{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:ATJWP6ZQDYS6JIZB3ROJHHON5E","short_pith_number":"pith:ATJWP6ZQ","schema_version":"1.0","canonical_sha256":"04d367fb301e25e4a321dc5c939dcde91317625b773a7fb1780be44772a24e6c","source":{"kind":"arxiv","id":"0903.2707","version":3},"attestation_state":"computed","paper":{"title":"Dielectric Breakdown in a Mott Insulator: Many-body Schwinger-Landau-Zener Mechanism studied with a Generalized Bethe Ansatz","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","hep-th"],"primary_cat":"cond-mat.stat-mech","authors_text":"Hideo Aoki, Takashi Oka","submitted_at":"2009-03-16T09:10:02Z","abstract_excerpt":"The nonadiabatic quantum tunneling picture, which may be called the many-body Schwinger-Landau-Zener mechanism, for the dielectric breakdown of Mott insulators in strong electric fields is studied in the one-dimensional Hubbard model. The tunneling probability is calculated by a metod due to Dykhne-Davis-Pechukas with an analytical continuation of the Bethe-ansatz solution for excited states to a non-Hermitian case. A remarkable agreement with the time-dependent density matrix renormalization group result is obtained."},"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":"0903.2707","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2009-03-16T09:10:02Z","cross_cats_sorted":["cond-mat.str-el","hep-th"],"title_canon_sha256":"ca38924a27e3f22fbfa16604d8f0e57939d2139ea98d1ede5a9e77879bb60fad","abstract_canon_sha256":"36c7f0cdc928bb5681fbc3fe5f62eb6c76504eb9a6cc6e8ba7b0b4b289197e78"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:35:00.399283Z","signature_b64":"gqYClFzzT3pixZUxMvc+GqqrJyqNoYw3Yx+H3LNrCnOJEEQXM9FzRRohqDSixc9EPIcAc3+gfzeA8N8ZLRfUAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"04d367fb301e25e4a321dc5c939dcde91317625b773a7fb1780be44772a24e6c","last_reissued_at":"2026-05-18T02:35:00.398917Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:35:00.398917Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dielectric Breakdown in a Mott Insulator: Many-body Schwinger-Landau-Zener Mechanism studied with a Generalized Bethe Ansatz","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","hep-th"],"primary_cat":"cond-mat.stat-mech","authors_text":"Hideo Aoki, Takashi Oka","submitted_at":"2009-03-16T09:10:02Z","abstract_excerpt":"The nonadiabatic quantum tunneling picture, which may be called the many-body Schwinger-Landau-Zener mechanism, for the dielectric breakdown of Mott insulators in strong electric fields is studied in the one-dimensional Hubbard model. The tunneling probability is calculated by a metod due to Dykhne-Davis-Pechukas with an analytical continuation of the Bethe-ansatz solution for excited states to a non-Hermitian case. A remarkable agreement with the time-dependent density matrix renormalization group result is obtained."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0903.2707","kind":"arxiv","version":3},"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":"0903.2707","created_at":"2026-05-18T02:35:00.398975+00:00"},{"alias_kind":"arxiv_version","alias_value":"0903.2707v3","created_at":"2026-05-18T02:35:00.398975+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0903.2707","created_at":"2026-05-18T02:35:00.398975+00:00"},{"alias_kind":"pith_short_12","alias_value":"ATJWP6ZQDYS6","created_at":"2026-05-18T12:25:58.837520+00:00"},{"alias_kind":"pith_short_16","alias_value":"ATJWP6ZQDYS6JIZB","created_at":"2026-05-18T12:25:58.837520+00:00"},{"alias_kind":"pith_short_8","alias_value":"ATJWP6ZQ","created_at":"2026-05-18T12:25:58.837520+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/ATJWP6ZQDYS6JIZB3ROJHHON5E","json":"https://pith.science/pith/ATJWP6ZQDYS6JIZB3ROJHHON5E.json","graph_json":"https://pith.science/api/pith-number/ATJWP6ZQDYS6JIZB3ROJHHON5E/graph.json","events_json":"https://pith.science/api/pith-number/ATJWP6ZQDYS6JIZB3ROJHHON5E/events.json","paper":"https://pith.science/paper/ATJWP6ZQ"},"agent_actions":{"view_html":"https://pith.science/pith/ATJWP6ZQDYS6JIZB3ROJHHON5E","download_json":"https://pith.science/pith/ATJWP6ZQDYS6JIZB3ROJHHON5E.json","view_paper":"https://pith.science/paper/ATJWP6ZQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0903.2707&json=true","fetch_graph":"https://pith.science/api/pith-number/ATJWP6ZQDYS6JIZB3ROJHHON5E/graph.json","fetch_events":"https://pith.science/api/pith-number/ATJWP6ZQDYS6JIZB3ROJHHON5E/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ATJWP6ZQDYS6JIZB3ROJHHON5E/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ATJWP6ZQDYS6JIZB3ROJHHON5E/action/storage_attestation","attest_author":"https://pith.science/pith/ATJWP6ZQDYS6JIZB3ROJHHON5E/action/author_attestation","sign_citation":"https://pith.science/pith/ATJWP6ZQDYS6JIZB3ROJHHON5E/action/citation_signature","submit_replication":"https://pith.science/pith/ATJWP6ZQDYS6JIZB3ROJHHON5E/action/replication_record"}},"created_at":"2026-05-18T02:35:00.398975+00:00","updated_at":"2026-05-18T02:35:00.398975+00:00"}