<p>This article builds upon our previous work, where we developed a numerical approach to solving quantum mechanical scattering problems using the phase function method. By employing the Runge-Kutta method to solve the non-linear phase equation derived from the time-independent Schrödinger equation, we modeled S-wave scattering phase shifts for neutron-proton (<i>np</i>) interactions using the Yukawa and Malfliet-Tjon potentials. In the present work, the model parameters for the Malfliet-Tjon (MT) potential have been determined using three-point analysis and global optimization. These parameters have been utilized to compute the scattering phase shifts for the triplet <sup>3</sup><i>S</i><sub>1</sub> and singlet <sup>1</sup><i>S</i><sub>0</sub> states of <i>np</i>-scattering. Furthermore, the low-energy scattering parameters and the total S-wave cross-section have been calculated from these phase shifts, showing consistency with experimental data. In addition, the deuteron binding energy calculated using the <sup>3</sup><i>S</i><sub>1</sub> MT potential obtained through global optimization is found to be (BE) = −2.1233659 MeV, which is very close to the experimental binding energy of the deuteron.</p>

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Numerical Simulation Study of Neutron-Proton Scattering Using Phase Function Method

  • Shikha Awasthi,
  • Anil Khachi,
  • Lalit Kumar,
  • O. S. K. S. Sastri

摘要

This article builds upon our previous work, where we developed a numerical approach to solving quantum mechanical scattering problems using the phase function method. By employing the Runge-Kutta method to solve the non-linear phase equation derived from the time-independent Schrödinger equation, we modeled S-wave scattering phase shifts for neutron-proton (np) interactions using the Yukawa and Malfliet-Tjon potentials. In the present work, the model parameters for the Malfliet-Tjon (MT) potential have been determined using three-point analysis and global optimization. These parameters have been utilized to compute the scattering phase shifts for the triplet 3S1 and singlet 1S0 states of np-scattering. Furthermore, the low-energy scattering parameters and the total S-wave cross-section have been calculated from these phase shifts, showing consistency with experimental data. In addition, the deuteron binding energy calculated using the 3S1 MT potential obtained through global optimization is found to be (BE) = −2.1233659 MeV, which is very close to the experimental binding energy of the deuteron.