Abstract:This short review article provides the reader with a summary of the history of organic conductors. To retain a neutral and objective point of view regarding the history, background, novelty, and details of each research subject within this field, a thousand references have been cited with full titles and arranged in chronological order. Among the research conducted over ~70 years, topics from the last two decades are discussed in more detail than the rest. Unlike other papers in this issue, this review will he… Show more
“…30) Note that single-crystal X-ray structural analyses revealed that all the inner four chalcogen atoms in Fig. 1(a) possess equal electron densities; 28,35) thus, all the electron densities are obtained by averaging all the inner chalcogen atoms, suggesting a delocalized wave function. Instead of the previous localized wave functions of patterns 1 and 2, our new method provides a delocalized wave function, which is given by a linear combination of the patterns 1 and 2.…”
Section: Introductionmentioning
confidence: 98%
“…In Sect. 4, our calculation is compared with experimental results, 34,35) by choosing a reasonable magnitude of λ. Section 5 is devoted to a summary and comparison of the σ x /σ y of α-STF 2 I 3 with those of α-ET 2 I 3 and α-BETS 2 I 3 .…”
The electric conductivity of Dirac electrons in the organic conductor α-STF2I3 (STF = bis(ethylenedithio)diselenadithiafulvalene), which has an isostructure of α-(BEDT-TTF)2I3, has been theoretically studied using a two-dimensional tight-binding model in the presence of both impurity and electron-phonon (e-p) scatterings. In contrast to α-(BEDT-TTF)2I3, which has a Dirac cone with almost isotropic velocity, α-STF2I3 provides a large anisotropy owing to a Dirac point that is close to merging. As a result, σx becomes much larger than σy, where σy and σx are diagonal conductivities parallel and perpendicular to a stacking axis of molecules, respectively. With increasing temperature (T ), σx takes a broad maximum because of e-p scattering and σy remains almost constant. The ratio σx/σy is analyzed in terms of the band structure. Such an exotic conductivity of α-STF2I3 is compared with that of an experiment showing a good correspondence. Finally, σx/σy values of α-ET2I3 and α-BETS2I3 are shown to demonstrate the dissimilarity with α-STF2I3.
“…30) Note that single-crystal X-ray structural analyses revealed that all the inner four chalcogen atoms in Fig. 1(a) possess equal electron densities; 28,35) thus, all the electron densities are obtained by averaging all the inner chalcogen atoms, suggesting a delocalized wave function. Instead of the previous localized wave functions of patterns 1 and 2, our new method provides a delocalized wave function, which is given by a linear combination of the patterns 1 and 2.…”
Section: Introductionmentioning
confidence: 98%
“…In Sect. 4, our calculation is compared with experimental results, 34,35) by choosing a reasonable magnitude of λ. Section 5 is devoted to a summary and comparison of the σ x /σ y of α-STF 2 I 3 with those of α-ET 2 I 3 and α-BETS 2 I 3 .…”
The electric conductivity of Dirac electrons in the organic conductor α-STF2I3 (STF = bis(ethylenedithio)diselenadithiafulvalene), which has an isostructure of α-(BEDT-TTF)2I3, has been theoretically studied using a two-dimensional tight-binding model in the presence of both impurity and electron-phonon (e-p) scatterings. In contrast to α-(BEDT-TTF)2I3, which has a Dirac cone with almost isotropic velocity, α-STF2I3 provides a large anisotropy owing to a Dirac point that is close to merging. As a result, σx becomes much larger than σy, where σy and σx are diagonal conductivities parallel and perpendicular to a stacking axis of molecules, respectively. With increasing temperature (T ), σx takes a broad maximum because of e-p scattering and σy remains almost constant. The ratio σx/σy is analyzed in terms of the band structure. Such an exotic conductivity of α-STF2I3 is compared with that of an experiment showing a good correspondence. Finally, σx/σy values of α-ET2I3 and α-BETS2I3 are shown to demonstrate the dissimilarity with α-STF2I3.
“…Concerning the general molecular systems, the electronic structures including those under high pressure are calculated by DFT methods [10][11][12]. Although DESs were initially found in graphene [13,14] and some inorganic compounds [15], those found in organic compounds [16] possess clear advantages over their inorganic counterparts. For example, most organic DESs are found in bulk systems with well-defined crystal structures and chemical stoichiometries, whereas inorganic DESs often lack either of these two features.…”
Topological materials with Dirac electron systems have been extensively studied. Organic crystalline materials form a unique group of such compounds with well-defined crystal structures. While most organic compounds require high pressures to exhibit Dirac-cone-type band structures, the title compound, α-STF2I3, has garnered increasing interest due to its Dirac-cone-type band structure under ambient pressure. Various experiments have been conducted under ambient pressure; their results can be compared with those of theoretical calculations to obtain insights into Dirac electron systems. However, structural disorder peculiar to the STF molecules in the solid-state has prevented any type of theoretical calculation of the states. In this study, we report a new method for calculating intermolecular interactions in disordered systems based on the extended Hückel approximation. This method enables band calculations, suggesting that this material is a rare example of a system close to merging. The obtained band structure indicates that the characteristic disorder in the STF solids distributed electrons equally on the sulphur and selenium atoms as if they belong to an imaginary element between sulphur and selenium and are arranged without disorder.
“…Radical-cation salts and charge transfer complexes based on derivatives of tetrathiafulvalene (TTF) constitute a wide class of organic materials with transport properties ranging from insulating to superconducting [1][2][3][4]. This work is part of the systematic study of radical-cation salts of tetrathiafulvalene and its derivatives with metallacarborane anions, of which earlier results were summarized in works [5][6][7].…”
Section: Introductionmentioning
confidence: 99%
“…Although most of the compounds studied were BEDT-TTF-based radical-cation salts, recently, we have synthesized radical-cation salts based on such unconventional and rather exotic donors as bis (1,3-propylenedithio)tetrathiafulvalene [8,9], dibenzotetrathiafulvalene [10], and 4,5-ethylenedithio-4 ,5 -(2-oxa-1,3-propylenedithio)-tetrathiafulvalene [9]. On the other hand, although compounds of the composition (TMTXF) 2 Y (X = T, S) are usually classical organic metals among which the first organic superconductors were discovered [4,7], and TMTTF and TMTSF radical-cation salts continue to attract the attention of researchers [11][12][13][14][15], very little attention has been paid to TMTTF and TMTSF radical-cation salts with metallacarborane anions [16][17][18][19]. This prompted us to prepare and investigate new TMTTF and TMTSF radical-cation salts with metallacarborane anions.…”
New radical-cation salts based on tetramethyltetrathiafulvalene (TMTTF) and tetramethyltetraselenefulvalene (TMsTSF) with metallacarborane anions (TMTTF)[3,3′-Cr(1,2-C2B9H11)2], (TMTTF)[3,3′-Fe(1,2-C2B9H11)2], and (TMTSF)2[3,3′-Cr(1,2-C2B9H11)2] were synthesized by electrocrystallization. Their crystal structures were determined by single crystal X-ray diffraction, and their electrophysical properties in a wide temperature range were studied. The first two salts are dielectrics, while the third one is a narrow-gap semiconductor: σRT = 5 × 10−3 Ohm−1cm−1; Ea ≈ 0.04 eV (aprox. 320 cm−1).
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.