We present the first BICAAC adducts of ECl3 (E=P, Sb) and a phosphaalkene, (BICAAC)=P−Ph stabilized by BICAAC (BICAAC=bicyclic (alkyl)(amino)carbene)). Further, strong π-acceptor character of BICAAC has been exploited in three electron...
![Irreversible Structural Phase Transition in [(9‐triptycylammonium) ([18]crown‐6)][Ni(dmit)2]: Origin and Effects on Electrical and Magnetic Properties](https://chemistry-europe.onlinelibrary.wiley.com/cms/asset/eab6cfdc-0425-4a44-ac7d-a71c13ef2843/ejic202300449-toc-0001-m.png)
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Irreversible Structural Phase Transition in [(9‐triptycylammonium) ([18]crown‐6)][Ni(dmit)2]: Origin and Effects on Electrical and Magnetic Properties
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Two salts, [(9-triptycylammonium)([18]crown-6)][Ni(dmit)2] (1) and [(9-triptycylammonium)([15]crown-5)][Ni(dmit)2] (2) were prepared and characterized. [Ni(dmit)2]− formed dimers in 1 but was arranged in zigzag stacks in 2. At 381 K, 1 underwent an irreversible phase transition originating from the rearrangement of [Ni(dmit)2] dimers and therefore experienced a drastic change in magnetic and electrical properties.
Abstract
Materials exhibiting irreversible phase transitions, leading to changes in their properties, have a potential for novel application in electronic components such as a non-rewritable high-security memory. Here, we focused on the two salts, [(9-triptycylammonium)([18]crown-6)][Ni(dmit)2] (1) and [(9-triptycylammonium)([15]crown-5)][Ni(dmit)2] (2), which featured 2D sheet structures with alternately stacked cation and anion layers. Both salts exhibit similar cation arrangements, however, their anion arrangements differ significantly. The temperature-dependent magnetic susceptibilities of 1 and 2 were well reproduced by the alternating chain model (J AC1/k B=−306(8), J AC2/k B=−239(3) K) and the Curie-Weiss model (θ=−3.9(1) K), respectively. 1 experience a reversible phase transition around 40–60 K, causing anomalies in magnetic behavior. Moreover, an irreversible single-crystal-to-single-crystal phase transition to 1′ undergo at ~381 K, inducing a rearrangement of [Ni(dmit)2]− anions and a resistivity decrease from 6.5×106 to 6.5×102 Ω cm. The susceptibility curve of 1′ was reproduced by a combination of the Curie-Weiss and dimer models (J dimer/k B=−407(5), θ=−26.7(5) K). The irreversible transition of 1 is the first example for such supramolecule and [Ni(dmit)2]− system to our knowledge, in opening potential new-type materials.
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