equipped with an Oxford Instruments ESR 900 continuous-liquid-helium-flow
system. Spectra were recorded at the following conditions (if not
specified): temperature, 3.8 K; microwave frequency, ∼9.36
GHz; microwave power, 2 mW; modulation amplitude, 9 G; time constant,
160 ms; field sweep speed, 28 G/s. Intra-EPR-cavity irradiation of
a sample placed inside the cryostat was performed with a Thorlabs
Inc. (Newton, NJ) PL450B, 450 nm, 80 mW Osram laser diode mounted
on the cavity access port. Cryoannealing protocol involved multiple
steps in which the sample frozen in liquid nitrogen was rapidly warmed
by immersion in a pentane bath held at the annealing temperature for
a fixed time and then cooled back to 77 K by immersion in liquid nitrogen.
Overlapping signals 1a and 1b in the obtained spectra were decomposed
as previously described.12 (link) Data points
of the E2/1b state were obtained as the intensity of the
1b signal g2 feature measured as the peak-to-peak
height and normalized to its maximum before irradiation. Data points
for changes in the 1c signal (denoted in the text as 1c*) were obtained
as the intensity of the resolved g1 feature,
normalized for kinetic plots as corresponding to the observed photoinduced
1b → 1c* conversion and shown after preirradiation background
subtraction.