{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2009:IUTF2ZZMZYPDQWZBI67IEKRBSV","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":"8f49b959001bdebf192a0d8fb70b6d80dcf2a86eaabe17adc230c7d69bee9cc4","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2009-04-26T14:34:58Z","title_canon_sha256":"10488cadb81ded6a9a6b8ecb9f1801752f428442107cc83ff5f7c0a7cf99de98"},"schema_version":"1.0","source":{"id":"0904.4033","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0904.4033","created_at":"2026-07-04T17:25:00Z"},{"alias_kind":"arxiv_version","alias_value":"0904.4033v2","created_at":"2026-07-04T17:25:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0904.4033","created_at":"2026-07-04T17:25:00Z"},{"alias_kind":"pith_short_12","alias_value":"IUTF2ZZMZYPD","created_at":"2026-07-04T17:25:00Z"},{"alias_kind":"pith_short_16","alias_value":"IUTF2ZZMZYPDQWZB","created_at":"2026-07-04T17:25:00Z"},{"alias_kind":"pith_short_8","alias_value":"IUTF2ZZM","created_at":"2026-07-04T17:25:00Z"}],"graph_snapshots":[{"event_id":"sha256:1e4e77a1e22d019d59cdbc1b2c2b2ec20cf6c4503903f9eeeb5bd51ff358205f","target":"graph","created_at":"2026-07-04T17:25:00Z","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/0904.4033/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study Landau-gauge gluon and ghost propagators in Yang-Mills theories at lattice parameter beta = 0, considering relatively large lattice volumes for the case of the SU(2) gauge group in three and four space-time dimensions. We compare the lattice data to the so-called massive and conformal-scaling solutions, examining the requirements for a good description of the propagators over various ranges of momenta and discussing possible systematic errors. Our analysis strongly supports the massive solution, i.e. a finite gluon propagator and an essentially free ghost propagator in the infrared li","authors_text":"Attilio Cucchieri, Tereza Mendes","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2009-04-26T14:34:58Z","title":"Landau-gauge propagators in Yang-Mills theories at beta = 0: massive solution versus conformal scaling"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0904.4033","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:ed6cf36eff731696164753037d4391da2f9bcd118081958be1087bcbe9f2c967","target":"record","created_at":"2026-07-04T17:25:00Z","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":"8f49b959001bdebf192a0d8fb70b6d80dcf2a86eaabe17adc230c7d69bee9cc4","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2009-04-26T14:34:58Z","title_canon_sha256":"10488cadb81ded6a9a6b8ecb9f1801752f428442107cc83ff5f7c0a7cf99de98"},"schema_version":"1.0","source":{"id":"0904.4033","kind":"arxiv","version":2}},"canonical_sha256":"45265d672cce1e385b2147be822a21956200e69cf43293b35be7460f744cca2d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"45265d672cce1e385b2147be822a21956200e69cf43293b35be7460f744cca2d","first_computed_at":"2026-07-04T17:25:00.821821Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T17:25:00.821821Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"xUeTv+oe2ANd5akO9k3ckJy9U2k5SZHZA6p+kpdr/aCJWmAGJTADidvkrM5YUshMePBv050Nims4ZyZ9t2osBw==","signature_status":"signed_v1","signed_at":"2026-07-04T17:25:00.822206Z","signed_message":"canonical_sha256_bytes"},"source_id":"0904.4033","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ed6cf36eff731696164753037d4391da2f9bcd118081958be1087bcbe9f2c967","sha256:1e4e77a1e22d019d59cdbc1b2c2b2ec20cf6c4503903f9eeeb5bd51ff358205f"],"state_sha256":"fb2031d522656fa00cdfcb9c6c417ad1c3e63e4577c162968e913e04c45d62a6"}