{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:JYKYK56S7FB7XI7WM6L5AWQHMQ","short_pith_number":"pith:JYKYK56S","canonical_record":{"source":{"id":"1211.4238","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-11-18T17:27:02Z","cross_cats_sorted":[],"title_canon_sha256":"91d3e51fc8e1c5c47181962b9e17607fe822e7e0fc0fd93dde92b5a63bc595fe","abstract_canon_sha256":"ab313128e0712ca4da51bb88cbb47c583bf2bf5f5fbab1ee3b9147bf9bee30e8"},"schema_version":"1.0"},"canonical_sha256":"4e158577d2f943fba3f66797d05a0764019791529ecc5b26c230ddaac7162c1a","source":{"kind":"arxiv","id":"1211.4238","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1211.4238","created_at":"2026-05-18T03:40:27Z"},{"alias_kind":"arxiv_version","alias_value":"1211.4238v1","created_at":"2026-05-18T03:40:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.4238","created_at":"2026-05-18T03:40:27Z"},{"alias_kind":"pith_short_12","alias_value":"JYKYK56S7FB7","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_16","alias_value":"JYKYK56S7FB7XI7W","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_8","alias_value":"JYKYK56S","created_at":"2026-05-18T12:27:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:JYKYK56S7FB7XI7WM6L5AWQHMQ","target":"record","payload":{"canonical_record":{"source":{"id":"1211.4238","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-11-18T17:27:02Z","cross_cats_sorted":[],"title_canon_sha256":"91d3e51fc8e1c5c47181962b9e17607fe822e7e0fc0fd93dde92b5a63bc595fe","abstract_canon_sha256":"ab313128e0712ca4da51bb88cbb47c583bf2bf5f5fbab1ee3b9147bf9bee30e8"},"schema_version":"1.0"},"canonical_sha256":"4e158577d2f943fba3f66797d05a0764019791529ecc5b26c230ddaac7162c1a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:40:27.553224Z","signature_b64":"eggSBQngcV4BLrHoY/bOhI0jubY06Tn/NvDBd3ZgGgYeaqfmNqyEU4kIdnUApMOglQO+QVQj0CjxAJt77KtoCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4e158577d2f943fba3f66797d05a0764019791529ecc5b26c230ddaac7162c1a","last_reissued_at":"2026-05-18T03:40:27.552339Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:40:27.552339Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1211.4238","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:40:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wsA8b73rWID+XOA7JxGi8nE10LrQtaPMQAJQqKNG0zFPYV1hHBfDW4FZ3l8S4+zGZkH/9ElNcEX4LbIdnMS+Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T16:29:14.951086Z"},"content_sha256":"26acb40acc3c7cdae95702120257be443d8e85954142ed82399873845e04f41b","schema_version":"1.0","event_id":"sha256:26acb40acc3c7cdae95702120257be443d8e85954142ed82399873845e04f41b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:JYKYK56S7FB7XI7WM6L5AWQHMQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Conformal finite size scaling of twelve fermion flavors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Chik Him Wong, Chris Schroeder, Daniel Nogradi, Julius Kuti, Kieran Holland, Zoltan Fodor","submitted_at":"2012-11-18T17:27:02Z","abstract_excerpt":"Extended simulation results and their analysis are reported in a strongly coupled gauge theory with twelve fermion flavors in the fundamental SU(3) color representation. The conformality of the model is probed using mass deformed conformal finite size scaling (FSS) theory driven by the fermion mass anomalous dimension. Two independent conformal FSS fitting procedures are used in the analysis. The first one deploys physics motivated scaling functions, complemented by a second fitting procedure with spline based general B-forms for the scaling functions. The results at fixed gauge coupling show "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.4238","kind":"arxiv","version":1},"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":"2026-05-18T03:40:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+4jCAx92YWDET7CcjPYQMnr5AT45hlYcGf6V/JQvI9fn0I1UzE5MCeLoftFNCbG2xHa/ewXOvDfN5PYDbvFSBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T16:29:14.951752Z"},"content_sha256":"4c9fcf7bf4e88b57407d4b731c61cea0fabe56ea116d9db1b61ff0fffa2bdb78","schema_version":"1.0","event_id":"sha256:4c9fcf7bf4e88b57407d4b731c61cea0fabe56ea116d9db1b61ff0fffa2bdb78"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JYKYK56S7FB7XI7WM6L5AWQHMQ/bundle.json","state_url":"https://pith.science/pith/JYKYK56S7FB7XI7WM6L5AWQHMQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JYKYK56S7FB7XI7WM6L5AWQHMQ/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":"2026-05-31T16:29:14Z","links":{"resolver":"https://pith.science/pith/JYKYK56S7FB7XI7WM6L5AWQHMQ","bundle":"https://pith.science/pith/JYKYK56S7FB7XI7WM6L5AWQHMQ/bundle.json","state":"https://pith.science/pith/JYKYK56S7FB7XI7WM6L5AWQHMQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JYKYK56S7FB7XI7WM6L5AWQHMQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:JYKYK56S7FB7XI7WM6L5AWQHMQ","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":"ab313128e0712ca4da51bb88cbb47c583bf2bf5f5fbab1ee3b9147bf9bee30e8","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-11-18T17:27:02Z","title_canon_sha256":"91d3e51fc8e1c5c47181962b9e17607fe822e7e0fc0fd93dde92b5a63bc595fe"},"schema_version":"1.0","source":{"id":"1211.4238","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1211.4238","created_at":"2026-05-18T03:40:27Z"},{"alias_kind":"arxiv_version","alias_value":"1211.4238v1","created_at":"2026-05-18T03:40:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.4238","created_at":"2026-05-18T03:40:27Z"},{"alias_kind":"pith_short_12","alias_value":"JYKYK56S7FB7","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_16","alias_value":"JYKYK56S7FB7XI7W","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_8","alias_value":"JYKYK56S","created_at":"2026-05-18T12:27:11Z"}],"graph_snapshots":[{"event_id":"sha256:4c9fcf7bf4e88b57407d4b731c61cea0fabe56ea116d9db1b61ff0fffa2bdb78","target":"graph","created_at":"2026-05-18T03:40:27Z","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":"Extended simulation results and their analysis are reported in a strongly coupled gauge theory with twelve fermion flavors in the fundamental SU(3) color representation. The conformality of the model is probed using mass deformed conformal finite size scaling (FSS) theory driven by the fermion mass anomalous dimension. Two independent conformal FSS fitting procedures are used in the analysis. The first one deploys physics motivated scaling functions, complemented by a second fitting procedure with spline based general B-forms for the scaling functions. The results at fixed gauge coupling show ","authors_text":"Chik Him Wong, Chris Schroeder, Daniel Nogradi, Julius Kuti, Kieran Holland, Zoltan Fodor","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-11-18T17:27:02Z","title":"Conformal finite size scaling of twelve fermion flavors"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.4238","kind":"arxiv","version":1},"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":"sha256:26acb40acc3c7cdae95702120257be443d8e85954142ed82399873845e04f41b","target":"record","created_at":"2026-05-18T03:40:27Z","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":"ab313128e0712ca4da51bb88cbb47c583bf2bf5f5fbab1ee3b9147bf9bee30e8","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-11-18T17:27:02Z","title_canon_sha256":"91d3e51fc8e1c5c47181962b9e17607fe822e7e0fc0fd93dde92b5a63bc595fe"},"schema_version":"1.0","source":{"id":"1211.4238","kind":"arxiv","version":1}},"canonical_sha256":"4e158577d2f943fba3f66797d05a0764019791529ecc5b26c230ddaac7162c1a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4e158577d2f943fba3f66797d05a0764019791529ecc5b26c230ddaac7162c1a","first_computed_at":"2026-05-18T03:40:27.552339Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:40:27.552339Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"eggSBQngcV4BLrHoY/bOhI0jubY06Tn/NvDBd3ZgGgYeaqfmNqyEU4kIdnUApMOglQO+QVQj0CjxAJt77KtoCw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:40:27.553224Z","signed_message":"canonical_sha256_bytes"},"source_id":"1211.4238","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:26acb40acc3c7cdae95702120257be443d8e85954142ed82399873845e04f41b","sha256:4c9fcf7bf4e88b57407d4b731c61cea0fabe56ea116d9db1b61ff0fffa2bdb78"],"state_sha256":"0283455a0dddf7683b78e439b5d9b9bd844216e3987c9970613839a1fe59ca84"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0UTpRyfEuVq8Y1FWfSp5KVjcdpWNj0mn1x5g69UboJpPEAk9FOWZHrI4xtnZNxbRPXVO7tOWR8WIPyM2A/0RAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T16:29:14.955377Z","bundle_sha256":"a8aba172fd434c446cede2dabf4b38cc3642b807429e97647b919e65a1c7390e"}}