Symmetry breaking and light-induced spin-state trapping in a mononuclear FeII complex with the two-step thermal conversion

M. Buron-Le Cointe, N. Ould Moussa, E. Trzop, A. Moréac, G. Molnar, L. Toupet, A. Bousseksou, J. F. Létard, and G. S. Matouzenko
Phys. Rev. B 82, 214106 – Published 10 December 2010

Abstract

Crystallographic, magnetic, and Raman investigations of the mononuclear [FeII(Hpy-DAPP)](BF4)2 complex are presented. Its particular feature is a two-step thermal spin conversion in spite of a unique symmetry-independent iron site per unit cell. The plateau around 140 K is associated with a symmetry breaking visible by the appearance of weak (0k0) k odd Bragg peaks. Symmetries of the high-temperature high-spin state and of the low-temperature low-spin state are both monoclinic P21/c, so that the symmetry breaking on the plateau is associated with a reentrant phase transition. It is discussed in relation with Ising-type microscopic models. At the plateau level, the two symmetry-independent molecules differ both by their spin state and the conformation (chair versus twist-boat) of one metallocycle. At low-temperature photoinduced phenomena have been investigated: a partial phototransformation [light-induced excited spin-state trapping (LIESST) effect] is observed under visible red irradiation. Raman spectroscopy shows that the molecular photoinduced state is the high-spin one. Nevertheless, as no macroscopic symmetry breaking is observed, the unique average cationic [FeII(Hpy-DAPP)] state of the unit cell is intermediate between pure low-spin and high-spin states and presents a conformational disorder for one metallocycle. Reverse-LIESST has also been evidenced using near infrared excitation. Thus, the mononuclear [Fe(Hpy-DAPP)](BF4)2 compound offers the opportunity to discuss the interplay between spin conversion, molecular conformational change, and ordering processes.

    • Received 7 September 2010

    DOI:https://doi.org/10.1103/PhysRevB.82.214106

    ©2010 American Physical Society

    Authors & Affiliations

    M. Buron-Le Cointe1,*, N. Ould Moussa1,2, E. Trzop1, A. Moréac1, G. Molnar2, L. Toupet1, A. Bousseksou2, J. F. Létard3, and G. S. Matouzenko4

    • 1Institut de Physique de Rennes, Université de Rennes 1–CNRS, UMR 6251, Bât. 11A Campus de Beaulieu, 35042 Rennes, France
    • 2Laboratoire de Chimie de Coordination, CNRS UPR-8241, Université de Toulouse, INP, UPS, 31077 Toulouse, France
    • 3ICMCB, CNRS–Université Bordeaux, 87 Av. du Doc. A. Schweitzer, 33608 Pessac, France
    • 4Laboratoire de Chimie, CNRS–Ecole Normale Supérieure de Lyon, UMR 5182, 46 allée d’Italie, 69364 Lyon Cédex 07, France

    • *Corresponding author; marylise.buron@univ-rennes1.fr

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    Issue

    Vol. 82, Iss. 21 — 1 December 2010

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