Issue
J. Phys. IV France
Volume 131, December 2005
Page(s) 307 - 311
DOI https://doi.org/10.1051/jp4:2005131078
Published online 18 January 2006
International Workshop on Electronic Crystals
S. Brazovskii, P. Monceau and N. Kirova
J. Phys. IV France 131 (2005) 307-311

DOI: 10.1051/jp4:2005131078

Functional $\pi$-donors with no symmetry and Mott physics

P. Batail1, 0, K. Heuzé1, S.A. Baudron1, M. Fourmigué1, C. Coulon2, R. Clérac2, E. Canadell3, V. Laukhin3, P. Auban-Senzier4, R. Melzi4, P. Wzietek4 and D. Jérome4

1  Chimie, Ingénierie Moléculaire et Matériaux UMR 6200 CNRS-Université d'Angers, 2 boulevard Lavoisier, 49045 Angers, France
2  Centre de Recherches Paul Pascal (CRPP-CNRS, UPR 8641), 115 avenue Dr. Schweitzer, 33600 Pessac, France
3  Institut de Ciència de Materials de Barcelona (ICMAB-CSIC), Campus de la UAB, 08193 Bellaterra, Spain
4  Laboratoire de Physique des Solides, UMR 8502 CNRS-Université de Paris-Sud, 91405 Orsay, France


Abstract
Crystal engineering principles serve as a guide for the design of quantum materials based on hydrogen-bond donor/acceptor-functionalized $\pi$-donors of C1 symmetry as illustrated by $\delta $-(EDT-TTF-CONMe2)2AsF6, a non-dimerized, 1/4-filled band Mott insulator and (EDT-TTF-CONH2)6[ Re6Se8(CN)6] , a metallic molecular Kagomé ( $\rm S = 1/2$)where molecular movements are coupled to a Mott localization.



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