Irreversible Structural Phase Transition in [(9‐triptycylammonium) ([18]crown‐6)][Ni(dmit)2]: Origin and Effects on Electrical and Magnetic Properties

Author:

Manabe Jun1ORCID,Sako Nagisa1,Ito Mizuki1,Fujibayashi Masaru2,Kato Chisato1,Cosquer Goulven34,Inoue Katsuya1345,Takahashi Kiyonori6,Nakamura Takayoshi6,Akutagawa Tomoyuki7,Shimono Seiya8,Ishibashi Hiroki9,Kubota Yoshiki9,Nishihara Sadafumi13510ORCID

Affiliation:

1. Department of Chemistry Graduate School of Advanced Science and Engineering Hiroshima University 1-3-1, Kagamiyama Higashi-hiroshima 739-8526 Japan

2. Department of Chemical and Biological Engineering National Institute of Technology, Ube College 2-14-1 Tokiwadai, Ube City Yamaguchi 755-8555 Japan

3. Chirality Research Center Hiroshima University 1-3-1, Kagamiyama Higashi-hiroshima 739-8526 Japan

4. International Institute for Sustainability with Knotted Chiral Meta Matter Hiroshima University 1-3-1, Kagamiyama Higashi-hiroshima 739-8526 Japan

5. Institute for Advanced Materials Research Hiroshima University 1-3-1, Kagamiyama Higashi-hiroshima 739-8526 Japan

6. Research Institute for Electronic Science Hokkaido University N20 W10, Kita-ku Sapporo 001-0020 Japan

7. Institute of Multidisciplinary Research for Advanced Materials Tohoku University 2-1-1 Katahira, Aoba-ku Sendai 980-8577 Japan

8. Japan Synchrotron Radiation Research Institute (JASRI), Spring-8 1-1-1, Kouto, Sayo Hyogo 679-5198 Japan

9. Department of Physics Osaka Metropolitan University Sakai Osaka 599-8531 Japan

10. Precursory Research for Embryonic Science and Technology Japan Science and Technology Agency 4-1-8, Honcho, Kawaguchi Saitama 332-0012 Japan

Abstract

AbstractMaterials 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 (JAC1/kB=−306(8), JAC2/kB=−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 (Jdimer/kB=−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.

Funder

Japan Society for the Promotion of Science

Japan Science and Technology Agency

Publisher

Wiley

Subject

Inorganic Chemistry

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