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. Author manuscript; available in PMC: 2021 Jan 5.
Published in final edited form as: J Am Chem Soc. 2020 Dec 16;142(52):21679–21690. doi: 10.1021/jacs.0c07914

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
a

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.

b

Isotropic coupling reported as average of coupling observed at canonical g-values in ENDOR; signs determined by PESTRE measurements.

c

As reported; obtained through ENDOR, PESTRE, and Triple.12

d

As reported; determined by Mossbauer spectroscopy.53

e

δA(%) = 100 × (AmA1)/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

f

Calculated from eqs 3 and 4 using atest = −20 MHz as described in the text; listed below site e because of uncertainties thus introduced.

g

Sign of aiso for κ and value for λ calculated from eq 3 and the analogues to eq 4 for one unknown aiso, using atest = −20 MHz.