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X-ray crystallographic analysis of the antiferromagnetic low-temperature phase of galvinoxyl: investigating magnetic duality in organic radicals.
Suizu, Rie; Shuku, Yoshiaki; Robert, Vincent; Roseiro, Pablo; Ben Amor, Nadia; Khawar, Zain; Robertson, Neil; Awaga, Kunio.
Afiliação
  • Suizu R; Department of Chemistry & Integrated Research Consortium on Chemical Sciences (IRCCS), Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan. awaga.kunio.h8@f.mail.nagoya-u.ac.jp.
  • Shuku Y; Japan Science and Technology Agency (JST), PRESTO, 4-1-8 Honcho, Kawaguchi, Saitama 332-0012, Japan.
  • Robert V; Department of Chemistry & Integrated Research Consortium on Chemical Sciences (IRCCS), Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan. awaga.kunio.h8@f.mail.nagoya-u.ac.jp.
  • Roseiro P; Université de Strasbourg, CNRS, Laboratoire de Chimie Quantique UMR 7177, 67000 Strasbourg, France.
  • Ben Amor N; Université de Strasbourg, CNRS, Laboratoire de Chimie Quantique UMR 7177, 67000 Strasbourg, France.
  • Khawar Z; Laboratoire de Physique et Chimie Quantiques, UMR 5626 Université Paul Sabatier, 118 route de Narbonne, 31062 Toulouse, France.
  • Robertson N; School of Chemistry, The University of Edinburgh, Joseph Black Building, David Brewster Road, Edinburgh EH9 3FJ, UK.
  • Awaga K; School of Chemistry, The University of Edinburgh, Joseph Black Building, David Brewster Road, Edinburgh EH9 3FJ, UK.
Dalton Trans ; 53(5): 1961-1965, 2024 Jan 30.
Article em En | MEDLINE | ID: mdl-38099702
ABSTRACT
Galvinoxyl, as one of the most extensively studied organic stable free radicals, exhibits a notable phase transition from a high-temperature (HT) phase with a ferromagnetic (FM) intermolecular interaction to a low-temperature (LT) phase with an antiferromagnetic (AFM) coupling at 85 K. Despite significant research efforts, the crystal structure of the AFM LT phase has remained elusive. This study successfully elucidates the crystal structure of the LT phase, which belongs to the P1̄ space group. The crystal structure of the LT phase is found to consist of a distorted dimer, wherein the distortion arises from the formation of short intermolecular distances between anti-node carbons in the singly-occupied molecular orbital (SOMO). Starting from the structure of the LT phase, wave function calculations show that the AFM coupling 2J/kB varies significantly from -1069 K to -54 K due to a parallel shift of the molecular planes within the dimer.

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2024 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2024 Tipo de documento: Article