Nuclear and electronic resonance approaches to magnetic and lattice fluctuations in the two-chain family of organic compounds (perylene)2[M(S2C2(CN)2)2] (M=Pt,Au)

C. Bourbonnais, R. T. Henriques, P. Wzietek, D. Köngeter, J. Voiron, and D. Jérme
Phys. Rev. B 44, 641 – Published 1 July 1991
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Abstract

In this work we present and analyze the temperature dependence of the H1 nuclear-spin-lattice relaxation rate and of the magnetic susceptibility of the two-chain organic compound (Per)2[Pt(mnt)2]. [Here, ‘‘Per’’ is perylene; ‘‘mnt’’ stands for maleonitriledithiolate, which is the same as cis-(2,3-dimercapto-2-butenedinitrile).] The analysis confirms the existence of localized spins on the Pt(mnt)2 chains and their dominant influence on the relaxation through an interstack dipolar coupling. A scaling relation of the form T11Tχs(T) is found to exist in the entire temperature domain, including the regime of one-dimensional spin-Peierls Pt(mnt)2 lattice fluctuations observed by x-ray experiments below 30 K. The magnetic-field dependence of the relaxation is also found to qualitatively agree with one-dimensional spin diffusion which is cut off in the low-field region. A comparison is made to data obtained for (Per)2[Au(mnt)2], which have a completely different T11 temperature dependence. This is demonstrated to be a characteristic of itinerant electrons. Finally we analyze the existing EPR data on (Per)2[Pt(mnt)2] and show that the observed low-temperature linear temperature profile of the EPR linewidth results from the existence of an exchange coupling between the itinerant and the localized spins of different stacks. Similar conclusions previously made for Per2[Pd(mnt)2] allow one to study such two-chain compounds as realizations of a one-dimensional Kondo lattice. We discussed several puzzling questions raised by the analysis concerning possible mechanisms that can lead to a spin-Peierls distortion.

  • Received 8 October 1990

DOI:https://doi.org/10.1103/PhysRevB.44.641

©1991 American Physical Society

Authors & Affiliations

C. Bourbonnais

  • Laboratoire de Physique des Solides, Université de Paris–Sud, Bâtiment 510, Orsay, F-91405, France
  • Centre de Recherche en Physique du Solide, Département de Physique, Université de Sherbrooke, Sherbrooke, PQ, Canada J1K 2R1

R. T. Henriques

  • Laboratoire de Physique des Solides, Université de Paris–Sud, Bâtiment 510, Orsay, F-91405, France
  • Laboratório Nacional de Engenharia e Tecnologia Industrial, Departamento de Química, P-2685 Sacavém, Portugal

P. Wzietek and D. Köngeter

  • Laboratoire de Physique des Solides, Université de Paris–Sud, Bâtiment 510, Orsay, F-91405, France

J. Voiron

  • Laboratoire Louis Néel, Centre National de Recherche Scientifique, 166X, F-38042 Grenoble CEDEX, France

D. Jérme

  • Laboratoire de Physique des Solides, Université de Paris–Sud, Bâtiment 510, Orsay, F-91405, France

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Issue

Vol. 44, Iss. 2 — 1 July 1991

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