<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>Murakami, Yuta</dc:creator>
  <dc:creator>Golež, Denis</dc:creator>
  <dc:creator>Kaneko, Tatsuya</dc:creator>
  <dc:creator>Koga, Akihisa</dc:creator>
  <dc:creator>Millis, Andrew J.</dc:creator>
  <dc:creator>Werner, Philipp</dc:creator>
  <dc:date>2020-05-11</dc:date>
  <dc:description xmlns:ns0="xml" ns0:lang="en">We consider a two-band spinless model describing an excitonic insulator (EI) on  the two-dimensional square lattice with anisotropic hopping parameters and  electron-phonon (el-ph) coupling, inspired by the EI candidate Ta2NiSe5. We  systematically study the nature of the collective excitations in the ordered phase  which originates from the interband Coulomb interaction and the el-ph coupling.  When the ordered phase is stabilized only by the Coulomb interaction (pure EI  phase), its collective response exhibits a massless phase mode in addition to  the amplitude mode. We show that in the BEC regime, the signal of the  amplitude mode becomes less prominent and that the anisotropy in the phase- mode velocities is reduced. Through coupling to the lattice, the phase mode  acquires a mass and the signal of the amplitude mode becomes less prominent.  Importantly, the character of the softening mode at the boundary between the  normal semiconductor phase and the ordered phase depends on the  parameters. In particular, we point out that even for el-ph coupling smaller than  the Coulomb interaction, the mode that softens to zero at the boundary can  have a phonon character. We also discuss how the collective modes can be  observed in the optical conductivity. Furthermore, we study the effects of  nonlocal interactions on the collective modes and show the possibility of  realizing a coexistence of an in-gap mode and an above-gap mode split off from  the single-amplitude mode in the system with local interactions only.</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:identifier>https://folia.unifr.ch/global/documents/308576</dc:identifier>
  <dc:identifier>https://folia.unifr.ch/documents/308576/files/wer_cme.pdf</dc:identifier>
  <dc:language>eng</dc:language>
  <dc:relation>info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevB.101.195118</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. 19, p. 195118</dc:source>
  <dc:subject>info:eu-repo/classification/udc/53</dc:subject>
  <dc:title xmlns:ns1="xml" ns1:lang="en">Collective modes in excitonic insulators: Effects of electron-phonon coupling and signatures in the optical response</dc:title>
  <dc:type>http://purl.org/coar/resource_type/c_6501</dc:type>
</oai_dc:dc>
