{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2009:PKUTMWJU5L4LRXB24N6UZZC2IG","short_pith_number":"pith:PKUTMWJU","canonical_record":{"source":{"id":"0912.4475","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2009-12-22T18:08:02Z","cross_cats_sorted":[],"title_canon_sha256":"f11e90839bd9f58b328573b68afafbdd84add8f6580eef3e9b22d71ee957b2e8","abstract_canon_sha256":"8d34549b605e7fcd47ac49cef9e2c6e9f09cf7d19b2ab2f78f6cadc84c1582f3"},"schema_version":"1.0"},"canonical_sha256":"7aa9365934eaf8b8dc3ae37d4ce45a418deac5f2867349745ba155b6ba64f24c","source":{"kind":"arxiv","id":"0912.4475","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"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2009:PKUTMWJU5L4LRXB24N6UZZC2IG","target":"record","payload":{"canonical_record":{"source":{"id":"0912.4475","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2009-12-22T18:08:02Z","cross_cats_sorted":[],"title_canon_sha256":"f11e90839bd9f58b328573b68afafbdd84add8f6580eef3e9b22d71ee957b2e8","abstract_canon_sha256":"8d34549b605e7fcd47ac49cef9e2c6e9f09cf7d19b2ab2f78f6cadc84c1582f3"},"schema_version":"1.0"},"canonical_sha256":"7aa9365934eaf8b8dc3ae37d4ce45a418deac5f2867349745ba155b6ba64f24c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:25:07.876767Z","signature_b64":"iZH/vDs/ZO+didTsBF4oKS187hu3TUEEw7nG519WEWGBZlvpD8BFheahxmkRBc5M2DvJxlB5GBBDZ5Bngo+bCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7aa9365934eaf8b8dc3ae37d4ce45a418deac5f2867349745ba155b6ba64f24c","last_reissued_at":"2026-07-04T17:25:07.876335Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:25:07.876335Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0912.4475","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T17:25:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"05BA1pmW5YSIg2NtoY5EE6NCVV8he1xjf1wijYUjSJ3WwY3QAX9ZbI+vkmviIV2NGVlC6a+E+EXzWI56M93jDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T18:35:52.907445Z"},"content_sha256":"7654508dc5d7cb39395449b9d8cacf222913044dbbd6f07fd998c87daf07cc25","schema_version":"1.0","event_id":"sha256:7654508dc5d7cb39395449b9d8cacf222913044dbbd6f07fd998c87daf07cc25"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2009:PKUTMWJU5L4LRXB24N6UZZC2IG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"SU(2) lattice gluon propagator: continuum limit, finite-volume effects and infrared mass scale m_IR","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"M. M\\\"uller-Preussker, V. G. Bornyakov, V. K. Mitrjushkin","submitted_at":"2009-12-22T18:08:02Z","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"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0912.4475","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/0912.4475/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T17:25:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nF5Ps5bS1AS+lSdf50dMX7SKhf5I2Eh65h5si8k4WV6DseeHR/ntHJ/1E1DTzP+smKiIkwlJ3TKH43rxEOcYDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T18:35:52.908376Z"},"content_sha256":"06a04465e6b34e89c099ff790028d1a6afabfca61ff9ea3b69bf5a2577682011","schema_version":"1.0","event_id":"sha256:06a04465e6b34e89c099ff790028d1a6afabfca61ff9ea3b69bf5a2577682011"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PKUTMWJU5L4LRXB24N6UZZC2IG/bundle.json","state_url":"https://pith.science/pith/PKUTMWJU5L4LRXB24N6UZZC2IG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PKUTMWJU5L4LRXB24N6UZZC2IG/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-08-05T18:35:52Z","links":{"resolver":"https://pith.science/pith/PKUTMWJU5L4LRXB24N6UZZC2IG","bundle":"https://pith.science/pith/PKUTMWJU5L4LRXB24N6UZZC2IG/bundle.json","state":"https://pith.science/pith/PKUTMWJU5L4LRXB24N6UZZC2IG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PKUTMWJU5L4LRXB24N6UZZC2IG/bundle.json"},"state":{"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"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sJpNFhSnALw42NcmrURicWE6Nv9Qz0eop9hPmxXgRF7FFsKfXKjK/XA2hOqYupAoUynJbS+DAarU/LnhS2sYDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-05T18:35:52.915954Z","bundle_sha256":"8f87ec458d67fe8b24cdefeece713a439601aee9a4a390895e1a4657898d8337"}}