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Tuning the Magnetic Properties of the High‐Spin Molecular Cluster Fe 8
Author(s) -
Barra AnneLaure,
Bencini Fabio,
Caneschi Andrea,
Gatteschi Dante,
Paulsen Carley,
Sangregorio Claudio,
Sessoli Roberta,
Sorace Lorenzo
Publication year - 2001
Publication title -
chemphyschem
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.016
H-Index - 140
eISSN - 1439-7641
pISSN - 1439-4235
DOI - 10.1002/1439-7641(20010917)2:8/9<523::aid-cphc523>3.0.co;2-d
Subject(s) - chemistry , electron paramagnetic resonance , magnetization , superparamagnetism , monoclinic crystal system , crystallography , cluster (spacecraft) , perchlorate , ion , crystal structure , condensed matter physics , nuclear magnetic resonance , magnetic field , physics , quantum mechanics , computer science , programming language , organic chemistry
The synthesis, crystal structure, and magnetic characterization of a high‐spin cluster comprising eight iron ions are presented in this contribution. The cluster has formula [(tacn) 6 Fe 8 O 2 (OH) 12 Br 4.3 (ClO 4 ) 3.7 ]⋅6 H 2 O (Fe 8 pcl), where tacn is the organic ligand 1,4,7‐triazacyclononane. It can be considered a derivative of Fe 8 Br 8 , a cluster whose low‐temperature magnetization dynamics has been extensively investigated, in which four of the bromide ions have been replaced by perchlorate anions. The structure of the central core of the two molecules, [Fe 8 O(OH) 12 (tacn) 6 ] 8+ , is essentially the same, but Fe 8 pcl has a higher symmetry (the bromide derivative crystallizes in the acentric P 1 space group while Fe 8 pcl crystallizes in the monoclinic P 2 1 / c space group). The magnetic properties of Fe 8 pcl suggest it is very similar to Fe 8 Br 8 having a S =10 ground state as well. The zero‐field splitting parameters were accurately determined by high field–high frequency EPR (HF‐EPR) measurements. The two clusters have similar axial anisotropy D but Fe 8 pcl has a larger transverse anisotropy E : The value of E / D is 0.21 for the perchlorate derivative but 0.19 for Fe 8 Br 8 . AC susceptibility measurements revealed the cluster behaves like a superparamagnetic particle. However, due to the occurrence of large terms in the transverse anisotropy, the temperature dependence of the relaxation time cannot be reproduced by a simple Arrhenius law model. As observed in the bromide derivative, below 350 mK the relaxation time becomes temperature independent and indicating that a pure tunneling regime is attained. The comparison of the tunneling rate in the two clusters shows that in the perchlorate derivative the relaxation process is 35 times faster. The observed ratio of the tunneling rates is in reasonable agreement with that calculated from the tunneling splitting, namely the energy difference between the two almost‐degenerate lowest levels M s =±10, in the two clusters.