{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:LZ2GA2RHETEQFU24EOCAAZZKSS","short_pith_number":"pith:LZ2GA2RH","schema_version":"1.0","canonical_sha256":"5e74606a2724c902d35c238400672a94b016bbb496809c58a1683f54b0998f0f","source":{"kind":"arxiv","id":"1104.1298","version":2},"attestation_state":"computed","paper":{"title":"Setting up tunneling conditions by means of Bohmian mechanics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.other","physics.atom-ph","physics.chem-ph"],"primary_cat":"quant-ph","authors_text":"A. S. Sanz, S. Miret-Artes","submitted_at":"2011-04-07T10:58:19Z","abstract_excerpt":"Usually tunneling is established after imposing some matching conditions on the (time-independent) wave function and its first derivative at the boundaries of a barrier. Here an alternative scheme is proposed to determine tunneling and estimate transmission probabilities in time-dependent problems, which takes advantage of the trajectory picture provided by Bohmian mechanics. From this theory a general functional expression for the transmission probability in terms of the system initial state can be reached. This expression is used here to analyze tunneling properties and estimate transmission"},"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":"1104.1298","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2011-04-07T10:58:19Z","cross_cats_sorted":["cond-mat.other","physics.atom-ph","physics.chem-ph"],"title_canon_sha256":"f208448b1ddbbf91148db9ff35f3b6338d1e1b9adfbbd5f5af5f85958db3ca56","abstract_canon_sha256":"2d12de5db2b62c4ee4762cff1770d7d7643a86ce06d3e3cf1d93017a04b2e7e2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:22:10.580387Z","signature_b64":"gXYFAZ3fMDHcJ3nvACWvPHYPtGoEJSnfsfDhaDaQGj7EfnNUd2sKPFrLjcqyZR0s1OiKYBLWeQYnvoRC5TOWDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5e74606a2724c902d35c238400672a94b016bbb496809c58a1683f54b0998f0f","last_reissued_at":"2026-05-18T02:22:10.579892Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:22:10.579892Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Setting up tunneling conditions by means of Bohmian mechanics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.other","physics.atom-ph","physics.chem-ph"],"primary_cat":"quant-ph","authors_text":"A. S. Sanz, S. Miret-Artes","submitted_at":"2011-04-07T10:58:19Z","abstract_excerpt":"Usually tunneling is established after imposing some matching conditions on the (time-independent) wave function and its first derivative at the boundaries of a barrier. Here an alternative scheme is proposed to determine tunneling and estimate transmission probabilities in time-dependent problems, which takes advantage of the trajectory picture provided by Bohmian mechanics. From this theory a general functional expression for the transmission probability in terms of the system initial state can be reached. This expression is used here to analyze tunneling properties and estimate transmission"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1104.1298","kind":"arxiv","version":2},"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":"1104.1298","created_at":"2026-05-18T02:22:10.579971+00:00"},{"alias_kind":"arxiv_version","alias_value":"1104.1298v2","created_at":"2026-05-18T02:22:10.579971+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1104.1298","created_at":"2026-05-18T02:22:10.579971+00:00"},{"alias_kind":"pith_short_12","alias_value":"LZ2GA2RHETEQ","created_at":"2026-05-18T12:26:34.985390+00:00"},{"alias_kind":"pith_short_16","alias_value":"LZ2GA2RHETEQFU24","created_at":"2026-05-18T12:26:34.985390+00:00"},{"alias_kind":"pith_short_8","alias_value":"LZ2GA2RH","created_at":"2026-05-18T12:26:34.985390+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/LZ2GA2RHETEQFU24EOCAAZZKSS","json":"https://pith.science/pith/LZ2GA2RHETEQFU24EOCAAZZKSS.json","graph_json":"https://pith.science/api/pith-number/LZ2GA2RHETEQFU24EOCAAZZKSS/graph.json","events_json":"https://pith.science/api/pith-number/LZ2GA2RHETEQFU24EOCAAZZKSS/events.json","paper":"https://pith.science/paper/LZ2GA2RH"},"agent_actions":{"view_html":"https://pith.science/pith/LZ2GA2RHETEQFU24EOCAAZZKSS","download_json":"https://pith.science/pith/LZ2GA2RHETEQFU24EOCAAZZKSS.json","view_paper":"https://pith.science/paper/LZ2GA2RH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1104.1298&json=true","fetch_graph":"https://pith.science/api/pith-number/LZ2GA2RHETEQFU24EOCAAZZKSS/graph.json","fetch_events":"https://pith.science/api/pith-number/LZ2GA2RHETEQFU24EOCAAZZKSS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LZ2GA2RHETEQFU24EOCAAZZKSS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LZ2GA2RHETEQFU24EOCAAZZKSS/action/storage_attestation","attest_author":"https://pith.science/pith/LZ2GA2RHETEQFU24EOCAAZZKSS/action/author_attestation","sign_citation":"https://pith.science/pith/LZ2GA2RHETEQFU24EOCAAZZKSS/action/citation_signature","submit_replication":"https://pith.science/pith/LZ2GA2RHETEQFU24EOCAAZZKSS/action/replication_record"}},"created_at":"2026-05-18T02:22:10.579971+00:00","updated_at":"2026-05-18T02:22:10.579971+00:00"}