Antiferromagnetic single-chain magnet slow relaxation in the {Tb(α-fur)3}n polymer with non-Kramers ions
Închide
Conţinutul numărului revistei
Articolul precedent
Articolul urmator
278 0
SM ISO690:2012
BARTOLOME, Bartolome, BARTOLOME, Juan, ARAUZO, A., LUZON, Javier, BADIA, L., CASES, Rafael, LUIS, Fernando, MELNYK, Silvia, PRODIUS, Denis, SHOVA, Sergiu, TURTA, Constantin. Antiferromagnetic single-chain magnet slow relaxation in the {Tb(α-fur)3}n polymer with non-Kramers ions. In: Journal of Materials Chemistry C, 2016, nr. 4(22), pp. 5038-5050. ISSN 2050-7534. DOI: https://doi.org/10.1039/c6tc00919k
EXPORT metadate:
Google Scholar
Crossref
CERIF

DataCite
Dublin Core
Journal of Materials Chemistry C
Numărul 4(22) / 2016 / ISSN 2050-7534

Antiferromagnetic single-chain magnet slow relaxation in the {Tb(α-fur)3}n polymer with non-Kramers ions

DOI:https://doi.org/10.1039/c6tc00919k

Pag. 5038-5050

Bartolome Bartolome1, Bartolome Juan2, Arauzo A.2, Luzon Javier3, Badia L.2, Cases Rafael2, Luis Fernando2, Melnyk Silvia4, Prodius Denis4, Shova Sergiu5, Turta Constantin4
 
1 Escola Universitària Salesiana de Sarrià (EUSS), Barcelona,
2 Universidad de Zaragoza,
3 Centro Universitario de la Defensa, Academia General Militar, Zaragoza,
4 Institute of Chemistry of the Academy of Sciences of Moldova,
5 “Petru Poni” Institute of Macromolecular Chemistry
 
 
Disponibil în IBN: 8 iulie 2022


Rezumat

We report the synthesis, crystal structure and magnetic properties of a new molecular complex based on a Tb(iii) ion supported by 2-furancarboxylic molecules: {Tb(α-fur)3(H2O)3}n (α-fur = C4H3OCOO). Two slightly different Tb sites (A and B) exist depending on the position of one of the dangling ligands. Ab initio calculations predict that, for both sites, the magnetic ground state is highly anisotropic (gz∗ = 17.8) and consists of a quasi-doublet with a small gap, well isolated from the next excited state. The α-fur ligand forms 1D polymeric chains of Tb ions of the same type (either A or B) running along the c-axis. The crystal structure is formed by the supramolecular stacking along the a-axis of 2D layers containing parallel chains of the same type. Static magnetization and heat capacity measurements show that, magnetically, the system can be modeled as an ensemble of Ising chains of non-Kramers Tb ions with effective spin S∗ = 1/2, antiferromagnetically (AF) coupled by a weak intrachain interaction (J∗/kB = -0.135 K). At very low temperatures, the static susceptibility reflects the presence of a 2-4% concentration of defects in the chains. Ac susceptibility measurements at H = 0 performed down to mK temperatures have enabled us to observe the slow relaxation of magnetization through two different pathways. They are assigned to Single-Chain-Magnet (SCM) behavior in two different types of AF chains (A and B), triggered by the existence of defects breaking the chains into segments with short-range order. At temperatures below 0.1 K this mechanism is replaced by individual relaxation of the ions through direct processes. Under the application of a magnetic field the system slowly relaxes by two distinct direct processes, strongly affected by a phonon bottleneck effect.

Cuvinte-cheie
Calculations, crystal structure, D region, defects, excited states, Ground state, Ions, ligands, magnetic susceptibility, magnetism, magnetization, Magnets, Polymers, Relaxation processes, specific heat, Synthesis (chemical)