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Doping-dependent superconducting gap anisotropy in the two-dimensional pnictide Ca(10)(Pt(3)As(8)) (Fe(1-x)Pt(x))(2)As(2) (5)

TitleDoping-dependent superconducting gap anisotropy in the two-dimensional pnictide Ca(10)(Pt(3)As(8)) (Fe(1-x)Pt(x))(2)As(2) (5)
Publication TypeJournal Article
Year of Publication2012
AuthorsCho K, Tanatar MA, Kim H, Straszheim WE, Ni N, Cava RJ, Prozorov R
Journal TitlePhysical Review B
Volume85
Pages020504
Date Published01
Type of ArticleArticle
ISBN Number1098-0121
Accession NumberWOS:000299270500001
Abstract

The characteristic features of the Ca(10)(Pt(3)As(8))[(Fe(1-x)Pt(x))(2)As(2)](5) (the "10-3-8" phase) superconductor are triclinic symmetry, high anisotropy, and a clear separation of superconducting and antiferromagnetic regions in the T versus doping (x) phase diagram, which enables the superconducting gap to be studied without complications due to the coexisting magnetic order. The London penetration depth, measured on the underdoped side of the superconducting "dome" (x = 0.028, 0.041, 0.042, and 0.097), shows behavior remarkably similar to other Fe-based superconductors, exhibiting a robust power law, Delta lambda (T) = AT(n). The exponent n decreases from 2.36 (x = 0.097, close to the optimal doping) to 1.7 (x = 0.028, a heavily underdoped composition), suggesting that the superconducting gap becomes more anisotropic at the dome edge. A similar trend is found in the lower anisotropy BaFe(2)As(2) ("122")-based superconductors, implying that it is an intrinsic property, unrelated to the coexistence of magnetic order and superconductivity or the anisotropy of the normal state.
URL<Go to ISI>://WOS:000299270500001
DOI10.1103/PhysRevB.85.020504
Alternate JournalPhys. Rev. B