On the $$\text{p}{-}^{{2}}\text{H}_{{1}} $$ and $$\text{p}{-}^{{16}}\text{O}\,$$ elastic scattering

Abstract

We solve the wave equation with the Manning-Rosen plus rank one separable non-local potential to obtain exact analytical solutions through ordinary differential equation method. The regular, Jost and physical state solutions are found to involve special functions of mathematics. As an application of the Jost function and Fredholm determinant, the bound-state energies and the scattering phase parameters for the p− 2 H 1 and p− 16 O systems are computed. The results achieved are in good agreement with the other methods published earlier.

Responsive Nanomaterial Delivery Systems for Pancreatic Cancer Management

“…[168] MFH involves the use of magnetic NPs and high-frequency (∼100-500 kHz) AMF and magnetic NPs to generate hyperthermia. [169][170][171] In the context of 2D cell cultures (Mia PaCa-2 and PANC-1), four MFH configurations were examined, including no ML, intracellular ML, intra-and extracellular ML, and extracellular ML. Notably, solely extracellular MFH exhibited pronounced cytotoxicity, leading to an immediate reduction in cell viability in both cell lines following treatment, although PANC-1 cells showed increased viability 24 hours post AMF exposure.…”

Low and intermediate energy cross section analysis of p-p and p-d elastic scattering using modified phase amplitude method for electromagnetic distorted nuclear interaction

“…The phase parameters thus obtained will, in turn, be exploited to estimate the cross sections for the concerned systems. Recently, one of us (UL) has also derived exact analytical solutions for the motion in MR plus Yamaguchi potential and applied to calculate scattering phase shifts of two body nuclear systems [30,31]. In the current text we consider MR plus nonlocal separable potentials in all partial waves for treating nucleon-nucleon and nucleon-nucleus elastic scattering thorough the modified PFM.…”