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Doping evolution of the absolute value of the London penetration depth and superfluid density in single crystals of Ba(Fe1−xCox)2As2

Source: Phys. Rev. B 82, 054507 (2010); doi:10.1103/PhysRevB.82.054507

Published 6 August 2010

PACS
  • 74.70.Xa
    Pnictides and chalcogenides
  • 74.25.N-
    Response to electromagnetic fields
  • 74.25.Bt
    Thermodynamic properties of superconductors
  • YEAR: 2010
PUBLICATION DATA
Publisher:
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R. T. Gordon,1,2 H. Kim,1,2 N. Salovich,3 R. W. Giannetta,3 R. M. Fernandes,1,2 V. G. Kogan,1 T. Prozorov,1 S. L. Bud'ko,1,2 P. C. Canfield,1,2 M. A. Tanatar,1 and R. Prozorov1,2
1Ames Laboratory, U.S. DOE, Ames, Iowa 50011, USA
2Department of Physics & Astronomy, Iowa State University, Ames, Iowa 50011, USA
3Loomis Laboratory of Physics, University of Illinois at Urbana–Champaign, 1110 West Green Street, Urbana, Illinois 61801, USA

The zero-temperature value of the in-plane London penetration depth, lambdaab(0), has been measured in single crystals of Ba(Fe1−xCox)2As2 as a function of the Co concentration, x, across both the underdoped and overdoped superconducting regions of the phase diagram. For x>~0.047, lambdaab(0) has been found to have values between 120±50 and 300±50  nm. A pronounced increase in lambdaab(0), to a value as high as 950±50  nm, has been observed for x<~0.047, corresponding to the region of the phase diagram where the itinerant antiferromagnetic and superconducting phases coexist and compete. Direct determination of the doping-dependent lambdaab(0) has allowed us to track the evolution of the temperature-dependent superfluid density, from which we infer the development of a pronounced superconducting gap anisotropy at the edges of the superconducting dome. ©2010 The American Physical Society
History: Received 10 June 2010; revised 15 July 2010; published 6 August 2010
Permalink: http://link.aps.org/abstract/PRB/v82/e054507
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