{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:WG22LOZL7OYCHEHJ2GICLNQHCP","short_pith_number":"pith:WG22LOZL","schema_version":"1.0","canonical_sha256":"b1b5a5bb2bfbb02390e9d19025b60713e88776cf1f788a0a6f2ee7f08bc7bcc6","source":{"kind":"arxiv","id":"2411.07969","version":2},"attestation_state":"computed","paper":{"title":"The hadronic vacuum polarization contribution to the muon $g-2$ at long distances","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Andreas Risch, Dalibor Djukanovic, Georg von Hippel, Hartmut Wittig, Harvey B. Meyer, Julian Parrino, Konstantin Ottnad, Nolan Miller, Simon Kuberski","submitted_at":"2024-11-12T17:48:53Z","abstract_excerpt":"We present our lattice QCD result for the long-distance part of the hadronic vacuum polarization contribution, $(a_\\mu^{\\rm hvp})^{\\rm LD}$, to the muon $g-2$ in the time-momentum representation. This is the numerically dominant, and at the same time the most challenging part regarding statistical precision. Our calculation is based on ensembles with dynamical up, down and strange quarks, employing the O($a$)-improved Wilson fermion action with lattice spacings ranging from $0.035-0.099$ fm. In order to reduce statistical noise in the long-distance part of the correlator to the per-mille level"},"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":"2411.07969","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-lat","submitted_at":"2024-11-12T17:48:53Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"b56398887d2c2a6f950faefe2b686f57e6422d10725018e085ddfbc99178639b","abstract_canon_sha256":"9e0b934b4c2919540a87162233fb07b5dccbcfb0bbbd374d77c0275e66d57678"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:21:05.569039Z","signature_b64":"v73LxZKXjMCHPw0evSxd2LfVLWcLQa1K+3Uk7gsO46ETF4DvmqoDZ+lSszj+Zd4R1Y5Jxvm2DUqv69eRfh8xBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b1b5a5bb2bfbb02390e9d19025b60713e88776cf1f788a0a6f2ee7f08bc7bcc6","last_reissued_at":"2026-07-05T10:21:05.568481Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:21:05.568481Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The hadronic vacuum polarization contribution to the muon $g-2$ at long distances","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Andreas Risch, Dalibor Djukanovic, Georg von Hippel, Hartmut Wittig, Harvey B. Meyer, Julian Parrino, Konstantin Ottnad, Nolan Miller, Simon Kuberski","submitted_at":"2024-11-12T17:48:53Z","abstract_excerpt":"We present our lattice QCD result for the long-distance part of the hadronic vacuum polarization contribution, $(a_\\mu^{\\rm hvp})^{\\rm LD}$, to the muon $g-2$ in the time-momentum representation. This is the numerically dominant, and at the same time the most challenging part regarding statistical precision. Our calculation is based on ensembles with dynamical up, down and strange quarks, employing the O($a$)-improved Wilson fermion action with lattice spacings ranging from $0.035-0.099$ fm. In order to reduce statistical noise in the long-distance part of the correlator to the per-mille level"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.07969","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/2411.07969/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":"2411.07969","created_at":"2026-07-05T10:21:05.568553+00:00"},{"alias_kind":"arxiv_version","alias_value":"2411.07969v2","created_at":"2026-07-05T10:21:05.568553+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.07969","created_at":"2026-07-05T10:21:05.568553+00:00"},{"alias_kind":"pith_short_12","alias_value":"WG22LOZL7OYC","created_at":"2026-07-05T10:21:05.568553+00:00"},{"alias_kind":"pith_short_16","alias_value":"WG22LOZL7OYCHEHJ","created_at":"2026-07-05T10:21:05.568553+00:00"},{"alias_kind":"pith_short_8","alias_value":"WG22LOZL","created_at":"2026-07-05T10:21:05.568553+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":17,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.27072","citing_title":"Performance of Low Mode Averaging on Twisted-Mass Fermion Ensembles at the physical pion mass point","ref_index":12,"is_internal_anchor":false},{"citing_arxiv_id":"2606.11181","citing_title":"Combined Analysis of Lattice QCD and Experimental Data on the Pion Transition Form Factor","ref_index":28,"is_internal_anchor":false},{"citing_arxiv_id":"2607.00564","citing_title":"Isospin-breaking effects in inclusive hadronic $\\tau$ data for the muon $(g-2)$ from first principles","ref_index":64,"is_internal_anchor":false},{"citing_arxiv_id":"2605.29902","citing_title":"Electromagnetic pion mass splitting using a Pauli-Villars-regulated photon propagator","ref_index":28,"is_internal_anchor":false},{"citing_arxiv_id":"2605.22444","citing_title":"Normalizing flows for all-orders QED corrections in lattice field theory","ref_index":22,"is_internal_anchor":false},{"citing_arxiv_id":"2506.16326","citing_title":"Bounding statistical errors in lattice field theory simulations","ref_index":35,"is_internal_anchor":false},{"citing_arxiv_id":"2509.08115","citing_title":"Field-theoretic versus data-driven evaluations of electromagnetic corrections to hadronic vacuum polarization in $(g-2)_\\mu$","ref_index":11,"is_internal_anchor":false},{"citing_arxiv_id":"2510.13966","citing_title":"Light new physics and the $\\tau$ lepton dipole moments: prospects at Belle II","ref_index":44,"is_internal_anchor":false},{"citing_arxiv_id":"2511.03786","citing_title":"Light new physics and the $\\tau$ lepton dipole moments","ref_index":50,"is_internal_anchor":false},{"citing_arxiv_id":"2512.10709","citing_title":"Disperon QED","ref_index":3,"is_internal_anchor":false},{"citing_arxiv_id":"2512.18382","citing_title":"Lepton anomalous magnetic moments: Theory","ref_index":156,"is_internal_anchor":false},{"citing_arxiv_id":"2603.06806","citing_title":"Higher-order hadronic vacuum polarization contribution to the muon $g-2$ from lattice QCD","ref_index":12,"is_internal_anchor":false},{"citing_arxiv_id":"2505.21476","citing_title":"The anomalous magnetic moment of the muon in the Standard Model: an update","ref_index":27,"is_internal_anchor":false},{"citing_arxiv_id":"2605.12205","citing_title":"Comparison of the hadronic vacuum polarization between hadronic $\\tau$-decay data and lattice QCD","ref_index":76,"is_internal_anchor":false},{"citing_arxiv_id":"2604.25004","citing_title":"Muon $g$$-$2: correlation-induced uncertainties in precision data combinations","ref_index":48,"is_internal_anchor":false},{"citing_arxiv_id":"2605.00643","citing_title":"Variance reduction strategies for lattice QCD","ref_index":51,"is_internal_anchor":false},{"citing_arxiv_id":"2604.08351","citing_title":"Lattice determination of the higher-order hadronic vacuum polarization contribution to the muon $g-2$","ref_index":8,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WG22LOZL7OYCHEHJ2GICLNQHCP","json":"https://pith.science/pith/WG22LOZL7OYCHEHJ2GICLNQHCP.json","graph_json":"https://pith.science/api/pith-number/WG22LOZL7OYCHEHJ2GICLNQHCP/graph.json","events_json":"https://pith.science/api/pith-number/WG22LOZL7OYCHEHJ2GICLNQHCP/events.json","paper":"https://pith.science/paper/WG22LOZL"},"agent_actions":{"view_html":"https://pith.science/pith/WG22LOZL7OYCHEHJ2GICLNQHCP","download_json":"https://pith.science/pith/WG22LOZL7OYCHEHJ2GICLNQHCP.json","view_paper":"https://pith.science/paper/WG22LOZL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2411.07969&json=true","fetch_graph":"https://pith.science/api/pith-number/WG22LOZL7OYCHEHJ2GICLNQHCP/graph.json","fetch_events":"https://pith.science/api/pith-number/WG22LOZL7OYCHEHJ2GICLNQHCP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WG22LOZL7OYCHEHJ2GICLNQHCP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WG22LOZL7OYCHEHJ2GICLNQHCP/action/storage_attestation","attest_author":"https://pith.science/pith/WG22LOZL7OYCHEHJ2GICLNQHCP/action/author_attestation","sign_citation":"https://pith.science/pith/WG22LOZL7OYCHEHJ2GICLNQHCP/action/citation_signature","submit_replication":"https://pith.science/pith/WG22LOZL7OYCHEHJ2GICLNQHCP/action/replication_record"}},"created_at":"2026-07-05T10:21:05.568553+00:00","updated_at":"2026-07-05T10:21:05.568553+00:00"}