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Phase Transitions and Crystal Structure of Dimethylammonium Tribromomercurate(II), (CH

3

)

2

NH

2

HgBr

3

, as Studied by

81

Br NQR and Single Crystal X-ray Diffraction*

Hiromitsu Terao

a

, Masao Hashimoto

b

, Tsutomu Okuda

c

, and Alarich Weiss

y

aDepartment of Chemistry, Faculty of Integrated Arts and Sciences, Tokushima University, Minamijosanjima-cho, Tokushima 770, Japan

bDepartment of Chemistry, Faculty of Science, Kobe University, Nadaku, Kobe 657, Japan

cDepartment of Chemistry, Faculty of Science, Hiroshima University, Kagamiyama, Higashihiroshima 724, Japan

Z. Naturforsch. 53 a, 559–567 (1998); received January 26, 1998

The temperature dependence of the81Br NQR frequencies of the title compound has revealed the presence of three phases (I, II and III, in the order of decreasing temperature): Tc1(II - I) = (318

10) K and Tc2(III - II) = (2021) K. The transitions were confirmed by thermal analysis (DTA).

Both of the II-I and I-II transitions exhibited strong hysteresis (i. e., superheating and supercooling, respectively). The crystal data, determined by single crystal X-ray diffraction, are: monoclinic, space group P2/a, a = 1384.8(3), b = 934.7(4), c = 1452.0(2) pm,= 104.10(1), Z = 8, R = 0.076.

The crystal has two crystallographically independent cations (CH3)2NH2

+and an infinite chain of anions almost in the c-direction. The anion chain is considered to consist of a HgBr2molecule and two different HgBr4

2 anions which are interconnected via weak intermolecular HgBr bonds.

The splitting patterns of the81Br NQR spectra indicate that rearrangements of the Hg-Br bonds are slight at the III-II transition but serious at the II-I transition. Some of the81Br NQR lines show anomalous temperature coefficients, attributable probably to thermal motions of cations.

Key words: (CH3)2NH2HgBr3; X-Ray Analysis; NQR; Phase Transition; Crystal Structure.

Reprint requests to Dr. H. Terao; E-mail: terao@ias.tokushima-u.ac.jp

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