Abstract

We have prepared two dmit-based salts with a stable organic radical-substituted ammonium cation, (PO-CONH-C2H4N(CH3)3)[Ni(dmit)2]2·CH3CN and (PO-CONH-C2H4N(CH3)3)[Pd(dmit)2]2 where PO is 2,2,5,5-Tetramethyl-3-pyrrolin-1-oxyl and dmit is 2-Thioxo-1,3-dithiol-4,5-dithiolate. The salts are not isostructural but have similar structural features in the anion and cation packing arrangements. The acceptor layers of both salts consist of tetramers, which gather to form 2D conducting layers. Magnetic susceptibility measurements indicate that the Ni salt is a Mott insulator and the Pd salt is a band insulator, which has been confirmed by band structure calculations. The cationic layers of both salts have a previously unreported polar structure, in which the cation dipoles order as ➚➘➚➘ along the acceptors stacking direction to provide dipole moments. The dipole moments of nearest neighbor cation layers are inverted in both salts, indicating no net dipole moments for the whole crystals. The magnetic network of the [Ni(dmit)2] layer of the Ni salt is two-dimensional so that the magnetic susceptibility would be expected to obey the 1D or 2D Heisenberg model that has a broad maximum around T ≈ θ. However, the magnetic susceptibility after subtraction of the contribution from the PO radical has no broad maximum. Instead, it shows Curie–Weiss behavior with C = 0.378 emu·K/mol and θ = −35.8 K. The magnetic susceptibility of the Pd salt obeys a Curie–Weiss model with C = 0.329 emu·K·mol−1 and θ = −0.88 K.

Highlights

  • Over the past two decades, organic magnetic conductors that combine electrical conductivity with magnetic moments have attracted great interest [1,2,3]. This is due to reports of unique and interesting properties that emerge from the interplay between itinerant and localized electrons

  • Λ-(BETS)2 FeCl4 (BETS = bis(ethylenedithio)tetraselenafulvalene) and its derivatives show unique physical properties such as a transition to antiferromagnetic order coupled to a metal-insulator transition, colossal magnetoresistance, field-induced superconductivity and a superconductor-to-insulator transition [1]

  • We report organic magnetic conductors consisting ofas salts have a dipole moment, which cancels that of the anionic layers

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Summary

Introduction

Over the past two decades, organic magnetic conductors that combine electrical conductivity with magnetic moments have attracted great interest [1,2,3]. 1a) centers is surrounded by the negative ends of the anionic layer’s dipole and the other noted that some of dipole these salts have unique structural which we Type have (B) isRecently, borderedwe byhave the positive ends of the moments. There are many types ofanionic organic conductors, salts with a conducting donor and acounter‐anion consequence,are salts have two crystallographically independent cation layers B), one the most widely researched, and it is clear that this type has the greatest number of (A in surrounded by the negative ends of the we anionic layer’sconcentrated dipole and the of which examples of Figure metals 1a) andissuperconductors This is the reason why previously on other (B) is bordered by the ends ofmagnetic the dipole moments. A new organic cation bearing PO radical, PO–CONH–C2H4N(CH3) (C1 ), the molecular shape of we do not understand theofreason why these specific salts apossess polarized anionicfeature, layers, it which is similar to that

Molecular
Discussion
Crystal
Materials and Methods
Table are listed in Tableresistance
C26 H27 O2 N3 S20 Pd2
Conclusions

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