{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:JTBC5SI65VHRXWSTX2W5IXK2YU","short_pith_number":"pith:JTBC5SI6","schema_version":"1.0","canonical_sha256":"4cc22ec91eed4f1bda53beadd45d5ac5084ba05b26c7b9a341155498387c7372","source":{"kind":"arxiv","id":"2412.19746","version":2},"attestation_state":"computed","paper":{"title":"Pulsed Laser as a Continuous Particle Stream","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Bruno Santos de Souza, Celso Jorge Villas B\\^oas, Ciro Micheletti Diniz, Franciele Renata Henrique, Lino Misoguti, Paulo Henrique Dias Ferreira","submitted_at":"2024-12-27T17:14:41Z","abstract_excerpt":"With the recently introduced particle interpretation of the double-slit experiment for light fields [Phys. Rev. Lett. 134, 13360 (2025)], all related interference phenomena can be reinterpreted in terms of light particle states that either couple (bright) or do not couple (dark) with detectors. Here, we apply this approach to multimode pulsed lasers, unifying the description of their generation inside optical cavities and propagation outside them, now relying solely on quantum mechanics, i.e., without invoking wave superposition to explain pulse shaping. Specifically, we demonstrate that multi"},"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":"2412.19746","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"quant-ph","submitted_at":"2024-12-27T17:14:41Z","cross_cats_sorted":[],"title_canon_sha256":"7c354bb8297b25628a6696fb3d134c342f65d5ad5198a2b3141a957afc3b65e9","abstract_canon_sha256":"02b3fff7146f741cf91008148fe94c5b105d84fe3b28ff06b4c1d6b8b5150e32"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:01:56.412501Z","signature_b64":"G6NNz3i+EZ86drNX00+YLjmpWV+DziYagoUluHs+1bUBbulj6E3aom8IpoYuqq/1lpZ+b6UvSTWrGmJ/pK4oBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4cc22ec91eed4f1bda53beadd45d5ac5084ba05b26c7b9a341155498387c7372","last_reissued_at":"2026-07-05T11:01:56.411989Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:01:56.411989Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Pulsed Laser as a Continuous Particle Stream","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Bruno Santos de Souza, Celso Jorge Villas B\\^oas, Ciro Micheletti Diniz, Franciele Renata Henrique, Lino Misoguti, Paulo Henrique Dias Ferreira","submitted_at":"2024-12-27T17:14:41Z","abstract_excerpt":"With the recently introduced particle interpretation of the double-slit experiment for light fields [Phys. Rev. Lett. 134, 13360 (2025)], all related interference phenomena can be reinterpreted in terms of light particle states that either couple (bright) or do not couple (dark) with detectors. Here, we apply this approach to multimode pulsed lasers, unifying the description of their generation inside optical cavities and propagation outside them, now relying solely on quantum mechanics, i.e., without invoking wave superposition to explain pulse shaping. Specifically, we demonstrate that multi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2412.19746","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2412.19746/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":"2412.19746","created_at":"2026-07-05T11:01:56.412048+00:00"},{"alias_kind":"arxiv_version","alias_value":"2412.19746v2","created_at":"2026-07-05T11:01:56.412048+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2412.19746","created_at":"2026-07-05T11:01:56.412048+00:00"},{"alias_kind":"pith_short_12","alias_value":"JTBC5SI65VHR","created_at":"2026-07-05T11:01:56.412048+00:00"},{"alias_kind":"pith_short_16","alias_value":"JTBC5SI65VHRXWST","created_at":"2026-07-05T11:01:56.412048+00:00"},{"alias_kind":"pith_short_8","alias_value":"JTBC5SI6","created_at":"2026-07-05T11:01:56.412048+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2510.16329","citing_title":"Quantum Origin of Diffraction from Bright and Dark States","ref_index":18,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JTBC5SI65VHRXWSTX2W5IXK2YU","json":"https://pith.science/pith/JTBC5SI65VHRXWSTX2W5IXK2YU.json","graph_json":"https://pith.science/api/pith-number/JTBC5SI65VHRXWSTX2W5IXK2YU/graph.json","events_json":"https://pith.science/api/pith-number/JTBC5SI65VHRXWSTX2W5IXK2YU/events.json","paper":"https://pith.science/paper/JTBC5SI6"},"agent_actions":{"view_html":"https://pith.science/pith/JTBC5SI65VHRXWSTX2W5IXK2YU","download_json":"https://pith.science/pith/JTBC5SI65VHRXWSTX2W5IXK2YU.json","view_paper":"https://pith.science/paper/JTBC5SI6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2412.19746&json=true","fetch_graph":"https://pith.science/api/pith-number/JTBC5SI65VHRXWSTX2W5IXK2YU/graph.json","fetch_events":"https://pith.science/api/pith-number/JTBC5SI65VHRXWSTX2W5IXK2YU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JTBC5SI65VHRXWSTX2W5IXK2YU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JTBC5SI65VHRXWSTX2W5IXK2YU/action/storage_attestation","attest_author":"https://pith.science/pith/JTBC5SI65VHRXWSTX2W5IXK2YU/action/author_attestation","sign_citation":"https://pith.science/pith/JTBC5SI65VHRXWSTX2W5IXK2YU/action/citation_signature","submit_replication":"https://pith.science/pith/JTBC5SI65VHRXWSTX2W5IXK2YU/action/replication_record"}},"created_at":"2026-07-05T11:01:56.412048+00:00","updated_at":"2026-07-05T11:01:56.412048+00:00"}