{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:CIQTKZGCAVF35JLLHUDEDTNDKT","short_pith_number":"pith:CIQTKZGC","schema_version":"1.0","canonical_sha256":"12213564c2054bbea56b3d0641cda354d43b353c093c8248ff443662442a8355","source":{"kind":"arxiv","id":"2404.01435","version":1},"attestation_state":"computed","paper":{"title":"Haro 11: The Spatially Resolved Lyman Continuum Sources","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"astro-ph.GA","authors_text":"Angela Adamo, Anne E. Jaskot, Arjan Bik, Claus Leitherer, Daniel Kunth, Edmund Hodges-Kluck, Goran Ostlin, Jens Melinder, J. M. Mas-Hesse, Lena Komarova, Matthew J. Hayes, Mattia Sirressi, M. S. Oey, Peter Laursen, Svea Hernandez, T. Emil Rivera-Thorsen","submitted_at":"2024-04-01T19:14:47Z","abstract_excerpt":"As the nearest confirmed Lyman continuum (LyC) emitter, Haro 11 is an exceptional laboratory for studying LyC escape processes crucial to cosmic reionization. Our new HST/COS G130M/1055 observations of its three star-forming knots now reveal that the observed LyC originates in Knots B and C, with $903 - 912~\\r{A}$ luminosities of $1.9\\pm1.5 \\times 10^{40}~\\rm erg~s^{-1}$ and $0.9\\pm0.7 \\times 10^{40}~\\rm erg~s^{-1}$, respectively. We derive local escape fractions $f_{\\rm{esc, 912}} = 3.4\\pm2.9\\%$ and $5.1\\pm4.3\\%$ for Knots B and C, respectively. Our Starburst99 modeling shows dominant populat"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2404.01435","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"astro-ph.GA","submitted_at":"2024-04-01T19:14:47Z","cross_cats_sorted":[],"title_canon_sha256":"22c4e5761a2473e7072beb726c35b730261371a2a58cd600c2ecf2bcb6261736","abstract_canon_sha256":"c9bcb21a39a95c56df8bc733f538d4de054fb5eebb08256e4b929e8faad71478"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:03:14.249001Z","signature_b64":"VHojoSQLD6Mse04wHnOROF1jANYqucTL/E4GRPZx5Rm7SGRsvTaP+gTLux3pHcAJNmDQfUohMzSLIvdrk1MzBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"12213564c2054bbea56b3d0641cda354d43b353c093c8248ff443662442a8355","last_reissued_at":"2026-07-05T08:03:14.248505Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:03:14.248505Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Haro 11: The Spatially Resolved Lyman Continuum Sources","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"astro-ph.GA","authors_text":"Angela Adamo, Anne E. Jaskot, Arjan Bik, Claus Leitherer, Daniel Kunth, Edmund Hodges-Kluck, Goran Ostlin, Jens Melinder, J. M. Mas-Hesse, Lena Komarova, Matthew J. Hayes, Mattia Sirressi, M. S. Oey, Peter Laursen, Svea Hernandez, T. Emil Rivera-Thorsen","submitted_at":"2024-04-01T19:14:47Z","abstract_excerpt":"As the nearest confirmed Lyman continuum (LyC) emitter, Haro 11 is an exceptional laboratory for studying LyC escape processes crucial to cosmic reionization. Our new HST/COS G130M/1055 observations of its three star-forming knots now reveal that the observed LyC originates in Knots B and C, with $903 - 912~\\r{A}$ luminosities of $1.9\\pm1.5 \\times 10^{40}~\\rm erg~s^{-1}$ and $0.9\\pm0.7 \\times 10^{40}~\\rm erg~s^{-1}$, respectively. We derive local escape fractions $f_{\\rm{esc, 912}} = 3.4\\pm2.9\\%$ and $5.1\\pm4.3\\%$ for Knots B and C, respectively. Our Starburst99 modeling shows dominant populat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2404.01435","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2404.01435/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2404.01435","created_at":"2026-07-05T08:03:14.248560+00:00"},{"alias_kind":"arxiv_version","alias_value":"2404.01435v1","created_at":"2026-07-05T08:03:14.248560+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2404.01435","created_at":"2026-07-05T08:03:14.248560+00:00"},{"alias_kind":"pith_short_12","alias_value":"CIQTKZGCAVF3","created_at":"2026-07-05T08:03:14.248560+00:00"},{"alias_kind":"pith_short_16","alias_value":"CIQTKZGCAVF35JLL","created_at":"2026-07-05T08:03:14.248560+00:00"},{"alias_kind":"pith_short_8","alias_value":"CIQTKZGC","created_at":"2026-07-05T08:03:14.248560+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CIQTKZGCAVF35JLLHUDEDTNDKT","json":"https://pith.science/pith/CIQTKZGCAVF35JLLHUDEDTNDKT.json","graph_json":"https://pith.science/api/pith-number/CIQTKZGCAVF35JLLHUDEDTNDKT/graph.json","events_json":"https://pith.science/api/pith-number/CIQTKZGCAVF35JLLHUDEDTNDKT/events.json","paper":"https://pith.science/paper/CIQTKZGC"},"agent_actions":{"view_html":"https://pith.science/pith/CIQTKZGCAVF35JLLHUDEDTNDKT","download_json":"https://pith.science/pith/CIQTKZGCAVF35JLLHUDEDTNDKT.json","view_paper":"https://pith.science/paper/CIQTKZGC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2404.01435&json=true","fetch_graph":"https://pith.science/api/pith-number/CIQTKZGCAVF35JLLHUDEDTNDKT/graph.json","fetch_events":"https://pith.science/api/pith-number/CIQTKZGCAVF35JLLHUDEDTNDKT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CIQTKZGCAVF35JLLHUDEDTNDKT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CIQTKZGCAVF35JLLHUDEDTNDKT/action/storage_attestation","attest_author":"https://pith.science/pith/CIQTKZGCAVF35JLLHUDEDTNDKT/action/author_attestation","sign_citation":"https://pith.science/pith/CIQTKZGCAVF35JLLHUDEDTNDKT/action/citation_signature","submit_replication":"https://pith.science/pith/CIQTKZGCAVF35JLLHUDEDTNDKT/action/replication_record"}},"created_at":"2026-07-05T08:03:14.248560+00:00","updated_at":"2026-07-05T08:03:14.248560+00:00"}