Thermodynamics, Statistical Physics, and Quantum Mechanics

Contents xxiii

5.27.

5.28.

5.29.

5.30.

Variational Calculations

5.31.

5.32.

5.33.

5.34.

5.35.

5.36.

5.37.

Perturbation Theory

5.38.

5.39.

5.40.

5.41.

5.42.

5.43.

5.44.

5.45.

5.46.

5.47.

5.48.

5.49.

5.50.

5.51.

5.52.

WKB

5.53.

5.54.

5.55.

5.56.

5.57.

5.58.

5.59.

5.60.

Three Spins (Stony Brook)

ConstantMatrix Perturbation (Stony Brook)

RotatingSpin (Maryland, MIT)

Nuclear Magnetic Resonance (Princeton, Stony Brook)

AnharmonicOscillator (Tennessee)

Linear Potential I (Tennessee)

LinearPotential II (MIT, Tennessee)

Return of Combined Potential (Tennessee)

Quarticin Three Dimensions (Tennessee)

Halved Harmonic Oscillator (Stony Brook, Chicago (b),

Princeton (b))

Helium Atom (Tennessee)

Momentum Perturbation (Princeton)

Ramp in Square Well (Colorado)

Circle with Field (Colorado, Michigan State)

Rotator in Field (Stony Brook)

Finite Size of Nucleus (Maryland, Michigan State,

Princeton, Stony Brook)

Uand Perturbation (Princeton)

Relativistic Oscillator(MIT, Moscow Phys-Tech, Stony

Brook (a))

Spin Interaction (Princeton)

Spin–Orbit Interaction (Princeton)

Interacting Electrons (MIT)

StarkEffect in Hydrogen (Tennessee)

Hydrogenwith Electric and Magnetic Fields (MIT)

Hydrogenin Capacitor (Maryland, Michigan State)

HarmonicOscillator in Field (Maryland, Michigan State)

ofTritium (Michigan State)

BouncingBall(Moscow Phys-Tech, Chicago)

Truncated Harmonic Oscillator (Tennessee)

Stretched Harmonic Oscillator (Tennessee)

Ramp Potential (Tennessee)

Charge and Plane (Stony Brook)

Ramp Phase Shift (Tennessee)

Parabolic Phase Shift (Tennessee)

Phase Shift for Inverse Quadratic(Tennessee)

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