{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:MFESQND6DBTPTJKTX464V55MZY","short_pith_number":"pith:MFESQND6","schema_version":"1.0","canonical_sha256":"614928347e1866f9a553bf3dcaf7acce2116113b2d4ecffe0bd5ba58f866367b","source":{"kind":"arxiv","id":"2312.10927","version":1},"attestation_state":"computed","paper":{"title":"Non-Abelian chiral soliton lattice in rotating QCD matter: Nambu-Goldstone and excited modes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Kentaro Nishimura, Minoru Eto, Muneto Nitta","submitted_at":"2023-12-18T04:36:13Z","abstract_excerpt":"The ground state of QCD with two flavors at a finite baryon chemical potential under rapid rotation is a chiral soliton lattice (CSL) of the $\\eta$ meson, consisting of a stack of sine-Gordon solitons carrying a baryon number, due to the anomalous coupling of the $\\eta$ meson to the rotation. In a large parameter region, the ground state becomes a non-Abelian CSL, in which due to the neutral pion condensation each $\\eta$ soliton decays into a pair of non-Abelian sine-Gordon solitons carrying $S^2$ moduli originated from Nambu-Goldstone (NG) modes localized around it, corresponding to the spont"},"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":"2312.10927","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2023-12-18T04:36:13Z","cross_cats_sorted":["hep-th","nucl-th"],"title_canon_sha256":"4377db79267077f98f51729803a12e54921da0262924486f02094fced71575b0","abstract_canon_sha256":"acb675ec9ff8a4b57af6cf5469d383de753485397a4634bf8c11278c800a19c9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:25:14.397512Z","signature_b64":"qx9dPZN1p2YO1CplRclmfeHZkBBojZpZ9m3qSBQWl0ViL9SOam02wZpgw5hkGywfA1uDOF1lp5/caj27DTqRCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"614928347e1866f9a553bf3dcaf7acce2116113b2d4ecffe0bd5ba58f866367b","last_reissued_at":"2026-07-05T07:25:14.397007Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:25:14.397007Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-Abelian chiral soliton lattice in rotating QCD matter: Nambu-Goldstone and excited modes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Kentaro Nishimura, Minoru Eto, Muneto Nitta","submitted_at":"2023-12-18T04:36:13Z","abstract_excerpt":"The ground state of QCD with two flavors at a finite baryon chemical potential under rapid rotation is a chiral soliton lattice (CSL) of the $\\eta$ meson, consisting of a stack of sine-Gordon solitons carrying a baryon number, due to the anomalous coupling of the $\\eta$ meson to the rotation. In a large parameter region, the ground state becomes a non-Abelian CSL, in which due to the neutral pion condensation each $\\eta$ soliton decays into a pair of non-Abelian sine-Gordon solitons carrying $S^2$ moduli originated from Nambu-Goldstone (NG) modes localized around it, corresponding to the spont"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2312.10927","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2312.10927/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2312.10927","created_at":"2026-07-05T07:25:14.397067+00:00"},{"alias_kind":"arxiv_version","alias_value":"2312.10927v1","created_at":"2026-07-05T07:25:14.397067+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2312.10927","created_at":"2026-07-05T07:25:14.397067+00:00"},{"alias_kind":"pith_short_12","alias_value":"MFESQND6DBTP","created_at":"2026-07-05T07:25:14.397067+00:00"},{"alias_kind":"pith_short_16","alias_value":"MFESQND6DBTPTJKT","created_at":"2026-07-05T07:25:14.397067+00:00"},{"alias_kind":"pith_short_8","alias_value":"MFESQND6","created_at":"2026-07-05T07:25:14.397067+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2512.22023","citing_title":"Fermionic domain-wall Skyrmions of QCD in a magnetic field","ref_index":22,"is_internal_anchor":false},{"citing_arxiv_id":"2603.29325","citing_title":"Baryonic vortices in rotating nuclear matter","ref_index":14,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MFESQND6DBTPTJKTX464V55MZY","json":"https://pith.science/pith/MFESQND6DBTPTJKTX464V55MZY.json","graph_json":"https://pith.science/api/pith-number/MFESQND6DBTPTJKTX464V55MZY/graph.json","events_json":"https://pith.science/api/pith-number/MFESQND6DBTPTJKTX464V55MZY/events.json","paper":"https://pith.science/paper/MFESQND6"},"agent_actions":{"view_html":"https://pith.science/pith/MFESQND6DBTPTJKTX464V55MZY","download_json":"https://pith.science/pith/MFESQND6DBTPTJKTX464V55MZY.json","view_paper":"https://pith.science/paper/MFESQND6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2312.10927&json=true","fetch_graph":"https://pith.science/api/pith-number/MFESQND6DBTPTJKTX464V55MZY/graph.json","fetch_events":"https://pith.science/api/pith-number/MFESQND6DBTPTJKTX464V55MZY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MFESQND6DBTPTJKTX464V55MZY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MFESQND6DBTPTJKTX464V55MZY/action/storage_attestation","attest_author":"https://pith.science/pith/MFESQND6DBTPTJKTX464V55MZY/action/author_attestation","sign_citation":"https://pith.science/pith/MFESQND6DBTPTJKTX464V55MZY/action/citation_signature","submit_replication":"https://pith.science/pith/MFESQND6DBTPTJKTX464V55MZY/action/replication_record"}},"created_at":"2026-07-05T07:25:14.397067+00:00","updated_at":"2026-07-05T07:25:14.397067+00:00"}