<span class="aps-inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mrow><msup><mrow><mn></mn><mo>(</mo><mi>sd</mi><mo>)</mo><mn></mn></mrow><mrow><mn>2</mn></mrow></msup></mrow></math></span> States in <span class="aps-inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mrow><mmultiscripts><mrow><mi mathvariant="normal">C</mi></mrow><mprescripts></mprescripts><mrow></mrow><mrow><mn>1</mn><mn>4</mn><mo>,</mo><mspace></mspace><mn>1</mn><mn>6</mn></mrow><mrow></mrow><mrow></mrow></mmultiscripts></mrow></math></span>

H. T. Fortune; M. E. Cobern; S. Mordechai; G. E. Moore; S. Lafrance; R. Middleton

doi:10.1103/PhysRevLett.40.1236

${(sd)}^{2}$ States in ${}^{14, 16}C$

H. T. Fortune, M. E. Cobern, S. Mordechai, G. E. Moore, S. Lafrance, and R. Middleton

Phys. Rev. Lett. 40, 1236 – Published 8 May 1978

Abstract

Simple shell-model calculations account for the remarkable similarity in excitation energies and ( $t, p$ ) strengths of predominantly ${(sd)}^{2}$ states in ${}^{14}C$ and ${}^{16}C$ .

Received 20 December 1977

DOI:https://doi.org/10.1103/PhysRevLett.40.1236

Authors & Affiliations

H. T. Fortune^*, M. E. Cobern^†, S. Mordechai^‡, G. E. Moore^§, S. Lafrance, and R. Middleton

Physics Department, University of Pennsylvania, Philadelphia, Pennsylvania 19104

^*Presently at University of Oxford on leave from University of Pennsylvania.
^†Present address: Westinghouse Electric Corporation, Bettis Atomic Power Laboratory, P. O. Box 79, West Mifflin, Penn. 15122.
^‡On leave from Department of Physics, Ben-Gurion University, Beer-Sheva, Israel.
^§Present address: Analytic Services Inc., Falls Church, Va. 22041.