## R = Bpyridinyl Scheme 4. Mechanism of the transmetalation via a six-membered transition state.
Composite Copper Chalcogenide Halides: Neutron Powder Diffraction of CuClCu2TeS3 and Electrical Properties of CuClCu2TeS3, (CuI)2Cu3SbS3, and (CuI)3Cu2TeS3
โ 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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โฆ 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 ุ and S 2ุ . The compound crystallizes in the rhombohedral system, space group R3m (No. 160) with a โซุโฌ 7.3502(1) A s , c โซุโฌ 10.3873(2) A s , V โซุโฌ 485.99 A s 3 , and Z โซุโฌ 3. The structure re5nement converged to R wp โซุโฌ 0.039 and R Bragg โซุโฌ 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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