1 l10 – qm in 3 dimensions. 2 v(r): separation of variables

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1 L10 – QM in 3 dimensions

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Page 1: 1 L10 – QM in 3 dimensions. 2 V(r): separation of variables

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L10 – QM in 3 dimensions

Page 2: 1 L10 – QM in 3 dimensions. 2 V(r): separation of variables

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V(r): separation of variables

Page 3: 1 L10 – QM in 3 dimensions. 2 V(r): separation of variables

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Page 4: 1 L10 – QM in 3 dimensions. 2 V(r): separation of variables

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The angular equation

Page 5: 1 L10 – QM in 3 dimensions. 2 V(r): separation of variables

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The angular equation -

Page 6: 1 L10 – QM in 3 dimensions. 2 V(r): separation of variables

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The angular equation -

Pl are the Legendre polynomials, defined by the Rodrigues formula:

Page 7: 1 L10 – QM in 3 dimensions. 2 V(r): separation of variables

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Page 8: 1 L10 – QM in 3 dimensions. 2 V(r): separation of variables

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Page 9: 1 L10 – QM in 3 dimensions. 2 V(r): separation of variables

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Spherical harmonics

= (-1)m for m>=0 and =1 for m<0. The Y are orthogonal, so

Page 10: 1 L10 – QM in 3 dimensions. 2 V(r): separation of variables

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The radial equation

Page 11: 1 L10 – QM in 3 dimensions. 2 V(r): separation of variables

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L11 – The H atom

u(r) = rR(r)

Page 12: 1 L10 – QM in 3 dimensions. 2 V(r): separation of variables

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Asymptotic behavior

u(r) = rR(r)

Page 13: 1 L10 – QM in 3 dimensions. 2 V(r): separation of variables

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The radial solution

u(r) = rR(r)

n > l

is the q-th Laguerre polynomial.

Page 14: 1 L10 – QM in 3 dimensions. 2 V(r): separation of variables

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The radial solution: energy

Page 15: 1 L10 – QM in 3 dimensions. 2 V(r): separation of variables

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Ground state

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n > 1

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n > 1 (continued)

Since they are eigenvectors for different eigenvalues

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Example

Page 19: 1 L10 – QM in 3 dimensions. 2 V(r): separation of variables

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Graphs

Page 20: 1 L10 – QM in 3 dimensions. 2 V(r): separation of variables

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Angular momentum

Poiche’

Poiche’ , l’equazione in si puo’ scrivere

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