Level structure of <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mrow><mmultiscripts><mrow><mi mathvariant="normal">Cr</mi></mrow><mprescripts></mprescripts><mrow></mrow><mrow><mn>52</mn></mrow><mrow></mrow><mrow></mrow></mmultiscripts></mrow></math> from the <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mrow><mmultiscripts><mrow><mi mathvariant="normal">V</mi></mrow><mprescripts></mprescripts><mrow></mrow><mrow><mn>51</mn></mrow><mrow></mrow><mrow></mrow></mmultiscripts></mrow></math><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mrow><msup><mrow><mo>(</mo></mrow><mrow><mn>3</mn></mrow></msup></mrow></math>He,d) reaction

M. A. Basher; H. R. Siddique; A. Husain; A. K. Basak; H. M. Sen Gupta

doi:10.1103/PhysRevC.45.1575

Level structure of ${}^{52}{Cr}$ from the ${}^{51}V$ $(^{3}$ He,d) reaction

M. A. Basher, H. R. Siddique, A. Husain, A. K. Basak, and H. M. Sen Gupta

Phys. Rev. C 45, 1575 – Published 1 April 1992

Abstract

The ${}^{51}V$ $(^{3}$ He,d $)^{52}$ Cr reaction has been studied at 15 MeV using the tandem Van de Graaff accelerator and the multichannel magnetic spectrograph of the Nuclear Physics Laboratory, Oxford. Angular distributions have been measured for levels up to $E_{x}$ =8.6 MeV over the laboratory angular range θ=3.75°–71.25°. Data are analyzed in terms of the distorted wave Born approximation theory of the direct reaction. The l transfers and the spectroscopic factors are obtained.