TY - JOUR
T1 - Superconductivity and intercalation state in the lithium-hexamethylenediamine-intercalated superconductor Lix(C6H16N2)yFe2-zSe2
T2 - Dependence on the intercalation temperature and lithium content
AU - Hosono, Shohei
AU - Noji, Takashi
AU - Hatakeda, Takehiro
AU - Kawamata, Takayuki
AU - Kato, Masatsune
AU - Koike, Yoji
N1 - Funding Information:
This work was supported by JSPS KAKENHI Grant Number 15K13512.
Publisher Copyright:
©2016 The Physical Society of Japan.
PY - 2016/10/15
Y1 - 2016/10/15
N2 - The superconductivity and intercalation state in the lithium- and hexamethylenediamine (HMDA)-intercalated superconductor Lix(C6H16N2)yFe2-zSe2 have been investigated from powder x-ray diffraction, thermogravimetric, and magnetic susceptibility measurements, changing the intercalation temperature Ti and the Li content x. Both Li and HMDA have been co-intercalated stably up to x = 2 roughly in a molar ratio of x : y = 2 : 1. In the case of Ti = 45°C, it has been found that both Li and HMDA are co-intercalated locally at the edge of FeSe crystals, indicating that both Li and HMDA are hard to diffuse into the inside of FeSe crystals at 45°C. In the case of Ti = 100°C, on the other hand, it has been found that both Li and HMDA diffuse into the inside of FeSe crystals, so that Tc tends to increase with increasing x from ∼30 K at x = 1 up to 38 K at x = 2 owing to the increase in the number of electron carriers doped from Li into the FeSe layers.
AB - The superconductivity and intercalation state in the lithium- and hexamethylenediamine (HMDA)-intercalated superconductor Lix(C6H16N2)yFe2-zSe2 have been investigated from powder x-ray diffraction, thermogravimetric, and magnetic susceptibility measurements, changing the intercalation temperature Ti and the Li content x. Both Li and HMDA have been co-intercalated stably up to x = 2 roughly in a molar ratio of x : y = 2 : 1. In the case of Ti = 45°C, it has been found that both Li and HMDA are co-intercalated locally at the edge of FeSe crystals, indicating that both Li and HMDA are hard to diffuse into the inside of FeSe crystals at 45°C. In the case of Ti = 100°C, on the other hand, it has been found that both Li and HMDA diffuse into the inside of FeSe crystals, so that Tc tends to increase with increasing x from ∼30 K at x = 1 up to 38 K at x = 2 owing to the increase in the number of electron carriers doped from Li into the FeSe layers.
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U2 - 10.7566/JPSJ.85.104701
DO - 10.7566/JPSJ.85.104701
M3 - Article
AN - SCOPUS:84990989970
SN - 0031-9015
VL - 85
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 10
M1 - 104701
ER -