{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:NZVPXZ3LMNSXO7ML2MKSQI2NCG","short_pith_number":"pith:NZVPXZ3L","schema_version":"1.0","canonical_sha256":"6e6afbe76b6365777d8bd31528234d11930fcf2f9336965f9e3edccb14fa6b02","source":{"kind":"arxiv","id":"2502.15087","version":1},"attestation_state":"computed","paper":{"title":"Dynamics of Excited BPS 3-Vortices","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Alonso-Izquierdo, A. Wereszczynski, J. Mateos Guilarte, M. Rees, N.S. Manton","submitted_at":"2025-02-20T23:00:09Z","abstract_excerpt":"We analyze the dynamics of BPS 3-vortex solutions. First, for unexcited vortices, we study the 2-dimensional moduli space of centred vortices with $y \\to -y$ symmetry, and its metric. We identify the 1-dimensional subspaces describing the head-on collisions of equidistant collinear and equilateral triangle configurations, where geodesic motion results in $90^\\circ$ and 60^\\circ$ scattering, respectively. Second, by studying the frequency spectrum of vibrational shape modes along these subspaces, we explain how the force-free, geodesic motion is modified by shape mode excitations into a pattern"},"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":"2502.15087","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2025-02-20T23:00:09Z","cross_cats_sorted":[],"title_canon_sha256":"eceec390e436e9184d6c23841fada5d3db3a6c77e239b4a3c00978ac04a5bff8","abstract_canon_sha256":"8d6c8c62e4ad4fc3319675ddec704bf3a5fd98ea42ca94e0b0b72f58c9fef79c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:17:56.013057Z","signature_b64":"5ZiAWGIJmG+eViECVqL9O+tgzgs7PlAlqtKc2Sum7LZb6yO31mYoJ3RiKJvMFJT2wCrVkXK+DyEr62BViloECg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6e6afbe76b6365777d8bd31528234d11930fcf2f9336965f9e3edccb14fa6b02","last_reissued_at":"2026-07-05T10:17:56.012621Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:17:56.012621Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dynamics of Excited BPS 3-Vortices","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Alonso-Izquierdo, A. Wereszczynski, J. Mateos Guilarte, M. Rees, N.S. Manton","submitted_at":"2025-02-20T23:00:09Z","abstract_excerpt":"We analyze the dynamics of BPS 3-vortex solutions. First, for unexcited vortices, we study the 2-dimensional moduli space of centred vortices with $y \\to -y$ symmetry, and its metric. We identify the 1-dimensional subspaces describing the head-on collisions of equidistant collinear and equilateral triangle configurations, where geodesic motion results in $90^\\circ$ and 60^\\circ$ scattering, respectively. Second, by studying the frequency spectrum of vibrational shape modes along these subspaces, we explain how the force-free, geodesic motion is modified by shape mode excitations into a pattern"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2502.15087","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/2502.15087/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":"2502.15087","created_at":"2026-07-05T10:17:56.012682+00:00"},{"alias_kind":"arxiv_version","alias_value":"2502.15087v1","created_at":"2026-07-05T10:17:56.012682+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2502.15087","created_at":"2026-07-05T10:17:56.012682+00:00"},{"alias_kind":"pith_short_12","alias_value":"NZVPXZ3LMNSX","created_at":"2026-07-05T10:17:56.012682+00:00"},{"alias_kind":"pith_short_16","alias_value":"NZVPXZ3LMNSXO7ML","created_at":"2026-07-05T10:17:56.012682+00:00"},{"alias_kind":"pith_short_8","alias_value":"NZVPXZ3L","created_at":"2026-07-05T10:17:56.012682+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.22680","citing_title":"Unified theory of oscillons and modes","ref_index":59,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NZVPXZ3LMNSXO7ML2MKSQI2NCG","json":"https://pith.science/pith/NZVPXZ3LMNSXO7ML2MKSQI2NCG.json","graph_json":"https://pith.science/api/pith-number/NZVPXZ3LMNSXO7ML2MKSQI2NCG/graph.json","events_json":"https://pith.science/api/pith-number/NZVPXZ3LMNSXO7ML2MKSQI2NCG/events.json","paper":"https://pith.science/paper/NZVPXZ3L"},"agent_actions":{"view_html":"https://pith.science/pith/NZVPXZ3LMNSXO7ML2MKSQI2NCG","download_json":"https://pith.science/pith/NZVPXZ3LMNSXO7ML2MKSQI2NCG.json","view_paper":"https://pith.science/paper/NZVPXZ3L","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2502.15087&json=true","fetch_graph":"https://pith.science/api/pith-number/NZVPXZ3LMNSXO7ML2MKSQI2NCG/graph.json","fetch_events":"https://pith.science/api/pith-number/NZVPXZ3LMNSXO7ML2MKSQI2NCG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NZVPXZ3LMNSXO7ML2MKSQI2NCG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NZVPXZ3LMNSXO7ML2MKSQI2NCG/action/storage_attestation","attest_author":"https://pith.science/pith/NZVPXZ3LMNSXO7ML2MKSQI2NCG/action/author_attestation","sign_citation":"https://pith.science/pith/NZVPXZ3LMNSXO7ML2MKSQI2NCG/action/citation_signature","submit_replication":"https://pith.science/pith/NZVPXZ3LMNSXO7ML2MKSQI2NCG/action/replication_record"}},"created_at":"2026-07-05T10:17:56.012682+00:00","updated_at":"2026-07-05T10:17:56.012682+00:00"}