{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:5NLNLB3OKAVJTRI3O7DFXOIVT4","short_pith_number":"pith:5NLNLB3O","schema_version":"1.0","canonical_sha256":"eb56d5876e502a99c51b77c65bb9159f3703a329b62833cf14302a544d46d95b","source":{"kind":"arxiv","id":"2508.05881","version":3},"attestation_state":"computed","paper":{"title":"Quantum Geometric Phases as a New Window on Gravitational Waves","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","quant-ph"],"primary_cat":"hep-th","authors_text":"Frederik G. Scholtz, Partha Nandi","submitted_at":"2025-08-07T22:22:24Z","abstract_excerpt":"We investigate how low-frequency gravitational waves (LFGWs), originating from distant astrophysical or cosmological sources, can induce purely quantum geometric phases in mesoscopic optomechanical systems. These phases represent subtle imprints with no classical counterpart, going beyond standard dynamical or Berry-type contributions that admit Hannay-angle analogues. Such ultra-weak waves couple to the motion of a mechanical mirror and generate distinctive phase shifts in the system's quantum state that cannot arise in any classical description. To access this effect, we propose a Ramsey-typ"},"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":"2508.05881","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2025-08-07T22:22:24Z","cross_cats_sorted":["gr-qc","quant-ph"],"title_canon_sha256":"acc28deec414c65b10a8c1663b2c8a799a1ace18613424a74de6ee79a62b1090","abstract_canon_sha256":"42678417ad5c1e753772a29c982d04eb4c44294068206ef23b279e308ace9b2d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:53:28.405031Z","signature_b64":"V9ZoO6GG1r2TigtgUFYXVPKsVXkEU5c9cT7lviPjfm8zJLdiEmKr7ikDvadSu+omzUPZyqWBRiRELCQ7hjJTCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"eb56d5876e502a99c51b77c65bb9159f3703a329b62833cf14302a544d46d95b","last_reissued_at":"2026-07-05T11:53:28.404527Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:53:28.404527Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum Geometric Phases as a New Window on Gravitational Waves","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","quant-ph"],"primary_cat":"hep-th","authors_text":"Frederik G. Scholtz, Partha Nandi","submitted_at":"2025-08-07T22:22:24Z","abstract_excerpt":"We investigate how low-frequency gravitational waves (LFGWs), originating from distant astrophysical or cosmological sources, can induce purely quantum geometric phases in mesoscopic optomechanical systems. These phases represent subtle imprints with no classical counterpart, going beyond standard dynamical or Berry-type contributions that admit Hannay-angle analogues. Such ultra-weak waves couple to the motion of a mechanical mirror and generate distinctive phase shifts in the system's quantum state that cannot arise in any classical description. To access this effect, we propose a Ramsey-typ"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2508.05881","kind":"arxiv","version":3},"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/2508.05881/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":"2508.05881","created_at":"2026-07-05T11:53:28.404590+00:00"},{"alias_kind":"arxiv_version","alias_value":"2508.05881v3","created_at":"2026-07-05T11:53:28.404590+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2508.05881","created_at":"2026-07-05T11:53:28.404590+00:00"},{"alias_kind":"pith_short_12","alias_value":"5NLNLB3OKAVJ","created_at":"2026-07-05T11:53:28.404590+00:00"},{"alias_kind":"pith_short_16","alias_value":"5NLNLB3OKAVJTRI3","created_at":"2026-07-05T11:53:28.404590+00:00"},{"alias_kind":"pith_short_8","alias_value":"5NLNLB3O","created_at":"2026-07-05T11:53:28.404590+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2503.13061","citing_title":"Decoherence from quantum spacetime noise: An open-systems framework with application to neutrino oscillations","ref_index":13,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5NLNLB3OKAVJTRI3O7DFXOIVT4","json":"https://pith.science/pith/5NLNLB3OKAVJTRI3O7DFXOIVT4.json","graph_json":"https://pith.science/api/pith-number/5NLNLB3OKAVJTRI3O7DFXOIVT4/graph.json","events_json":"https://pith.science/api/pith-number/5NLNLB3OKAVJTRI3O7DFXOIVT4/events.json","paper":"https://pith.science/paper/5NLNLB3O"},"agent_actions":{"view_html":"https://pith.science/pith/5NLNLB3OKAVJTRI3O7DFXOIVT4","download_json":"https://pith.science/pith/5NLNLB3OKAVJTRI3O7DFXOIVT4.json","view_paper":"https://pith.science/paper/5NLNLB3O","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2508.05881&json=true","fetch_graph":"https://pith.science/api/pith-number/5NLNLB3OKAVJTRI3O7DFXOIVT4/graph.json","fetch_events":"https://pith.science/api/pith-number/5NLNLB3OKAVJTRI3O7DFXOIVT4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5NLNLB3OKAVJTRI3O7DFXOIVT4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5NLNLB3OKAVJTRI3O7DFXOIVT4/action/storage_attestation","attest_author":"https://pith.science/pith/5NLNLB3OKAVJTRI3O7DFXOIVT4/action/author_attestation","sign_citation":"https://pith.science/pith/5NLNLB3OKAVJTRI3O7DFXOIVT4/action/citation_signature","submit_replication":"https://pith.science/pith/5NLNLB3OKAVJTRI3O7DFXOIVT4/action/replication_record"}},"created_at":"2026-07-05T11:53:28.404590+00:00","updated_at":"2026-07-05T11:53:28.404590+00:00"}