These conversion matrices are to be applied to particle and to GRMA γ -ray widths alike: GRMA capture width amplitudes matrix γγ is to be transformed just like that of particle-channel partial widths amplitudes, that is, γγ = aT γγ

  • This implies that transformation of conventional RMA capture widths of a diagonal γγ matrix would yield γγ with finite off-diagonal elements

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Summary

Introduction

In this generalization the reduced number of capture channels, NγG RM A, turns out to be equal to the number of levels Nλ. Diagonal elements of GRMA capture width matrix correspond to capture widths in the conventional RMA. Implications, and drawbacks of generalized GRMA are discussed. Statistical properties of matrix elements of GRMA’s reduced capture-width matrix are discussed in Sect. 4. Section 5 provides a formula for converting generalized Reich-Moore resonance parameters into alternative R-matrix parameters defined via Brune transform [9].

Formalism
Variance of GRMA matrix elements
Alternative GRMA parameters
Conclusions and outlook
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