{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:JYKRJDU62SFYJ7BSPF6JUDQNZ4","short_pith_number":"pith:JYKRJDU6","schema_version":"1.0","canonical_sha256":"4e15148e9ed48b84fc32797c9a0e0dcf0dd4afde7daa5a109cbf5359e4e1f751","source":{"kind":"arxiv","id":"1710.04041","version":1},"attestation_state":"computed","paper":{"title":"Asymptotic analysis of the Berry curvature in the $E\\otimes e$ Jahn-Teller model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.other","quant-ph"],"primary_cat":"physics.chem-ph","authors_text":"Cesar R. Proetto, E. K. U. Gross, Ryan Requist","submitted_at":"2017-10-11T12:54:56Z","abstract_excerpt":"The effective Hamiltonian for the linear $E\\otimes e$ Jahn-Teller model describes the coupling between two electronic states and two vibrational modes in molecules or bulk crystal impurities. While in the Born-Oppenheimer approximation the Berry curvature has a delta function singularity at the conical intersection of the potential energy surfaces, the exact Berry curvature is a smooth peaked function. Numerical calculations revealed that the characteristic width of the peak is $\\hbar K^{1/2}/gM^{1/2}$, where $M$ is the mass associated with the relevant nuclear coordinates, $K$ is the effectiv"},"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":"1710.04041","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2017-10-11T12:54:56Z","cross_cats_sorted":["cond-mat.other","quant-ph"],"title_canon_sha256":"5b5bc537bead611e83d9784d8e7adf97272bacb514a5c7f089897fe6d9626131","abstract_canon_sha256":"6ecd87af419ce66db1dd725e7e9930e44074648de6810d4a83b54a906dd755a2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:27:52.113356Z","signature_b64":"jG/3+q91VoQVmc1kG2UZiD0VWfZbofGbmR3YHzdV1cHUJDAJHFUf4IOPzguvx8hdiC9sFboZC4aVjs7yppvuCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4e15148e9ed48b84fc32797c9a0e0dcf0dd4afde7daa5a109cbf5359e4e1f751","last_reissued_at":"2026-05-18T00:27:52.112746Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:27:52.112746Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Asymptotic analysis of the Berry curvature in the $E\\otimes e$ Jahn-Teller model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.other","quant-ph"],"primary_cat":"physics.chem-ph","authors_text":"Cesar R. Proetto, E. K. U. Gross, Ryan Requist","submitted_at":"2017-10-11T12:54:56Z","abstract_excerpt":"The effective Hamiltonian for the linear $E\\otimes e$ Jahn-Teller model describes the coupling between two electronic states and two vibrational modes in molecules or bulk crystal impurities. While in the Born-Oppenheimer approximation the Berry curvature has a delta function singularity at the conical intersection of the potential energy surfaces, the exact Berry curvature is a smooth peaked function. Numerical calculations revealed that the characteristic width of the peak is $\\hbar K^{1/2}/gM^{1/2}$, where $M$ is the mass associated with the relevant nuclear coordinates, $K$ is the effectiv"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.04041","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":"1710.04041","created_at":"2026-05-18T00:27:52.112868+00:00"},{"alias_kind":"arxiv_version","alias_value":"1710.04041v1","created_at":"2026-05-18T00:27:52.112868+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.04041","created_at":"2026-05-18T00:27:52.112868+00:00"},{"alias_kind":"pith_short_12","alias_value":"JYKRJDU62SFY","created_at":"2026-05-18T12:31:24.725408+00:00"},{"alias_kind":"pith_short_16","alias_value":"JYKRJDU62SFYJ7BS","created_at":"2026-05-18T12:31:24.725408+00:00"},{"alias_kind":"pith_short_8","alias_value":"JYKRJDU6","created_at":"2026-05-18T12:31:24.725408+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/JYKRJDU62SFYJ7BSPF6JUDQNZ4","json":"https://pith.science/pith/JYKRJDU62SFYJ7BSPF6JUDQNZ4.json","graph_json":"https://pith.science/api/pith-number/JYKRJDU62SFYJ7BSPF6JUDQNZ4/graph.json","events_json":"https://pith.science/api/pith-number/JYKRJDU62SFYJ7BSPF6JUDQNZ4/events.json","paper":"https://pith.science/paper/JYKRJDU6"},"agent_actions":{"view_html":"https://pith.science/pith/JYKRJDU62SFYJ7BSPF6JUDQNZ4","download_json":"https://pith.science/pith/JYKRJDU62SFYJ7BSPF6JUDQNZ4.json","view_paper":"https://pith.science/paper/JYKRJDU6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1710.04041&json=true","fetch_graph":"https://pith.science/api/pith-number/JYKRJDU62SFYJ7BSPF6JUDQNZ4/graph.json","fetch_events":"https://pith.science/api/pith-number/JYKRJDU62SFYJ7BSPF6JUDQNZ4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JYKRJDU62SFYJ7BSPF6JUDQNZ4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JYKRJDU62SFYJ7BSPF6JUDQNZ4/action/storage_attestation","attest_author":"https://pith.science/pith/JYKRJDU62SFYJ7BSPF6JUDQNZ4/action/author_attestation","sign_citation":"https://pith.science/pith/JYKRJDU62SFYJ7BSPF6JUDQNZ4/action/citation_signature","submit_replication":"https://pith.science/pith/JYKRJDU62SFYJ7BSPF6JUDQNZ4/action/replication_record"}},"created_at":"2026-05-18T00:27:52.112868+00:00","updated_at":"2026-05-18T00:27:52.112868+00:00"}