<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>Xu, Bing</dc:creator>
  <dc:creator>Munzar, Dominik</dc:creator>
  <dc:creator>Dubroka, Adam</dc:creator>
  <dc:creator>Sheveleva, Evgeniia</dc:creator>
  <dc:creator>Lyzwa, Fryderyk</dc:creator>
  <dc:creator>Marsik, Premysl</dc:creator>
  <dc:creator>Wang, C. N.</dc:creator>
  <dc:creator>Wang, Z. C.</dc:creator>
  <dc:creator>Cao, G. H.</dc:creator>
  <dc:creator>Bernhard, Christian</dc:creator>
  <dc:date>2020-06-09</dc:date>
  <dc:description xmlns:ns0="xml" ns0:lang="en">We studied the infrared response of polycrystalline samples of the iron arsenide  superconductor (Rb,Cs)Ca2Fe4As4F2 (Rb,Cs-12442), which has a bilayer structure  similar to the high-Tc cuprates YBa2Cu3O7 (YBCO) and Bi2Sr2CaCu2O8. The c-axis  reflectivity spectra Rc have been derived from the reflectivity spectra of the  polycrystalline samples Rpoly and the in-plane spectrum of a corresponding Cs-12442  crystal Rab using a geometrical averaging approach with Rc=3Rpoly−2Rab. In  analogy to the c-axis response of the cuprates, we observe a superconductivity- induced transverse plasma mode and a phonon anomaly that are both signatures of  local electric field effects that arise from a large difference between the local  conductivities in the intra- and interbilayer regions. Using a multilayer model  developed for the cuprates, we obtain a good description of the c-axis response and  derive the local conductivities at T≃Tc of σbl1(ω→0)≃1000Ω−1cm−1 and  σint1(ω→0)≃15Ω−1cm−1, respectively, that are similar to the ones previously found in  underdoped YBCO. Different from the cuprates, we find no evidence of a normal-state  pseudogap in terms of a partial suppression of the low-energy electronic states that  sets in already well above Tc. There is also no clear sign of an onset of precursor  superconducting pairing correlations well above Tc≃ 30 K. This highlights that the  pseudogap and the precursor superconducting pairing well above Tc are unique  features of the cuprates with their strong electronic correlations and, for example, not  just the result of a strongly anisotropic electronic response due to the layered crystal  structure.</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:identifier>https://folia.unifr.ch/global/documents/308844</dc:identifier>
  <dc:identifier>https://folia.unifr.ch/documents/308844/files/ber_sit.pdf</dc:identifier>
  <dc:language>eng</dc:language>
  <dc:relation>info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevB.101.214512</dc:relation>
  <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
  <dc:rights>License undefined</dc:rights>
  <dc:source>Physical Review B. - 2020, vol. 101, no. 21, p. 214512</dc:source>
  <dc:subject>info:eu-repo/classification/udc/53</dc:subject>
  <dc:title xmlns:ns1="xml" ns1:lang="en">Superconductivity-induced transverse plasma mode and phonon anomaly in the $c$-axis response of the bilayer compound ${\mathrm{RbCa}}_{2}{\mathrm{Fe}}_{4}{\mathrm{As}}_{4}{\mathrm{F}}_{2}$</dc:title>
  <dc:type>http://purl.org/coar/resource_type/c_6501</dc:type>
</oai_dc:dc>
