{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:FEFZHW2I2XYKQ4V6VIRC473DKO","short_pith_number":"pith:FEFZHW2I","schema_version":"1.0","canonical_sha256":"290b93db48d5f0a872beaa222e7f63539eacdddbab66d9d067658ffd9ec14849","source":{"kind":"arxiv","id":"2605.16621","version":1},"attestation_state":"computed","paper":{"title":"Extending the model of rotating acoustic geometries to include non-vanishing solid-body rotation: quasibound spectra","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"H. S. Vieira","submitted_at":"2026-05-15T20:42:36Z","abstract_excerpt":"In a very recent paper, we computed the quasibound states of massless acoustic excitations interacting with a new (effective) acoustic geometry with circulation. Notably, the behavior of this acoustic black hole aligns with the phenomenology observed in recent experiments that include superfluids. Such vortex fluid flow bundles exhibit solid-body rotation at length scales larger than the inter-vortex distance, which adds some complexity to the study of quantum fluid behaviour. To theoretically deal with this issue, we present an extension of our previous results by including a solid-body rotat"},"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":"2605.16621","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2026-05-15T20:42:36Z","cross_cats_sorted":[],"title_canon_sha256":"7403cc05388800c259d52b160100a751c436db9908394d4820532729a9cb4b34","abstract_canon_sha256":"dc55d5e617ecf2c00bb186983e01c1d02fdfd20408fd68dad9f2820ad87504ec"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-20T00:02:32.919710Z","signature_b64":"rz+RaqGoQNq3ftNwSxIFtS65tJivRMQJEnZX5BhrcPN7CVxnP/s5op0U4YL1xKQO0URMJCzndqMiN8TrXtZ4CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"290b93db48d5f0a872beaa222e7f63539eacdddbab66d9d067658ffd9ec14849","last_reissued_at":"2026-05-20T00:02:32.918974Z","signature_status":"signed_v1","first_computed_at":"2026-05-20T00:02:32.918974Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Extending the model of rotating acoustic geometries to include non-vanishing solid-body rotation: quasibound spectra","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"H. S. Vieira","submitted_at":"2026-05-15T20:42:36Z","abstract_excerpt":"In a very recent paper, we computed the quasibound states of massless acoustic excitations interacting with a new (effective) acoustic geometry with circulation. Notably, the behavior of this acoustic black hole aligns with the phenomenology observed in recent experiments that include superfluids. Such vortex fluid flow bundles exhibit solid-body rotation at length scales larger than the inter-vortex distance, which adds some complexity to the study of quantum fluid behaviour. To theoretically deal with this issue, we present an extension of our previous results by including a solid-body rotat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2605.16621","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/2605.16621/integrity.json","findings":[],"available":true,"detectors_run":[{"name":"claim_evidence","ran_at":"2026-05-19T19:21:56.768746Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"ai_meta_artifact","ran_at":"2026-05-19T18:33:26.587701Z","status":"skipped","version":"1.0.0","findings_count":0}],"snapshot_sha256":"9f2ff7124f20b8a349c5251bcda24ab40ece89965f26736cf861b6d795c590b6"},"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":"2605.16621","created_at":"2026-05-20T00:02:32.919092+00:00"},{"alias_kind":"arxiv_version","alias_value":"2605.16621v1","created_at":"2026-05-20T00:02:32.919092+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.16621","created_at":"2026-05-20T00:02:32.919092+00:00"},{"alias_kind":"pith_short_12","alias_value":"FEFZHW2I2XYK","created_at":"2026-05-20T00:02:32.919092+00:00"},{"alias_kind":"pith_short_16","alias_value":"FEFZHW2I2XYKQ4V6","created_at":"2026-05-20T00:02:32.919092+00:00"},{"alias_kind":"pith_short_8","alias_value":"FEFZHW2I","created_at":"2026-05-20T00:02:32.919092+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/FEFZHW2I2XYKQ4V6VIRC473DKO","json":"https://pith.science/pith/FEFZHW2I2XYKQ4V6VIRC473DKO.json","graph_json":"https://pith.science/api/pith-number/FEFZHW2I2XYKQ4V6VIRC473DKO/graph.json","events_json":"https://pith.science/api/pith-number/FEFZHW2I2XYKQ4V6VIRC473DKO/events.json","paper":"https://pith.science/paper/FEFZHW2I"},"agent_actions":{"view_html":"https://pith.science/pith/FEFZHW2I2XYKQ4V6VIRC473DKO","download_json":"https://pith.science/pith/FEFZHW2I2XYKQ4V6VIRC473DKO.json","view_paper":"https://pith.science/paper/FEFZHW2I","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2605.16621&json=true","fetch_graph":"https://pith.science/api/pith-number/FEFZHW2I2XYKQ4V6VIRC473DKO/graph.json","fetch_events":"https://pith.science/api/pith-number/FEFZHW2I2XYKQ4V6VIRC473DKO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FEFZHW2I2XYKQ4V6VIRC473DKO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FEFZHW2I2XYKQ4V6VIRC473DKO/action/storage_attestation","attest_author":"https://pith.science/pith/FEFZHW2I2XYKQ4V6VIRC473DKO/action/author_attestation","sign_citation":"https://pith.science/pith/FEFZHW2I2XYKQ4V6VIRC473DKO/action/citation_signature","submit_replication":"https://pith.science/pith/FEFZHW2I2XYKQ4V6VIRC473DKO/action/replication_record"}},"created_at":"2026-05-20T00:02:32.919092+00:00","updated_at":"2026-05-20T00:02:32.919092+00:00"}