{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:UBT4RNHLHP33CY7VA3LHQNNYET","short_pith_number":"pith:UBT4RNHL","schema_version":"1.0","canonical_sha256":"a067c8b4eb3bf7b163f506d67835b824fc58b9535833097558f3ee08fdb4db64","source":{"kind":"arxiv","id":"1706.07771","version":1},"attestation_state":"computed","paper":{"title":"Stark resonance parameters for the $3a_{1}$ orbital of the water molecule","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph","quant-ph"],"primary_cat":"physics.chem-ph","authors_text":"Marko Horbatsch, Susana Arias Laso","submitted_at":"2017-06-23T16:28:49Z","abstract_excerpt":"The Stark resonance parameters for the $3a_{1}$ molecular orbital of H$_{2}$O are computed by solving a system of partial differential equations in spherical polar coordinates. The starting point of the calculation is the quantum potential derived for this orbital from a single-center expanded Hartree-Fock orbital. The resonance positions and widths are obtained after applying an exterior complex scaling technique to describe the ionization regime for external fields applied along the two distinct $\\hat{z}$ directions associated with the symmetry axis. The procedure thus avoids the computation"},"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":"1706.07771","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2017-06-23T16:28:49Z","cross_cats_sorted":["physics.atom-ph","quant-ph"],"title_canon_sha256":"28cd06753fbf7d09da9501ee6b7ad1af06f8a802fa54bf2768aba8fa01245f98","abstract_canon_sha256":"a2dd4e7fb5c6fe89ff670a42a134ae257ec08d62c1d6bca0c538d8133d863b0a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:30:03.588105Z","signature_b64":"uh+fPtPGGKKP8WHSkbRaqlj7wXohX0pMkGDND95YL2V0VlBGCPhAuT+N7130Hl8R6X8WkRmb6bmcLWuJDHEKDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a067c8b4eb3bf7b163f506d67835b824fc58b9535833097558f3ee08fdb4db64","last_reissued_at":"2026-05-18T00:30:03.587704Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:30:03.587704Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Stark resonance parameters for the $3a_{1}$ orbital of the water molecule","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph","quant-ph"],"primary_cat":"physics.chem-ph","authors_text":"Marko Horbatsch, Susana Arias Laso","submitted_at":"2017-06-23T16:28:49Z","abstract_excerpt":"The Stark resonance parameters for the $3a_{1}$ molecular orbital of H$_{2}$O are computed by solving a system of partial differential equations in spherical polar coordinates. The starting point of the calculation is the quantum potential derived for this orbital from a single-center expanded Hartree-Fock orbital. The resonance positions and widths are obtained after applying an exterior complex scaling technique to describe the ionization regime for external fields applied along the two distinct $\\hat{z}$ directions associated with the symmetry axis. The procedure thus avoids the computation"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.07771","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":"1706.07771","created_at":"2026-05-18T00:30:03.587766+00:00"},{"alias_kind":"arxiv_version","alias_value":"1706.07771v1","created_at":"2026-05-18T00:30:03.587766+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.07771","created_at":"2026-05-18T00:30:03.587766+00:00"},{"alias_kind":"pith_short_12","alias_value":"UBT4RNHLHP33","created_at":"2026-05-18T12:31:46.661854+00:00"},{"alias_kind":"pith_short_16","alias_value":"UBT4RNHLHP33CY7V","created_at":"2026-05-18T12:31:46.661854+00:00"},{"alias_kind":"pith_short_8","alias_value":"UBT4RNHL","created_at":"2026-05-18T12:31:46.661854+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/UBT4RNHLHP33CY7VA3LHQNNYET","json":"https://pith.science/pith/UBT4RNHLHP33CY7VA3LHQNNYET.json","graph_json":"https://pith.science/api/pith-number/UBT4RNHLHP33CY7VA3LHQNNYET/graph.json","events_json":"https://pith.science/api/pith-number/UBT4RNHLHP33CY7VA3LHQNNYET/events.json","paper":"https://pith.science/paper/UBT4RNHL"},"agent_actions":{"view_html":"https://pith.science/pith/UBT4RNHLHP33CY7VA3LHQNNYET","download_json":"https://pith.science/pith/UBT4RNHLHP33CY7VA3LHQNNYET.json","view_paper":"https://pith.science/paper/UBT4RNHL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1706.07771&json=true","fetch_graph":"https://pith.science/api/pith-number/UBT4RNHLHP33CY7VA3LHQNNYET/graph.json","fetch_events":"https://pith.science/api/pith-number/UBT4RNHLHP33CY7VA3LHQNNYET/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UBT4RNHLHP33CY7VA3LHQNNYET/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UBT4RNHLHP33CY7VA3LHQNNYET/action/storage_attestation","attest_author":"https://pith.science/pith/UBT4RNHLHP33CY7VA3LHQNNYET/action/author_attestation","sign_citation":"https://pith.science/pith/UBT4RNHLHP33CY7VA3LHQNNYET/action/citation_signature","submit_replication":"https://pith.science/pith/UBT4RNHLHP33CY7VA3LHQNNYET/action/replication_record"}},"created_at":"2026-05-18T00:30:03.587766+00:00","updated_at":"2026-05-18T00:30:03.587766+00:00"}