London penetration depth and superfluid density of single-crystalline Fe1+y(Te1-xSex)and Fe1+y(Te1-xSx)

被引:71
|
作者
Kim, H. [1 ,2 ]
Martin, C. [1 ,2 ]
Gordon, R. T. [1 ,2 ]
Tanatar, M. A. [1 ,2 ]
Hu, J. [3 ]
Qian, B. [3 ]
Mao, Z. Q. [3 ]
Hu, Rongwei [4 ]
Petrovic, C. [4 ]
Salovich, N. [5 ]
Giannetta, R. [5 ]
Prozorov, R. [1 ,2 ]
机构
[1] Iowa State Univ, Ames Lab, Ames, IA 50011 USA
[2] Iowa State Univ, Dept Phys, Ames, IA 50011 USA
[3] Tulane Univ, Dept Phys & Engn Phys, New Orleans, LA 70118 USA
[4] Brookhaven Natl Lab, Condensed Matter Phys & Mat Sci Dept, Upton, NY 11973 USA
[5] Univ Illinois, Loomis Lab Phys, Urbana, IL 61801 USA
来源
PHYSICAL REVIEW B | 2010年 / 81卷 / 18期
关键词
LAYERED SUPERCONDUCTOR;
D O I
10.1103/PhysRevB.81.180503
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The in-plane London penetration depth, lambda(T), was measured in single crystals of the iron-chalcogenide superconductors Fe-1.03(Te0.63Se0.37) and Fe-1.06(Te0.88S0.14) by using a radio-frequency tunnel diode resonator. Similar to the iron-arsenides and in stark contrast to the iron-phosphides, iron-chalcogenides exhibit a nearly quadratic temperature variation of lambda(T) at low temperatures. The absolute value of the penetration depth in the T -> 0 limit was determined for Fe-1.03(Te0.63Se0.37) by using an Al coating technique, giving lambda(0) approximate to 560 +/- 20 nm. The superfluid density rho(s)(T)=lambda(2)(0)/lambda(2)(T) was fitted with a self-consistent two-gap gamma model. While two different gaps are needed to describe the full-range temperature variation in rho(s)(T), a nonexponential low-temperature behavior requires pair-breaking scattering, and therefore an unconventional (e.g., s(+/-) or nodal) order parameter.
引用
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页数:4
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