1971
DOI: 10.1103/physrevlett.27.1294
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Investigation of Compound Elastic Scattering Near Isobaric Analog Resonances with Polarized Protons

Abstract: A rather model-independent separation of direct and compound elastic cross sections has been obtained from the analysis of elastic scattering of polarized protons near the lowest d 5 / 2 isobaric analog resonances in 89 Y and 91 Nb.

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Cited by 41 publications
(3 citation statements)
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References 9 publications
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“…We have used both methods: First we have applied the method of Henneck and Graw, 11 where a combination of the normalized variances of cr and uA yields the relative direct contribution y D to the reaction without any assumption about the effective number of spin channels iV eff 0 We then checked the consistency of this method by describing the extracted cP l with the optical potential obtained by fitting the artifically energy-averaged observable (cx(0)A(0)) which contains no compound-nucleus contribution. 10 A target nucleus 30 Si was chosen because in the energy region of interest (JE P = 9.8 MeV) all final levels of the competing (P?P')> (P,n), and (p,a) compound -nucleus reactions were known and therefore the Hauser-Feshbach cross section a HF could be calculated explicitly without the introduction of free parameter s c Finally, W aa was calculated as the ratio a CE /a HF 0…”
Section: W Kretschmer and M Wanglermentioning
confidence: 99%
“…We have used both methods: First we have applied the method of Henneck and Graw, 11 where a combination of the normalized variances of cr and uA yields the relative direct contribution y D to the reaction without any assumption about the effective number of spin channels iV eff 0 We then checked the consistency of this method by describing the extracted cP l with the optical potential obtained by fitting the artifically energy-averaged observable (cx(0)A(0)) which contains no compound-nucleus contribution. 10 A target nucleus 30 Si was chosen because in the energy region of interest (JE P = 9.8 MeV) all final levels of the competing (P?P')> (P,n), and (p,a) compound -nucleus reactions were known and therefore the Hauser-Feshbach cross section a HF could be calculated explicitly without the introduction of free parameter s c Finally, W aa was calculated as the ratio a CE /a HF 0…”
Section: W Kretschmer and M Wanglermentioning
confidence: 99%
“…The requirement of maximizing the CN cross section in the channels coupled through the isobaric analogue resonance is met by nuclei in the vicinity of mass 90, for which comparatively few neutron channels are open. Several experimental groups have measured the angular distribu tion, analyzing power, spin-flip probability, spin-flip asymmetry, and cross-correlation functions fo r the outgoing protons (Kretschmer & Graw 1971, Albrecht et al 1973, Graw et a1 1974, Blanke et a1 1975, Davis et al 1975, Clement et al 1977, Haynes et al 1976, Feist et al 1977, King & Slater 1977. Typically, the cross section is written in the form 2.3, and two different fits to the data are performed: one is based on the expression for <a;b N > where DI are neglected, and one is based on Equation 6.3.…”
Section: Intermediate Structurementioning
confidence: 99%
“…For elastic proton scattering from 88 Sr and 90 Zr near the d 5/2 IAR at E p = 5.07 and 4.707 MeV, preliminary fits based on visual agreement have been presented previously. 3 In this Letter, the results of a x 2 fit procedure are reported for these IAR and also for IAR's observed with the spin-1" target 89 Y for the doublet (d 5/2 ®V) with spin 2" and 3** at £^ = 4.822 and 5.023 MeV, respectively, and with 92 Zr for the spin-| + (d 5/2 ) 3 ground-state analog at E p = 5.044 MeV. A detailed description of these experiments is given elsewhere.…”
mentioning
confidence: 99%