M. Afeworki et al., PREPARATION AND EPR STUDIES OF LITHIUM PHTHALOCYANINE RADICAL AS AN OXYMETRIC PROBE, Free radical biology & medicine, 25(1), 1998, pp. 72-78
The electron paramagnetic resonance (EPR) spectrum of the paramagnetic
center in solid lithium phthalocyanine, LiPc, exhibits a pO(2) (parti
al pressure of oxygen)-dependent line width. The compound is insoluble
in water and is not easily biodegradable and, therefore, is a useful
spin probe for quantitative in vivo oxymetry. Because EPR spectrometry
is potentially a useful technique to quantitatively obtain in vivo ti
ssue pO(2), such probes can be used to obtain physiological informatio
n. In this paper, a simple experimental procedure for the preparation
of LiPc using potentiostatic electrochemical methods is described. The
setup was relatively inexpensive and easy to implement. A constant po
tential ranging from 0.05 to 0.75 V versus Ag+/AgCl(s) was used for ob
taining LiPc. The EPR spectral studies were carried out using spectrom
eters operating at X-band and at radiofrequency (RF) at different pO(2
) values to characterize the spectral response of these crystals. The
results indicate that, depending on the electrolysis conditions, the p
roducts contain mixtures of crystals exhibiting pO(2)-sensitive and pO
(2)-insensitive line widths, Electrolysis conditions are reported wher
eby the pO(2)-sensitive LiPc crystals were the predominant product. Th
e influence of the working surface of the electrode and the electrolys
is time on the yield were also evaluated. The crystals of LiPc were al
so studied using a time-domain RF EPR spectrometer. In time-domain EPR
, the signals that survive beyond the spectrometer dead time are mainl
y the narrow lines corresponding to the pO(2)-sensitive crystals, wher
eas the signals arising from the pO(2)-insensitive component of LiPc w
ere found not to survive beyond the spectrometer dead time. This signa
l survival makes the time-domain EPR method more sensitive for pO(2) m
easurements using LiPc because the line width becomes very narrow at v
ery low pO(2) and, concomitantly, the relaxation time T-2 longer, with
no modulation or power saturation artifacts that are encountered as i
n the continuous wave (cw) mode. Further, minimal contributions from o
bject motion in the spectral data obtained using time-domain methods m
ake it an advantage for in vivo applications. Published by Elsevier Sc
ience Inc.