Table 1.
Isotropic 57Fe Hyperfine Couplingsa
E4(2H)*b |
E4(4H)c |
E0d |
|||
---|---|---|---|---|---|
57Fe |
aiso/δAe (MHz/%) |
57Fe |
aiso/δAe (MHz/%) |
57Fe |
aiso/δAe (MHz/%) |
a | −30/+17 | α | −35/−34 | A1 | −18/+41 |
b | −27/+18 | β | −27/+26 | A2 | −17.1/23 |
e | +23 | κ | ~+20g | A3 | −11.8 |
f | ~+25f | γ1 | +17 | B1 | +11.7 |
g | ~+25f | γ2 | −16 | B1 | +11.7 |
c | −19 | δ | +13 | B2 | +9.3 |
d | −17 | λ | ~+8g | A4 | −3.7 |
Isotropic hyperfine couplings (aiso) or 57Fe sites of photoreduced E4(2H)*, Janus intermediate E4(4H), and resting state E0, arranged in order of absolute values; it is argued in the text that a/b, α/β and A1/A2 refer to the same pair of Fe sites.
Isotropic coupling reported as average of coupling observed at canonical g-values in ENDOR; signs determined by PESTRE measurements.
As reported; obtained through ENDOR, PESTRE, and Triple.12
As reported; determined by Mossbauer spectroscopy.53
δA(%) = 100 × (Am – A1)/aiso, where A1 corresponds to g1 and is in each case an extreme value (max or min) and m = 2 or 3 is the other extreme, as observed in the 2D plots of 57Fe ENDOR spectra for E4(2H)* and E4(4H) of Figure 5, Figure S3 and as reported for E0.53