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<https://d-nb.info/1328657620> a bibo:Issue;
  dcterms:medium <http://rdaregistry.info/termList/RDACarrierType/1018>;
  rdau:P60049 <http://rdaregistry.info/termList/RDAContentType/1020>;
  rdau:P60050 <http://rdaregistry.info/termList/RDAMediaType/1003>;
  rdau:P60048 <http://rdaregistry.info/termList/RDACarrierType/1018>;
  dc:identifier "(DE-101)1328657620";
  umbel:isLike <https://doi.org/10.1002/pssb.2220730212>, <https://nbn-resolving.org/urn:nbn:de:101:1-2405080454205.451855696228>;
  dcterms:format <https://www.iana.org/assignments/media-types/application/pdf>;
  foaf:primaryTopic <https://doi.org/10.1002/pssb.2220730212>;
  dcterms:language <http://id.loc.gov/vocabulary/iso639-2/eng>;
  a bibo:Article;
  dc:title "The Influence of the Electron–Hole Exchange Interaction on the Biexciton Ground State in CuCl and CuBr and Related Optical Transitions";
  dcterms:creator _:node1jup961v3x91105705 .

_:node1jup961v3x91105705 gndo:preferredName "Ekardt, W." .

<https://d-nb.info/1328657620> marcRole:aut _:node1jup961v3x91105706 .

_:node1jup961v3x91105706 gndo:preferredName "Ekardt, W." .

<https://d-nb.info/1328657620> marcRole:aut _:node1jup961v3x91105707 .

_:node1jup961v3x91105707 gndo:preferredName "Sheboul, M. I." .

<https://d-nb.info/1328657620> bibo:pageStart "475";
  bibo:pageEnd "482";
  dcterms:extent "8 S.";
  dcterms:isPartOf <https://ld.zdb-services.de/resource/1481096-7>;
  dcterms:description "Abstract: The influence of the electron‐hole exchange interaction on the biexciton ground state is recalculated. Due to the analytical and nonanalytical parts of the electron‐hole exchange interaction of the single exciton there exist two analytical parts. Both can be quite different in the order of magnitude. General formulas for s‐type states in cubic crystals are derived and numerical results for the ground states in CuCl and CuBr are given. Finally the results are compared with experimental data."@de,
    "Der Einfluß der Elektron‐Loch‐Austauschwechselwirkung auf den Grundzustand des Biexzitons wird berechnet. Infolge des analytischen und nichtanalytischen Anteils im einzelnen Exziton erhält man für das Biexziton zwei analytische Anteile. Beide können in ihrer Größenordnung völlig verschieden sein. Allgemeine Formeln für Zustände vom s‐Typ in kubischen Kristallen werden abgeleitet, und numerische Resultate für den Grundzustand in CuCl und CuBr werden angegeben. Zum Schluß werden die Ergebnisse mit dem Experiment verglichen."@de;
  dcterms:license <http://onlinelibrary.wiley.com/termsAndConditions#vor>;
  wdrs:describedby <https://d-nb.info/1328657620/about> .

<https://d-nb.info/1328657620/about> dcterms:license <http://creativecommons.org/publicdomain/zero/1.0/>;
  dcterms:modified "2024-05-08T21:42:00.000"^^xsd:dateTime .

<https://d-nb.info/1328657620> dcterms:issued "2006";
  bibo:issue "73.2006, 2";
  owl:sameAs <http://hub.culturegraph.org/resource/DNB-1328657620> .

