The cesium-
richest ph
ase in the Cs-Tl system, CsTl, c
an beisol
ated
as
a pure cryst
alline ph
ase through slowcooling of cesium-richer compositions in T
a followed by
vacuumsublim
ation of the excess Cs
at ~100
ages/entities/deg.gif">C. Thecompound melts incongruently in the neighborhood of 150
ages/entities/deg.gif">C. Thestructure w
as est
ablished by single cryst
alX-r
ay diffr
action
at room temper
ature (orthorhombic
Fddd,
Z = 48,
a = 32.140(3) Å,
b= 15.136(1) Å,
and
c =9.2400(7) Å. The isol
atedTl
66- ions in the structure,tetr
agon
ally compressed oct
ahedr
a, exhibit
D2symmetrywith
ages/entities/le.gif">0.063(4) Å differences in edge lengths from
D4h. ExtendedHückel c
alcul
ations confirm the cl
assic
aln
ature of the distortion in lowering the cluster electron count
andch
arge. The di
am
agnetic CsTl differs fromKTl, which cont
ains more distortedTl
66- ions(
C2h), in
a doubled
a axis
and
an
addition
al interpenetr
atingcluster
anion subl
attice. The sm
aller distortion of the clusters in CsTlorigin
ates with the lower field of the s
ame numberof c
ation neighbors in
a more symmetric
arr
angement. Thestructur
al trend from LiTl (CsCl type) through thecl
assic N
aTl (stuffed di
amond) to the rel
ated KTl
and CsTl withcompressed oct
ahedr
a (
and the
absence of
anysuch Rb ph
ase) rel
ates to the efficient p
acking of A
+ and(Tl
-)
n o
ver
a widely
varying r
angeof A
+ sizes, withonly N
a+ fitting well within
ajourn
als/inoc
aj/35/i08/eqn/ic951265
ve10001.gif">l
attice. Simil
arly 4-bonded th
allium in KTl
and CsTl withsomewh
atshorter Tl-Tl dist
ances is
a necess
ary
altern
ati
ve when the infinitel
attice c
annot toler
ate l
arger c
ations.