{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2009:PKUTMWJU5L4LRXB24N6UZZC2IG","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"8d34549b605e7fcd47ac49cef9e2c6e9f09cf7d19b2ab2f78f6cadc84c1582f3","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2009-12-22T18:08:02Z","title_canon_sha256":"f11e90839bd9f58b328573b68afafbdd84add8f6580eef3e9b22d71ee957b2e8"},"schema_version":"1.0","source":{"id":"0912.4475","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0912.4475","created_at":"2026-07-04T17:25:07Z"},{"alias_kind":"arxiv_version","alias_value":"0912.4475v2","created_at":"2026-07-04T17:25:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0912.4475","created_at":"2026-07-04T17:25:07Z"},{"alias_kind":"pith_short_12","alias_value":"PKUTMWJU5L4L","created_at":"2026-07-04T17:25:07Z"},{"alias_kind":"pith_short_16","alias_value":"PKUTMWJU5L4LRXB2","created_at":"2026-07-04T17:25:07Z"},{"alias_kind":"pith_short_8","alias_value":"PKUTMWJU","created_at":"2026-07-04T17:25:07Z"}],"graph_snapshots":[{"event_id":"sha256:06a04465e6b34e89c099ff790028d1a6afabfca61ff9ea3b69bf5a2577682011","target":"graph","created_at":"2026-07-04T17:25:07Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/0912.4475/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study the scaling behavior and finite (physical) volume effects as well as the Gribov copy dependence of the SU(2) Landau gauge gluon propagator on the lattice. Our physical lattice sizes range from $(3.0 \\mathrm{fm})^4$ to $(7.3 \\mathrm{fm})^4$. Considering lattices with decreasing lattice spacing but fixed physical volume we confirm (non-perturbative) multiplicative renormalizability and the approach to the {\\it continuum limit} for the renormalized gluon propagator $D_{ren}(p)$ at momenta $|p| \\ageq 0.6$ GeV >. The finite-volume effects and Gribov copy influence turn out small in this re","authors_text":"M. M\\\"uller-Preussker, V. G. Bornyakov, V. K. Mitrjushkin","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2009-12-22T18:08:02Z","title":"SU(2) lattice gluon propagator: continuum limit, finite-volume effects and infrared mass scale m_IR"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0912.4475","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:7654508dc5d7cb39395449b9d8cacf222913044dbbd6f07fd998c87daf07cc25","target":"record","created_at":"2026-07-04T17:25:07Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"8d34549b605e7fcd47ac49cef9e2c6e9f09cf7d19b2ab2f78f6cadc84c1582f3","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2009-12-22T18:08:02Z","title_canon_sha256":"f11e90839bd9f58b328573b68afafbdd84add8f6580eef3e9b22d71ee957b2e8"},"schema_version":"1.0","source":{"id":"0912.4475","kind":"arxiv","version":2}},"canonical_sha256":"7aa9365934eaf8b8dc3ae37d4ce45a418deac5f2867349745ba155b6ba64f24c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7aa9365934eaf8b8dc3ae37d4ce45a418deac5f2867349745ba155b6ba64f24c","first_computed_at":"2026-07-04T17:25:07.876335Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T17:25:07.876335Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"iZH/vDs/ZO+didTsBF4oKS187hu3TUEEw7nG519WEWGBZlvpD8BFheahxmkRBc5M2DvJxlB5GBBDZ5Bngo+bCA==","signature_status":"signed_v1","signed_at":"2026-07-04T17:25:07.876767Z","signed_message":"canonical_sha256_bytes"},"source_id":"0912.4475","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7654508dc5d7cb39395449b9d8cacf222913044dbbd6f07fd998c87daf07cc25","sha256:06a04465e6b34e89c099ff790028d1a6afabfca61ff9ea3b69bf5a2577682011"],"state_sha256":"9c920c9fe27cfe6d0d67a3bb2d13a7b31c0dde6821949c75ec1d91dfbaa0a215"}