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Composite Copper Chalcogenide Halides: Neutron Powder Diffraction of CuClCu2TeS3 and Electrical Properties of CuClCu2TeS3, (CuI)2Cu3SbS3, and (CuI)3Cu2TeS3

โœ Scribed by Arno Pfitzner; Sara Reiser; Tom Nilges; Winfried Kockelmann


Book ID
102608993
Publisher
Elsevier Science
Year
1999
Tongue
English
Weight
241 KB
Volume
147
Category
Article
ISSN
0022-4596

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โœฆ Synopsis


The crystal structure of CuClCu TeS was re5ned from TOF neutron powder di4raction data in order to verify the distribution of chlorine and sulfur. It is a novel derivative of the zincblende type with an ordered distribution both of the cations Cu ุ‰ and Te 4ุ‰ and of the anions Cl ุŠ and S 2ุŠ . The compound crystallizes in the rhombohedral system, space group R3m (No. 160) with a โ€ซุโ€ฌ 7.3502(1) A s , c โ€ซุโ€ฌ 10.3873(2) A s , V โ€ซุโ€ฌ 485.99 A s 3 , and Z โ€ซุโ€ฌ 3. The structure re5nement converged to R wp โ€ซุโ€ฌ 0.039 and R Bragg โ€ซุโ€ฌ 0.032. From the neutron data it can be derived that there is no signi5cant disorder of Cl and S atoms. Impedance spectroscopic measurements in the temperature range 140+2803 3C reveal that CuClCu 2 TeS 3 is a semiconductor with an activation energy of 0.75 eV (T < 2003 3C) and 1.25 eV (T > 2003 3C), respectively. On the other hand (CuI) 3 Cu 2 TeS 3 and (CuI) 2 Cu 3 SbS 3 exhibit high copper ion conductivity with activation energies of 0.2 and 0.35 eV, respectively, but a negligible electronic conduction.


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(CuI)3Cu2TeS3: Layers of Cu2TeS3 in Copp
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