{"_buckets": {"deposit": "56d487a5-f3f0-4a8f-a473-20733000f55d"}, "_deposit": {"id": "10156", "owners": [], "pid": {"revision_id": 0, "type": "depid", "value": "10156"}, "status": "published"}, "_oai": {"id": "oai:nagoya.repo.nii.ac.jp:00010156"}, "item_10_biblio_info_6": {"attribute_name": "\u66f8\u8a8c\u60c5\u5831", "attribute_value_mlt": [{"bibliographicIssueDates": {"bibliographicIssueDate": "2007-12-10", "bibliographicIssueDateType": "Issued"}, "bibliographicIssueNumber": "24", "bibliographicPageEnd": "242102", "bibliographicPageStart": "242102", "bibliographicVolumeNumber": "91", "bibliographic_titles": [{"bibliographic_title": "APPLIED PHYSICS LETTERS"}]}]}, "item_10_description_4": {"attribute_name": "\u6284\u9332", "attribute_value_mlt": [{"subitem_description": "We found that Sm^3+ substitution in SrO(SrTiO_3)_2 is effective in improving the Seebeck coefficient (S). The |S| value increases notably with temperature, benefiting from an enhancement of the density of states (DOS) effective mass m_d from \u30303m_0 (300 K) to \u30307.5m_0 (1000 K), due to an improvement of the local symmetry of TiO_6 octahedra, enhancing the degeneracy in the Ti 3d orbitals, which form the conduction band (CB), and also to an accompanying lattice expansion, which gives rise to a higher DOS at the bottom of the CB and, consequently, a larger m_d.", "subitem_description_type": "Abstract"}]}, "item_10_identifier_60": {"attribute_name": "URI", "attribute_value_mlt": [{"subitem_identifier_type": "DOI", "subitem_identifier_uri": "http://dx.doi.org/10.1063/1.2820447"}, {"subitem_identifier_type": "HDL", "subitem_identifier_uri": "http://hdl.handle.net/2237/11974"}]}, "item_10_publisher_32": {"attribute_name": "\u51fa\u7248\u8005", "attribute_value_mlt": [{"subitem_publisher": "American Institite of Physics"}]}, "item_10_rights_12": {"attribute_name": "\u6a29\u5229", "attribute_value_mlt": [{"subitem_rights": "Copyright (2007) American Institute of Physics. 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