{"paper":{"title":"Basic properties of Fermi blazars and the \"blazar sequence\"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"astro-ph.HE","authors_text":"Dingrong Xiong, Haojing Zhang, Jinming Bai, Xiong Zhang","submitted_at":"2015-04-10T15:21:55Z","abstract_excerpt":"By statistically analyzing a large sample which includes blazars of Fermi detection (FBs) and non-Fermi detection (NFBs), we find that there are significant differences between FBs and NFBs for redshift, black hole mass, jet kinetic power from \"cavity\" power, broad-line luminosity, and ratio of core luminosity to absolute V-band magnitude ($R_{\\rm v}$), but not for ratio of radio core to extended flux ($R_{\\rm c}$) and Eddington ratio. Compared with NFBs, FBs have larger mean jet power, $R_{\\rm c}$ and $R_{\\rm v}$ while smaller mean redshift, black hole mass, broad-line luminosity. These resul"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1504.02706","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"}