{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:YAOP547SC4ZJF6RPH7PWQRJLFH","short_pith_number":"pith:YAOP547S","schema_version":"1.0","canonical_sha256":"c01cfef3f2173292fa2f3fdf68452b29cbdbe8de32550f9ba963cf609b469ea4","source":{"kind":"arxiv","id":"1311.2939","version":3},"attestation_state":"computed","paper":{"title":"Topological energy bounds in generalized Skyrme models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"A. Wereszczynski, C. Adam","submitted_at":"2013-11-12T21:00:05Z","abstract_excerpt":"The Skyrme model has a natural generalization amenable to a standard hamiltonian treatment, consisting of the standard sigma model and the Skyrme terms, a potential, and a certain term sextic in first derivatives. Here we demonstrate that, in this theory, each pair of terms in the static energy functional which may support topological solitons according to the Derrick criterion (i.e., each pair of terms with opposite Derrick scaling) separately posesses a topological energy bound. As a consequence, there exists a four-parameter family of topological bounds for the full generalized Skyrme model"},"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":"1311.2939","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-11-12T21:00:05Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"ab27e638d0d9619e598515b03bc635a894d695ee3cac409758415b096f126e4f","abstract_canon_sha256":"ee0f62ac8e83dfa69ee11d72d7c50d49be5c78d6371717af4a73f49b18044f54"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:56:11.301098Z","signature_b64":"aXLRQABEfMtAyOv/+/5wU51hCDzD+ZGFaQgb1MoLjz0W3MLBQyHA5sNlAy9tQ1mQrIG5CrJYIQGcPCUgQ6AnDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c01cfef3f2173292fa2f3fdf68452b29cbdbe8de32550f9ba963cf609b469ea4","last_reissued_at":"2026-05-18T02:56:11.300723Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:56:11.300723Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Topological energy bounds in generalized Skyrme models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"A. Wereszczynski, C. Adam","submitted_at":"2013-11-12T21:00:05Z","abstract_excerpt":"The Skyrme model has a natural generalization amenable to a standard hamiltonian treatment, consisting of the standard sigma model and the Skyrme terms, a potential, and a certain term sextic in first derivatives. Here we demonstrate that, in this theory, each pair of terms in the static energy functional which may support topological solitons according to the Derrick criterion (i.e., each pair of terms with opposite Derrick scaling) separately posesses a topological energy bound. As a consequence, there exists a four-parameter family of topological bounds for the full generalized Skyrme model"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.2939","kind":"arxiv","version":3},"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":"1311.2939","created_at":"2026-05-18T02:56:11.300784+00:00"},{"alias_kind":"arxiv_version","alias_value":"1311.2939v3","created_at":"2026-05-18T02:56:11.300784+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.2939","created_at":"2026-05-18T02:56:11.300784+00:00"},{"alias_kind":"pith_short_12","alias_value":"YAOP547SC4ZJ","created_at":"2026-05-18T12:28:06.772260+00:00"},{"alias_kind":"pith_short_16","alias_value":"YAOP547SC4ZJF6RP","created_at":"2026-05-18T12:28:06.772260+00:00"},{"alias_kind":"pith_short_8","alias_value":"YAOP547S","created_at":"2026-05-18T12:28:06.772260+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/YAOP547SC4ZJF6RPH7PWQRJLFH","json":"https://pith.science/pith/YAOP547SC4ZJF6RPH7PWQRJLFH.json","graph_json":"https://pith.science/api/pith-number/YAOP547SC4ZJF6RPH7PWQRJLFH/graph.json","events_json":"https://pith.science/api/pith-number/YAOP547SC4ZJF6RPH7PWQRJLFH/events.json","paper":"https://pith.science/paper/YAOP547S"},"agent_actions":{"view_html":"https://pith.science/pith/YAOP547SC4ZJF6RPH7PWQRJLFH","download_json":"https://pith.science/pith/YAOP547SC4ZJF6RPH7PWQRJLFH.json","view_paper":"https://pith.science/paper/YAOP547S","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1311.2939&json=true","fetch_graph":"https://pith.science/api/pith-number/YAOP547SC4ZJF6RPH7PWQRJLFH/graph.json","fetch_events":"https://pith.science/api/pith-number/YAOP547SC4ZJF6RPH7PWQRJLFH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YAOP547SC4ZJF6RPH7PWQRJLFH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YAOP547SC4ZJF6RPH7PWQRJLFH/action/storage_attestation","attest_author":"https://pith.science/pith/YAOP547SC4ZJF6RPH7PWQRJLFH/action/author_attestation","sign_citation":"https://pith.science/pith/YAOP547SC4ZJF6RPH7PWQRJLFH/action/citation_signature","submit_replication":"https://pith.science/pith/YAOP547SC4ZJF6RPH7PWQRJLFH/action/replication_record"}},"created_at":"2026-05-18T02:56:11.300784+00:00","updated_at":"2026-05-18T02:56:11.300784+00:00"}