M. Kato

New FeSe-based intercalation superconductors, $A_{x}$ (C $_{8}$ H $_{11}$ N) $_{y}$ Fe $_{1 - z}$ Se ( $A$ = Li, Na), with $T_{c}$ = 39-44 K have been successfully synthesized via the interca…

cond-mat.supr-con2016★ 8 cited

Pairing Symmetry Studied from Impurity Effects in the Undoped Superconductor T'-La $_{1.8}$ Eu $_{0.2}$ CuO $_{4}$

Koki Ohashi, Takayuki Kawamata, Tomohisa Takamatsu +3

We have investigated the effects of magnetic Ni and nonmagnetic Zn impurities on the superconductivity in undoped T'-La $_{1.8}$ Eu $_{0.2}$ CuO $_{4}$ (T'-LECO) with the Nd $_{2}$ CuO $_{4}$ -ty…

cond-mat.supr-con2016★ 12 cited

Superconductivity and Intercalation Statein the Lithium-Hexamethylenediamine-Intercalated Superconductor Li $_{x}$ (C $_{6}$ H $_{16}$ N $_{2}$ ) $_{y}$ Fe $_{2 - z}$ Se $_{2}$ : Dependence on the Intercalation Temperature and Lithium Content

Shohei Hosono, Takashi Noji, Takehiro Hatakeda +3

The superconductivity and intercalation statein the lithium-and hexamethylenediamine (HMDA)-intercalated superconductor Li $_{x}$ (C $_{6}$ H $_{16}$ N $_{2}$ ) $_{y}$ Fe $_{2 - z}$ Se $_{2}$ have been inv…

cond-mat.supr-con2016★ 42 cited

New Superconducting Phase of Li $_{x}$ (C $_{6}$ H $_{16}$ N $_{2}$ ) $_{y}$ Fe $_{2 - z}$ Se $_{2}$ with $T_{c}$ = 41 K Obtained through the Post-Annealing

Shohei Hosono, Takashi Noji, Takehiro Hatakeda +3

Post-annealing effects on the crystal structure and superconductivity of the lithium- and hexamethylenediamine (HMDA)-intercalated superconductor Lix(C6H16N2)yFe2-zSe2 have been in…

New Alkali-Metal- and 2-Phenethylamine-Intercalated Superconductors Ax​(C8​H11​N)y​Fe1−z​Se (A = Li, Na) with the Largest Interlayer Spacings and Tc​ ∼ 40 K

Pairing Symmetry Studied from Impurity Effects in the Undoped Superconductor T'-La1.8​Eu0.2​CuO4​

Superconductivity and Intercalation Statein the Lithium-Hexamethylenediamine-Intercalated Superconductor Lix​(C6​H16​N2​)y​Fe2−z​Se2​: Dependence on the Intercalation Temperature and Lithium Content

New Superconducting Phase of Lix​(C6​H16​N2​)y​Fe2−z​Se2​ with Tc​ = 41 K Obtained through the Post-Annealing

New Alkali-Metal- and 2-Phenethylamine-Intercalated Superconductors $A_{x}$ (C $_{8}$ H $_{11}$ N) $_{y}$ Fe $_{1 - z}$ Se ( $A$ = Li, Na) with the Largest Interlayer Spacings and $T_{c}$ $\sim$ 40 K

Pairing Symmetry Studied from Impurity Effects in the Undoped Superconductor T'-La $_{1.8}$ Eu $_{0.2}$ CuO $_{4}$

Superconductivity and Intercalation Statein the Lithium-Hexamethylenediamine-Intercalated Superconductor Li $_{x}$ (C $_{6}$ H $_{16}$ N $_{2}$ ) $_{y}$ Fe $_{2 - z}$ Se $_{2}$ : Dependence on the Intercalation Temperature and Lithium Content

New Superconducting Phase of Li $_{x}$ (C $_{6}$ H $_{16}$ N $_{2}$ ) $_{y}$ Fe $_{2 - z}$ Se $_{2}$ with $T_{c}$ = 41 K Obtained through the Post-Annealing