{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:4NVZ3IMO5LRIMTMQ7TUD45ZCKK","short_pith_number":"pith:4NVZ3IMO","schema_version":"1.0","canonical_sha256":"e36b9da18eeae2864d90fce83e772252b605cf87809291bb9c38b11cfdb1367c","source":{"kind":"arxiv","id":"hep-th/0701294","version":1},"attestation_state":"computed","paper":{"title":"A Phase Transition in U(1) Configuration Space: Oscillons as Remnants of Vortex-Antivortex Annihilation","license":"","headline":"","cross_cats":["astro-ph","cond-mat.supr-con"],"primary_cat":"hep-th","authors_text":"Joel Thorarinson, Marcelo Gleiser","submitted_at":"2007-01-31T19:58:59Z","abstract_excerpt":"We show that the low-momentum scattering of vortex-antivortex pairs can lead to very long-lived oscillon states in 2d Abelian Higgs models. The emergence of oscillons is controlled by the ratio of scalar and vector field masses, $\\beta=(m_s/m_v)^2$ and can be described as a phase transition in field configuration space with critical value $\\beta_c\\simeq 0.13(6)\\pm 2 $: only models with $\\beta<\\beta_c$ lead to oscillon-like remnants. The critical behavior of the system obeys a power law $O(\\beta)\\sim |\\beta-\\beta_c|^o$, where $O$ is an order parameter indicating the presence of oscillons and $o"},"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":"hep-th/0701294","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2007-01-31T19:58:59Z","cross_cats_sorted":["astro-ph","cond-mat.supr-con"],"title_canon_sha256":"e98e286070874c4903675fd9d422a068c74d104c893129cd6525bd93eac1e770","abstract_canon_sha256":"373348b06d99159d61f93c56e37f1ca5ba904cbd36d6fe45947c352e096d0e03"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:22:11.758527Z","signature_b64":"SVlFi64K0ufIIEWaCsVhbBj4cQYpIaW5yEv18ShlLtSrFT8dFJTiW50lvSDUEEW4eJt39HExnkkHGDfz5/wMAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e36b9da18eeae2864d90fce83e772252b605cf87809291bb9c38b11cfdb1367c","last_reissued_at":"2026-07-04T15:22:11.758130Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:22:11.758130Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A Phase Transition in U(1) Configuration Space: Oscillons as Remnants of Vortex-Antivortex Annihilation","license":"","headline":"","cross_cats":["astro-ph","cond-mat.supr-con"],"primary_cat":"hep-th","authors_text":"Joel Thorarinson, Marcelo Gleiser","submitted_at":"2007-01-31T19:58:59Z","abstract_excerpt":"We show that the low-momentum scattering of vortex-antivortex pairs can lead to very long-lived oscillon states in 2d Abelian Higgs models. The emergence of oscillons is controlled by the ratio of scalar and vector field masses, $\\beta=(m_s/m_v)^2$ and can be described as a phase transition in field configuration space with critical value $\\beta_c\\simeq 0.13(6)\\pm 2 $: only models with $\\beta<\\beta_c$ lead to oscillon-like remnants. The critical behavior of the system obeys a power law $O(\\beta)\\sim |\\beta-\\beta_c|^o$, where $O$ is an order parameter indicating the presence of oscillons and $o"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0701294","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/hep-th/0701294/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":"hep-th/0701294","created_at":"2026-07-04T15:22:11.758192+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0701294v1","created_at":"2026-07-04T15:22:11.758192+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0701294","created_at":"2026-07-04T15:22:11.758192+00:00"},{"alias_kind":"pith_short_12","alias_value":"4NVZ3IMO5LRI","created_at":"2026-07-04T15:22:11.758192+00:00"},{"alias_kind":"pith_short_16","alias_value":"4NVZ3IMO5LRIMTMQ","created_at":"2026-07-04T15:22:11.758192+00:00"},{"alias_kind":"pith_short_8","alias_value":"4NVZ3IMO","created_at":"2026-07-04T15:22:11.758192+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":23,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4NVZ3IMO5LRIMTMQ7TUD45ZCKK","json":"https://pith.science/pith/4NVZ3IMO5LRIMTMQ7TUD45ZCKK.json","graph_json":"https://pith.science/api/pith-number/4NVZ3IMO5LRIMTMQ7TUD45ZCKK/graph.json","events_json":"https://pith.science/api/pith-number/4NVZ3IMO5LRIMTMQ7TUD45ZCKK/events.json","paper":"https://pith.science/paper/4NVZ3IMO"},"agent_actions":{"view_html":"https://pith.science/pith/4NVZ3IMO5LRIMTMQ7TUD45ZCKK","download_json":"https://pith.science/pith/4NVZ3IMO5LRIMTMQ7TUD45ZCKK.json","view_paper":"https://pith.science/paper/4NVZ3IMO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0701294&json=true","fetch_graph":"https://pith.science/api/pith-number/4NVZ3IMO5LRIMTMQ7TUD45ZCKK/graph.json","fetch_events":"https://pith.science/api/pith-number/4NVZ3IMO5LRIMTMQ7TUD45ZCKK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4NVZ3IMO5LRIMTMQ7TUD45ZCKK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4NVZ3IMO5LRIMTMQ7TUD45ZCKK/action/storage_attestation","attest_author":"https://pith.science/pith/4NVZ3IMO5LRIMTMQ7TUD45ZCKK/action/author_attestation","sign_citation":"https://pith.science/pith/4NVZ3IMO5LRIMTMQ7TUD45ZCKK/action/citation_signature","submit_replication":"https://pith.science/pith/4NVZ3IMO5LRIMTMQ7TUD45ZCKK/action/replication_record"}},"created_at":"2026-07-04T15:22:11.758192+00:00","updated_at":"2026-07-04T15:22:11.758192+00:00"}