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Synchrotron X-ray Absorption Spectroscopy - Stanford Synchrotron ...

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Transition<br />

Dipole<br />

Quadrupole<br />

Transition<br />

Dipole<br />

Quadrupole<br />

Selection Rules for X-<strong>ray</strong> absorption<br />

near-edge spectra<br />

Selection rule<br />

∆l=±1<br />

∆l=±2<br />

K, L I , M I<br />

ns →n´p<br />

ns →n´d<br />

Strength<br />

Intense<br />

Weak<br />

K-edge<br />

np →n´d<br />

np →n´f<br />

1s →np<br />

1s →nd<br />

L II , L III , M II , M III<br />

LIII-edge 2p →nd<br />

2p →nf<br />

M IV , M V<br />

nd →n´f<br />

nd →n´g<br />

I. J. Pickering and G. N. George GEOL 498.3/898.3<br />

Tungsten L-edges – Selection Rules<br />

XAS L-edge spectra of Na 2 WO 4 –W(VI) is 5d 0 , so we expect strong dipole<br />

allowed transitions to the 5d manifold at the L III and L II edges from the<br />

2p 3/2 and 2p 1/2 , respectively. No such intense transitions are expected at<br />

the L I near-edge (2s excitation).<br />

W L III W L II<br />

W L I<br />

I. J. Pickering and G. N. George GEOL 498.3/898.3<br />

Uranium M-edges – Selection Rules<br />

XAS M-edge spectra of UO 2 (CH 3 CO 2 ) 2 (H 2 O) 2 –U(VI) is 5f 0 , so we expect<br />

strong dipole-allowed transitions to the 5f manifold at the M V and M IV edges<br />

from the 3d 3/2 and 3d 1/2 , respectively. No such intense transitions are<br />

expected at the M III , M II (3p 3/2 and 3p 1/2 excitation, respectively) or M I (3s<br />

excitation) near-edges.<br />

M V<br />

M IV MIII<br />

O O OH2 O U<br />

O<br />

H2O O<br />

O<br />

I. J. Pickering and G. N. George GEOL 498.3/898.3<br />

M II<br />

M I

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