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Phys. Rev. B 39, 10682–10692 (1989)

Long-range carrier-mediated Cu-Cu interactions and low-temperature transitions in the quasi-one-dimensional CuxNi1-x(phthalocyanine)I alloys

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Michael Y. Ogawa, Sharon M. Palmer, and Kwangkyoung Liou
Department of Chemistry and Materials Research Center, Northwestern University, Evanston, Illinois 60201

Guy Quirion
Centre de Recherche en Physique du Solide, Départment de Physique, Université de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1

Julia A. Thompson
Department of Chemistry and Materials Research Center, Northwestern University, Evanston, Illinois 60201

Mario Poirier
Centre de Recherche en Physique du Solide, Départment de Physique, Université de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1

Brian M. Hoffman
Department of Chemistry and Materials Research Center, Northwestern University, Evanston, Illinois 60201

Received 8 September 1988; published in the issue dated 15 May 1989

A series of alloys CuxNi1-x(PC)I (PC = phthalocyanine) of the two isostructural molecular conductors, phthalocyaninato nickel(II) iodide, Ni(PC)I, and phthalocyaninato copper(II) iodide, Cu(PC)I, have been prepared. These crystals contain partially oxidized M(PC) stacks and are quasi-one-dimensional molecular metals whose charge carriers are associated with the highest occupied π molecular orbitals of the PC macrocycles. The Cu2+ (S=(1/2) local moments of CuxNi1-x (PC)I remain exchange coupled even when the paramagnetic metal-ion chain incorporated within the M(PC) stacks is diluted (x≪1) with the diamagnetic Ni2+ ions and the Cu magnetization is also coupled to the itinerant π-electron charge carriers. For alloys with x≥0.1, the EPR signal of the coupled magnetization exhibits two anomalies at low temperature. The g values and linewidths first begin to deviate from their high-temperature behavior at Ta∼25 K, roughly independent of composition for 0.05≤x<1. A more dramatic response of the linewidth occurs upon cooling through Tb, which decreases from ∼8 K as x is reduced from 1.0. Surprisingly, the g value of the x=0.50 alloy at low temperature shows a field dependence: At X-band frequency, g? increases to ∼2.21 by T∼2.3 K, a g value much larger than that of the parent Cu(PC) (g?=2.18); this anomaly is quenched at a higher observing field (Q-band frequency). These alloys are highly conducting, as are the two parent materials. The dependence of the conductivity on x indicates that σ(T) is governed by magnetic scattering by the Cu2+ ions. In the low-temperature region, the results for the four-probe and microwave conductivity differ sharply in a composition-dependent fashion and indicate a novel coupling between dielectric and magnetic properties.

© 1989 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.39.10682
DOI:
10.1103/PhysRevB.39.10682
PACS:
72.15.Nj, 72.15.Qm, 75.30.Mb