{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:N3JQXUBPWLBCW3B27A4WZVKBM3","short_pith_number":"pith:N3JQXUBP","canonical_record":{"source":{"id":"1207.3854","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2012-07-17T01:19:03Z","cross_cats_sorted":["physics.atom-ph"],"title_canon_sha256":"2e76e261942be7f50a1b005ffb8a6a4c1de0c276da4e2e540d100745b0eed6aa","abstract_canon_sha256":"cbeb1d53ea41dce5f8e983fe593b00cc0ca94699f81e8730dde18c06ee334af4"},"schema_version":"1.0"},"canonical_sha256":"6ed30bd02fb2c22b6c3af8396cd54166d9476adba3bcac1ba7e73c23a65e3e51","source":{"kind":"arxiv","id":"1207.3854","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1207.3854","created_at":"2026-05-18T01:56:17Z"},{"alias_kind":"arxiv_version","alias_value":"1207.3854v4","created_at":"2026-05-18T01:56:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.3854","created_at":"2026-05-18T01:56:17Z"},{"alias_kind":"pith_short_12","alias_value":"N3JQXUBPWLBC","created_at":"2026-05-18T12:27:16Z"},{"alias_kind":"pith_short_16","alias_value":"N3JQXUBPWLBCW3B2","created_at":"2026-05-18T12:27:16Z"},{"alias_kind":"pith_short_8","alias_value":"N3JQXUBP","created_at":"2026-05-18T12:27:16Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:N3JQXUBPWLBCW3B27A4WZVKBM3","target":"record","payload":{"canonical_record":{"source":{"id":"1207.3854","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2012-07-17T01:19:03Z","cross_cats_sorted":["physics.atom-ph"],"title_canon_sha256":"2e76e261942be7f50a1b005ffb8a6a4c1de0c276da4e2e540d100745b0eed6aa","abstract_canon_sha256":"cbeb1d53ea41dce5f8e983fe593b00cc0ca94699f81e8730dde18c06ee334af4"},"schema_version":"1.0"},"canonical_sha256":"6ed30bd02fb2c22b6c3af8396cd54166d9476adba3bcac1ba7e73c23a65e3e51","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:56:17.676552Z","signature_b64":"0bit26uEajjiK1GldKRgM3yiPSjfmLXtlYJ4ktRHnM6wQwbZ6NU3YG2blNEoMHR1lRXIE+Cb2oO4aYF4RrMxCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6ed30bd02fb2c22b6c3af8396cd54166d9476adba3bcac1ba7e73c23a65e3e51","last_reissued_at":"2026-05-18T01:56:17.676038Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:56:17.676038Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1207.3854","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:56:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oRe7+lVnnXSiiZTTxXlPKV3RX0X+vh6nf1F35BhabKO6gIWFns7iB00v3cDpY6F+lXTLifc02YbJ9Rfduq6lDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T00:55:20.592306Z"},"content_sha256":"2b8a7cc1b4d50cae4554118e3a062b8d1a79ffb537a93bce8133d7f024df16e2","schema_version":"1.0","event_id":"sha256:2b8a7cc1b4d50cae4554118e3a062b8d1a79ffb537a93bce8133d7f024df16e2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:N3JQXUBPWLBCW3B27A4WZVKBM3","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quantum dynamics in a time-dependent cylindrical trap","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph"],"primary_cat":"quant-ph","authors_text":"S. V. Mousavi","submitted_at":"2012-07-17T01:19:03Z","abstract_excerpt":"Solutions to the Schr\\\"{o}dinger equation are examined for a particle inside a cylindrical trap of a circular time-dependent cross-section. Analytical expressions for energy and momentum expectation values are derived with respect to the exact solutions; and the adiabatic and sudden change of the boundary are discussed. The density profile as a function of time in a given observation point, resembles the diffraction-in-time pattern observed in a suddenly released particle but with an enhanced fringe visibility. Numerical computations are presented for both contracting and expanding boxes."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.3854","kind":"arxiv","version":4},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:56:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ge/JrFKFJTWFQcK8JeHt1Rv4uEommAdb+Sf4dQwAtncxUAgS54eaKOcN4+L48/7gYGVTRM8mUNADtXGoHeABAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T00:55:20.592873Z"},"content_sha256":"1920e0d73325a1d0a841d74c5d8629b420a4b16d42e2b03115fed20e35acd44f","schema_version":"1.0","event_id":"sha256:1920e0d73325a1d0a841d74c5d8629b420a4b16d42e2b03115fed20e35acd44f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/N3JQXUBPWLBCW3B27A4WZVKBM3/bundle.json","state_url":"https://pith.science/pith/N3JQXUBPWLBCW3B27A4WZVKBM3/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/N3JQXUBPWLBCW3B27A4WZVKBM3/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-11T00:55:20Z","links":{"resolver":"https://pith.science/pith/N3JQXUBPWLBCW3B27A4WZVKBM3","bundle":"https://pith.science/pith/N3JQXUBPWLBCW3B27A4WZVKBM3/bundle.json","state":"https://pith.science/pith/N3JQXUBPWLBCW3B27A4WZVKBM3/state.json","well_known_bundle":"https://pith.science/.well-known/pith/N3JQXUBPWLBCW3B27A4WZVKBM3/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:N3JQXUBPWLBCW3B27A4WZVKBM3","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":"cbeb1d53ea41dce5f8e983fe593b00cc0ca94699f81e8730dde18c06ee334af4","cross_cats_sorted":["physics.atom-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2012-07-17T01:19:03Z","title_canon_sha256":"2e76e261942be7f50a1b005ffb8a6a4c1de0c276da4e2e540d100745b0eed6aa"},"schema_version":"1.0","source":{"id":"1207.3854","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1207.3854","created_at":"2026-05-18T01:56:17Z"},{"alias_kind":"arxiv_version","alias_value":"1207.3854v4","created_at":"2026-05-18T01:56:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.3854","created_at":"2026-05-18T01:56:17Z"},{"alias_kind":"pith_short_12","alias_value":"N3JQXUBPWLBC","created_at":"2026-05-18T12:27:16Z"},{"alias_kind":"pith_short_16","alias_value":"N3JQXUBPWLBCW3B2","created_at":"2026-05-18T12:27:16Z"},{"alias_kind":"pith_short_8","alias_value":"N3JQXUBP","created_at":"2026-05-18T12:27:16Z"}],"graph_snapshots":[{"event_id":"sha256:1920e0d73325a1d0a841d74c5d8629b420a4b16d42e2b03115fed20e35acd44f","target":"graph","created_at":"2026-05-18T01:56:17Z","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"},"paper":{"abstract_excerpt":"Solutions to the Schr\\\"{o}dinger equation are examined for a particle inside a cylindrical trap of a circular time-dependent cross-section. Analytical expressions for energy and momentum expectation values are derived with respect to the exact solutions; and the adiabatic and sudden change of the boundary are discussed. The density profile as a function of time in a given observation point, resembles the diffraction-in-time pattern observed in a suddenly released particle but with an enhanced fringe visibility. Numerical computations are presented for both contracting and expanding boxes.","authors_text":"S. V. Mousavi","cross_cats":["physics.atom-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2012-07-17T01:19:03Z","title":"Quantum dynamics in a time-dependent cylindrical trap"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.3854","kind":"arxiv","version":4},"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":"sha256:2b8a7cc1b4d50cae4554118e3a062b8d1a79ffb537a93bce8133d7f024df16e2","target":"record","created_at":"2026-05-18T01:56:17Z","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":"cbeb1d53ea41dce5f8e983fe593b00cc0ca94699f81e8730dde18c06ee334af4","cross_cats_sorted":["physics.atom-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2012-07-17T01:19:03Z","title_canon_sha256":"2e76e261942be7f50a1b005ffb8a6a4c1de0c276da4e2e540d100745b0eed6aa"},"schema_version":"1.0","source":{"id":"1207.3854","kind":"arxiv","version":4}},"canonical_sha256":"6ed30bd02fb2c22b6c3af8396cd54166d9476adba3bcac1ba7e73c23a65e3e51","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6ed30bd02fb2c22b6c3af8396cd54166d9476adba3bcac1ba7e73c23a65e3e51","first_computed_at":"2026-05-18T01:56:17.676038Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:56:17.676038Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"0bit26uEajjiK1GldKRgM3yiPSjfmLXtlYJ4ktRHnM6wQwbZ6NU3YG2blNEoMHR1lRXIE+Cb2oO4aYF4RrMxCw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:56:17.676552Z","signed_message":"canonical_sha256_bytes"},"source_id":"1207.3854","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2b8a7cc1b4d50cae4554118e3a062b8d1a79ffb537a93bce8133d7f024df16e2","sha256:1920e0d73325a1d0a841d74c5d8629b420a4b16d42e2b03115fed20e35acd44f"],"state_sha256":"a6fe6af4e3317600824ee78470a5805fac67a7d7403f5bb8b1a842d38194fc8e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lCB+vq72yUDdbbj5OkKjsA2wOPeEKXIwYAmIDcBUXsSdryWNSnoc53IjophHiBHe7WX9RQXY50PtL13kvqiRAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-11T00:55:20.596103Z","bundle_sha256":"c6e044e5405c4d9582baf4cd68cb4a5b70c313a100f3d144a7c71678bad592f6"}}