Phys. Rev. Lett. 88, 072501 (2002) [4 pages]

Elastic α-12C Scattering and the 12C(α,γ)16O E2 S Factor

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P. Tischhauser1, R. E. Azuma2, L. Buchmann3, R. Detwiler1, U. Giesen1,3, J. Görres1, M. Heil4, J. Hinnefeld5, F. Käppeler4, J. J. Kolata1, H. Schatz1,6, A. Shotter7, E. Stech1, S. Vouzoukas1, and M. Wiescher1
1University of Notre Dame, Notre Dame, Indiana
2University of Toronto, Toronto, Ontario, Canada
3TRIUMF, Vancouver, British Columbia, Canada
4Forschungszentrum Karlsruhe, Karlsruhe, Germany
5Indiana University of South Bend, South Bend, Indiana
6Michigan State University, East Lansing, Michigan
7University of Edinburgh, Edinburgh, United Kingdom

Received 6 September 2001; published 31 January 2002

Angular distributions of 12C(α,α)12C have been measured for Eα  =  2.6–8.2 MeV, at angles from 24° to 166°, yielding 12 864 data points. R-matrix analysis of the ratios of elastic scattering yields a reduced width amplitude of γ12  =  0.47±0.06 MeV1/2 for the Ex  =  6.917 MeV(2+) state in 16O(a  =  5.5 fm). The dependence of the χ2 surface on the interaction radius a has been investigated and a deep minimum is found at a  =  5.42-0.27+0.16 fm. Using this value of γ12, radiative α capture and 16N β-delayed α-decay data, the S factor is calculated at Ec.m.  =  300 keV to be SE2(300)  =  53-18+13 keV b for destructive interference between the subthreshold resonance tail and the ground state E2 direct capture.


©2002 The American Physical Society

URL: http://link.aps.org/doi/10.1103/PhysRevLett.88.072501
DOI: 10.1103/PhysRevLett.88.072501
PACS: 26.30.+k, 25.40.Ny, 26.50.+x

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