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Uncommon lanthanide ions in purely 4f Single Molecule Magnets

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TLDR
The use of lanthanide ions in the design of SMMs exploded with the discovery of the first example of mononuclear TbIII-based complex which displayed a slow magnetic relaxation in 2003 as discussed by the authors.
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This article is published in Coordination Chemistry Reviews.The article was published on 2017-09-01 and is currently open access. It has received 229 citations till now. The article focuses on the topics: Lanthanide.

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Revised effective ionic radii and systematic studies of interatomic distances in halides and chalcogenides

TL;DR: The effective ionic radii of Shannon & Prewitt [Acta Cryst. (1969), B25, 925-945] are revised to include more unusual oxidation states and coordinations as mentioned in this paper.
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Magnetic bistability in a metal-ion cluster

TL;DR: In this article, it was shown that the magnetization of the Mn12 cluster is highly anisotropic and the magnetisation relaxation time becomes very long below a temperature of 4 K, giving rise to pronounced hysteresis.
Journal ArticleDOI

Exploiting single-ion anisotropy in the design of f-element single-molecule magnets

TL;DR: In this paper, a qualitative method for predicting the ligand architectures that will generate magnetic anisotropy for a variety of f-element ions is presented to guide the design of stronger single-molecule magnets incorporating the f-elements.
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Q1. What contributions have the authors mentioned in the paper "Uncommon lanthanide ions in purely 4f single molecule magnets" ?

This review presents the research endeavour in the area of these uncommon lanthanide-based SMMs and underlines the different approaches to better understand their physical properties. 

The possibility to observe slow magnetic relaxation for the Ce III ion in eight-coordination was discarded due to the low symmetry of the coordination sphere and the isotropic nature of the ligands composing the coordination sphere. 

One can take in his mind that the rarity of Ho III -based SMM can be due to the non-Kramers nature of such lanthanide, which places constraints on the symmetry of the coordination environment needed for SMM behaviour, and to the fact the 4f electron density is not very anisotropic. 

The absence of SMM behaviour without external field wasattributed to the significant transversal g factors and the large tunnelling gap in the ground exchange doublet (0.01 cm -1 ) allowing a strong quantum tunnelling of the magnetization. 

Above 3K, the extracted energy barrier of 19.5 K is one of the highest for Yb-based SMM while the relaxation time of 1.0×10-7 s is classical for such systems. 

In this molecule the antiferromagnetic interactions between spins of Mn III and Mn IV ions stabilize a S=10 spin ground-state which can be trapped in up (Ms = +S) or down (Ms = -S) orientations. 

Attempts to reproduce the static magnetic properties were done using an extendedStevens operators technique taking into account both crystal field effects and possible ferromagnetic interactions (because of the increase of χMT vs. T curve below 9 K (Figure 9b)). 

As for almost all YbIII-based SMMs, no out-of-phase signal of the magneticsusceptibility is observed without applied magnetic field, whereas an optimal field of 1000 

The lanthanide mononuclear SMM started in 2003 with the association of a Dy III ionand double Decker ligands [95], while the first uncommon lanthanide ion involved in a SMM was HoIII in 2005 [96]. 

Gao et al. associated an equatorial ligand such as COT ligand (L 21 , Scheme 3) in order to satisfy the Ising limit condition for a lanthanide ion with a prolate electron density. 

two other strategies to obtain SMM with this kind of lanthanide ions were already successful: i) the insertion of diamagnetic ions such as Zn II which add an electrostatic effect on the active centre and ii) the doping of the active SMM with a second 4f element. 

As for 17, no out-of-phase signal of the magnetic susceptibility is observed without magnetic field while a weak field leads to its appearance (200 Oe). 

The energy gap between the ground- and first excited-states was estimated to 130 cm-1 for 4 which is one order of magnitude higher than the energy gap found for the Er III and Dy III analogues. 

the NdIII ion which possesses a 4f3 electronic configuration could be also a potential candidate for the elaboration of SMM. 

In other words, the nature of the first neighbouring atoms (oxygen vs. nitrogen) induces two different distortion of the D4d coordination polyhedron (compressed vs. elongated).