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Structural phase transition and superlattice misfit strain of RFeAsO (R = La, Pr, Nd and Sm) (Articolo in rivista)
- Type
- Label
- Structural phase transition and superlattice misfit strain of RFeAsO (R = La, Pr, Nd and Sm) (Articolo in rivista) (literal)
- Anno
- 2010-01-01T00:00:00+01:00 (literal)
- Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#doi
- 10.1103/PhysRevB.82.144507 (literal)
- Alternative label
A Ricci,N Poccia, B. Joseph, L Barba, G Arrighetti, G Ciasca, J.-Q. Yan, R. W. McCallum, T. A. Lograsso, N. D. Zhigadlo, J. Karpinski, and A Bianconi (2010)
Structural phase transition and superlattice misfit strain of RFeAsO (R = La, Pr, Nd and Sm)
in Physical review. B, Rapid communications (print)
(literal)
- Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#autori
- A Ricci,N Poccia, B. Joseph, L Barba, G Arrighetti, G Ciasca, J.-Q. Yan, R. W. McCallum, T. A. Lograsso, N. D. Zhigadlo, J. Karpinski, and A Bianconi (literal)
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- Scopu (literal)
- ISI Web of Science (WOS) (literal)
- Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#affiliazioni
- A Ricci,N Poccia, B. Joseph, L Barba, G Arrighetti, G Ciasca, J.-Q. Yan, R. W. McCallum, T. A. Lograsso, N. D. Zhigadlo, J. Karpinski, and A Bianconi (literal)
- Titolo
- Structural phase transition and superlattice misfit strain of RFeAsO (R = La, Pr, Nd and Sm) (literal)
- Abstract
- The tetragonal-to-orthorhombic structural phase transition (SPT) in LaFeAsO (La-1111) and
SmFeAsO (Sm-1111) single crystals measured by high resolution x-ray diffraction is found to be
sharp while the RFeAsO (R=La, Nd, Pr, Sm) polycrystalline samples show a broad continuous
SPT. Comparing the polycrystalline and the single crystal 1111 samples, the critical exponents of
the SPT are found to be the same while the correlation length critical exponents are found to be
very different. These results imply that the lattice fluctuations in 1111 systems change in samples
with different surface to volume ratio that is assigned to the relieve of the temperature dependent
superlattice misfit strain between active iron layers and the spacer layers in 1111 systems. This
phenomenon that is missing in the AFe2As2 (A=Ca, Sr, Ba) 122 systems, with the same electronic
structure but different for the thickness and the elastic constant of the spacer layers, is related with
the different maximum superconducting transition temperature in the 1111 (55 K) versus 122 (35
K) systems and implies the surface reconstruction in 1111 single crystals. (literal)
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