{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:PADCUKHUO3LVRAB5J2PDWU2TCP","short_pith_number":"pith:PADCUKHU","canonical_record":{"source":{"id":"1805.00198","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-05-01T06:18:55Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"791905ea54791fdae3ccd81492e68ba455bd18b75eefd020fe471f0dc1104c23","abstract_canon_sha256":"90e7d23949b5e88ed8c68cfd4df8f19961749a826de24eb414062e26516afe2b"},"schema_version":"1.0"},"canonical_sha256":"78062a28f476d758803d4e9e3b535313ccc6dafdcc53be04f275a97020b0498d","source":{"kind":"arxiv","id":"1805.00198","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1805.00198","created_at":"2026-05-18T00:04:17Z"},{"alias_kind":"arxiv_version","alias_value":"1805.00198v2","created_at":"2026-05-18T00:04:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.00198","created_at":"2026-05-18T00:04:17Z"},{"alias_kind":"pith_short_12","alias_value":"PADCUKHUO3LV","created_at":"2026-05-18T12:32:43Z"},{"alias_kind":"pith_short_16","alias_value":"PADCUKHUO3LVRAB5","created_at":"2026-05-18T12:32:43Z"},{"alias_kind":"pith_short_8","alias_value":"PADCUKHU","created_at":"2026-05-18T12:32:43Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:PADCUKHUO3LVRAB5J2PDWU2TCP","target":"record","payload":{"canonical_record":{"source":{"id":"1805.00198","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-05-01T06:18:55Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"791905ea54791fdae3ccd81492e68ba455bd18b75eefd020fe471f0dc1104c23","abstract_canon_sha256":"90e7d23949b5e88ed8c68cfd4df8f19961749a826de24eb414062e26516afe2b"},"schema_version":"1.0"},"canonical_sha256":"78062a28f476d758803d4e9e3b535313ccc6dafdcc53be04f275a97020b0498d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:04:17.347081Z","signature_b64":"nr0c75xEZL3u34TksJraM6znMBhAIOLX3MCY3F2O31rW0f3XucBNUADY8ipx/gSJRzZsJJsFUVFU5O+JdaNhCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"78062a28f476d758803d4e9e3b535313ccc6dafdcc53be04f275a97020b0498d","last_reissued_at":"2026-05-18T00:04:17.346333Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:04:17.346333Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1805.00198","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":"2026-05-18T00:04:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mLJrTXXZmhuM2NeT3LaEW4g45WevV+q8FLJTz4Vg+ndM6Hhamv3VdKK7CeSuN/qbj7Igsd3X/WGZT5Sj9fuoCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T15:38:35.394259Z"},"content_sha256":"0608fa8f9ead2fdc244b831558f5b910e17632a363f3740e22d74974b5095987","schema_version":"1.0","event_id":"sha256:0608fa8f9ead2fdc244b831558f5b910e17632a363f3740e22d74974b5095987"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:PADCUKHUO3LVRAB5J2PDWU2TCP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The large-mass regime of the dilaton-pion low-energy effective theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"Maarten Golterman, Yigal Shamir","submitted_at":"2018-05-01T06:18:55Z","abstract_excerpt":"Numerical data of the SU(3) gauge theory with $N_f=8$ fermions in the fundamental representation suggest the existence of a large-mass regime, where the fermion mass is not small relative to the confinement scale, but nevertheless the dilaton-pion low-energy theory is applicable thanks to the parametric proximity of the conformal window. In this regime, the leading hyperscaling relations are similar to those of a mass-deformed conformal theory, so that distinguishing infrared conformality from confinement requires the study of subleading effects. Assuming that the $N_f=8$ theory confines, we e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.00198","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":"2026-05-18T00:04:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0HGQGesXN4J9yqhovSUMINSOxB6uqaNVgxjUH9P/gi8mGgoRujTuHu1tj8lFqYKgvNvVSfm8wKlrc0x6/0uJDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T15:38:35.394815Z"},"content_sha256":"4e41c757e1061ecf72dbf31d059fca0f6485ae6e04b9ec5333beefdacb8d756f","schema_version":"1.0","event_id":"sha256:4e41c757e1061ecf72dbf31d059fca0f6485ae6e04b9ec5333beefdacb8d756f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PADCUKHUO3LVRAB5J2PDWU2TCP/bundle.json","state_url":"https://pith.science/pith/PADCUKHUO3LVRAB5J2PDWU2TCP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PADCUKHUO3LVRAB5J2PDWU2TCP/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":"2026-05-27T15:38:35Z","links":{"resolver":"https://pith.science/pith/PADCUKHUO3LVRAB5J2PDWU2TCP","bundle":"https://pith.science/pith/PADCUKHUO3LVRAB5J2PDWU2TCP/bundle.json","state":"https://pith.science/pith/PADCUKHUO3LVRAB5J2PDWU2TCP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PADCUKHUO3LVRAB5J2PDWU2TCP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:PADCUKHUO3LVRAB5J2PDWU2TCP","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":"90e7d23949b5e88ed8c68cfd4df8f19961749a826de24eb414062e26516afe2b","cross_cats_sorted":["hep-lat"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-05-01T06:18:55Z","title_canon_sha256":"791905ea54791fdae3ccd81492e68ba455bd18b75eefd020fe471f0dc1104c23"},"schema_version":"1.0","source":{"id":"1805.00198","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1805.00198","created_at":"2026-05-18T00:04:17Z"},{"alias_kind":"arxiv_version","alias_value":"1805.00198v2","created_at":"2026-05-18T00:04:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.00198","created_at":"2026-05-18T00:04:17Z"},{"alias_kind":"pith_short_12","alias_value":"PADCUKHUO3LV","created_at":"2026-05-18T12:32:43Z"},{"alias_kind":"pith_short_16","alias_value":"PADCUKHUO3LVRAB5","created_at":"2026-05-18T12:32:43Z"},{"alias_kind":"pith_short_8","alias_value":"PADCUKHU","created_at":"2026-05-18T12:32:43Z"}],"graph_snapshots":[{"event_id":"sha256:4e41c757e1061ecf72dbf31d059fca0f6485ae6e04b9ec5333beefdacb8d756f","target":"graph","created_at":"2026-05-18T00:04:17Z","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":"Numerical data of the SU(3) gauge theory with $N_f=8$ fermions in the fundamental representation suggest the existence of a large-mass regime, where the fermion mass is not small relative to the confinement scale, but nevertheless the dilaton-pion low-energy theory is applicable thanks to the parametric proximity of the conformal window. In this regime, the leading hyperscaling relations are similar to those of a mass-deformed conformal theory, so that distinguishing infrared conformality from confinement requires the study of subleading effects. Assuming that the $N_f=8$ theory confines, we e","authors_text":"Maarten Golterman, Yigal Shamir","cross_cats":["hep-lat"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-05-01T06:18:55Z","title":"The large-mass regime of the dilaton-pion low-energy effective theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.00198","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":"sha256:0608fa8f9ead2fdc244b831558f5b910e17632a363f3740e22d74974b5095987","target":"record","created_at":"2026-05-18T00:04:17Z","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":"90e7d23949b5e88ed8c68cfd4df8f19961749a826de24eb414062e26516afe2b","cross_cats_sorted":["hep-lat"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-05-01T06:18:55Z","title_canon_sha256":"791905ea54791fdae3ccd81492e68ba455bd18b75eefd020fe471f0dc1104c23"},"schema_version":"1.0","source":{"id":"1805.00198","kind":"arxiv","version":2}},"canonical_sha256":"78062a28f476d758803d4e9e3b535313ccc6dafdcc53be04f275a97020b0498d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"78062a28f476d758803d4e9e3b535313ccc6dafdcc53be04f275a97020b0498d","first_computed_at":"2026-05-18T00:04:17.346333Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:04:17.346333Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nr0c75xEZL3u34TksJraM6znMBhAIOLX3MCY3F2O31rW0f3XucBNUADY8ipx/gSJRzZsJJsFUVFU5O+JdaNhCw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:04:17.347081Z","signed_message":"canonical_sha256_bytes"},"source_id":"1805.00198","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0608fa8f9ead2fdc244b831558f5b910e17632a363f3740e22d74974b5095987","sha256:4e41c757e1061ecf72dbf31d059fca0f6485ae6e04b9ec5333beefdacb8d756f"],"state_sha256":"f84fed62823fce718402744effcce2826626e13d24620f9d94360b74f6f95854"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"a6p+RxHYBYUAL09LiAm5feCEJHBrbzOM11YLhhFp0dYqS0fYJO0BEprhfxNFLWl3uzbPbXagziSPTxOvQaUoBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T15:38:35.397881Z","bundle_sha256":"08fd3304a1a29ea8ec26dc6e4c30dcdd4c8eb2c5a6407408d69ca55fb0615dfd"}}