{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:6HAQCGJ3FT5KF4EN734O7SDSGO","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":"ba85fdba979103c15018c1dc750cc205b8ef2b57e6c6f01c4be6b6d168fe3389","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2023-10-26T00:44:35Z","title_canon_sha256":"8475f2854499357719587cd9d2438376a280be3ae9f88638bf3d34506b062c27"},"schema_version":"1.0","source":{"id":"2310.17079","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2310.17079","created_at":"2026-07-05T08:03:27Z"},{"alias_kind":"arxiv_version","alias_value":"2310.17079v2","created_at":"2026-07-05T08:03:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2310.17079","created_at":"2026-07-05T08:03:27Z"},{"alias_kind":"pith_short_12","alias_value":"6HAQCGJ3FT5K","created_at":"2026-07-05T08:03:27Z"},{"alias_kind":"pith_short_16","alias_value":"6HAQCGJ3FT5KF4EN","created_at":"2026-07-05T08:03:27Z"},{"alias_kind":"pith_short_8","alias_value":"6HAQCGJ3","created_at":"2026-07-05T08:03:27Z"}],"graph_snapshots":[{"event_id":"sha256:74258bf6c4bc1e27a85e4b01d085fd40843764da3a9f6fcf7367960362a055b3","target":"graph","created_at":"2026-07-05T08:03:27Z","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/2310.17079/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Near two-body unitarity, the three-boson system is characterized by an approximate discrete scale invariance manifest in a geometric tower of bound states (the Efimov effect). In the absence of a strong four-body force, the four-boson system has two states associated with each Efimov state, one very nearly unstable, the other several times deeper. We study correlations between the excited- and ground-state properties, such as binding energies and radii, up to next-to-leading order in an effective field theory for short-range forces. We obtain the parameters in these correlations from similar c","authors_text":"Feng Wu, R. Higa, T. Frederico, U. van Kolck","cross_cats":["nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2023-10-26T00:44:35Z","title":"The Four-Boson First-Excited State Near Two-Body Unitarity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2310.17079","kind":"arxiv","version":2},"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":"sha256:7115df80bfe7eaf5bf0eaf7facbebc2c59f9593188cc31c517b893e9e02ce5b4","target":"record","created_at":"2026-07-05T08:03:27Z","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":"ba85fdba979103c15018c1dc750cc205b8ef2b57e6c6f01c4be6b6d168fe3389","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2023-10-26T00:44:35Z","title_canon_sha256":"8475f2854499357719587cd9d2438376a280be3ae9f88638bf3d34506b062c27"},"schema_version":"1.0","source":{"id":"2310.17079","kind":"arxiv","version":2}},"canonical_sha256":"f1c101193b2cfaa2f08dfef8efc8723391ef5256851565b474a86a41ce077ee4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f1c101193b2cfaa2f08dfef8efc8723391ef5256851565b474a86a41ce077ee4","first_computed_at":"2026-07-05T08:03:27.388578Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:03:27.388578Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"WlJoi0G6A6EJCnt15kQ7gIcU50Pzjqqo2Acb5UUwAL6P+BKJmUnQOuLQiEsl1d7nYQvY0nxdYZv6UMoAM8XNDQ==","signature_status":"signed_v1","signed_at":"2026-07-05T08:03:27.389069Z","signed_message":"canonical_sha256_bytes"},"source_id":"2310.17079","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7115df80bfe7eaf5bf0eaf7facbebc2c59f9593188cc31c517b893e9e02ce5b4","sha256:74258bf6c4bc1e27a85e4b01d085fd40843764da3a9f6fcf7367960362a055b3"],"state_sha256":"4372df94ed14392958155f162e514ba0229fdfcd1979fa4fd14b94a5ecc21d43"}