{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:RVRYWXCR6UD6AZAU7BAD7UYDWB","short_pith_number":"pith:RVRYWXCR","schema_version":"1.0","canonical_sha256":"8d638b5c51f507e06414f8403fd303b04d2163e977925536a61c637de5e5573a","source":{"kind":"arxiv","id":"2310.00045","version":1},"attestation_state":"computed","paper":{"title":"Phases of Wilson Lines: Conformality and Screening","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"hep-th","authors_text":"Avia Raviv-Moshe, Gabriel Cuomo, M\\'ark Mezei, Ofer Aharony, Zohar Komargodski","submitted_at":"2023-09-29T18:00:02Z","abstract_excerpt":"We study the rich dynamics resulting from introducing static charged particles (Wilson lines) in 2+1 and 3+1 dimensional gauge theories. Depending on the charges of the external particles, there may be multiple defect fixed points with interesting renormalization group flows connecting them, or an exponentially large screening cloud can develop (defining a new emergent length scale), screening the bare charge entirely or partially. We investigate several examples where the dynamics can be solved in various weak coupling or double scaling limits. Sometimes even the elementary Wilson lines, corr"},"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":"2310.00045","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2023-09-29T18:00:02Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"4b8bcd274f9c8e0de7a409dd8aae0aa1d2f9b821e679c0e99bff393d186137db","abstract_canon_sha256":"0ef08d3295a8d2023cafda52abb2a296786c0604890d2591a9af8c9b552a5429"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:56:00.762837Z","signature_b64":"9jdh+jHcjJP3Jh9ZzqqRz2+tFvvy7K5y3rZn+L1mZLRB2dT1Saf37UUvrEbxaxVcJpK8FEXLjioo/hqf++I2Dw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8d638b5c51f507e06414f8403fd303b04d2163e977925536a61c637de5e5573a","last_reissued_at":"2026-07-05T06:56:00.762356Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:56:00.762356Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Phases of Wilson Lines: Conformality and Screening","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"hep-th","authors_text":"Avia Raviv-Moshe, Gabriel Cuomo, M\\'ark Mezei, Ofer Aharony, Zohar Komargodski","submitted_at":"2023-09-29T18:00:02Z","abstract_excerpt":"We study the rich dynamics resulting from introducing static charged particles (Wilson lines) in 2+1 and 3+1 dimensional gauge theories. Depending on the charges of the external particles, there may be multiple defect fixed points with interesting renormalization group flows connecting them, or an exponentially large screening cloud can develop (defining a new emergent length scale), screening the bare charge entirely or partially. We investigate several examples where the dynamics can be solved in various weak coupling or double scaling limits. Sometimes even the elementary Wilson lines, corr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2310.00045","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/2310.00045/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":"2310.00045","created_at":"2026-07-05T06:56:00.762417+00:00"},{"alias_kind":"arxiv_version","alias_value":"2310.00045v1","created_at":"2026-07-05T06:56:00.762417+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2310.00045","created_at":"2026-07-05T06:56:00.762417+00:00"},{"alias_kind":"pith_short_12","alias_value":"RVRYWXCR6UD6","created_at":"2026-07-05T06:56:00.762417+00:00"},{"alias_kind":"pith_short_16","alias_value":"RVRYWXCR6UD6AZAU","created_at":"2026-07-05T06:56:00.762417+00:00"},{"alias_kind":"pith_short_8","alias_value":"RVRYWXCR","created_at":"2026-07-05T06:56:00.762417+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2607.01328","citing_title":"Quark Anti-Quark Fusion and Walking RG Flows","ref_index":29,"is_internal_anchor":false},{"citing_arxiv_id":"2606.30720","citing_title":"Complex Conformal Manifolds","ref_index":84,"is_internal_anchor":false},{"citing_arxiv_id":"2605.13947","citing_title":"Conformal defects and Goldstone bosons in Anti-de Sitter space","ref_index":41,"is_internal_anchor":false},{"citing_arxiv_id":"2605.13961","citing_title":"A Twist on Scattering from Defect Anomalies","ref_index":8,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RVRYWXCR6UD6AZAU7BAD7UYDWB","json":"https://pith.science/pith/RVRYWXCR6UD6AZAU7BAD7UYDWB.json","graph_json":"https://pith.science/api/pith-number/RVRYWXCR6UD6AZAU7BAD7UYDWB/graph.json","events_json":"https://pith.science/api/pith-number/RVRYWXCR6UD6AZAU7BAD7UYDWB/events.json","paper":"https://pith.science/paper/RVRYWXCR"},"agent_actions":{"view_html":"https://pith.science/pith/RVRYWXCR6UD6AZAU7BAD7UYDWB","download_json":"https://pith.science/pith/RVRYWXCR6UD6AZAU7BAD7UYDWB.json","view_paper":"https://pith.science/paper/RVRYWXCR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2310.00045&json=true","fetch_graph":"https://pith.science/api/pith-number/RVRYWXCR6UD6AZAU7BAD7UYDWB/graph.json","fetch_events":"https://pith.science/api/pith-number/RVRYWXCR6UD6AZAU7BAD7UYDWB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RVRYWXCR6UD6AZAU7BAD7UYDWB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RVRYWXCR6UD6AZAU7BAD7UYDWB/action/storage_attestation","attest_author":"https://pith.science/pith/RVRYWXCR6UD6AZAU7BAD7UYDWB/action/author_attestation","sign_citation":"https://pith.science/pith/RVRYWXCR6UD6AZAU7BAD7UYDWB/action/citation_signature","submit_replication":"https://pith.science/pith/RVRYWXCR6UD6AZAU7BAD7UYDWB/action/replication_record"}},"created_at":"2026-07-05T06:56:00.762417+00:00","updated_at":"2026-07-05T06:56:00.762417+00:00"}