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Learn about the selection rules governing electric dipole transitions, including ΔL=±1 and ΔS=0, and the role of magnetic dipole transitions. Explore the intensity ratio of magnetic dipole to electric dipole transitions and its connection to the fine-structure constant α. Delve into Eddington's electric quadrupole transitions and the significance of ΔJ=±2.
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Selection Rules Electric Dipole
Selection Rules Electric Dipole L = 1 S = 0
Selection Rules Electric Dipole L = 1 S = 0 S S T T S T
Selection Rules Electric Dipole L = 1 S = 0 S S T T S T Magnetic Dipole
Selection Rules Electric Dipole L = 1 S = 0 S S T T S T Magnetic Dipole S = 1 S T
Selection Rules Electric Dipole L = 1 S = 0 S S T T S T Magnetic Dipole S = 1 S T Intensity - Magnetic Dipole / Electric Dipole
Selection Rules Electric Dipole L = 1 S = 0 S S T T S T Magnetic Dipole S = 1 S T Intensity - Magnetic Dipole / Electric Dipole = 1/2 = 1/137 2 = 5.327x 10-5
Selection Rules Electric Dipole L = 1 S = 0 S S T T S T Magnetic Dipole S = 1 S T Intensity - Magnetic Dipole / Electric Dipole = 1/2 = 1/137 2 = 5.327x 10-5 1/(102 + 62 + 1) (+ one for the pot) Eddington
Selection Rules Electric Dipole L = 1 S = 0 S S T T S T Magnetic Dipole S = 1 S T Intensity - Magnetic Dipole / Electric Dipole = 1/2 = 1/137 2 = 5.327x 10-5 1/(102 + 62 + 1) (+ one for the pot) Eddington Electric Quadrupole 1/108
Selection Rules Electric Dipole L = 1 S = 0 S S T T S T Magnetic Dipole S = 1 S T Intensity - Magnetic Dipole / Electric Dipole = 1/2 = 1/137 2 = 5.327x 10-5 1/(102 + 62 + 1) (+ one for the pot) Eddington Electric Quadrupole 1/108 J = 2