<span class="aps-inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mrow><mmultiscripts><mrow><mi mathvariant="normal">N</mi></mrow><mprescripts></mprescripts><mrow></mrow><mrow><mn>14</mn></mrow><mrow></mrow><mrow></mrow></mmultiscripts></mrow><mo>(</mo><mi>α</mi><mo>,</mo><mi>d</mi><mo>)</mo><mrow><mmultiscripts><mrow><mi mathvariant="normal">O</mi></mrow><mprescripts></mprescripts><mrow></mrow><mrow><mn>16</mn></mrow><mrow></mrow><mrow></mrow></mmultiscripts></mrow></math></span> Reaction at 40 MeV

M. S. Zisman; E. A. McClatchie; B. G. Harvey

doi:10.1103/PhysRevC.2.1271

${}^{14}N (α, d) {}^{16}O$ Reaction at 40 MeV

M. S. Zisman, E. A. McClatchie, and B. G. Harvey

Phys. Rev. C 2, 1271 – Published 1 October 1970

Abstract

The ${}^{14}N (α, d) {}^{16}O$ reaction has been investigated up to an excitation energy of 20 MeV using a 40-MeV $α$ -particle beam from the Berkeley 88-in. cyclotron. Angular distributions were obtained for the three strongest levels at 14.40 ± 0.03, 14.82 ± 0.03, and 16.24 ± 0.04 MeV. Widths for these states, with the experimental resolution subtracted in quadrature, are 30 ± 30, 69 ± 30, and 125 ± 50 keV, respectively. Evidence for the probable [ ${}^{14}N (1^{+}) + {(d_{\frac{5}{2}})}^{2}_{5^{+}}$ ] configuration of the three states is discussed.

Received 22 June 1970

DOI:https://doi.org/10.1103/PhysRevC.2.1271

Authors & Affiliations

M. S. Zisman, E. A. McClatchie^*, and B. G. Harvey

Lawrence Radiation Laboratory, University of California, Berkeley, California 94720

^*Present address: ARKON Scientific Laboratories, Berkeley, California.

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Vol. 2, Iss. 4 — October 1970

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Physical Review C

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