<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>He, Liming</dc:creator>
  <dc:creator>Cao, Wei</dc:creator>
  <dc:date>2006</dc:date>
  <dc:description xmlns:ns0="xml" ns0:lang="en">With many-body perturbation theory, ¹D–³D term intervals of helium 1&lt;i&gt;snd&lt;/i&gt;  (&lt;i&gt;n&lt;/i&gt; = 12 ∼ 20) configurations are calculated. Based on two different models,  Rayleigh-Schrodinger perturbation expansion terms consisting of bound states only,  and those of continua are evaluated, respectively. As for bound states, zeroth-order  wave functions are strictly generated from self-iteration solutions of the Hartree  equation and residues of infinite expansion series are dealt with by the integral  processing method, while a simplified hydrogen potential is adopted to get the  continua. Using Rayleigh–Schrodinger expansions, we evaluate exchange energy up  to third-order terms. It is found that level splittings are mainly attributed to summations  over bound states. The fine-structure level splittings yielded here are found to agree  quite well with experimental results.</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:identifier>https://folia.unifr.ch/global/documents/300328</dc:identifier>
  <dc:identifier>https://folia.unifr.ch/documents/300328/files/cao_mbc.pdf</dc:identifier>
  <dc:language>eng</dc:language>
  <dc:relation>info:eu-repo/semantics/altIdentifier/doi/10.1139/p07-002</dc:relation>
  <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
  <dc:rights>License undefined</dc:rights>
  <dc:source>Canadian Journal of Physics. - 2006, vol. 84, no. 12, p. 1097-1106</dc:source>
  <dc:subject>info:eu-repo/classification/udc/53</dc:subject>
  <dc:title xmlns:ns1="xml" ns1:lang="en">Many-body calculation of helium ¹D–³D term intervals for 1&lt;i&gt;snd&lt;/i&gt; (&lt;i&gt;n&lt;/i&gt; = 12 ∼ 20) high Rydberg states</dc:title>
  <dc:type>http://purl.org/coar/resource_type/c_6501</dc:type>
</oai_dc:dc>
