{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1997:IWEUYKOT5DO6D36XJASAZTJYYZ","short_pith_number":"pith:IWEUYKOT","schema_version":"1.0","canonical_sha256":"45894c29d3e8dde1efd748240ccd38c655f9fae179676510d1bd79fac8215688","source":{"kind":"arxiv","id":"hep-th/9710109","version":1},"attestation_state":"computed","paper":{"title":"Fine-Tuning Renormalization and Two-particle States in Nonrelativistic Four-fermion Model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. B. Tanaev, A. N. Vall, A. V. Sinitskaya, S. E. Korenblit, V. M. Leviant","submitted_at":"1997-10-14T05:01:17Z","abstract_excerpt":"Various exact solutions of two-particle eigenvalue problems for nonrelativistic contact four-fermion current-current interaction are obtained. Specifics of Goldstone mode is investigated. The connection between a renormalization procedure and construction of self-adjoint extensions is revealed."},"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":"hep-th/9710109","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1997-10-14T05:01:17Z","cross_cats_sorted":[],"title_canon_sha256":"68744112034cc3427ffb18f3c4d7850a73a6d65c83b2dacd6de54bfaaea2419a","abstract_canon_sha256":"cba8a95e6e47796a62eb291f68cc95b4c04897e2a582562fa287d3fc128fc8c3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:36:02.069342Z","signature_b64":"cw5Nvtajg/ZRHIKFkMu788L5usumAK3+2h+/UW2xwc65op9KbFH9CW7Cpax65c12PkQNJIjOYxeWPjzT6k8YCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"45894c29d3e8dde1efd748240ccd38c655f9fae179676510d1bd79fac8215688","last_reissued_at":"2026-05-18T02:36:02.068617Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:36:02.068617Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Fine-Tuning Renormalization and Two-particle States in Nonrelativistic Four-fermion Model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. B. Tanaev, A. N. Vall, A. V. Sinitskaya, S. E. Korenblit, V. M. Leviant","submitted_at":"1997-10-14T05:01:17Z","abstract_excerpt":"Various exact solutions of two-particle eigenvalue problems for nonrelativistic contact four-fermion current-current interaction are obtained. Specifics of Goldstone mode is investigated. The connection between a renormalization procedure and construction of self-adjoint extensions is revealed."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9710109","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":"hep-th/9710109","created_at":"2026-05-18T02:36:02.068722+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9710109v1","created_at":"2026-05-18T02:36:02.068722+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9710109","created_at":"2026-05-18T02:36:02.068722+00:00"},{"alias_kind":"pith_short_12","alias_value":"IWEUYKOT5DO6","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_16","alias_value":"IWEUYKOT5DO6D36X","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_8","alias_value":"IWEUYKOT","created_at":"2026-05-18T12:25:48.327863+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/IWEUYKOT5DO6D36XJASAZTJYYZ","json":"https://pith.science/pith/IWEUYKOT5DO6D36XJASAZTJYYZ.json","graph_json":"https://pith.science/api/pith-number/IWEUYKOT5DO6D36XJASAZTJYYZ/graph.json","events_json":"https://pith.science/api/pith-number/IWEUYKOT5DO6D36XJASAZTJYYZ/events.json","paper":"https://pith.science/paper/IWEUYKOT"},"agent_actions":{"view_html":"https://pith.science/pith/IWEUYKOT5DO6D36XJASAZTJYYZ","download_json":"https://pith.science/pith/IWEUYKOT5DO6D36XJASAZTJYYZ.json","view_paper":"https://pith.science/paper/IWEUYKOT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9710109&json=true","fetch_graph":"https://pith.science/api/pith-number/IWEUYKOT5DO6D36XJASAZTJYYZ/graph.json","fetch_events":"https://pith.science/api/pith-number/IWEUYKOT5DO6D36XJASAZTJYYZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IWEUYKOT5DO6D36XJASAZTJYYZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IWEUYKOT5DO6D36XJASAZTJYYZ/action/storage_attestation","attest_author":"https://pith.science/pith/IWEUYKOT5DO6D36XJASAZTJYYZ/action/author_attestation","sign_citation":"https://pith.science/pith/IWEUYKOT5DO6D36XJASAZTJYYZ/action/citation_signature","submit_replication":"https://pith.science/pith/IWEUYKOT5DO6D36XJASAZTJYYZ/action/replication_record"}},"created_at":"2026-05-18T02:36:02.068722+00:00","updated_at":"2026-05-18T02:36:02.068722+00:00"}