The Effective M3Y Residual Interaction In 41Ca As a Nuclear Diffraction Grating of Electrons

Abstract

The total and individual multipole moments of magnetic electron scattering form factors in 41Ca have been investigated using a widely successful model which is the nuclear shell model configurations keeping in mind of 1f7/2 subshell as an L-S shell and Millinar, Baymann, Zamick as L-S shell (F7MBZ) to give the model space wave vector. Also, harmonic oscillator wave functions have been used as wave function of a single particle in 1f7/2 shell. Nucleus 40Ca as core closed and Core polarization effects have been used as a corrective with first order correction concept to basic computation of L-S shell and the excitement energy has been implemented with 2ћω. The core polarizability effect has been utilized to incorporate the rejected space (core + higher arrangement) via L-S shell with a realism interaction of effective M3Y P2 interaction to connect the model space particles in motion with the spouse (p-h). The two body M3Y interactions have been utilized as an interaction residue to calculate the core polarizability matrix elements. Finally, the theoretical result of the form factor has been compared with the experimental results.

Nuclear Energy Levels Scheme of 46Cr Using FPD6, FPY, and KB3G Interactions

“…A model space factor has been constructed using F7MBZ that considers the single-particle potential (harmonic oscillator) and elastic magnetic electron scattering form factors for 41 Ca with 40 Ca as the inert core. The entire theory is then examined using the nuclear shell theory [16] and calculating Ca quadrupole moments (41, 43, 45, and 47) using the shell model [17].…”