{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:RNF4RIIEG2S2ZWTP6FTB4MSC27","short_pith_number":"pith:RNF4RIIE","canonical_record":{"source":{"id":"1711.01860","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-11-06T12:36:00Z","cross_cats_sorted":[],"title_canon_sha256":"3c7f20a6c4a1c42da8951813290bb1e5804a714599569409fcf4eddd84fca94e","abstract_canon_sha256":"f1f17897a47bd8f117aed5ab9f717970eff49109ea8df9ebb25521fff10d1da0"},"schema_version":"1.0"},"canonical_sha256":"8b4bc8a10436a5acda6ff1661e3242d7e72fbc8aa73696d866c218b2673f6eb3","source":{"kind":"arxiv","id":"1711.01860","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.01860","created_at":"2026-05-18T00:18:15Z"},{"alias_kind":"arxiv_version","alias_value":"1711.01860v1","created_at":"2026-05-18T00:18:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.01860","created_at":"2026-05-18T00:18:15Z"},{"alias_kind":"pith_short_12","alias_value":"RNF4RIIEG2S2","created_at":"2026-05-18T12:31:39Z"},{"alias_kind":"pith_short_16","alias_value":"RNF4RIIEG2S2ZWTP","created_at":"2026-05-18T12:31:39Z"},{"alias_kind":"pith_short_8","alias_value":"RNF4RIIE","created_at":"2026-05-18T12:31:39Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:RNF4RIIEG2S2ZWTP6FTB4MSC27","target":"record","payload":{"canonical_record":{"source":{"id":"1711.01860","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-11-06T12:36:00Z","cross_cats_sorted":[],"title_canon_sha256":"3c7f20a6c4a1c42da8951813290bb1e5804a714599569409fcf4eddd84fca94e","abstract_canon_sha256":"f1f17897a47bd8f117aed5ab9f717970eff49109ea8df9ebb25521fff10d1da0"},"schema_version":"1.0"},"canonical_sha256":"8b4bc8a10436a5acda6ff1661e3242d7e72fbc8aa73696d866c218b2673f6eb3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:18:15.485413Z","signature_b64":"pMoxNlX+UdSWLezoHg83+T/yqM/CSg6pa8RiT+AqdfPXcBkrAkJm8ZKH8/mPEnBYdW0QvW9DwN/jebKMJRW4Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8b4bc8a10436a5acda6ff1661e3242d7e72fbc8aa73696d866c218b2673f6eb3","last_reissued_at":"2026-05-18T00:18:15.485014Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:18:15.485014Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1711.01860","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":"2026-05-18T00:18:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Gvzam9YwUfgqYx+m6oNz21buU59j2rDGGw0rbmwUnZYe3dVjhLAfw34XOE8xpO0fMYELdzZOP+N0YENYP9aQBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T22:05:51.087766Z"},"content_sha256":"0e57ab4159457b17e3e0e0ca28e3f2d800a8d1b40e0734df2d60a3d6554165c6","schema_version":"1.0","event_id":"sha256:0e57ab4159457b17e3e0e0ca28e3f2d800a8d1b40e0734df2d60a3d6554165c6"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:RNF4RIIEG2S2ZWTP6FTB4MSC27","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"SU(3) Yang Mills theory at small distances and fine lattices","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Mateusz Koren, Nikolai Husung, Philipp Krah, Rainer Sommer","submitted_at":"2017-11-06T12:36:00Z","abstract_excerpt":"We investigate the SU(3) Yang Mills theory at small gradient flow time and at short distances. Lattice spacings down to $a=0.015$ fm are simulated with open boundary conditions to allow topology to flow in and out. We study the behaviour of the action density $E(t)$ close to the boundaries, the feasibility of the small flow-time expansion and the extraction of the $\\Lambda$-parameter from the static force at small distances. For the latter, significant deviations from the 4-loop perturbative $\\beta$-function are visible at $\\alpha\\approx 0.2\\,$. We still can extrapolate to extract $r_0\\Lambda$"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.01860","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":"2026-05-18T00:18:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"C1IzPaAgl+rWpuRWtOCAxsi+iNVCCZB+ug3vY5R/+HVk6DnK8/UaDPdv+L4lpsFBzd2p3TiGx7+qM1YvdNtbBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T22:05:51.088117Z"},"content_sha256":"1ba5ad924ea8fd060ae2d897e3d9cb80ca250a0f9c464d741ec95d066284ee10","schema_version":"1.0","event_id":"sha256:1ba5ad924ea8fd060ae2d897e3d9cb80ca250a0f9c464d741ec95d066284ee10"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RNF4RIIEG2S2ZWTP6FTB4MSC27/bundle.json","state_url":"https://pith.science/pith/RNF4RIIEG2S2ZWTP6FTB4MSC27/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RNF4RIIEG2S2ZWTP6FTB4MSC27/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":"2026-06-03T22:05:51Z","links":{"resolver":"https://pith.science/pith/RNF4RIIEG2S2ZWTP6FTB4MSC27","bundle":"https://pith.science/pith/RNF4RIIEG2S2ZWTP6FTB4MSC27/bundle.json","state":"https://pith.science/pith/RNF4RIIEG2S2ZWTP6FTB4MSC27/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RNF4RIIEG2S2ZWTP6FTB4MSC27/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:RNF4RIIEG2S2ZWTP6FTB4MSC27","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":"f1f17897a47bd8f117aed5ab9f717970eff49109ea8df9ebb25521fff10d1da0","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-11-06T12:36:00Z","title_canon_sha256":"3c7f20a6c4a1c42da8951813290bb1e5804a714599569409fcf4eddd84fca94e"},"schema_version":"1.0","source":{"id":"1711.01860","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.01860","created_at":"2026-05-18T00:18:15Z"},{"alias_kind":"arxiv_version","alias_value":"1711.01860v1","created_at":"2026-05-18T00:18:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.01860","created_at":"2026-05-18T00:18:15Z"},{"alias_kind":"pith_short_12","alias_value":"RNF4RIIEG2S2","created_at":"2026-05-18T12:31:39Z"},{"alias_kind":"pith_short_16","alias_value":"RNF4RIIEG2S2ZWTP","created_at":"2026-05-18T12:31:39Z"},{"alias_kind":"pith_short_8","alias_value":"RNF4RIIE","created_at":"2026-05-18T12:31:39Z"}],"graph_snapshots":[{"event_id":"sha256:1ba5ad924ea8fd060ae2d897e3d9cb80ca250a0f9c464d741ec95d066284ee10","target":"graph","created_at":"2026-05-18T00:18:15Z","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 investigate the SU(3) Yang Mills theory at small gradient flow time and at short distances. Lattice spacings down to $a=0.015$ fm are simulated with open boundary conditions to allow topology to flow in and out. We study the behaviour of the action density $E(t)$ close to the boundaries, the feasibility of the small flow-time expansion and the extraction of the $\\Lambda$-parameter from the static force at small distances. For the latter, significant deviations from the 4-loop perturbative $\\beta$-function are visible at $\\alpha\\approx 0.2\\,$. We still can extrapolate to extract $r_0\\Lambda$","authors_text":"Mateusz Koren, Nikolai Husung, Philipp Krah, Rainer Sommer","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-11-06T12:36:00Z","title":"SU(3) Yang Mills theory at small distances and fine lattices"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.01860","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":"sha256:0e57ab4159457b17e3e0e0ca28e3f2d800a8d1b40e0734df2d60a3d6554165c6","target":"record","created_at":"2026-05-18T00:18:15Z","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":"f1f17897a47bd8f117aed5ab9f717970eff49109ea8df9ebb25521fff10d1da0","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-11-06T12:36:00Z","title_canon_sha256":"3c7f20a6c4a1c42da8951813290bb1e5804a714599569409fcf4eddd84fca94e"},"schema_version":"1.0","source":{"id":"1711.01860","kind":"arxiv","version":1}},"canonical_sha256":"8b4bc8a10436a5acda6ff1661e3242d7e72fbc8aa73696d866c218b2673f6eb3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8b4bc8a10436a5acda6ff1661e3242d7e72fbc8aa73696d866c218b2673f6eb3","first_computed_at":"2026-05-18T00:18:15.485014Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:18:15.485014Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"pMoxNlX+UdSWLezoHg83+T/yqM/CSg6pa8RiT+AqdfPXcBkrAkJm8ZKH8/mPEnBYdW0QvW9DwN/jebKMJRW4Ag==","signature_status":"signed_v1","signed_at":"2026-05-18T00:18:15.485413Z","signed_message":"canonical_sha256_bytes"},"source_id":"1711.01860","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0e57ab4159457b17e3e0e0ca28e3f2d800a8d1b40e0734df2d60a3d6554165c6","sha256:1ba5ad924ea8fd060ae2d897e3d9cb80ca250a0f9c464d741ec95d066284ee10"],"state_sha256":"160fca42ab8ad23c18f9b2cbcff3baf02b9090aa558554412cedb20817147ea5"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RbPp2f//97iZgTbNRllNIQ3lriI2ZzLaGzwW6KwF9IEYUNBjkv34wZ8l+bcd5YuJgrb0fmdL8uIZoJQC36WSBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T22:05:51.090102Z","bundle_sha256":"5b2660481eee67c31ba2ff182fafbad59106c6c7d58b200d71e7f6e672085808"}}