Login / Signup

Bulky anion effect on the architecture of chiral dysprosium single-molecule magnets.

Haiet DouibKais DhbaibiBertrand LefeuvreVincent DorcetThierry GuizouarnFabrice Pointillart
Published in: Chirality (2022)
The interest for chiral tris(β-diketonato)lanthanide complexes in coordination chemistry is huge due to its Lewis acid character, optical activity, and the control of the final compound architecture. The reaction of equimolar quantities of [Dy((-)/(+)hfc) 3 (H 2 O)] (hfc -  = 3-(heptafluoropropylhydroxymethylene)-(+/-)-camphorate) and L led to the formation of a pair of enantiomers for dinuclear complexes [Dy((-)/(+)hfc) 3 (L)] 2 ⋅C 7 H 16 ([(-)/(+)1]⋅C 7 H 16 ) (L = 4'-(4'''-pyridyl-N-oxide)-1,2':6'1''-bis-(pyrazolyl)pyridine]). Starting from the previous experimental protocol with the addition of bulky BArF anions, a partial dissociation of the chiral [Dy((-)/(+)hfc) 3 (H 2 O)] was observed leading to the isolation of a mono-dimensional cationic chiral polymer {[Dy((-)/(+)hfc) 2 (L)][BarF]} n ⋅nCH 3 NO 2 ([(-)/(+)2] n ⋅nCH 3 NO 2 ). Natural circular dichroism (NCD) highlighted an exciton CD couplet for [(-)/(+)2] n but not for (-)/(+)1. The latter behaves as a single-molecule magnet (SMM) with a blocking temperature up to 4 K, whereas [(-)/(+)2] n is a 1D assembly of field-induced SMMs with a magnetic relaxation occurring through a Raman process only.
Keyphrases