{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:BAYU5DTLECVERLQCF7MLTTRRLW","short_pith_number":"pith:BAYU5DTL","canonical_record":{"source":{"id":"1111.3946","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-11-16T21:00:00Z","cross_cats_sorted":["hep-lat","hep-th"],"title_canon_sha256":"07b6fda7d8b12934fff1a433691e65dac475249e2100b0a3067e911f9e9edd0d","abstract_canon_sha256":"88c680c55f01e45ed435d3ba1a5d146ea3e9a0c4ccb056336f35e9ed7b129ca6"},"schema_version":"1.0"},"canonical_sha256":"08314e8e6b20aa48ae022fd8b9ce315da04d127938eaa82fd3aebcc8b8bd94c4","source":{"kind":"arxiv","id":"1111.3946","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1111.3946","created_at":"2026-05-18T03:53:42Z"},{"alias_kind":"arxiv_version","alias_value":"1111.3946v2","created_at":"2026-05-18T03:53:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1111.3946","created_at":"2026-05-18T03:53:42Z"},{"alias_kind":"pith_short_12","alias_value":"BAYU5DTLECVE","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_16","alias_value":"BAYU5DTLECVERLQC","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_8","alias_value":"BAYU5DTL","created_at":"2026-05-18T12:26:24Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:BAYU5DTLECVERLQCF7MLTTRRLW","target":"record","payload":{"canonical_record":{"source":{"id":"1111.3946","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-11-16T21:00:00Z","cross_cats_sorted":["hep-lat","hep-th"],"title_canon_sha256":"07b6fda7d8b12934fff1a433691e65dac475249e2100b0a3067e911f9e9edd0d","abstract_canon_sha256":"88c680c55f01e45ed435d3ba1a5d146ea3e9a0c4ccb056336f35e9ed7b129ca6"},"schema_version":"1.0"},"canonical_sha256":"08314e8e6b20aa48ae022fd8b9ce315da04d127938eaa82fd3aebcc8b8bd94c4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:53:42.382921Z","signature_b64":"DGOyi2eltMbxYyllhuEPmyX+K7d8docWtKvlSBf37MdnQg887Xn4bhZpW7neVCrhkiEPZFbwDyyLM9wS5FmqBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"08314e8e6b20aa48ae022fd8b9ce315da04d127938eaa82fd3aebcc8b8bd94c4","last_reissued_at":"2026-05-18T03:53:42.382361Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:53:42.382361Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1111.3946","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":"2026-05-18T03:53:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nWRk2fxvFq6SVUWyoLaQDRUpk+F4+eLMEaJ7Jh95r3WYlr/HGp5hkJBObcCMmoSjz0ovO9KXNcfuXDwTZYltBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-19T17:00:34.312802Z"},"content_sha256":"61b8ca3abd4483399b76757dc912da54ce0fd5ee7feffb8cf7e599eee7617ac8","schema_version":"1.0","event_id":"sha256:61b8ca3abd4483399b76757dc912da54ce0fd5ee7feffb8cf7e599eee7617ac8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:BAYU5DTLECVERLQCF7MLTTRRLW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Compelling evidence of renormalons in QCD from high order perturbative expansions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-th"],"primary_cat":"hep-ph","authors_text":"Antonio Pineda, Clemens Bauer, Gunnar S. Bali","submitted_at":"2011-11-16T21:00:00Z","abstract_excerpt":"We compute the static self-energy of SU(3) gauge theory in four spacetime dimensions to order \\alpha^{20} in the strong coupling constant. We employ lattice regularization to enable a numerical simulation within the framework of stochastic perturbation theory. We find perfect agreement with the factorial growth of high order coefficients predicted by the conjectured renormalon picture based on the operator product expansion."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1111.3946","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":""},"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":"2026-05-18T03:53:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PoJTL8zHYx8JoX44qeKYBDSvkw1xKHg9RJGk/UJfJGp2ClgPKVkLSuNt6ZTIFbHF7wuYaP6zGaewlXPN0Jz2DA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-19T17:00:34.313153Z"},"content_sha256":"ae61164929eb43022b5a4fb0b0651e530e3566a5cf349c163f640505b24eb2ac","schema_version":"1.0","event_id":"sha256:ae61164929eb43022b5a4fb0b0651e530e3566a5cf349c163f640505b24eb2ac"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/BAYU5DTLECVERLQCF7MLTTRRLW/bundle.json","state_url":"https://pith.science/pith/BAYU5DTLECVERLQCF7MLTTRRLW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/BAYU5DTLECVERLQCF7MLTTRRLW/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":"2026-05-19T17:00:34Z","links":{"resolver":"https://pith.science/pith/BAYU5DTLECVERLQCF7MLTTRRLW","bundle":"https://pith.science/pith/BAYU5DTLECVERLQCF7MLTTRRLW/bundle.json","state":"https://pith.science/pith/BAYU5DTLECVERLQCF7MLTTRRLW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/BAYU5DTLECVERLQCF7MLTTRRLW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:BAYU5DTLECVERLQCF7MLTTRRLW","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":"88c680c55f01e45ed435d3ba1a5d146ea3e9a0c4ccb056336f35e9ed7b129ca6","cross_cats_sorted":["hep-lat","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-11-16T21:00:00Z","title_canon_sha256":"07b6fda7d8b12934fff1a433691e65dac475249e2100b0a3067e911f9e9edd0d"},"schema_version":"1.0","source":{"id":"1111.3946","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1111.3946","created_at":"2026-05-18T03:53:42Z"},{"alias_kind":"arxiv_version","alias_value":"1111.3946v2","created_at":"2026-05-18T03:53:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1111.3946","created_at":"2026-05-18T03:53:42Z"},{"alias_kind":"pith_short_12","alias_value":"BAYU5DTLECVE","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_16","alias_value":"BAYU5DTLECVERLQC","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_8","alias_value":"BAYU5DTL","created_at":"2026-05-18T12:26:24Z"}],"graph_snapshots":[{"event_id":"sha256:ae61164929eb43022b5a4fb0b0651e530e3566a5cf349c163f640505b24eb2ac","target":"graph","created_at":"2026-05-18T03:53:42Z","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"},"paper":{"abstract_excerpt":"We compute the static self-energy of SU(3) gauge theory in four spacetime dimensions to order \\alpha^{20} in the strong coupling constant. We employ lattice regularization to enable a numerical simulation within the framework of stochastic perturbation theory. We find perfect agreement with the factorial growth of high order coefficients predicted by the conjectured renormalon picture based on the operator product expansion.","authors_text":"Antonio Pineda, Clemens Bauer, Gunnar S. Bali","cross_cats":["hep-lat","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-11-16T21:00:00Z","title":"Compelling evidence of renormalons in QCD from high order perturbative expansions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1111.3946","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":"sha256:61b8ca3abd4483399b76757dc912da54ce0fd5ee7feffb8cf7e599eee7617ac8","target":"record","created_at":"2026-05-18T03:53:42Z","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":"88c680c55f01e45ed435d3ba1a5d146ea3e9a0c4ccb056336f35e9ed7b129ca6","cross_cats_sorted":["hep-lat","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-11-16T21:00:00Z","title_canon_sha256":"07b6fda7d8b12934fff1a433691e65dac475249e2100b0a3067e911f9e9edd0d"},"schema_version":"1.0","source":{"id":"1111.3946","kind":"arxiv","version":2}},"canonical_sha256":"08314e8e6b20aa48ae022fd8b9ce315da04d127938eaa82fd3aebcc8b8bd94c4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"08314e8e6b20aa48ae022fd8b9ce315da04d127938eaa82fd3aebcc8b8bd94c4","first_computed_at":"2026-05-18T03:53:42.382361Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:53:42.382361Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"DGOyi2eltMbxYyllhuEPmyX+K7d8docWtKvlSBf37MdnQg887Xn4bhZpW7neVCrhkiEPZFbwDyyLM9wS5FmqBw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:53:42.382921Z","signed_message":"canonical_sha256_bytes"},"source_id":"1111.3946","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:61b8ca3abd4483399b76757dc912da54ce0fd5ee7feffb8cf7e599eee7617ac8","sha256:ae61164929eb43022b5a4fb0b0651e530e3566a5cf349c163f640505b24eb2ac"],"state_sha256":"af1ce2994fe2f6712c451e98c325e9ceccebd895efa194d2598a322f496fdf2f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yTPJRwuZ1tbJvtdHVr/2ehXUhkn8JlOZSabC/sMbo2C57CxZvLs4XubkaUh62yf1eehfmJ5oSeGtVqaQ3mlvBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-19T17:00:34.315117Z","bundle_sha256":"bd9a5b2e98541e17e25c4ce968c62d715b2801c893c7684ea911cdfb4c5c0b93"}}