<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>Kovaleva, N. N.</dc:creator>
  <dc:creator>Boris, A. V.</dc:creator>
  <dc:creator>Yordanov, P.</dc:creator>
  <dc:creator>Maljuk, A.</dc:creator>
  <dc:creator>Brücher, E.</dc:creator>
  <dc:creator>Strempfer, J.</dc:creator>
  <dc:creator>Konuma, M.</dc:creator>
  <dc:creator>Zegkinoglou, I.</dc:creator>
  <dc:creator>Bernhard, Christian</dc:creator>
  <dc:creator>Stoneham, A. M.</dc:creator>
  <dc:creator>Keimer, B.</dc:creator>
  <dc:date>2007-10-26</dc:date>
  <dc:description xmlns:ns0="xml" ns0:lang="en">We have studied the temperature dependence of spectroscopic ellipsometry spectra of an electrically insulating, nearly stoichiometric YTiO₃ single crystal with ferromagnetic Curie temperature &lt;i&gt;T&lt;/i&gt;&lt;sub&gt;&lt;i&gt;C&lt;/i&gt;&lt;/sub&gt;=30 K. The optical response exhibits a weak but noticeable anisotropy. Using a classical dispersion analysis, we identify three low-energy optical bands at 2.0, 2.9, and 3.7 eV. Although the optical conductivity spectra are only weakly temperature dependent below 300 K, we are able to distinguish high- and low-temperature regimes with a distinct crossover point around 100 K. The low-temperature regime in the optical response coincides with the temperature range in which significant deviations from a Curie-Weiss mean-field behavior are observed in the magnetization. Using an analysis based on a simple superexchange model, the spectral weight rearrangement can be attributed to intersite &lt;i&gt;d&lt;/i&gt; &lt;sub&gt;i&lt;/sub&gt;¹&lt;i&gt;d&lt;/i&gt; &lt;sub&gt;j&lt;/sub&gt;¹→&lt;i&gt;d&lt;/i&gt; &lt;sub&gt;i&lt;/sub&gt;² &lt;i&gt;d&lt;/i&gt; &lt;sub&gt;j&lt;/sub&gt;⁰ optical transitions. In particular, Kramers-Kronig consistent changes in optical spectra around 2.9 eV can be associated with the high-spin-state (³&lt;i&gt;T&lt;/i&gt;₁) optical transition. This indicates that other mechanisms, such as weakly dipole-allowed &lt;i&gt;p&lt;/i&gt;-&lt;i&gt;d&lt;/i&gt; transitions and/or exciton-polaron excitations, can contribute significantly to the optical band at 2 eV. The recorded optical spectral weight gain of the 2.9 eV optical band is significantly suppressed and anisotropic, which we associate with complex &lt;i&gt;spin-orbit-lattice&lt;/i&gt; phenomena near the ferromagnetic ordering temperature in YTiO₃.</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:identifier>https://folia.unifr.ch/global/documents/300599</dc:identifier>
  <dc:identifier>https://folia.unifr.ch/documents/300599/files/bernhard_orf.pdf</dc:identifier>
  <dc:language>eng</dc:language>
  <dc:relation>info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevB.76.155125</dc:relation>
  <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
  <dc:rights>License undefined</dc:rights>
  <dc:source>Physical Review B: Condensend Matter and Materials Physics. - 2007, vol. 76, no. 15, p. 155125</dc:source>
  <dc:subject>info:eu-repo/classification/udc/57</dc:subject>
  <dc:title xmlns:ns1="xml" ns1:lang="en">Optical response of ferromagnetic YTiO₃ studied by spectral ellipsometry</dc:title>
  <dc:type>http://purl.org/coar/resource_type/c_6501</dc:type>
</oai_dc:dc>
