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