{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:QEIF3ULCV6HFZPRGRGTBZXB6C3","short_pith_number":"pith:QEIF3ULC","schema_version":"1.0","canonical_sha256":"81105dd162af8e5cbe2689a61cdc3e16f0f54f2c6a9a82acddc3a6318f719cbf","source":{"kind":"arxiv","id":"1311.3673","version":2},"attestation_state":"computed","paper":{"title":"Vortices in holographic superfluids and superconductors as conformal defects","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"hep-th","authors_text":"Gary T. Horowitz, Jorge E. Santos, Nabil Iqbal, Oscar J.C. Dias","submitted_at":"2013-11-14T21:07:15Z","abstract_excerpt":"We present a detailed study of a single vortex in a holographic symmetry breaking phase. At low energies the system flows to an nontrivial conformal fixed point. Novel vortex physics arises from the interaction of these gapless degrees of freedom with the vortex: at low energies the vortex may be understood as a conformal defect in this low energy theory. Defect conformal symmetry allows the construction of a simple infrared geometry describing a new kind of extremal horizon: a Poincare horizon with a small bubble of magnetic Reissner-Nordstrom horizon inside it that carries a single unit of m"},"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":"1311.3673","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-11-14T21:07:15Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"682c1c166138da4423626352520f2a3336e81a189b5f0f0ffa40ee31dfd4c8a1","abstract_canon_sha256":"41e8beb14e38e71d65197a28335de9ca82f4f6f4fb9fbd629eeccc87c3b1c0d8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:46:24.671082Z","signature_b64":"oA5tdsl02l6+ZPiz8sTpgoQlu06vmljGh5SlUuaUG8otk2oIBBRj6SfWpWEE341jjLdpkrghYABC8qqSxoo3BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"81105dd162af8e5cbe2689a61cdc3e16f0f54f2c6a9a82acddc3a6318f719cbf","last_reissued_at":"2026-05-18T01:46:24.670421Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:46:24.670421Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Vortices in holographic superfluids and superconductors as conformal defects","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"hep-th","authors_text":"Gary T. Horowitz, Jorge E. Santos, Nabil Iqbal, Oscar J.C. Dias","submitted_at":"2013-11-14T21:07:15Z","abstract_excerpt":"We present a detailed study of a single vortex in a holographic symmetry breaking phase. At low energies the system flows to an nontrivial conformal fixed point. Novel vortex physics arises from the interaction of these gapless degrees of freedom with the vortex: at low energies the vortex may be understood as a conformal defect in this low energy theory. Defect conformal symmetry allows the construction of a simple infrared geometry describing a new kind of extremal horizon: a Poincare horizon with a small bubble of magnetic Reissner-Nordstrom horizon inside it that carries a single unit of m"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.3673","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":""},"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":"1311.3673","created_at":"2026-05-18T01:46:24.670536+00:00"},{"alias_kind":"arxiv_version","alias_value":"1311.3673v2","created_at":"2026-05-18T01:46:24.670536+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.3673","created_at":"2026-05-18T01:46:24.670536+00:00"},{"alias_kind":"pith_short_12","alias_value":"QEIF3ULCV6HF","created_at":"2026-05-18T12:27:57.521954+00:00"},{"alias_kind":"pith_short_16","alias_value":"QEIF3ULCV6HFZPRG","created_at":"2026-05-18T12:27:57.521954+00:00"},{"alias_kind":"pith_short_8","alias_value":"QEIF3ULC","created_at":"2026-05-18T12:27:57.521954+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.18628","citing_title":"Field Theory Models for a Holographic Superconductor in Two Dimensions","ref_index":25,"is_internal_anchor":true},{"citing_arxiv_id":"2604.02133","citing_title":"Effective Field Theory for Superconducting Phase Transitions","ref_index":73,"is_internal_anchor":false},{"citing_arxiv_id":"2605.04145","citing_title":"When AdS$_3$ Grows Hair: Boson Stars, Black Holes, and Double-Trace Deformations","ref_index":33,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QEIF3ULCV6HFZPRGRGTBZXB6C3","json":"https://pith.science/pith/QEIF3ULCV6HFZPRGRGTBZXB6C3.json","graph_json":"https://pith.science/api/pith-number/QEIF3ULCV6HFZPRGRGTBZXB6C3/graph.json","events_json":"https://pith.science/api/pith-number/QEIF3ULCV6HFZPRGRGTBZXB6C3/events.json","paper":"https://pith.science/paper/QEIF3ULC"},"agent_actions":{"view_html":"https://pith.science/pith/QEIF3ULCV6HFZPRGRGTBZXB6C3","download_json":"https://pith.science/pith/QEIF3ULCV6HFZPRGRGTBZXB6C3.json","view_paper":"https://pith.science/paper/QEIF3ULC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1311.3673&json=true","fetch_graph":"https://pith.science/api/pith-number/QEIF3ULCV6HFZPRGRGTBZXB6C3/graph.json","fetch_events":"https://pith.science/api/pith-number/QEIF3ULCV6HFZPRGRGTBZXB6C3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QEIF3ULCV6HFZPRGRGTBZXB6C3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QEIF3ULCV6HFZPRGRGTBZXB6C3/action/storage_attestation","attest_author":"https://pith.science/pith/QEIF3ULCV6HFZPRGRGTBZXB6C3/action/author_attestation","sign_citation":"https://pith.science/pith/QEIF3ULCV6HFZPRGRGTBZXB6C3/action/citation_signature","submit_replication":"https://pith.science/pith/QEIF3ULCV6HFZPRGRGTBZXB6C3/action/replication_record"}},"created_at":"2026-05-18T01:46:24.670536+00:00","updated_at":"2026-05-18T01:46:24.670536+00:00"}