<oai_dc:dc xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
  <dc:creator>Bernhard, Christian</dc:creator>
  <dc:creator>Wang, Chen Nan</dc:creator>
  <dc:creator>Nuccio, Laura</dc:creator>
  <dc:creator>Schulz, Leander</dc:creator>
  <dc:creator>Zaharko, O.</dc:creator>
  <dc:creator>Larsen, J.</dc:creator>
  <dc:creator>Aristizabal, C.</dc:creator>
  <dc:creator>Willis, M.</dc:creator>
  <dc:creator>Drew, Alan J.</dc:creator>
  <dc:creator>Varma, G. D.</dc:creator>
  <dc:creator>Wolf, T.</dc:creator>
  <dc:creator>Niedermayer, Ch.</dc:creator>
  <dc:date>2012-10-19</dc:date>
  <dc:description xmlns:ns0="xml" ns0:lang="en">Using muon spin rotation (μSR) we investigated the magnetic and superconducting properties of a series of Ba(Fe&lt;sub&gt;1−x&lt;/sub&gt;Co&lt;sub&gt;x&lt;/sub&gt;)₂As₂ single crystals with 0≤x≤0.15. Our study details how the antiferromagnetic order is suppressed upon Co substitution and how it coexists with superconductivity. In the nonsuperconducting samples at 0&lt;x&lt;0.04 the antiferromagnetic order parameter is only moderately suppressed. With the onset of superconductivity this suppression becomes faster and it is most rapid between x=0.045 and 0.05. As was previously demonstrated by μSR at x=0.055 [ P. Marsik et al. Phys. Rev. Lett. 105 57001 (2010)], the strongly weakened antiferromagnetic order is still a bulk phenomenon that competes with superconductivity. The comparison with neutron diffraction data suggests that the antiferromagnetic order remains commensurate whereas the amplitude exhibits a spatial variation that is likely caused by the randomly distributed Co atoms. A different kind of magnetic order that was also previously identified [ C. Bernhard et al. New J. Phys. 11 055050 (2009)] occurs at 0.055&lt;x&lt;0.075 where T&lt;sub&gt;c&lt;/sub&gt; approaches the maximum value. The magnetic order develops here only in parts of the sample volume and it seems to cooperate with superconductivity since its onset temperature coincides with T&lt;sub&gt;c&lt;/sub&gt;. Even in the strongly overdoped regime at x = 0.11, where the static magnetic order has disappeared, we find that the low-energy spin fluctuations are anomalously enhanced below T&lt;sub&gt;c&lt;/sub&gt;. These findings point toward a drastic change in the relationship between the magnetic and superconducting orders from a competitive one in the strongly underdoped regime to a constructive one in near-optimally and overdoped samples.</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:identifier>https://folia.unifr.ch/global/documents/302716</dc:identifier>
  <dc:identifier>https://folia.unifr.ch/documents/302716/files/ber_msr.pdf</dc:identifier>
  <dc:language>eng</dc:language>
  <dc:relation>info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevB.86.184509</dc:relation>
  <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
  <dc:rights>License undefined</dc:rights>
  <dc:source>Physical Review B - Condensed Matter and Materials Physics. - 2012, vol. 86, no. 14, p. 144112</dc:source>
  <dc:subject>info:eu-repo/classification/udc/53</dc:subject>
  <dc:title xmlns:ns1="xml" ns1:lang="en">Muon spin rotation study of magnetism and superconductivity in Ba(Fe&lt;sub&gt;1−x&lt;/sub&gt;Co&lt;sub&gt;x&lt;/sub&gt;)₂As₂ single crystals</dc:title>
  <dc:type>http://purl.org/coar/resource_type/c_6501</dc:type>
</oai_dc:dc>
