Organic–inorganic hybrid metallic conductors based on bis(ethylenedithio)tetrathiafulvalene cations and antiferromagnetic oxalate-bridged copper(ii) dinuclear anions. Issue 7 (7th February 2022)

• Record Type: Journal Article
• Authors: Zhang, Bin; Zhang, Yan; Wang, Zheming; Wang, Dongwei; Yang, Deliang; Gao, Zengqiang; Chang, Guangcai; Guo, Yanjun; Mori, Takehiko; Zhao, Zhijuan; Liu, Fen; Li, Qiaolian; Zhu, Daoben
• Is Part Of: Journal of materials chemistry. Volume 10:Issue 7(2022)
• Page Start: 2845
• Page End: 2852
• Publication Date: 2022-02-07
• Subjects: Materials -- Periodicals; Chemistry, Analytic -- Periodicals; Optical materials -- Research -- Periodicals; Electronics -- Materials -- Research -- Periodicals; 543.0284
• DOI: 10.1039/d1tc04305f
• Languages: English
• ISSNs: 2050-7526

Abstract

Abstract : In (BEDT-TTF)3 [Cu2 (μ-C2 O4 )(C2 O4 )2 (CH3 OH)(H2 O)], BEDT-TTF stacks in β′′ mode and shows metallic conductivity. Hydrogen bonds between antiferromagnetic oxalate-bridged binuclear anions form a square lattice. No long range order observed to 2 K. Abstract : The organic–inorganic hybrid β′′-(BEDT-TTF)3 [Cu2 (μ–C2 O4 )(C2 O4 )2 (CH3 OH)(H2 O)] (BEDT-TTF = bis(ethylenedithio)tetrathia-fulvalene) composed of a BEDT-TTF donor and the oxalate-bridged binuclear anion [Cu2 (μ–C2 O4 )(C2 O4 )2 (CH3 OH)(H2 O) ]2− has been obtained by electrocrystallization. It crystallizes in the triclinic P 1̄ space group with cell parameters of a = 7.4803(3) Å, b = 9.3547(3) Å, c = 18.6711(7) Å, α = 95.797(3)°, β = 90.974(3)°, γ = 93.508(3)°, V = 1297.06(8) Å 3, and Z = 1 at 100 K. The donor arrangement belongs to the β′′ phase. From the TTF core bond lengths and Raman spectroscopy, the oxidation state of BEDT-TTF is assigned to ∼ + 2/3. CH3 OH or H2 O molecules bond to the metal atoms at the apical position of the square pyramid with an occupancy of 0.5. A supramolecular square lattice forms through hydrogen bonds between the antiferromagnetic binuclear anions in the anion sheet. From the band structure at 100 K, metallic conductivity is expected, which agrees with four-probe conductivity measurements: its conductivity is 11.5 S cm −1 at room temperature, increases to 160 S cm −1 at 7.6 K, and then decreases to 150 S cm −1 at 2 K. From magnetic measurements, there is no long-range magnetic ordering, which is confirmed by specific heat measurements.