{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:XH7VJBXUWKRDIYP3VQIKIND74Y","short_pith_number":"pith:XH7VJBXU","schema_version":"1.0","canonical_sha256":"b9ff5486f4b2a23461fbac10a4347fe621e60db14bb0ebfe1ff61db5d720ac0c","source":{"kind":"arxiv","id":"1704.05975","version":1},"attestation_state":"computed","paper":{"title":"Re-interpretation of Skyrme Theory: New Topological structures","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Kyoungtae Kimm, Liping Zou, Pengming Zhang, Y. M. Cho","submitted_at":"2017-04-20T01:29:24Z","abstract_excerpt":"Recently it has been pointed out that the skyrmions carry two independent topology, the baryon topology and the monopole topology. We provide more evidence to support this. In specific, we prove that the baryon number $B$ can be decomposed to the monopole number $m$ and the shell number $n$, so that $B$ is given by $B=mn$. This tells that the skyrmions may more conveniently be classified by two integers $(m,n)$. This is because the rational map which determines the baryon number in the popular multi-skyrmion solutions actually describes the monopole topology $\\pi_2(S^2)$ which is different fro"},"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":"1704.05975","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-04-20T01:29:24Z","cross_cats_sorted":[],"title_canon_sha256":"39777ec9aec4dd9e52bc8e23d0473811f9b8d85e3d0dc68883c92168bf5c755f","abstract_canon_sha256":"769f20b3f072d0d40fcb61615611436523db4b1f155535ef9bae92ddf373b78a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:20:30.342820Z","signature_b64":"jedeVkJzQueUCJoz8Fk2EvAPYEVEryzB6SIudXGeGdP4wpMwJnMFsP0Mu57XW39YXnKgxcZE5dOL5NiYS5pvBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b9ff5486f4b2a23461fbac10a4347fe621e60db14bb0ebfe1ff61db5d720ac0c","last_reissued_at":"2026-05-18T00:20:30.342132Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:20:30.342132Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Re-interpretation of Skyrme Theory: New Topological structures","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Kyoungtae Kimm, Liping Zou, Pengming Zhang, Y. M. Cho","submitted_at":"2017-04-20T01:29:24Z","abstract_excerpt":"Recently it has been pointed out that the skyrmions carry two independent topology, the baryon topology and the monopole topology. We provide more evidence to support this. In specific, we prove that the baryon number $B$ can be decomposed to the monopole number $m$ and the shell number $n$, so that $B$ is given by $B=mn$. This tells that the skyrmions may more conveniently be classified by two integers $(m,n)$. This is because the rational map which determines the baryon number in the popular multi-skyrmion solutions actually describes the monopole topology $\\pi_2(S^2)$ which is different fro"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.05975","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":"1704.05975","created_at":"2026-05-18T00:20:30.342237+00:00"},{"alias_kind":"arxiv_version","alias_value":"1704.05975v1","created_at":"2026-05-18T00:20:30.342237+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.05975","created_at":"2026-05-18T00:20:30.342237+00:00"},{"alias_kind":"pith_short_12","alias_value":"XH7VJBXUWKRD","created_at":"2026-05-18T12:31:53.515858+00:00"},{"alias_kind":"pith_short_16","alias_value":"XH7VJBXUWKRDIYP3","created_at":"2026-05-18T12:31:53.515858+00:00"},{"alias_kind":"pith_short_8","alias_value":"XH7VJBXU","created_at":"2026-05-18T12:31:53.515858+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.04939","citing_title":"From Nuclear Matter with Quenched $g_A$ to Compact-Star Matter with a Signal for Emergent Hidden Scale Symmetry","ref_index":30,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XH7VJBXUWKRDIYP3VQIKIND74Y","json":"https://pith.science/pith/XH7VJBXUWKRDIYP3VQIKIND74Y.json","graph_json":"https://pith.science/api/pith-number/XH7VJBXUWKRDIYP3VQIKIND74Y/graph.json","events_json":"https://pith.science/api/pith-number/XH7VJBXUWKRDIYP3VQIKIND74Y/events.json","paper":"https://pith.science/paper/XH7VJBXU"},"agent_actions":{"view_html":"https://pith.science/pith/XH7VJBXUWKRDIYP3VQIKIND74Y","download_json":"https://pith.science/pith/XH7VJBXUWKRDIYP3VQIKIND74Y.json","view_paper":"https://pith.science/paper/XH7VJBXU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1704.05975&json=true","fetch_graph":"https://pith.science/api/pith-number/XH7VJBXUWKRDIYP3VQIKIND74Y/graph.json","fetch_events":"https://pith.science/api/pith-number/XH7VJBXUWKRDIYP3VQIKIND74Y/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XH7VJBXUWKRDIYP3VQIKIND74Y/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XH7VJBXUWKRDIYP3VQIKIND74Y/action/storage_attestation","attest_author":"https://pith.science/pith/XH7VJBXUWKRDIYP3VQIKIND74Y/action/author_attestation","sign_citation":"https://pith.science/pith/XH7VJBXUWKRDIYP3VQIKIND74Y/action/citation_signature","submit_replication":"https://pith.science/pith/XH7VJBXUWKRDIYP3VQIKIND74Y/action/replication_record"}},"created_at":"2026-05-18T00:20:30.342237+00:00","updated_at":"2026-05-18T00:20:30.342237+00:00"}