TY - JOUR
T1 - Pressure-induced superconductivity in Eu0.5Ca 0.5Fe2As2
T2 - Wide zero-resistivity region due to suppression of Eu magnetic order and chemical pressure
AU - Mitsuda, Akihiro
AU - Matoba, Tomohiro
AU - Ishikawa, Fumihiro
AU - Yamada, Yuh
AU - Wada, Hirofumi
PY - 2010/7
Y1 - 2010/7
N2 - To clarify competition between FeAs-based superconductivity and antiferromagnetism of Eu2+, and the superconducting properties in EuFe2As2, we investigated a Ca-substituted sample, Eu 0.5Ca0.5Fe2As2, under high pressure. Under ambient pressure, the sample exhibits a spin-density-wave (SDW) transition at TSDW = 191K and antiferromagnetic order at T N = 4K, but no evidence of superconductivity down to 2 K. The Ca-substitution certainly weakens the antiferromagnetism. With increasing pressure, TSDW shifts to lower temperature and becomes more unclear. Above 1.27 GPa, pressure-induced superconductivity with zero resistivity is observed at around Tc = 20K. At 2.14 GPa, Tc reaches a maximum value of 24 K and the superconducting transition becomes sharpest. The chemical pressure and the suppression of Eu magnetic order induced by Ca substitution enlarge the zero resistivity region compared to pure EuFe 2As2.
AB - To clarify competition between FeAs-based superconductivity and antiferromagnetism of Eu2+, and the superconducting properties in EuFe2As2, we investigated a Ca-substituted sample, Eu 0.5Ca0.5Fe2As2, under high pressure. Under ambient pressure, the sample exhibits a spin-density-wave (SDW) transition at TSDW = 191K and antiferromagnetic order at T N = 4K, but no evidence of superconductivity down to 2 K. The Ca-substitution certainly weakens the antiferromagnetism. With increasing pressure, TSDW shifts to lower temperature and becomes more unclear. Above 1.27 GPa, pressure-induced superconductivity with zero resistivity is observed at around Tc = 20K. At 2.14 GPa, Tc reaches a maximum value of 24 K and the superconducting transition becomes sharpest. The chemical pressure and the suppression of Eu magnetic order induced by Ca substitution enlarge the zero resistivity region compared to pure EuFe 2As2.
UR - http://www.scopus.com/inward/record.url?scp=77956237654&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=77956237654&partnerID=8YFLogxK
U2 - 10.1143/JPSJ.79.073704
DO - 10.1143/JPSJ.79.073704
M3 - Article
AN - SCOPUS:77956237654
SN - 0031-9015
VL - 79
JO - journal of the physical society of japan
JF - journal of the physical society of japan
IS - 7
M1 - 073704
ER -