We herein present the synthesis, crystal
structure, and magnetic properties of a new heterometallicchain of Mn
III and Ni
II ions, [Mn
2(saltmen)
2Ni(pao)
2(py)
2](ClO
4)
2 (
1) (saltmen
2- =
N,
N'-(1,1,2,2-tetramethylethylene) bis(salicylideneiminate) and pao
- = pyridine-2-aldoximate). The crystal
structure of
1 wasinvestigated by X-ray crystallographic analysis: compound
1 crystallized in monoclinic, space group
C2/
c(No. 15) with
a = 21.140(3) Å,
b = 15.975(1) Å,
c = 18.6212(4) Å,
![](/images/gifchars/beta2.gif)
= 98.0586(4)
![](/images/entities/deg.gif)
,
V = 6226.5(7) Å
3, and
Z = 4. This compound consists of two fragments, the out-of-plane dimer [Mn
2(saltmen)
2]
2+ as a coordinationacceptor building block and the neutral mononuclear unit [Ni(pao)
2(py)
2] as a coordination donor buildingblock, forming an alternating chain having the repeating unit [-Mn-(O)
2-Mn-ON-Ni-NO-]
n. In the crystal
structure, each chain is well separated with a minimum intermetallic distance between Mn and Ni ions of10.39 Å and with the absence of interchain
![](/images/gifchars/pi.gif)
overlaps between organic ligands. These features ensure agood magnetic isolation of the chains. The dc and ac magnetic measurements were performed on boththe polycrystalline sample and the aligned single crystals of
1. Above 30 K, the magnetic susceptibility ofthis one-dimensional compound was successfully described in a mean field approximation as an assemblyof trimers (Mn···Ni···Mn) with a Ni
II···Mn
III antiferromagnetic interaction (
J = -21 K) connected through aferromagnetic Mn
III···Mn
III interaction (
J'). However, the mean field theory fails to describe the magneticbehavior below 30 K emphasizing the one-dimensional magnetic character of the title compound. Between5 and 15 K, the susceptibility in the chain direction was fitted to a one-dimensional Ising model leading tothe same value of
J'. Hysteresis loops are observed below 3.5 K, indicating a magnet-type behavior. In thesame range of temperature, combined ac and dc measurements show a slow relaxation of the magnetization.This result indicates the presence of a metastable state without magnetic long-range order. This materialis the first experimental design of a heterometallic chain with
ST = 3 magnetic units showing a "single-chain magnet" behavior predicted in 1963 by R. J. Glauber for an Ising one-dimensional system. This workopens new perspectives for one-dimensional systems to obtain high temperature metastable magnets bycombining high spin magnetic units, strong interunit interactions, and uniaxial anisotropy.