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Last hour: Generalized angular momentum EV’s: j·(j+1)·ħ2 for ; m·ħ for ; -j ≤ m ≤ j in steps of 1 The quantum numbers j can be.

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Presentation on theme: "Last hour: Generalized angular momentum EV’s: j·(j+1)·ħ2 for ; m·ħ for ; -j ≤ m ≤ j in steps of 1 The quantum numbers j can be."— Presentation transcript:

1 Last hour: Generalized angular momentum EV’s: j·(j+1)·ħ2 for ; m·ħ for ; -j ≤ m ≤ j in steps of 1 The quantum numbers j can be integer or half-integer; j ≥ 0 can never point exactly along the z-axis, since H atom Hamiltonian Solutions have the form (r,,) = R(r)·Yℓm(,) Radial Schrödinger equation: New, “effective” potential

2 Solutions of the radial Schrödinger equation:
where “associated Laguerre polynomials”

3 From Levine “Quantum Chemistry”

4 From Levine “Quantum Chemistry”

5 Learning Goals for Chapter 16 – The H-Atom
After this chapter, the related homework problems, and reading the relevant parts of the textbook, you should be able to: explain the structure of the Hamiltonian of the H-atom; explain the terms in the radial Schrödinger equation of the H-atom; discuss the level structure of the H-atom and nodal structure of its eigenfunctions; discuss the probability density of the H-atom; calculate properties of the H-atoms for a given quantum state.


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