2013
DOI: 10.1039/c3dt52346b
|View full text |Cite
|
Sign up to set email alerts
|

Structures and properties of a BEDT-TTF-based organic charge transfer salt and the zwitterion of ferrocenesulfonate

Abstract: The structure and properties of a new semiconducting BEDT-TTF-based charge-transfer salt containing the ferrocenesulfonate (Fc-SO3(-)) anion, α-(BEDT-TTF)2Fc-SO3·2.5H2O, are described. The structure and magnetic properties of a zwitterion of ferrocenesulfonate, Fc(+)-SO3(-), are also reported.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2

Citation Types

2
3
0

Year Published

2015
2015
2022
2022

Publication Types

Select...
6

Relationship

3
3

Authors

Journals

citations
Cited by 7 publications
(5 citation statements)
references
References 19 publications
(18 reference statements)
2
3
0
Order By: Relevance
“…The magnetic data can be fitted by the combination of a Curie–Weiss ( C = 0.721 emu K mol –1 ) and 2D Heisenberg (2DH) models with θ = –5.5 K and J 2DH = –80.3 K. This suggests that the spins of the Fc moieties and BEDT‐TTF layers obey 2D Heisenberg and Curie–Weiss models, respectively. The J 2DH value of –80.3 K caused by the interaction between spins on the BEDT‐TTF layers almost corresponds to those observed in other salts having 2D magnetic BEDT‐TTF layers , . The spins seem to form a square lattice and to interact with each other along the a and b directions (see Figure b).…”
Section: Resultssupporting
confidence: 70%
See 2 more Smart Citations
“…The magnetic data can be fitted by the combination of a Curie–Weiss ( C = 0.721 emu K mol –1 ) and 2D Heisenberg (2DH) models with θ = –5.5 K and J 2DH = –80.3 K. This suggests that the spins of the Fc moieties and BEDT‐TTF layers obey 2D Heisenberg and Curie–Weiss models, respectively. The J 2DH value of –80.3 K caused by the interaction between spins on the BEDT‐TTF layers almost corresponds to those observed in other salts having 2D magnetic BEDT‐TTF layers , . The spins seem to form a square lattice and to interact with each other along the a and b directions (see Figure b).…”
Section: Resultssupporting
confidence: 70%
“…375) of 1.096 emu K mol –1 , suggesting that the stable radical parts and also the BEDT‐TTF layers possess spins. Since the observed χT value is approximately 0.1 emu K mol –1 smaller than the expected value, this implies that there are strong antiferromagnetic interactions, which are usually observed between spins on BEDT‐TTF layers , . These results support the hypothesis that spins are located on the BEDT‐TTF layers.…”
Section: Resultssupporting
confidence: 63%
See 1 more Smart Citation
“…TTF analogues have been synthesized by coupling and without coupling methods [ 45 46 ]. Depending on the presence of electron-withdrawing groups on the TTF, they exhibit various oxidation potential ranges [ 15 , 26 ]. Recently, TTF and analogues have received widespread attention involving the development of new materials by using various anions to form different charge transfer salts.…”
Section: Introductionmentioning
confidence: 99%
“…For the insulators and semiconductors, the charge carriers cannot freely move and are localized on the donor layers, providing various magnetic ground states. The range of ground states include antiferromagnetic and canted ferromagnetic orderings, spin density wave, 1D and 2D Heisenberg magnets, and compounds characterized by a singlet–triplet model . The magnetic moment is not localized in an atomic orbital, as in transition-metal magnets, and not localized in a specific part of a molecule, as in organic radicals, but is delocalized across a whole BEDT-TTF molecule.…”
mentioning
confidence: 99%