{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:JXJ253XEGXM2SFHRLKBONGHECG","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"4002ee98df42817e1a2e03504feac60a012b466a59d0aa2d052129f8c3241553","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2026-05-26T18:25:49Z","title_canon_sha256":"71217b239b59bd573ada2f0d69802fa00679bca9012208095166ddb50f0e93c8"},"schema_version":"1.0","source":{"id":"2605.27558","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.27558","created_at":"2026-05-28T01:04:15Z"},{"alias_kind":"arxiv_version","alias_value":"2605.27558v1","created_at":"2026-05-28T01:04:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.27558","created_at":"2026-05-28T01:04:15Z"},{"alias_kind":"pith_short_12","alias_value":"JXJ253XEGXM2","created_at":"2026-05-28T01:04:15Z"},{"alias_kind":"pith_short_16","alias_value":"JXJ253XEGXM2SFHR","created_at":"2026-05-28T01:04:15Z"},{"alias_kind":"pith_short_8","alias_value":"JXJ253XE","created_at":"2026-05-28T01:04:15Z"}],"graph_snapshots":[{"event_id":"sha256:dd34b54a1dea47f6d6be332d1ac90c27f418bc3a723148ff7b89abad5195a9c7","target":"graph","created_at":"2026-05-28T01:04:15Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2605.27558/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The natural electromagnetic modes spontaneously emitted by an atom in free space are spherical vector waves (SVWs). Each SVW mode is uniquely linked to a specific dynamical--spherical--multipole--moment of the atomic system. In this work, we introduce a general formalism for evaluating spherical multipole transition rates under different boundary conditions, considering the superposition between a given SVW and the modes resulting from the boundary conditions. This formalism is applied to study the radiative properties of an atomic system trapped near the focus of a 4$\\pi$ optical array. By ap","authors_text":"F. Camas-Aquino, R. J\\'auregui","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2026-05-26T18:25:49Z","title":"Radiative Response of Atomic Systems Illuminated with Approximate Spherical Vector Waves"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2605.27558","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:b0f6162a87c6fe785b9973d656b325b315790e9f6c0fc9e97dc30acd76dd7432","target":"record","created_at":"2026-05-28T01:04:15Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"4002ee98df42817e1a2e03504feac60a012b466a59d0aa2d052129f8c3241553","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2026-05-26T18:25:49Z","title_canon_sha256":"71217b239b59bd573ada2f0d69802fa00679bca9012208095166ddb50f0e93c8"},"schema_version":"1.0","source":{"id":"2605.27558","kind":"arxiv","version":1}},"canonical_sha256":"4dd3aeeee435d9a914f15a82e698e411b36ffaaad314b52893816a66d6566881","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4dd3aeeee435d9a914f15a82e698e411b36ffaaad314b52893816a66d6566881","first_computed_at":"2026-05-28T01:04:15.803171Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-28T01:04:15.803171Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"do0z1Y+FjuL5pMrNpuDlTpWO2zGnwe9z7OdCYX86jo82YfNxOTASx2d6VHgUGCWhJcgkhuUN/RFELAZ4/6d4AA==","signature_status":"signed_v1","signed_at":"2026-05-28T01:04:15.803910Z","signed_message":"canonical_sha256_bytes"},"source_id":"2605.27558","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b0f6162a87c6fe785b9973d656b325b315790e9f6c0fc9e97dc30acd76dd7432","sha256:dd34b54a1dea47f6d6be332d1ac90c27f418bc3a723148ff7b89abad5195a9c7"],"state_sha256":"88bf08964750baa6df0f2d8acc561d107672110a8efafcb7b2df56b5d26e310f"}