Slow Neutron Total and Fission Cross Sections of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="normal">U</mml:mi></mml:mrow><mml:mrow><mml:mn>233</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>

Moore, M. S.; Miller, L.G.; Simpson, O.D.

doi:10.1103/physrev.118.714

Cited by 24 publications

(3 citation statements)

References 3 publications

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“…based on multi-level analysis 18,19 ; they hypothesized that two groups of levels of different width exist in 233 U, that these groups can be explained as 7=2+ (broad) and J =3+ (narrow), and that the 2+ and 3+ levels are characterized by higher and lower fission symmetry, respectively, compared to thermal fission. Moore et al 20 have also proposed the existence of two groups of levels of different average width for 241 Pu.…”

Section: Discussionmentioning

confidence: 99%

Symmetry of Neutron-InducedPu239Fission at Individual Resonances

et al. 1966

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979could not be achieved, a more complete and systematic study might prove this preliminary conclusion incorrect. In fact, it has been demonstrated 14 that the need for a six-parameter potential is not fully realized unless the elastic data is fit over a wide angular range. Moreover, the use of a six-parameter potential (i.e., real and imaginary wells of different shapes) admits an extension to DW calculations with complex coupling.

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Section: Discussionmentioning

confidence: 99%

Symmetry of Neutron-InducedPu239Fission at Individual Resonances

et al. 1966

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“…The average spacing of the 738 resonances is 0.81 eV which is much larger than the expected value. The meaning of the resonance parameters in the high energy 33 Moore et al data 32 (multiplied by 10) and Pattenden et al data 31 (multiplied by 100). range of the data, i.e., parameters of true or pseudo-resonances, will be discussed in the section on the statistical properties of the parameters.…”

Section: Iv-the Results Of the Sammy Analysismentioning

confidence: 99%

“…The total cross sections are from Moore et al 31 Pattenden and Harvey, 30 Harvey et al 32 The fission cross sections are from Weston et al, 12 Deruyter and Wagemans 25 and Wagemans et al 27 The capture cross sections from Weston et al 12 The fission and capture data were renormalized according to Axton standard.…”

Section: Iii-the Experimental Data Basementioning

confidence: 99%