{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:PJK5NSEI2RXJVZY6W2PARBA363","short_pith_number":"pith:PJK5NSEI","schema_version":"1.0","canonical_sha256":"7a55d6c888d46e9ae71eb69e08841bf6ef68679cb2f4e159456f9a706e29d05c","source":{"kind":"arxiv","id":"2405.06030","version":1},"attestation_state":"computed","paper":{"title":"Excited Abelian-Higgs vortices: decay rate and radiation emission","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"A. Alonso-Izquierdo, D. Migu\\'elez-Caballero, J. J. Blanco-Pillado, J. Queiruga, S. Navarro-Obreg\\'on","submitted_at":"2024-05-09T18:00:45Z","abstract_excerpt":"The evolution of 1-vortices when their massive bound mode is excited is investigated in detail (both analytically and numerically) in the Abelian-Higgs model for different ranges of the self-coupling constant. The dependence of the spectrum of the 1-vortex fluctuation operator on the model parameter is discussed initially. A perturbative approach is employed to study the radiation emission in both the scalar and the vector channels. Our findings reveal that the oscillating initial configuration of the 1-vortex radiates at a frequency twice that of the internal mode. Through energy conservation"},"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":"2405.06030","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-05-09T18:00:45Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"75cf72491206f15d4552c97db0c2e94e99367ef9cf4e2e87099d0dfb88fba395","abstract_canon_sha256":"b417dae307558ba000b600a4f43f64e0e96205634ddfbc8bd516c01a5a84510b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:17:34.427341Z","signature_b64":"vceAXSYHgyeDHApJVGj4Sc5ePEv6INj/ldthyCQ27TZLyr3QU/SUmU/ZIEa6KApUrxpu8d4O1l5uRMvobpRSBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7a55d6c888d46e9ae71eb69e08841bf6ef68679cb2f4e159456f9a706e29d05c","last_reissued_at":"2026-07-05T08:17:34.426712Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:17:34.426712Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Excited Abelian-Higgs vortices: decay rate and radiation emission","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"A. Alonso-Izquierdo, D. Migu\\'elez-Caballero, J. J. Blanco-Pillado, J. Queiruga, S. Navarro-Obreg\\'on","submitted_at":"2024-05-09T18:00:45Z","abstract_excerpt":"The evolution of 1-vortices when their massive bound mode is excited is investigated in detail (both analytically and numerically) in the Abelian-Higgs model for different ranges of the self-coupling constant. The dependence of the spectrum of the 1-vortex fluctuation operator on the model parameter is discussed initially. A perturbative approach is employed to study the radiation emission in both the scalar and the vector channels. Our findings reveal that the oscillating initial configuration of the 1-vortex radiates at a frequency twice that of the internal mode. Through energy conservation"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2405.06030","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/2405.06030/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":"2405.06030","created_at":"2026-07-05T08:17:34.426789+00:00"},{"alias_kind":"arxiv_version","alias_value":"2405.06030v1","created_at":"2026-07-05T08:17:34.426789+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2405.06030","created_at":"2026-07-05T08:17:34.426789+00:00"},{"alias_kind":"pith_short_12","alias_value":"PJK5NSEI2RXJ","created_at":"2026-07-05T08:17:34.426789+00:00"},{"alias_kind":"pith_short_16","alias_value":"PJK5NSEI2RXJVZY6","created_at":"2026-07-05T08:17:34.426789+00:00"},{"alias_kind":"pith_short_8","alias_value":"PJK5NSEI","created_at":"2026-07-05T08:17:34.426789+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.04799","citing_title":"The Domain Wall String's Anti-Stokes Scattering Cross Section","ref_index":30,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PJK5NSEI2RXJVZY6W2PARBA363","json":"https://pith.science/pith/PJK5NSEI2RXJVZY6W2PARBA363.json","graph_json":"https://pith.science/api/pith-number/PJK5NSEI2RXJVZY6W2PARBA363/graph.json","events_json":"https://pith.science/api/pith-number/PJK5NSEI2RXJVZY6W2PARBA363/events.json","paper":"https://pith.science/paper/PJK5NSEI"},"agent_actions":{"view_html":"https://pith.science/pith/PJK5NSEI2RXJVZY6W2PARBA363","download_json":"https://pith.science/pith/PJK5NSEI2RXJVZY6W2PARBA363.json","view_paper":"https://pith.science/paper/PJK5NSEI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2405.06030&json=true","fetch_graph":"https://pith.science/api/pith-number/PJK5NSEI2RXJVZY6W2PARBA363/graph.json","fetch_events":"https://pith.science/api/pith-number/PJK5NSEI2RXJVZY6W2PARBA363/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PJK5NSEI2RXJVZY6W2PARBA363/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PJK5NSEI2RXJVZY6W2PARBA363/action/storage_attestation","attest_author":"https://pith.science/pith/PJK5NSEI2RXJVZY6W2PARBA363/action/author_attestation","sign_citation":"https://pith.science/pith/PJK5NSEI2RXJVZY6W2PARBA363/action/citation_signature","submit_replication":"https://pith.science/pith/PJK5NSEI2RXJVZY6W2PARBA363/action/replication_record"}},"created_at":"2026-07-05T08:17:34.426789+00:00","updated_at":"2026-07-05T08:17:34.426789+00:00"}