G. Kordas, EPR SPECTROSCOPY AND MNDO CALCULATIONS FOR THE INTERPRETATION OF THE H-4(+) CENTER DETECTED IN OXYNITRIDE GLASSES, Physics and Chemistry of Glasses, 36(6), 1995, pp. 259-263
gamma-irradiated oxynitride glass was investigated by EPR spectroscopy
at the X-band. A paramagnetic centre was detected at high (10 dB) mic
rowave power. The high power spectrum was attributed to the H-4(+) cen
tre. The signal of 2,2,6,6-tetramethylpiperidine-1-oxyl (TEMPO) in eth
anol solution at 116 K was also detected. The simulation of both spect
ra yielded the hfs spectroscopic parameters A(x)=101 . 41, A(y)=5 . 60
and A(x)=5 . 60 MHz. The linewidths of the signal were 5 G in the gla
ss and 14 G in TEMPO. The ratio of the g value strain distributions we
re 1200, 1, and 1500 for Delta(x), Delta(y), and Delta(z), respectivel
y. The hfs constants allowed the calculation of the spin densities of
the 2s(N), and 2p(N), orbitals. These spin densities were compared wit
h the spin densities of several centres calculated using a MNDO progra
m. This comparison suggested that both centres are due to (=R(R=Si,C))
(2)N-O structure. This new model for the H-4(+) centre is confirmed b
y the comparison between hfs parameters and line shape of the two cent
res' signals. Furthermore there is able experimental and theoretical e
vidence for the explanation of the paramagnetic centre obtained in nit
roxide spin labels such as TEMPO that have attributed this state to (=
R(R=Si,C))(2)N-O. Linewidth differences ave due to the separate spin
lattice relaxation time constants affected by the lattice vibrations o
f the host environment. The g strain is greater for the H-4(+) centre
due to the random Si-N-Si bond angles while the C-N-C bond angle in th
e TEMPO molecule are move restricted in the well defined environment.