{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2000:FZBQMTEOZAW4GILSW7HMAKPI3R","short_pith_number":"pith:FZBQMTEO","schema_version":"1.0","canonical_sha256":"2e43064c8ec82dc32172b7cec029e8dc49f8cec63b40d855efd030baa3a6148d","source":{"kind":"arxiv","id":"hep-ph/0009006","version":1},"attestation_state":"computed","paper":{"title":"Nucleons as chiral solitons","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Dmitri Diakonov (NORDITA, St. Petersburg NPI), Victor Petrov (St. Petersburg NPI)","submitted_at":"2000-09-01T10:24:23Z","abstract_excerpt":"In the limit of large number of colors N the nucleon consisting of N quarks is heavy, and one can treat it semiclassically, like the large-Z Thomas--Fermi atom. The role of the semiclassical field binding the quarks in the nucleon is played by the pion or chiral field; its saddle-point distribution inside the nucleon is called the chiral soliton. The old Skyrme model for this soliton is an over-simplification. One can do far better by exploiting a realistic and theoretically-motivated effective chiral lagrangian presented in this paper. As a result one gets not only the static characteristics "},"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-ph/0009006","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2000-09-01T10:24:23Z","cross_cats_sorted":[],"title_canon_sha256":"7b6c1554fc5d0cb87cb5ed86ba56394c94381e34296806eb826ba96b78c94bdc","abstract_canon_sha256":"f9e9bbc44a7eac6d284bdde733c00fbd98e761983953dfbe85b9c1fd3018b0ae"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:57:06.073818Z","signature_b64":"W6jkvDEhacH/fjm3bUAkHa7a6yruatztto2q/A9EcZps3c1wbY3/oSu73IQbVQ8Wt/OTjG+RKrK0X5cKpA3ECQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2e43064c8ec82dc32172b7cec029e8dc49f8cec63b40d855efd030baa3a6148d","last_reissued_at":"2026-05-18T00:57:06.073328Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:57:06.073328Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nucleons as chiral solitons","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Dmitri Diakonov (NORDITA, St. Petersburg NPI), Victor Petrov (St. Petersburg NPI)","submitted_at":"2000-09-01T10:24:23Z","abstract_excerpt":"In the limit of large number of colors N the nucleon consisting of N quarks is heavy, and one can treat it semiclassically, like the large-Z Thomas--Fermi atom. The role of the semiclassical field binding the quarks in the nucleon is played by the pion or chiral field; its saddle-point distribution inside the nucleon is called the chiral soliton. The old Skyrme model for this soliton is an over-simplification. One can do far better by exploiting a realistic and theoretically-motivated effective chiral lagrangian presented in this paper. As a result one gets not only the static characteristics "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0009006","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-ph/0009006","created_at":"2026-05-18T00:57:06.073401+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0009006v1","created_at":"2026-05-18T00:57:06.073401+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0009006","created_at":"2026-05-18T00:57:06.073401+00:00"},{"alias_kind":"pith_short_12","alias_value":"FZBQMTEOZAW4","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_16","alias_value":"FZBQMTEOZAW4GILS","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_8","alias_value":"FZBQMTEO","created_at":"2026-05-18T12:25:49.631198+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/FZBQMTEOZAW4GILSW7HMAKPI3R","json":"https://pith.science/pith/FZBQMTEOZAW4GILSW7HMAKPI3R.json","graph_json":"https://pith.science/api/pith-number/FZBQMTEOZAW4GILSW7HMAKPI3R/graph.json","events_json":"https://pith.science/api/pith-number/FZBQMTEOZAW4GILSW7HMAKPI3R/events.json","paper":"https://pith.science/paper/FZBQMTEO"},"agent_actions":{"view_html":"https://pith.science/pith/FZBQMTEOZAW4GILSW7HMAKPI3R","download_json":"https://pith.science/pith/FZBQMTEOZAW4GILSW7HMAKPI3R.json","view_paper":"https://pith.science/paper/FZBQMTEO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0009006&json=true","fetch_graph":"https://pith.science/api/pith-number/FZBQMTEOZAW4GILSW7HMAKPI3R/graph.json","fetch_events":"https://pith.science/api/pith-number/FZBQMTEOZAW4GILSW7HMAKPI3R/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FZBQMTEOZAW4GILSW7HMAKPI3R/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FZBQMTEOZAW4GILSW7HMAKPI3R/action/storage_attestation","attest_author":"https://pith.science/pith/FZBQMTEOZAW4GILSW7HMAKPI3R/action/author_attestation","sign_citation":"https://pith.science/pith/FZBQMTEOZAW4GILSW7HMAKPI3R/action/citation_signature","submit_replication":"https://pith.science/pith/FZBQMTEOZAW4GILSW7HMAKPI3R/action/replication_record"}},"created_at":"2026-05-18T00:57:06.073401+00:00","updated_at":"2026-05-18T00:57:06.073401+00:00"}