{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2023,9,14]],"date-time":"2023-09-14T06:12:39Z","timestamp":1694671959744},"reference-count":0,"publisher":"Wiley","issue":"5","license":[{"start":{"date-parts":[[2011,3,31]],"date-time":"2011-03-31T00:00:00Z","timestamp":1301529600000},"content-version":"vor","delay-in-days":0,"URL":"http:\/\/onlinelibrary.wiley.com\/termsAndConditions#vor"}],"content-domain":{"domain":[],"crossmark-restriction":false},"short-container-title":["Phys. Status Solidi C"],"published-print":{"date-parts":[[2011,5]]},"abstract":"<jats:title>Abstract<\/jats:title><jats:p>In this work we study the optical properties of two high quality fifty\u2010periods of In\u2010polarity InN\/In<jats:sub>0.73<\/jats:sub>Ga<jats:sub>0.27<\/jats:sub>N MQWs samples, grown by radio\u2010frequency plasma\u2010assisted molecular beam epitaxy, with different well (0.5\u20101 nm) and barrier thicknesses (3\u20104 nm). We employ spectroscopic ellipsometry at room temperature in the energy range from 0.6 to 6 eV, and incidence angles of 60 and 70\u00b0. Ellipsometric data were successfully modelled using the model dielectric function approach and a multilayer model assuming the MQWs as a homogeneous layer. The E<jats:sub>0<\/jats:sub>, A and E<jats:sub>1<\/jats:sub> MQWs transition energies were determined and found to exhibit a blueshift with decreasing the well thickness. (\u00a9 2011 WILEY\u2010VCH Verlag GmbH &amp; Co. KGaA, Weinheim)<\/jats:p>","DOI":"10.1002\/pssc.201000792","type":"journal-article","created":{"date-parts":[[2011,3,31]],"date-time":"2011-03-31T11:42:33Z","timestamp":1301571753000},"page":"1629-1632","source":"Crossref","is-referenced-by-count":1,"title":["Optical properties of InN\/In<sub>0.73<\/sub>Ga<sub>0.27<\/sub>N multiple quantum wells studied by spectroscopic ellipsometry"],"prefix":"10.1002","volume":"8","author":[{"given":"N.","family":"Ben Sedrine","sequence":"first","affiliation":[]},{"given":"V.","family":"Darakchieva","sequence":"additional","affiliation":[]},{"given":"D.","family":"Lindgren","sequence":"additional","affiliation":[]},{"given":"B.","family":"Monemar","sequence":"additional","affiliation":[]},{"given":"S. B.","family":"Che","sequence":"additional","affiliation":[]},{"given":"Y.","family":"Ishitani","sequence":"additional","affiliation":[]},{"given":"A.","family":"Yoshikawa","sequence":"additional","affiliation":[]}],"member":"311","published-online":{"date-parts":[[2011,3,31]]},"container-title":["physica status solidi c"],"original-title":[],"language":"en","link":[{"URL":"https:\/\/api.wiley.com\/onlinelibrary\/tdm\/v1\/articles\/10.1002%2Fpssc.201000792","content-type":"unspecified","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/onlinelibrary.wiley.com\/doi\/pdf\/10.1002\/pssc.201000792","content-type":"application\/pdf","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/onlinelibrary.wiley.com\/doi\/pdf\/10.1002\/pssc.201000792","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2023,9,13]],"date-time":"2023-09-13T18:00:37Z","timestamp":1694628037000},"score":1,"resource":{"primary":{"URL":"https:\/\/onlinelibrary.wiley.com\/doi\/10.1002\/pssc.201000792"}},"subtitle":[],"short-title":[],"issued":{"date-parts":[[2011,3,31]]},"references-count":0,"journal-issue":{"issue":"5","published-print":{"date-parts":[[2011,5]]}},"alternative-id":["10.1002\/pssc.201000792"],"URL":"https:\/\/doi.org\/10.1002\/pssc.201000792","archive":["Portico"],"relation":{},"ISSN":["1862-6351","1610-1642"],"issn-type":[{"value":"1862-6351","type":"print"},{"value":"1610-1642","type":"electronic"}],"subject":[],"published":{"date-parts":[[2011,3,31]]}}}