{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:WQJL42FOO3KAFM63ACXH4HBCJZ","short_pith_number":"pith:WQJL42FO","canonical_record":{"source":{"id":"1306.6879","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-06-28T15:38:40Z","cross_cats_sorted":[],"title_canon_sha256":"36df3eecbdbde0183538602ff94dc2ab32ae84bc2744309d9269e698e80e23a0","abstract_canon_sha256":"b3da21cc16902593a7328d18397aa260e6e4455645cd9e02a35147364b77f1a8"},"schema_version":"1.0"},"canonical_sha256":"b412be68ae76d402b3db00ae7e1c224e66920fd8b451e8297b543e5d0b610104","source":{"kind":"arxiv","id":"1306.6879","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1306.6879","created_at":"2026-05-18T03:06:03Z"},{"alias_kind":"arxiv_version","alias_value":"1306.6879v2","created_at":"2026-05-18T03:06:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.6879","created_at":"2026-05-18T03:06:03Z"},{"alias_kind":"pith_short_12","alias_value":"WQJL42FOO3KA","created_at":"2026-05-18T12:28:04Z"},{"alias_kind":"pith_short_16","alias_value":"WQJL42FOO3KAFM63","created_at":"2026-05-18T12:28:04Z"},{"alias_kind":"pith_short_8","alias_value":"WQJL42FO","created_at":"2026-05-18T12:28:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:WQJL42FOO3KAFM63ACXH4HBCJZ","target":"record","payload":{"canonical_record":{"source":{"id":"1306.6879","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-06-28T15:38:40Z","cross_cats_sorted":[],"title_canon_sha256":"36df3eecbdbde0183538602ff94dc2ab32ae84bc2744309d9269e698e80e23a0","abstract_canon_sha256":"b3da21cc16902593a7328d18397aa260e6e4455645cd9e02a35147364b77f1a8"},"schema_version":"1.0"},"canonical_sha256":"b412be68ae76d402b3db00ae7e1c224e66920fd8b451e8297b543e5d0b610104","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:06:03.140181Z","signature_b64":"1dcKi28t8jK7IiFCbZ1Oo2m/wFEOPqqZ02dHTXER0v8CEQe8oEA8gf/j+kYkzzJLl1Ys206xU9BxnKAHrlBeBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b412be68ae76d402b3db00ae7e1c224e66920fd8b451e8297b543e5d0b610104","last_reissued_at":"2026-05-18T03:06:03.139566Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:06:03.139566Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1306.6879","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":"2026-05-18T03:06:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ca5hiuGHxd/DBzL2/DXnBqpdGjGMBxfgx0CNj1zT7GCdJwpn9ChmPnCi5I2nw5gZ3LKz7lb9g/JVX9lEP7SpBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T22:06:48.674756Z"},"content_sha256":"bd78b085a9f0ae124bcae2a1ccf50d48d9ca7af504b2ad730718bbcdc6b061c6","schema_version":"1.0","event_id":"sha256:bd78b085a9f0ae124bcae2a1ccf50d48d9ca7af504b2ad730718bbcdc6b061c6"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:WQJL42FOO3KAFM63ACXH4HBCJZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Running quark and lepton parameters at various scales","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Stefan Antusch, Vinzenz Maurer","submitted_at":"2013-06-28T15:38:40Z","abstract_excerpt":"We calculate the values and 1 sigma ranges of the running quark and lepton Yukawa couplings as well as of the quark mixing parameters at various energy scales, i.e. at M_Z, 1 TeV, 3 TeV, 10 TeV and at the GUT scale, to provide useful input for model building. Above TeV energies, we assume the minimal supersymmetric extension of the Standard Model, and include the tan(beta)-enhanced one-loop supersymmetric threshold corrections which arise when matching the SM to its SUSY extension. We calculate the GUT scale values of the running parameters as well as their 1 sigma ranges, with the supersymmet"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.6879","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":"2026-05-18T03:06:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kQiwrbGU3OlFSAn2qyonX6HlTrI8rxP38i32Q+dXIjtEuegOsPJE1HtRFCowesgXKpValTFrbs5k7mXA9IA7CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T22:06:48.675445Z"},"content_sha256":"161c7586b05051726b989658a5fec4258b911bd0ef0bb05065470b799e98d850","schema_version":"1.0","event_id":"sha256:161c7586b05051726b989658a5fec4258b911bd0ef0bb05065470b799e98d850"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/WQJL42FOO3KAFM63ACXH4HBCJZ/bundle.json","state_url":"https://pith.science/pith/WQJL42FOO3KAFM63ACXH4HBCJZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/WQJL42FOO3KAFM63ACXH4HBCJZ/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":"2026-06-05T22:06:48Z","links":{"resolver":"https://pith.science/pith/WQJL42FOO3KAFM63ACXH4HBCJZ","bundle":"https://pith.science/pith/WQJL42FOO3KAFM63ACXH4HBCJZ/bundle.json","state":"https://pith.science/pith/WQJL42FOO3KAFM63ACXH4HBCJZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/WQJL42FOO3KAFM63ACXH4HBCJZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:WQJL42FOO3KAFM63ACXH4HBCJZ","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":"b3da21cc16902593a7328d18397aa260e6e4455645cd9e02a35147364b77f1a8","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-06-28T15:38:40Z","title_canon_sha256":"36df3eecbdbde0183538602ff94dc2ab32ae84bc2744309d9269e698e80e23a0"},"schema_version":"1.0","source":{"id":"1306.6879","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1306.6879","created_at":"2026-05-18T03:06:03Z"},{"alias_kind":"arxiv_version","alias_value":"1306.6879v2","created_at":"2026-05-18T03:06:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.6879","created_at":"2026-05-18T03:06:03Z"},{"alias_kind":"pith_short_12","alias_value":"WQJL42FOO3KA","created_at":"2026-05-18T12:28:04Z"},{"alias_kind":"pith_short_16","alias_value":"WQJL42FOO3KAFM63","created_at":"2026-05-18T12:28:04Z"},{"alias_kind":"pith_short_8","alias_value":"WQJL42FO","created_at":"2026-05-18T12:28:04Z"}],"graph_snapshots":[{"event_id":"sha256:161c7586b05051726b989658a5fec4258b911bd0ef0bb05065470b799e98d850","target":"graph","created_at":"2026-05-18T03:06:03Z","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 calculate the values and 1 sigma ranges of the running quark and lepton Yukawa couplings as well as of the quark mixing parameters at various energy scales, i.e. at M_Z, 1 TeV, 3 TeV, 10 TeV and at the GUT scale, to provide useful input for model building. Above TeV energies, we assume the minimal supersymmetric extension of the Standard Model, and include the tan(beta)-enhanced one-loop supersymmetric threshold corrections which arise when matching the SM to its SUSY extension. We calculate the GUT scale values of the running parameters as well as their 1 sigma ranges, with the supersymmet","authors_text":"Stefan Antusch, Vinzenz Maurer","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-06-28T15:38:40Z","title":"Running quark and lepton parameters at various scales"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.6879","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:bd78b085a9f0ae124bcae2a1ccf50d48d9ca7af504b2ad730718bbcdc6b061c6","target":"record","created_at":"2026-05-18T03:06:03Z","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":"b3da21cc16902593a7328d18397aa260e6e4455645cd9e02a35147364b77f1a8","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-06-28T15:38:40Z","title_canon_sha256":"36df3eecbdbde0183538602ff94dc2ab32ae84bc2744309d9269e698e80e23a0"},"schema_version":"1.0","source":{"id":"1306.6879","kind":"arxiv","version":2}},"canonical_sha256":"b412be68ae76d402b3db00ae7e1c224e66920fd8b451e8297b543e5d0b610104","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b412be68ae76d402b3db00ae7e1c224e66920fd8b451e8297b543e5d0b610104","first_computed_at":"2026-05-18T03:06:03.139566Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:06:03.139566Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"1dcKi28t8jK7IiFCbZ1Oo2m/wFEOPqqZ02dHTXER0v8CEQe8oEA8gf/j+kYkzzJLl1Ys206xU9BxnKAHrlBeBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:06:03.140181Z","signed_message":"canonical_sha256_bytes"},"source_id":"1306.6879","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:bd78b085a9f0ae124bcae2a1ccf50d48d9ca7af504b2ad730718bbcdc6b061c6","sha256:161c7586b05051726b989658a5fec4258b911bd0ef0bb05065470b799e98d850"],"state_sha256":"5f8dcb8bc1721075f7e510e8f13556ba9cf8cd1e62c23dbd420c349c69b614c8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZmB3AM3uMzNq6eg3b0+UoNSqgd0CnTT8Zen0nvqPCj/iM5N9m9vOKjLsEkih7pO6G5hBhd635ZlxhFA/Po12Bw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-05T22:06:48.679296Z","bundle_sha256":"a22ca1ab1850fd7d6d6af64570fe19adf1a6bd1ab876858e2992dfb3881fe40f"}}