{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:S7HPOZVALEESCFZ543RCJOB7UJ","short_pith_number":"pith:S7HPOZVA","schema_version":"1.0","canonical_sha256":"97cef766a0590921173de6e224b83fa26ab8a84a631f60efb17db035b501e555","source":{"kind":"arxiv","id":"2110.04730","version":3},"attestation_state":"computed","paper":{"title":"Fingerprints of the quantum space-time in time-dependent quantum mechanics: An emergent geometric phase","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"hep-th","authors_text":"Anwesha Chakraborty, Biswajit Chakraborty, Partha Nandi","submitted_at":"2021-10-10T08:05:18Z","abstract_excerpt":"We show the emergence of Berry phase in a forced harmonic oscillator system placed in the quantum space-time of Moyal type, where the time 't' is also an operator. An effective commutative description of the system gives a time dependent generalised harmonic oscillator system with perturbation linear in position and momentum. The system is then diagonalised to get a generalised harmonic oscillator and then its adiabatic evolution over time-period $\\mathcal{T}$ is studied in Heisenberg picture to compute the expression of geometric phase-shift."},"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":"2110.04730","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2021-10-10T08:05:18Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"f81b5117addbff7ec309f30f911aa8e7de9f4d09673ed354145968bdb942b430","abstract_canon_sha256":"dafcee9fcb4e573990bc94f9a96c9b8ad0bab68f709f99cfa2c8e265e821e438"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:58:35.060220Z","signature_b64":"mmoak7R6ePgMJLsePaLyszJ3TSRFjVJtQ+CsJBh28kDDCspjttO35Qiak+dW9HC3ZTXdzSkrPVgKzWjZWVY1CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"97cef766a0590921173de6e224b83fa26ab8a84a631f60efb17db035b501e555","last_reissued_at":"2026-07-05T03:58:35.059878Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:58:35.059878Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Fingerprints of the quantum space-time in time-dependent quantum mechanics: An emergent geometric phase","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"hep-th","authors_text":"Anwesha Chakraborty, Biswajit Chakraborty, Partha Nandi","submitted_at":"2021-10-10T08:05:18Z","abstract_excerpt":"We show the emergence of Berry phase in a forced harmonic oscillator system placed in the quantum space-time of Moyal type, where the time 't' is also an operator. An effective commutative description of the system gives a time dependent generalised harmonic oscillator system with perturbation linear in position and momentum. The system is then diagonalised to get a generalised harmonic oscillator and then its adiabatic evolution over time-period $\\mathcal{T}$ is studied in Heisenberg picture to compute the expression of geometric phase-shift."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2110.04730","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/2110.04730/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":"2110.04730","created_at":"2026-07-05T03:58:35.059932+00:00"},{"alias_kind":"arxiv_version","alias_value":"2110.04730v3","created_at":"2026-07-05T03:58:35.059932+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2110.04730","created_at":"2026-07-05T03:58:35.059932+00:00"},{"alias_kind":"pith_short_12","alias_value":"S7HPOZVALEES","created_at":"2026-07-05T03:58:35.059932+00:00"},{"alias_kind":"pith_short_16","alias_value":"S7HPOZVALEESCFZ5","created_at":"2026-07-05T03:58:35.059932+00:00"},{"alias_kind":"pith_short_8","alias_value":"S7HPOZVA","created_at":"2026-07-05T03:58:35.059932+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2508.05881","citing_title":"Quantum Geometric Phases as a New Window on Gravitational Waves","ref_index":29,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/S7HPOZVALEESCFZ543RCJOB7UJ","json":"https://pith.science/pith/S7HPOZVALEESCFZ543RCJOB7UJ.json","graph_json":"https://pith.science/api/pith-number/S7HPOZVALEESCFZ543RCJOB7UJ/graph.json","events_json":"https://pith.science/api/pith-number/S7HPOZVALEESCFZ543RCJOB7UJ/events.json","paper":"https://pith.science/paper/S7HPOZVA"},"agent_actions":{"view_html":"https://pith.science/pith/S7HPOZVALEESCFZ543RCJOB7UJ","download_json":"https://pith.science/pith/S7HPOZVALEESCFZ543RCJOB7UJ.json","view_paper":"https://pith.science/paper/S7HPOZVA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2110.04730&json=true","fetch_graph":"https://pith.science/api/pith-number/S7HPOZVALEESCFZ543RCJOB7UJ/graph.json","fetch_events":"https://pith.science/api/pith-number/S7HPOZVALEESCFZ543RCJOB7UJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/S7HPOZVALEESCFZ543RCJOB7UJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/S7HPOZVALEESCFZ543RCJOB7UJ/action/storage_attestation","attest_author":"https://pith.science/pith/S7HPOZVALEESCFZ543RCJOB7UJ/action/author_attestation","sign_citation":"https://pith.science/pith/S7HPOZVALEESCFZ543RCJOB7UJ/action/citation_signature","submit_replication":"https://pith.science/pith/S7HPOZVALEESCFZ543RCJOB7UJ/action/replication_record"}},"created_at":"2026-07-05T03:58:35.059932+00:00","updated_at":"2026-07-05T03:58:35.059932+00:00"}