{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:HMNTRKCBZKEFJCJXKKZY3YQ2JB","short_pith_number":"pith:HMNTRKCB","schema_version":"1.0","canonical_sha256":"3b1b38a841ca8854893752b38de21a4845ba1af795bc732af40a0bc8a1cd3f2e","source":{"kind":"arxiv","id":"1610.01942","version":1},"attestation_state":"computed","paper":{"title":"Calculation of Stark resonance parameters for valence orbitals of the water molecule","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"Marko Horbatsch, Susana Arias Laso","submitted_at":"2016-10-06T16:43:58Z","abstract_excerpt":"An exterior complex scaling technique is applied to compute Stark resonance parameters for two molecular orbitals ($1b_{1}$ and $1b_{2}$) represented in the field-free limit in a single-center expansion. For electric DC field configurations that guarantee azimuthal symmetry of the solution the calculation is carried out by solving a two-dimensional partial differential equation in spherical polar coordinates using a finite-element method. The resonance positions and widths as a function of electric field strengths are shown for field strengths starting in the tunnelling ionization regime, and "},"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":"1610.01942","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2016-10-06T16:43:58Z","cross_cats_sorted":[],"title_canon_sha256":"117fdb32a5833b299e9d1bb6722cd485846bcd03ddcc9cbaf84b1bd3794a5dc3","abstract_canon_sha256":"be1827315eaa370788e49c562dffe985f26062f410169f315be0a72cc75d6f92"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:57:07.041748Z","signature_b64":"RH/7YMP3V/O3Fnqj31p3+LpI3W90fEoq08uq9F/HI1ZNevcuWO/nWVt7YNWnDuHNSp1bU1V9sUZU3jhX+VOJAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3b1b38a841ca8854893752b38de21a4845ba1af795bc732af40a0bc8a1cd3f2e","last_reissued_at":"2026-05-18T00:57:07.041275Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:57:07.041275Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Calculation of Stark resonance parameters for valence orbitals of the water molecule","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"Marko Horbatsch, Susana Arias Laso","submitted_at":"2016-10-06T16:43:58Z","abstract_excerpt":"An exterior complex scaling technique is applied to compute Stark resonance parameters for two molecular orbitals ($1b_{1}$ and $1b_{2}$) represented in the field-free limit in a single-center expansion. For electric DC field configurations that guarantee azimuthal symmetry of the solution the calculation is carried out by solving a two-dimensional partial differential equation in spherical polar coordinates using a finite-element method. The resonance positions and widths as a function of electric field strengths are shown for field strengths starting in the tunnelling ionization regime, and "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.01942","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":"1610.01942","created_at":"2026-05-18T00:57:07.041352+00:00"},{"alias_kind":"arxiv_version","alias_value":"1610.01942v1","created_at":"2026-05-18T00:57:07.041352+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.01942","created_at":"2026-05-18T00:57:07.041352+00:00"},{"alias_kind":"pith_short_12","alias_value":"HMNTRKCBZKEF","created_at":"2026-05-18T12:30:19.053100+00:00"},{"alias_kind":"pith_short_16","alias_value":"HMNTRKCBZKEFJCJX","created_at":"2026-05-18T12:30:19.053100+00:00"},{"alias_kind":"pith_short_8","alias_value":"HMNTRKCB","created_at":"2026-05-18T12:30:19.053100+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/HMNTRKCBZKEFJCJXKKZY3YQ2JB","json":"https://pith.science/pith/HMNTRKCBZKEFJCJXKKZY3YQ2JB.json","graph_json":"https://pith.science/api/pith-number/HMNTRKCBZKEFJCJXKKZY3YQ2JB/graph.json","events_json":"https://pith.science/api/pith-number/HMNTRKCBZKEFJCJXKKZY3YQ2JB/events.json","paper":"https://pith.science/paper/HMNTRKCB"},"agent_actions":{"view_html":"https://pith.science/pith/HMNTRKCBZKEFJCJXKKZY3YQ2JB","download_json":"https://pith.science/pith/HMNTRKCBZKEFJCJXKKZY3YQ2JB.json","view_paper":"https://pith.science/paper/HMNTRKCB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1610.01942&json=true","fetch_graph":"https://pith.science/api/pith-number/HMNTRKCBZKEFJCJXKKZY3YQ2JB/graph.json","fetch_events":"https://pith.science/api/pith-number/HMNTRKCBZKEFJCJXKKZY3YQ2JB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HMNTRKCBZKEFJCJXKKZY3YQ2JB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HMNTRKCBZKEFJCJXKKZY3YQ2JB/action/storage_attestation","attest_author":"https://pith.science/pith/HMNTRKCBZKEFJCJXKKZY3YQ2JB/action/author_attestation","sign_citation":"https://pith.science/pith/HMNTRKCBZKEFJCJXKKZY3YQ2JB/action/citation_signature","submit_replication":"https://pith.science/pith/HMNTRKCBZKEFJCJXKKZY3YQ2JB/action/replication_record"}},"created_at":"2026-05-18T00:57:07.041352+00:00","updated_at":"2026-05-18T00:57:07.041352+00:00"}