{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:X5LOUS573ICHJTGSNDCQUGPAXH","short_pith_number":"pith:X5LOUS57","schema_version":"1.0","canonical_sha256":"bf56ea4bbfda0474ccd268c50a19e0b9e9a6a5ced2682ff91817f61121e923c4","source":{"kind":"arxiv","id":"1410.8407","version":2},"attestation_state":"computed","paper":{"title":"Baryonic torii: Toroidal baryons in a generalized Skyrme model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Muneto Nitta, Sven Bjarke Gudnason","submitted_at":"2014-10-30T15:31:57Z","abstract_excerpt":"We study a Skyrme-type model with a potential term motivated by Bose-Einstein condensates (BECs), which we call the BEC Skyrme model. We consider two flavors of the model, the first is the Skyrme model and the second has a sixth-order derivative term instead of the Skyrme term; both with the added BEC-motivated potential. The model contains toroidally shaped Skyrmions and they are characterized by two integers P and Q, representing the winding numbers of two complex scalar fields along the toroidal and poloidal cycles of the torus, respectively. The baryon number is B=PQ. We find stable Skyrmi"},"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":"1410.8407","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-10-30T15:31:57Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"4cfe8a4d500d6edc9e70e38068daa3d02e94bc5dc9e515e9b968627564b3e8ab","abstract_canon_sha256":"4764ccd0adbfd0af24c4b7c3badeb0488609a651105623bb370d70c02db133dc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:26:38.635373Z","signature_b64":"eNP2Tiyv/1V3YFl5KtehBmcvn/a8zuYSpp1fwFnKmkPjMctS3eXBZYMpmafWbLlPZKhe72syZmednktT03m1CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bf56ea4bbfda0474ccd268c50a19e0b9e9a6a5ced2682ff91817f61121e923c4","last_reissued_at":"2026-05-18T02:26:38.634886Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:26:38.634886Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Baryonic torii: Toroidal baryons in a generalized Skyrme model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Muneto Nitta, Sven Bjarke Gudnason","submitted_at":"2014-10-30T15:31:57Z","abstract_excerpt":"We study a Skyrme-type model with a potential term motivated by Bose-Einstein condensates (BECs), which we call the BEC Skyrme model. We consider two flavors of the model, the first is the Skyrme model and the second has a sixth-order derivative term instead of the Skyrme term; both with the added BEC-motivated potential. The model contains toroidally shaped Skyrmions and they are characterized by two integers P and Q, representing the winding numbers of two complex scalar fields along the toroidal and poloidal cycles of the torus, respectively. The baryon number is B=PQ. We find stable Skyrmi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.8407","kind":"arxiv","version":2},"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":"1410.8407","created_at":"2026-05-18T02:26:38.634972+00:00"},{"alias_kind":"arxiv_version","alias_value":"1410.8407v2","created_at":"2026-05-18T02:26:38.634972+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.8407","created_at":"2026-05-18T02:26:38.634972+00:00"},{"alias_kind":"pith_short_12","alias_value":"X5LOUS573ICH","created_at":"2026-05-18T12:28:57.508820+00:00"},{"alias_kind":"pith_short_16","alias_value":"X5LOUS573ICHJTGS","created_at":"2026-05-18T12:28:57.508820+00:00"},{"alias_kind":"pith_short_8","alias_value":"X5LOUS57","created_at":"2026-05-18T12:28:57.508820+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2603.29325","citing_title":"Baryonic vortices in rotating nuclear matter","ref_index":46,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/X5LOUS573ICHJTGSNDCQUGPAXH","json":"https://pith.science/pith/X5LOUS573ICHJTGSNDCQUGPAXH.json","graph_json":"https://pith.science/api/pith-number/X5LOUS573ICHJTGSNDCQUGPAXH/graph.json","events_json":"https://pith.science/api/pith-number/X5LOUS573ICHJTGSNDCQUGPAXH/events.json","paper":"https://pith.science/paper/X5LOUS57"},"agent_actions":{"view_html":"https://pith.science/pith/X5LOUS573ICHJTGSNDCQUGPAXH","download_json":"https://pith.science/pith/X5LOUS573ICHJTGSNDCQUGPAXH.json","view_paper":"https://pith.science/paper/X5LOUS57","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1410.8407&json=true","fetch_graph":"https://pith.science/api/pith-number/X5LOUS573ICHJTGSNDCQUGPAXH/graph.json","fetch_events":"https://pith.science/api/pith-number/X5LOUS573ICHJTGSNDCQUGPAXH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/X5LOUS573ICHJTGSNDCQUGPAXH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/X5LOUS573ICHJTGSNDCQUGPAXH/action/storage_attestation","attest_author":"https://pith.science/pith/X5LOUS573ICHJTGSNDCQUGPAXH/action/author_attestation","sign_citation":"https://pith.science/pith/X5LOUS573ICHJTGSNDCQUGPAXH/action/citation_signature","submit_replication":"https://pith.science/pith/X5LOUS573ICHJTGSNDCQUGPAXH/action/replication_record"}},"created_at":"2026-05-18T02:26:38.634972+00:00","updated_at":"2026-05-18T02:26:38.634972+00:00"}