{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:YNGS4ETJKRXFHBYGSP5N5AOA24","short_pith_number":"pith:YNGS4ETJ","schema_version":"1.0","canonical_sha256":"c34d2e1269546e53870693fade81c0d704973143e4435eb3fa2bbd48aff11726","source":{"kind":"arxiv","id":"1406.2165","version":1},"attestation_state":"computed","paper":{"title":"Phenomenological Potential Wells for C60 Shell","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atm-clus"],"primary_cat":"physics.atom-ph","authors_text":"A S Baltenkov","submitted_at":"2014-06-09T13:07:46Z","abstract_excerpt":"A spatial distribution of electric charges forming a square potential well has been studied. It is shown that this potential is created by two spherical double charge layers, which is in contradiction with a real molecular structure of C60 cage. A C60 shell potential has been calculated in the assumption that it is formed by the averaged charge density of a neutral atom. It is shown that the phenomenological potentials simulating the C60 shell potential should be selected from a family of potentials with a none-flat bottom. Two possible types of C60 model potentials have been considered and th"},"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":"1406.2165","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2014-06-09T13:07:46Z","cross_cats_sorted":["physics.atm-clus"],"title_canon_sha256":"8657e91e3941812c01c150f24a39dad3e51fa95bbb2294c29bfc42a1f3e04469","abstract_canon_sha256":"f6ab4410549e649e9ea4821602139e78a164266e57ff440da3caee6477953bde"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:50:11.407781Z","signature_b64":"2tuSlCkzTO3Gk88KC3Eo83xxOTtdiHY5SxCxXZbA9Ey4RNBPkA01qX/dbppf+qiGmUfe8tZo989iFXbQWXTTCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c34d2e1269546e53870693fade81c0d704973143e4435eb3fa2bbd48aff11726","last_reissued_at":"2026-05-18T02:50:11.407201Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:50:11.407201Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Phenomenological Potential Wells for C60 Shell","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atm-clus"],"primary_cat":"physics.atom-ph","authors_text":"A S Baltenkov","submitted_at":"2014-06-09T13:07:46Z","abstract_excerpt":"A spatial distribution of electric charges forming a square potential well has been studied. It is shown that this potential is created by two spherical double charge layers, which is in contradiction with a real molecular structure of C60 cage. A C60 shell potential has been calculated in the assumption that it is formed by the averaged charge density of a neutral atom. It is shown that the phenomenological potentials simulating the C60 shell potential should be selected from a family of potentials with a none-flat bottom. Two possible types of C60 model potentials have been considered and th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1406.2165","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":"1406.2165","created_at":"2026-05-18T02:50:11.407308+00:00"},{"alias_kind":"arxiv_version","alias_value":"1406.2165v1","created_at":"2026-05-18T02:50:11.407308+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1406.2165","created_at":"2026-05-18T02:50:11.407308+00:00"},{"alias_kind":"pith_short_12","alias_value":"YNGS4ETJKRXF","created_at":"2026-05-18T12:28:57.508820+00:00"},{"alias_kind":"pith_short_16","alias_value":"YNGS4ETJKRXFHBYG","created_at":"2026-05-18T12:28:57.508820+00:00"},{"alias_kind":"pith_short_8","alias_value":"YNGS4ETJ","created_at":"2026-05-18T12:28:57.508820+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/YNGS4ETJKRXFHBYGSP5N5AOA24","json":"https://pith.science/pith/YNGS4ETJKRXFHBYGSP5N5AOA24.json","graph_json":"https://pith.science/api/pith-number/YNGS4ETJKRXFHBYGSP5N5AOA24/graph.json","events_json":"https://pith.science/api/pith-number/YNGS4ETJKRXFHBYGSP5N5AOA24/events.json","paper":"https://pith.science/paper/YNGS4ETJ"},"agent_actions":{"view_html":"https://pith.science/pith/YNGS4ETJKRXFHBYGSP5N5AOA24","download_json":"https://pith.science/pith/YNGS4ETJKRXFHBYGSP5N5AOA24.json","view_paper":"https://pith.science/paper/YNGS4ETJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1406.2165&json=true","fetch_graph":"https://pith.science/api/pith-number/YNGS4ETJKRXFHBYGSP5N5AOA24/graph.json","fetch_events":"https://pith.science/api/pith-number/YNGS4ETJKRXFHBYGSP5N5AOA24/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YNGS4ETJKRXFHBYGSP5N5AOA24/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YNGS4ETJKRXFHBYGSP5N5AOA24/action/storage_attestation","attest_author":"https://pith.science/pith/YNGS4ETJKRXFHBYGSP5N5AOA24/action/author_attestation","sign_citation":"https://pith.science/pith/YNGS4ETJKRXFHBYGSP5N5AOA24/action/citation_signature","submit_replication":"https://pith.science/pith/YNGS4ETJKRXFHBYGSP5N5AOA24/action/replication_record"}},"created_at":"2026-05-18T02:50:11.407308+00:00","updated_at":"2026-05-18T02:50:11.407308+00:00"}