List of Tables

• 4.2. First few one-di­mensional eigen­functions of the harmonic oscillator.
• 4.2. The first few spherical harmonics.
• 4.3. The first few spherical harmonics rewritten.
• 4.4. The first few radial wave functions for hydrogen.
• 6.1. Energy of the lowest single-particle state in a cube with 1 cm sides.
• 7.1. Properties of photons emitted in electric and magnetic multipole transitions.
• 12.1. Possible combined angular momentum of identical fermions in shells of single-particle states that differ in magnetic quantum number. The top shows odd numbers of particles, the bottom even numbers.
• 12.2. Possible combined angular momentum of identical bosons.
• 13.1. Electromagnetics I: Fundamental equations and basic solutions.
• 13.2. Electromagnetics II: Electromagnetostatic solutions.
• 14.1. Properties of the electron and of the simplest nuclei.
• 14.2. Alternate names for nuclei.
• 14.3. Candidates for nuclei ejected by uranium-238, radium-223, and fermium-256.
• 14.4. Nuclear spin and parity changes in electro­magnetic multipole transitions.
• 14.5. Half lifes for E0 transitions.
• A.1. Radial integral correction factors for hydrogen atom wave functions.
• A.2. More realistic radial integral correction factors for nuclei.
• A.3. Angular integral correction factors $f^{{\rm{ang}},\vert\Delta{j}\vert}_{\rm{LH}}$ and $f^{{\rm{ang}},\vert\Delta{j}\vert+1}_{\rm{LH}}$ for the Weisskopf electric unit and the Moszkowski magnetic one. The correction for the Weisskopf magnetic unit is to cross it out and write in the Moszkowski unit.
• A.4. Deuteron model data. The top half of the table allows some deviation from the experi­mental nucleon root-mean-square radial position. The bottom half allows some deviation from the experi­mental energy.
• A.5. Deuteron model data with a repulsive core of 0.5 fm.
• D.1. Additional combined angular momentum values.