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Anion-Templated Assembly and Magnetocaloric Properties of a Nanoscale {Gd38} Cage versus a {Gd48} Barrel.
- Source :
- Chemistry - A European Journal; Oct2013, Vol. 19 Issue 44, p14876-14885, 10p
- Publication Year :
- 2013
-
Abstract
- The comprehensive study reported herein provides compelling evidence that anion templates are the main driving force in the formation of two novel nanoscale lanthanide hydroxide clusters, {Gd<subscript>38</subscript>(ClO<subscript>4</subscript>)<subscript>6</subscript>} ( 1) and {Gd<subscript>48</subscript>Cl<subscript>2</subscript>(NO<subscript>3</subscript>)} ( 2), characterized by single-crystal X-ray crystallography, infrared spectroscopy, and magnetic measurements. {Gd<subscript>38</subscript>(ClO<subscript>4</subscript>)<subscript>6</subscript>}, encapsulating six ClO<subscript>4</subscript><superscript>−</superscript> ions, features a cage core composed of twelve vertex-sharing {Gd<subscript>4</subscript>} tetrahedrons and one Gd⋅⋅⋅Gd pillar. When Cl<superscript>−</superscript> and NO<subscript>3</subscript><superscript>−</superscript> were incorporated in the reaction instead of ClO<subscript>4</subscript><superscript>−</superscript>, {Gd<subscript>48</subscript>Cl<subscript>2</subscript>(NO<subscript>3</subscript>)} is obtained with a barrel shape constituted by twelve vertex-sharing {Gd<subscript>4</subscript>} tetrahedrons and six {Gd<subscript>5</subscript>} pyramids. What is more, the cage-like {Gd<subscript>38</subscript>} can be dynamically converted into the barrel-shaped {Gd<subscript>48</subscript>} upon Cl<superscript>−</superscript> and NO<subscript>3</subscript><superscript>−</superscript> stimulus. To our knowledge, it is the first time that the linear M-O-M′ fashion and the unique μ<subscript>8</subscript>-ClO<subscript>4</subscript><superscript>−</superscript> mode have been crystallized in pure lanthanide complex, and complex 2 represents the largest gadolinium cluster. Both of the complexes display large magnetocaloric effect in units of J kg<superscript>−1</superscript> K<superscript>−1</superscript> and mJ cm<superscript>−3</superscript> K<superscript>−1</superscript> on account of the weak antiferromagnetic exchange, the high N<subscript>Gd</subscript>/ M<subscript>W</subscript> ratio (magnetic density), and the relatively compact crystal lattice (mass density). [ABSTRACT FROM AUTHOR]
Details
- Language :
- English
- ISSN :
- 09476539
- Volume :
- 19
- Issue :
- 44
- Database :
- Complementary Index
- Journal :
- Chemistry - A European Journal
- Publication Type :
- Academic Journal
- Accession number :
- 91103274
- Full Text :
- https://doi.org/10.1002/chem.201302093