Hg-199 NMR measurements have been performed both in the normal and in
the superconducting state for an oriented HgBa2CuO4+delta superconduct
ing powder sample with T-c = 96 K. The large anisotropic Knight shift
of Hg-199, K-199(ax) = -0.15% at room temperature, is explained by the
chemical shift related to the linear Hg-O(2) bonding configuration. B
oth K-199(iso) and K-199(ax) decrease below T-c and scale linearly wit
h each other in the whole temperature range investigated. The Hg-199 K
night shift K-199 slowly decreases with decreasing temperature on appr
oaching T-c in the normal state, reflecting the decrease of the unifor
m spin susceptibility chi '(0,0) with lowering temperature. The Hg-199
spin-echo decay can be fit by the product of a Gaussian component T-G
(-1) and an exponential one (T-L(-1)). The Gaussian component T-G(-1)
which is dominant above T-c, is shown to be due mainly to an indirect
nuclear interaction via the conduction electrons (holes) and is found
to be directly proportional to the spin contribution (K-199(sp)) of th
e Knight shift. The exponential component T-L(-1) becomes dominant wel
l below T-c and is ascribed to the effect of thermal motion of flux li
nes. The Hg-199 nuclear spin-lattice relaxation rate T-1(-1) in the no
rmal state shows a Korringa behavior well above T-c with (T1T)(-1) = 0
.1 sec(-1) K-1. Reduction of (T1T)(-1) with decreasing temperature is
observed starting about 10 K above T-1 and is consistent with the decr
ease of chi '(0,0) in the normal state observed in K(T) and T-G(-1) K-
199(sp)(T) was extracted using the Korringa relation and below T-c, is
found to fit the d-wave pairing scheme with a superconducting gap par
ameter 2 Delta(0)=3.5k(B)T(c). The d-wave pairing is also supported by
the temperature dependence of Hg-199 T-1(-1) in the superconducting s
tate. The (CU)-C-63 T-1(-1) and T-2(-1) measurements have been perform
ed in the normal state. In contrast to the Korringa behavior of Hg-199
T-1(-1) in the normal state, the preliminary results show the increas
e of the (63) Cu (T1T)(-1) with decreasing temperature, indicating the
enhancement of the antiferromagnetic fluctuations of CU2+ moments com
mon in the high-T-c cuprates. The reduction of (CU)-C-63 (T1T)(-1) is
observed starting above T-c and is compared with the decrease of Hg-19
9 K-sp, T-G(-1), and (T1T)(-1) in the normal state. The (CU)-C-63 nucl
ear spin-spin relaxation T-2(-1) is found to follow an exponential dec
ay in the normal state and to decrease with decreasing temperature sim
ilar to the Hg-199 K-sp and T-G(-1).