Chapter 41. One-Dimensional Quantum Mechanics - Physics

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Finite Potential well: 11. Solve Schrodinger’s Schrodinger s equation in the three regions (we already did this!) 2. ‘Connect’ the three regions by using the following boundary conditions: 1. This will give quantized k’s and E’s 2. Normalize wave function
Finite Potential well: Finite number of bound states, energy spacing smaller since wave function more spread out (like bigger L), wave functions extend into classically forbidden region
Page 1 and 2: Chapter 41. One‐Dimensional Quant
Page 3 and 4: The Schrödinger Equation Consider
Page 5 and 6: There is a more general form of the
Page 7: E, KE, and and PE
Page 15 and 16: A Particle in a Rigid Box
Page 23 and 24: Zero point energy: even at T=0K, a
Page 25: The Correspondence Principle When w
Page 29 and 30: Finite Potential well example - Qua
Page 31 and 32: Qualitative wave function shapes Ex
Page 34 and 35: Molecular vibrations ‐ Harmonic O
Page 36 and 37: Particle in a capacitor
Page 38 and 39: Covalent Bond: H2+ (single electron
Page 40 and 41: Quantum Tunneling
Page 42: Quantum Tunneling - Resonant tunnel

Chapter 41. One-Dimensional Quantum Mechanics - Physics

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