g bosons and the third <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mrow><msup><mrow><mn>4</mn></mrow><mrow><mo>+</mo></mrow></msup></mrow></math> state in <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mrow><mmultiscripts><mrow><mi mathvariant="normal">Os</mi></mrow><mprescripts></mprescripts><mrow></mrow><mrow><mn>192</mn></mrow><mrow></mrow><mrow></mrow></mmultiscripts></mrow></math>

F. Todd Baker; A. Sethi; V. Penumetcha; G. T. Emery; W. P. Jones; M. A. Grimm; M. L. Whiten

doi:10.1103/PhysRevC.32.2212

Rapid Communication

g bosons and the third $4^{+}$ state in ${}^{192}{Os}$

F. Todd Baker, A. Sethi, V. Penumetcha, G. T. Emery, W. P. Jones, M. A. Grimm, and M. L. Whiten

Phys. Rev. C 32, 2212(R) – Published 1 December 1985

Abstract

Reduced matrix elements for excitation of the first three $4^{+}$ states in ${}^{192}{Os}$ have been measured using inelastic scattering of 135 MeV polarized protons. These data, as well as the known quadrupole properties of ${}^{192}{Os}$ , are best described if the third $4^{+}$ state is interpreted as a g-boson intruder state.