Enhancement of superconducting transition temperature of FeSe by intercalation of a molecular spacer layer
The recent discovery of high temperature superconductivity in a layered iron arsenide has led to an intensive search to optimize the superconducting properties of iron-based superconductors by changing the chemical composition of the spacer layer that is inserted between adjacent anionic iron arseni...
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Main Authors | , , , , , , , , , , |
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Abstract | The recent discovery of high temperature superconductivity in a layered iron arsenide has led to an intensive search to optimize the superconducting properties of iron-based superconductors by changing the chemical composition of the spacer layer that is inserted between adjacent anionic iron arsenide layers. Until now, superconductivity has only been found in compounds with a cationic spacer layer consisting of metal ions: Li+, Na+, K+, Ba2+ or a PbO-type or perovskite-type oxide layer. Electronic doping is usually necessary to control the fine balance between antiferromagnetism and superconductivity. Superconductivity has also been reported in FeSe, which contains neutral layers similar in structure to those found in the iron arsenides but without the spacer layer. Here we demonstrate the synthesis of Lix(NH2)y(NH3)1-yFe2Se2 (x ~0.6 ; y ~ 0.2), with lithium ions, lithium amide and ammonia acting as the spacer layer, which exhibits superconductivity at 43(1) K, higher than in any FeSe-derived compound reported so far and four times higher at ambient pressure than the transition temperature, Tc, of the parent Fe1.01Se. We have determined the crystal structure using neutron powder diffraction and used magnetometry and muon-spin rotation data to determine the superconducting properties. This new synthetic route opens up the possibility of further exploitation of related molecular intercalations in this and other systems in order to greatly optimize the superconducting properties in this family. |
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AbstractList | The recent discovery of high temperature superconductivity in a layered iron
arsenide has led to an intensive search to optimize the superconducting
properties of iron-based superconductors by changing the chemical composition
of the spacer layer that is inserted between adjacent anionic iron arsenide
layers. Until now, superconductivity has only been found in compounds with a
cationic spacer layer consisting of metal ions: Li+, Na+, K+, Ba2+ or a
PbO-type or perovskite-type oxide layer. Electronic doping is usually necessary
to control the fine balance between antiferromagnetism and superconductivity.
Superconductivity has also been reported in FeSe, which contains neutral layers
similar in structure to those found in the iron arsenides but without the
spacer layer. Here we demonstrate the synthesis of Lix(NH2)y(NH3)1-yFe2Se2 (x
~0.6 ; y ~ 0.2), with lithium ions, lithium amide and ammonia acting as the
spacer layer, which exhibits superconductivity at 43(1) K, higher than in any
FeSe-derived compound reported so far and four times higher at ambient pressure
than the transition temperature, Tc, of the parent Fe1.01Se. We have determined
the crystal structure using neutron powder diffraction and used magnetometry
and muon-spin rotation data to determine the superconducting properties. This
new synthetic route opens up the possibility of further exploitation of related
molecular intercalations in this and other systems in order to greatly optimize
the superconducting properties in this family. The recent discovery of high temperature superconductivity in a layered iron arsenide has led to an intensive search to optimize the superconducting properties of iron-based superconductors by changing the chemical composition of the spacer layer that is inserted between adjacent anionic iron arsenide layers. Until now, superconductivity has only been found in compounds with a cationic spacer layer consisting of metal ions: Li+, Na+, K+, Ba2+ or a PbO-type or perovskite-type oxide layer. Electronic doping is usually necessary to control the fine balance between antiferromagnetism and superconductivity. Superconductivity has also been reported in FeSe, which contains neutral layers similar in structure to those found in the iron arsenides but without the spacer layer. Here we demonstrate the synthesis of Lix(NH2)y(NH3)1-yFe2Se2 (x ~0.6 ; y ~ 0.2), with lithium ions, lithium amide and ammonia acting as the spacer layer, which exhibits superconductivity at 43(1) K, higher than in any FeSe-derived compound reported so far and four times higher at ambient pressure than the transition temperature, Tc, of the parent Fe1.01Se. We have determined the crystal structure using neutron powder diffraction and used magnetometry and muon-spin rotation data to determine the superconducting properties. This new synthetic route opens up the possibility of further exploitation of related molecular intercalations in this and other systems in order to greatly optimize the superconducting properties in this family. |
Author | Corkett, Alex J Baker, Peter J Free, David G Sedlmaier, Stefan J Wright, Jack D Burrard-Lucas, Matthew Hara, Yoshiaki Clarke, Simon J Cassidy, Simon J Lancaster, Tom Blundell, Stephen J |
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BackLink | https://doi.org/10.48550/arXiv.1203.5046$$DView paper in arXiv https://doi.org/10.1038/nmat3464$$DView published paper (Access to full text may be restricted) |
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Snippet | The recent discovery of high temperature superconductivity in a layered iron arsenide has led to an intensive search to optimize the superconducting properties... The recent discovery of high temperature superconductivity in a layered iron arsenide has led to an intensive search to optimize the superconducting properties... |
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SubjectTerms | Ammonia Antiferromagnetism Arsenides Chemical composition Crystal structure High temperature Intermetallic compounds Iron Lithium ions Magnetic measurement Magnetic properties Muon spin rotation Organic chemistry Perovskites Physics - Superconductivity Pressure Superconductivity Transition temperature |
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Title | Enhancement of superconducting transition temperature of FeSe by intercalation of a molecular spacer layer |
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