{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:ZRHELUY7NXH4JFRL3JESKXVY2K","short_pith_number":"pith:ZRHELUY7","schema_version":"1.0","canonical_sha256":"cc4e45d31f6dcfc4962bda49255eb8d29965727e798479f82528d2a5af496274","source":{"kind":"arxiv","id":"1601.06132","version":1},"attestation_state":"computed","paper":{"title":"Gravitationally induced quantum transitions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","quant-ph"],"primary_cat":"gr-qc","authors_text":"A. Landry, M. B. Paranjape","submitted_at":"2016-01-22T19:57:18Z","abstract_excerpt":"In this letter, we calculate the probability for resonantly induced transitions in quantum states due to time dependent gravitational perturbations. Contrary to common wisdom, the probability of inducing transitions is not infinitesimally small. We consider a system of ultra cold neutrons (UCN), which are organized according to the energy levels of the Schr\\\"odinger equation in the presence of the earth's gravitational field. Transitions between energy levels are induced by an oscillating driving force of frequency $\\omega$. The driving force is created by oscillating a macroscopic mass in the"},"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":"1601.06132","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2016-01-22T19:57:18Z","cross_cats_sorted":["hep-th","quant-ph"],"title_canon_sha256":"77307773e48d0daa2e627fcfcc5e6bae05aef39a6d27642da63eb608634fe928","abstract_canon_sha256":"209d0fced2701cd36d5766a1f78f35317a55dda06b21068e0ec91408240f6116"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:11:12.899875Z","signature_b64":"ITmNFwLxyRza95GaYTbvuZHqLDw9Qong74v5jPl1V15StZgiiGYb508wVwqLPJX6OqESGwUxqyt4ZfPcJklnBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cc4e45d31f6dcfc4962bda49255eb8d29965727e798479f82528d2a5af496274","last_reissued_at":"2026-05-18T01:11:12.899474Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:11:12.899474Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gravitationally induced quantum transitions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","quant-ph"],"primary_cat":"gr-qc","authors_text":"A. Landry, M. B. Paranjape","submitted_at":"2016-01-22T19:57:18Z","abstract_excerpt":"In this letter, we calculate the probability for resonantly induced transitions in quantum states due to time dependent gravitational perturbations. Contrary to common wisdom, the probability of inducing transitions is not infinitesimally small. We consider a system of ultra cold neutrons (UCN), which are organized according to the energy levels of the Schr\\\"odinger equation in the presence of the earth's gravitational field. Transitions between energy levels are induced by an oscillating driving force of frequency $\\omega$. The driving force is created by oscillating a macroscopic mass in the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1601.06132","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":""},"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":"1601.06132","created_at":"2026-05-18T01:11:12.899530+00:00"},{"alias_kind":"arxiv_version","alias_value":"1601.06132v1","created_at":"2026-05-18T01:11:12.899530+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1601.06132","created_at":"2026-05-18T01:11:12.899530+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZRHELUY7NXH4","created_at":"2026-05-18T12:30:55.937587+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZRHELUY7NXH4JFRL","created_at":"2026-05-18T12:30:55.937587+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZRHELUY7","created_at":"2026-05-18T12:30:55.937587+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/ZRHELUY7NXH4JFRL3JESKXVY2K","json":"https://pith.science/pith/ZRHELUY7NXH4JFRL3JESKXVY2K.json","graph_json":"https://pith.science/api/pith-number/ZRHELUY7NXH4JFRL3JESKXVY2K/graph.json","events_json":"https://pith.science/api/pith-number/ZRHELUY7NXH4JFRL3JESKXVY2K/events.json","paper":"https://pith.science/paper/ZRHELUY7"},"agent_actions":{"view_html":"https://pith.science/pith/ZRHELUY7NXH4JFRL3JESKXVY2K","download_json":"https://pith.science/pith/ZRHELUY7NXH4JFRL3JESKXVY2K.json","view_paper":"https://pith.science/paper/ZRHELUY7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1601.06132&json=true","fetch_graph":"https://pith.science/api/pith-number/ZRHELUY7NXH4JFRL3JESKXVY2K/graph.json","fetch_events":"https://pith.science/api/pith-number/ZRHELUY7NXH4JFRL3JESKXVY2K/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZRHELUY7NXH4JFRL3JESKXVY2K/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZRHELUY7NXH4JFRL3JESKXVY2K/action/storage_attestation","attest_author":"https://pith.science/pith/ZRHELUY7NXH4JFRL3JESKXVY2K/action/author_attestation","sign_citation":"https://pith.science/pith/ZRHELUY7NXH4JFRL3JESKXVY2K/action/citation_signature","submit_replication":"https://pith.science/pith/ZRHELUY7NXH4JFRL3JESKXVY2K/action/replication_record"}},"created_at":"2026-05-18T01:11:12.899530+00:00","updated_at":"2026-05-18T01:11:12.899530+00:00"}