{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:MVQ7B6IC5G4IUTKNRS3JRK4OJS","short_pith_number":"pith:MVQ7B6IC","schema_version":"1.0","canonical_sha256":"6561f0f902e9b88a4d4d8cb698ab8e4ca326c0e0dab795a8e1557491a3c241f0","source":{"kind":"arxiv","id":"2206.14487","version":1},"attestation_state":"computed","paper":{"title":"Infrared physics of the 3D SU(2) adjoint Higgs model at the crossover transition","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"David J. Weir, Kari Rummukainen, Lauri Niemi, Riikka Sepp\\\"a","submitted_at":"2022-06-29T09:21:26Z","abstract_excerpt":"We study the crossover phase transition of the SU(2) Georgi-Glashow model in three dimensions. In this model, a confining condensate of topological 't Hooft-Polyakov monopoles exists in the Higgs regime. We use lattice Monte Carlo simulations to study the monopole gas across a crossover transition, and demonstrate that gradient flow can be used to renormalize the otherwise divergent monopole number density. The condensation of the monopoles means that the theory admits also a massive photon-like excitation. We show that the renormalized monopole number density is approximately proportional to "},"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":"2206.14487","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2022-06-29T09:21:26Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"cad3935b197bbc1eb8316de94f75f6bac81c4e5ffca470a9a6340519003a7410","abstract_canon_sha256":"93c8e74460b1cae52d276ecf5ef4e897f9b0c6968a4dc9307549e223e52714a0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:52:56.757300Z","signature_b64":"Dnrh1gEITDa1TiqL2sqi1Hc8qxm4/XUxsQfAaWHvqw4flENWuX2XfeMx779Xc5rV0yo4v3OTWlrOJMRkfUSjBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6561f0f902e9b88a4d4d8cb698ab8e4ca326c0e0dab795a8e1557491a3c241f0","last_reissued_at":"2026-07-05T05:52:56.756743Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:52:56.756743Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Infrared physics of the 3D SU(2) adjoint Higgs model at the crossover transition","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"David J. Weir, Kari Rummukainen, Lauri Niemi, Riikka Sepp\\\"a","submitted_at":"2022-06-29T09:21:26Z","abstract_excerpt":"We study the crossover phase transition of the SU(2) Georgi-Glashow model in three dimensions. In this model, a confining condensate of topological 't Hooft-Polyakov monopoles exists in the Higgs regime. We use lattice Monte Carlo simulations to study the monopole gas across a crossover transition, and demonstrate that gradient flow can be used to renormalize the otherwise divergent monopole number density. The condensation of the monopoles means that the theory admits also a massive photon-like excitation. We show that the renormalized monopole number density is approximately proportional to "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2206.14487","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/2206.14487/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":"2206.14487","created_at":"2026-07-05T05:52:56.756803+00:00"},{"alias_kind":"arxiv_version","alias_value":"2206.14487v1","created_at":"2026-07-05T05:52:56.756803+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2206.14487","created_at":"2026-07-05T05:52:56.756803+00:00"},{"alias_kind":"pith_short_12","alias_value":"MVQ7B6IC5G4I","created_at":"2026-07-05T05:52:56.756803+00:00"},{"alias_kind":"pith_short_16","alias_value":"MVQ7B6IC5G4IUTKN","created_at":"2026-07-05T05:52:56.756803+00:00"},{"alias_kind":"pith_short_8","alias_value":"MVQ7B6IC","created_at":"2026-07-05T05:52:56.756803+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.21380","citing_title":"Theoretical consistency and phenomenology of supercooled cosmological phase transitions","ref_index":104,"is_internal_anchor":false},{"citing_arxiv_id":"2604.21972","citing_title":"Matchotter: An Automated Tool for Dimensional Reduction at Finite Temperature","ref_index":34,"is_internal_anchor":false},{"citing_arxiv_id":"2605.06775","citing_title":"SIRENA -- Sum-Integral REductioN Algorithm","ref_index":23,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MVQ7B6IC5G4IUTKNRS3JRK4OJS","json":"https://pith.science/pith/MVQ7B6IC5G4IUTKNRS3JRK4OJS.json","graph_json":"https://pith.science/api/pith-number/MVQ7B6IC5G4IUTKNRS3JRK4OJS/graph.json","events_json":"https://pith.science/api/pith-number/MVQ7B6IC5G4IUTKNRS3JRK4OJS/events.json","paper":"https://pith.science/paper/MVQ7B6IC"},"agent_actions":{"view_html":"https://pith.science/pith/MVQ7B6IC5G4IUTKNRS3JRK4OJS","download_json":"https://pith.science/pith/MVQ7B6IC5G4IUTKNRS3JRK4OJS.json","view_paper":"https://pith.science/paper/MVQ7B6IC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2206.14487&json=true","fetch_graph":"https://pith.science/api/pith-number/MVQ7B6IC5G4IUTKNRS3JRK4OJS/graph.json","fetch_events":"https://pith.science/api/pith-number/MVQ7B6IC5G4IUTKNRS3JRK4OJS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MVQ7B6IC5G4IUTKNRS3JRK4OJS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MVQ7B6IC5G4IUTKNRS3JRK4OJS/action/storage_attestation","attest_author":"https://pith.science/pith/MVQ7B6IC5G4IUTKNRS3JRK4OJS/action/author_attestation","sign_citation":"https://pith.science/pith/MVQ7B6IC5G4IUTKNRS3JRK4OJS/action/citation_signature","submit_replication":"https://pith.science/pith/MVQ7B6IC5G4IUTKNRS3JRK4OJS/action/replication_record"}},"created_at":"2026-07-05T05:52:56.756803+00:00","updated_at":"2026-07-05T05:52:56.756803+00:00"}