P. Ganal et al., STRUCTURAL AND PHYSICAL-PROPERTIES OF THE MISFIT INTERCALATION COMPOUNDS HGXTAS2 (X=0.58, 1.19, AND 1.3), Physical review. B, Condensed matter, 52(15), 1995, pp. 11359-11371
Time-differential perturbed angular correlation (TDPAC) and x-ray powd
er diffraction (XPD) have been used to investigate the complex physica
l and structural properties of mercury intercalation compounds derived
from 1T-TaS2 and 2H-TaS2, respectively. In situ TDPAC studies of the
Ta-181 nuclear quadrupole interaction during Hg intercalation and ther
mal deintercalation proved the complete reversibility of the intercala
tion process and revealed the formation of three distinct phases (alph
a-Hg1.19TaS2, beta-Hg1.3TaS2, and a disordered second-stage phase Hg0.
58TaS2 derived from alpha-Hg1.19TaS2) The stage-1 compounds alpha-Hg1.
19TaS2 and beta-Hg1.3TaS2 are characterized by two different structura
l arrangements of the intercalated Hg that bear a strong resemblance t
o those realized in solid-state phases of beta-Hg and alpha-Hg, respec
tively. alpha-Hg1.19TaS2 adopts an unusual (3 + 1)-dimensional composi
te crystal structure which can be described as two interpenetrating su
blattices formed by the TaS2 host and the Hg guest. These C-face-cente
red orthorhombic sublattices share common a and c axes but are incomme
nsurate along the b axis [a = 5.765(1) Angstrom, b = 3.309(1) Angstrom
, c = 17.842(1) Angstrom, and b(Hg) = 2.782(1) Angstrom]. The in-plane
Hg-Hg distances of 2.782 and 3.201 Angstrom indicate a chainlike Hg a
rrangement similar to that found in Hg1.24TiS2. In the case of beta-Hg
1.3TaS2 the Hg arrangement is such that the TaS2 host lattice (a = 3.3
18 Angstrom) can be considered as a 2X2 superstructure formed upon hex
agonal close-packed Hg layers (a(Hg) = 2.902 Angstrom). Hg intercalati
on into 1T-TaS2 requires an elevated reaction temperature of 423 K, wh
ereas 2H-TaS2 intercalates Hg already at ambient temperature. Both the
TDPAC and x-ray-diffraction data indicate that in the case of 1T-TaS2
the Hg intercalation process is accompanied by an irreversible change
of the TaS2 host layers from octahedral to a trigonal-prismatic arran
gement.