{"paper":{"title":"Completing the optical spectroscopy of the $6p_{J}$ manifold: the $5p_{3/2}\\rightarrow 6p_{1/2}$ electric dipole forbidden transition in atomic rubidium","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"Cristian Mojica-Casique, Daniel Sahag\\'un, Fernando Ram\\'irez-Mart\\'inez, Francisco Ponciano-Ojeda, Jes\\'us Flores-Mijangos, Jos\\'e Jim\\'enez-Mier, Oscar L\\'opez-Hern\\'andez, Roc\\'io J\\'auregui, Santiago Hern\\'andez-G\\'omez","submitted_at":"2018-09-14T14:56:41Z","abstract_excerpt":"We present the first evidence of excitation of the $5p_{3/2} \\rightarrow 6p_{1/2}$ electric dipole-forbidden transition in atomic rubidium. The experiments were carried out in a rubidium vapor cell using Doppler-free optical-optical double-resonance spectroscopy with counter-propagating beams. This a similar scheme to the excitation of the other fine transition $J=3/2$ in the $6p_{J}$ manifold previously reported. A $5s_{1/2} \\rightarrow 5p_{3/2}$ electric dipole preparation step using a diode laser locked to the maximum F cyclic transition of the $D_2$ line is used to prepare the atoms in the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1809.05451","kind":"arxiv","version":2},"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"}