Summary

A manilla folder with the title '21 Nuclear Physics' containing program documentation for:
- Handwritten notes on nuclear physics programs.
- T550 B150 Legendre Polynomial Functions.
- T551-551.2 B150 1st Associated Legendre Polynomial Function.
- T552 B151 Associated Legendre Polynomials.
- T553-553.2 B151 Spherical Bessel & Spherical Neumann Functions in floating binary.
- T554 B152 Coulomb phase shifts for elastic scattering of point charges by coulomb field.
- T555 B152 Nuclear Phase shifts in presence of a Coulomb field.
- T556 B152 First Derivative of Function by 9-point formula.
- T557 B152 Scattering phase-shifts for square well-neutral & charged particles.
- T558 B153 Faxen-Holtsmark Elastic Scattering Formula for neutral particles, real phases, no symmetry.
- T559 B153 Faxen-Holtsmark scattering formula, neutral particles, complex phases, no symmetry.
- T560 B153 Coulumb scattering amplitudes for non-identical particles (no symmetry).
- T561&T161 B153 Coulomb scattering amplitudes for identical particles.
- T562&T162 B154 Scattering of non-identical charged particles by nuclear + Coulomb field, with real phase shifts.
- T563 B154 Nuclear scattering for non-identical particles in a Coulomb field,complex phases.
- T564 B154 Scattering of identical particles (fermions) by nuclear potential in a Coulomb field (real phases).
- T565 B154 Scattering of identical particles (bosons) by nuclear + Coulomb field, with real phase shifts.
- T566 B152 Solution of the Schrodinger wave equation.
- T567 B155 Born Approximation for phase-shift in scattering by central potential.
- T568 B155 Swan-Born Approximation for the Phase-shift
- T570(b) B155 Swan-Born Integrals for the elastic scattering amplitude.
- T570(c.) B154 Swan-Born Integrals for the elastic scattering amplitude.
- T572 B156 Scattering of non-identical neutral particles by nuclear spin-orbit coupling potential (real phases).
- T573 B156 Scattering of non-identical charged particles by Coulomb field + nuclear spin-orbit coupling potential (real phases), spin 1/2-spin 0 case.

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