Chapter 5
The Intermediate Coupling Model
Notation (Sect. 5.1)
Two electron systems (Sect. 5.2)
Three electron systems (Sect 5.4)
Three open-shell p electrons
p3 matrix diagonalization
Inversion of coefficients from known roots
Application
Matrices
LS to jj
p3 matrix diagonalization
Slater determinant (Sect. 5.5)
Antisymmetrization: the Slater determinant
Paper size needed to specify wave functions
Chapt. 1
Chapt. 2
Chapt. 3
Chapt. 4
Chapt. 6
Chapt. 7
Chapt. 8
Chapt. 9
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Deferred Topics
Intermediate coupling amplitudes
LS and j coupling
Example 1: nsnl
Construction
(continued)
(continued)
Characterizing IC
Mixing angles
Generalized Landé by mixing angles
Semiempirical mapping of Slater quantities
Forbidden transitions
Sm construction
Gyromagnetic ratios
Mixing Angle Formulations of M1 Line Strengths and E1 Branching Fractions
M1 line strengths
Shortley-Pasternack formula
Applications
Mixed transitions
p2 case
sp case
Pb sequence mixing angles
Eigenvectors
Application
Self-consistent field methods
Self-consistent potential
(cont.)
(cont.)
PE of symmetric distribution
SCSCF
Koopman's theorem
(cont.)
Measurement of wavelengths and establishment of levels
Wavelength measurement
Establishing energy levels and uncertainties
Lithium-like quartets
F VII data
Ne VIII data
Measured wavelengths and uncertainties
Least squares constraints
Coefficients
Isoelectronic plot
Parametrized output
QM Many-Body Problems
Two Body Problem
Three Body Problem
Different from Sequential Two-Body Problems
Two Particle QM Problem
Product Solutions
Slater Parameters
Self-Consistent Field
SCF Applied
Potential energy with screening
SCF Applied (continued)