{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:KVX7MWRZ3U5KZD4W3IEGF66R3B","short_pith_number":"pith:KVX7MWRZ","schema_version":"1.0","canonical_sha256":"556ff65a39dd3aac8f96da0862fbd1d87f4f0c78c7a22b84652e6ec9ffc4a024","source":{"kind":"arxiv","id":"2209.12945","version":2},"attestation_state":"computed","paper":{"title":"The dynamics of Domain Wall Strings","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["astro-ph.CO","gr-qc"],"primary_cat":"hep-th","authors_text":"Daniel Jim\\'enez-Aguilar, Jon Urrestilla, Jose J. Blanco-Pillado, Jose M. Queiruga","submitted_at":"2022-09-26T18:30:00Z","abstract_excerpt":"We study the dynamics of domain wall solitons in $(2+1)d$ field theories. These objects are extended along one of the spatial directions, so they also behave as strings; hence the name of domain wall strings. We show analytically and numerically that the amount of radiation from the propagation of wiggles on these objects is negligible except for regions of high curvature. Therefore, at low curvatures, the domain wall strings behave exactly as the Nambu-Goto action predicts. We show this explicitly with the use of several different numerical experiments of the evolution of these objects in a l"},"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":"2209.12945","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-09-26T18:30:00Z","cross_cats_sorted":["astro-ph.CO","gr-qc"],"title_canon_sha256":"003679719103b36d5b7f0623910df95d4e6db343bc26966caacb1b07f0f6d03e","abstract_canon_sha256":"2147b450a6f03a2de5f436c714750c23c5dbe6f5062e0e32f252242fac07dca0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:08:08.952428Z","signature_b64":"Tacu3bjhkZ8wTXURjSW2xWG39YQuBi4jKSWAjDCV3lps/yNcu7aU4OzfMJNQcapmAqXt/6wxyGPMH26Q5gQmBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"556ff65a39dd3aac8f96da0862fbd1d87f4f0c78c7a22b84652e6ec9ffc4a024","last_reissued_at":"2026-07-05T06:08:08.951829Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:08:08.951829Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The dynamics of Domain Wall Strings","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["astro-ph.CO","gr-qc"],"primary_cat":"hep-th","authors_text":"Daniel Jim\\'enez-Aguilar, Jon Urrestilla, Jose J. Blanco-Pillado, Jose M. Queiruga","submitted_at":"2022-09-26T18:30:00Z","abstract_excerpt":"We study the dynamics of domain wall solitons in $(2+1)d$ field theories. These objects are extended along one of the spatial directions, so they also behave as strings; hence the name of domain wall strings. We show analytically and numerically that the amount of radiation from the propagation of wiggles on these objects is negligible except for regions of high curvature. Therefore, at low curvatures, the domain wall strings behave exactly as the Nambu-Goto action predicts. We show this explicitly with the use of several different numerical experiments of the evolution of these objects in a l"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2209.12945","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2209.12945/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":"2209.12945","created_at":"2026-07-05T06:08:08.951891+00:00"},{"alias_kind":"arxiv_version","alias_value":"2209.12945v2","created_at":"2026-07-05T06:08:08.951891+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2209.12945","created_at":"2026-07-05T06:08:08.951891+00:00"},{"alias_kind":"pith_short_12","alias_value":"KVX7MWRZ3U5K","created_at":"2026-07-05T06:08:08.951891+00:00"},{"alias_kind":"pith_short_16","alias_value":"KVX7MWRZ3U5KZD4W","created_at":"2026-07-05T06:08:08.951891+00:00"},{"alias_kind":"pith_short_8","alias_value":"KVX7MWRZ","created_at":"2026-07-05T06:08:08.951891+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.22944","citing_title":"Gravitational waves from cosmic strings with friction: analytical approximations and parameter space","ref_index":38,"is_internal_anchor":false},{"citing_arxiv_id":"2505.11553","citing_title":"Holographic entanglement entropy and complexity for the cosmological braneworld model","ref_index":90,"is_internal_anchor":false},{"citing_arxiv_id":"2604.08142","citing_title":"Caustic formation in DBI models: Wave propagation on planar domain walls","ref_index":50,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KVX7MWRZ3U5KZD4W3IEGF66R3B","json":"https://pith.science/pith/KVX7MWRZ3U5KZD4W3IEGF66R3B.json","graph_json":"https://pith.science/api/pith-number/KVX7MWRZ3U5KZD4W3IEGF66R3B/graph.json","events_json":"https://pith.science/api/pith-number/KVX7MWRZ3U5KZD4W3IEGF66R3B/events.json","paper":"https://pith.science/paper/KVX7MWRZ"},"agent_actions":{"view_html":"https://pith.science/pith/KVX7MWRZ3U5KZD4W3IEGF66R3B","download_json":"https://pith.science/pith/KVX7MWRZ3U5KZD4W3IEGF66R3B.json","view_paper":"https://pith.science/paper/KVX7MWRZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2209.12945&json=true","fetch_graph":"https://pith.science/api/pith-number/KVX7MWRZ3U5KZD4W3IEGF66R3B/graph.json","fetch_events":"https://pith.science/api/pith-number/KVX7MWRZ3U5KZD4W3IEGF66R3B/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KVX7MWRZ3U5KZD4W3IEGF66R3B/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KVX7MWRZ3U5KZD4W3IEGF66R3B/action/storage_attestation","attest_author":"https://pith.science/pith/KVX7MWRZ3U5KZD4W3IEGF66R3B/action/author_attestation","sign_citation":"https://pith.science/pith/KVX7MWRZ3U5KZD4W3IEGF66R3B/action/citation_signature","submit_replication":"https://pith.science/pith/KVX7MWRZ3U5KZD4W3IEGF66R3B/action/replication_record"}},"created_at":"2026-07-05T06:08:08.951891+00:00","updated_at":"2026-07-05T06:08:08.951891+00:00"}