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The synthesis and crystal structure of Rb4TmI6 : Lattice energy calculations on networks of condensed cubes

Identifieur interne : 002817 ( Main/Exploration ); précédent : 002816; suivant : 002818

The synthesis and crystal structure of Rb4TmI6 : Lattice energy calculations on networks of condensed cubes

Auteurs : G. Miller [États-Unis] ; M. Smith [États-Unis] ; MEITIAN WANG [République populaire de Chine] ; SHIHUA WANG [République populaire de Chine]

Source :

RBID : Pascal:98-0150740

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English descriptors

Abstract

Single crystals of Rb4TmI6 were obtained by heating a mixture of RbI, Tm, and HgI2 in Ta ampoules. Using single crystal X-ray diffraction, the crystal structure of Rb4TmI6 was assigned to the K4CdCl6 structure type; space group R3c (no. 167); a=14.159(2) Å, c=17.46(3) Å; Z=6, R=0.056; Rw=0.098 (F>4σ(F)) for 450 observed reflections with 2θmax =45°. This structure features a one-dimensional chain along the c axis, which is composed of alternating, face-sharing [TmI6] trigonal antiprisms (distorted octahedra) and distorted (RbI6] trigonal prisms. Alternatively, Rb4TmI6 is a three-dimensional network of TmI6-centered Rb8 distorted cubes which share vertices according to the formula [(TmI6)Rb8/2]. This viewpoint establishes its relationship to the tetragonal Tl4HgBr6 structure type. Lattice energy and extended Hiickel calculations were carried out on several models of A4MI6 with s0 and s2 A+ cations: the rhombohedral K4CdCl6 structure type always shows the lower lattice energy, but a s2-s2 attractive interaction (via sp hybridization) enhances the stability of the tetragonal Tl4HgBr6 structure type.


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Le document en format XML

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<title xml:lang="en" level="a">The synthesis and crystal structure of Rb
<sub>4</sub>
TmI
<sub>6</sub>
: Lattice energy calculations on networks of condensed cubes</title>
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<title xml:lang="en" level="a">The synthesis and crystal structure of Rb
<sub>4</sub>
TmI
<sub>6</sub>
: Lattice energy calculations on networks of condensed cubes</title>
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<term>Crystal structure</term>
<term>Experimental study</term>
<term>Lattice energy</term>
<term>Rhombohedral crystals</term>
<term>Rubidium iodides</term>
<term>Ternary compounds</term>
<term>Tetragonal crystals</term>
<term>Thulium iodides</term>
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<keywords scheme="Pascal" xml:lang="fr">
<term>Etude expérimentale</term>
<term>Structure cristalline</term>
<term>Energie réticulaire</term>
<term>Cristal rhomboédrique</term>
<term>Cristal quadratique</term>
<term>Rubidium iodure</term>
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<div type="abstract" xml:lang="en">Single crystals of Rb
<sub>4</sub>
TmI
<sub>6</sub>
were obtained by heating a mixture of RbI, Tm, and HgI
<sub>2</sub>
in Ta ampoules. Using single crystal X-ray diffraction, the crystal structure of Rb
<sub>4</sub>
TmI
<sub>6</sub>
was assigned to the K
<sub>4</sub>
CdCl
<sub>6</sub>
structure type; space group R3c (no. 167); a=14.159(2) Å, c=17.46(3) Å; Z=6, R=0.056; R
<sub>w</sub>
=0.098 (F>4σ(F)) for 450 observed reflections with 2θ
<sub>max</sub>
=45°. This structure features a one-dimensional chain along the c axis, which is composed of alternating, face-sharing [TmI
<sub>6</sub>
] trigonal antiprisms (distorted octahedra) and distorted (RbI
<sub>6</sub>
] trigonal prisms. Alternatively, Rb
<sub>4</sub>
TmI
<sub>6</sub>
is a three-dimensional network of TmI
<sub>6</sub>
-centered Rb
<sub>8</sub>
distorted cubes which share vertices according to the formula [(TmI
<sub>6</sub>
)Rb
<sub>8/2</sub>
]. This viewpoint establishes its relationship to the tetragonal Tl
<sub>4</sub>
HgBr
<sub>6</sub>
structure type. Lattice energy and extended Hiickel calculations were carried out on several models of A
<sub>4</sub>
MI
<sub>6</sub>
with s
<sup>0</sup>
and s
<sup>2</sup>
A
<sup>+</sup>
cations: the rhombohedral K
<sub>4</sub>
CdCl
<sub>6</sub>
structure type always shows the lower lattice energy, but a s
<sup>2</sup>
-s
<sup>2</sup>
attractive interaction (via sp hybridization) enhances the stability of the tetragonal Tl
<sub>4</sub>
HgBr
<sub>6</sub>
structure type.</div>
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