{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2003:BCVM4DDIN6X5BKYJNXR6X3CHUQ","short_pith_number":"pith:BCVM4DDI","canonical_record":{"source":{"id":"hep-ph/0308301","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-08-28T16:29:49Z","cross_cats_sorted":[],"title_canon_sha256":"8daa954ad26a99266282d06a1d49ac003731ea47806f7ca2d6b6cc922c1a6dd3","abstract_canon_sha256":"01f0de82e8c8f29216db36fd8b566274fb759e3f5f0f727c017e138859e11a9e"},"schema_version":"1.0"},"canonical_sha256":"08aace0c686fafd0ab096de3ebec47a420036dbf4a0badcaaed58e88acff6cde","source":{"kind":"arxiv","id":"hep-ph/0308301","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0308301","created_at":"2026-05-18T01:39:06Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0308301v3","created_at":"2026-05-18T01:39:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0308301","created_at":"2026-05-18T01:39:06Z"},{"alias_kind":"pith_short_12","alias_value":"BCVM4DDIN6X5","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_16","alias_value":"BCVM4DDIN6X5BKYJ","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_8","alias_value":"BCVM4DDI","created_at":"2026-05-18T12:25:51Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2003:BCVM4DDIN6X5BKYJNXR6X3CHUQ","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0308301","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-08-28T16:29:49Z","cross_cats_sorted":[],"title_canon_sha256":"8daa954ad26a99266282d06a1d49ac003731ea47806f7ca2d6b6cc922c1a6dd3","abstract_canon_sha256":"01f0de82e8c8f29216db36fd8b566274fb759e3f5f0f727c017e138859e11a9e"},"schema_version":"1.0"},"canonical_sha256":"08aace0c686fafd0ab096de3ebec47a420036dbf4a0badcaaed58e88acff6cde","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:39:06.282349Z","signature_b64":"Q/v1QgNDnby9/Bd4RhkeupuxnOMX++DehPZtDR9oKUcGxf3JW60GyQV4ieg5oO+uSF1eYx9JKSL6bj/kgJ8JAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"08aace0c686fafd0ab096de3ebec47a420036dbf4a0badcaaed58e88acff6cde","last_reissued_at":"2026-05-18T01:39:06.281866Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:39:06.281866Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0308301","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:39:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5oMP/kXSORd/LbgZuMlSHaxgEnxymffVwqPbz3NOT7IHWUIAfFi5jOKt9koYXv+eQOcW4mnr91IHJb3ZxqYqAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T02:54:43.144413Z"},"content_sha256":"715cf7f3d4ab8211b3453b9d9e55362d21f76f69669d8a22383074158e208a1a","schema_version":"1.0","event_id":"sha256:715cf7f3d4ab8211b3453b9d9e55362d21f76f69669d8a22383074158e208a1a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2003:BCVM4DDIN6X5BKYJNXR6X3CHUQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Optimal Renormalization-Group Improvement of Two Radiatively-Broken Gauge Theories","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"D.G.C. McKeon, R.B. Mann, T.G. Steele, V. Elias","submitted_at":"2003-08-28T16:29:49Z","abstract_excerpt":"In the absence of a tree-level scalar-field mass, renormalization-group (RG) methods permit the explicit summation of leading-logarithm contributions to all orders of the perturbative series for the effective-potential functions utilized in radiative symmetry breaking. For scalar-field electrodynamics, such a summation of leading logarithm contributions leads to upper bounds on the magnitudes of both gauge and scalar-field coupling constants, and suggests the possibility of an additional phase of spontaneous symmetry breaking characterized by a scalar-field mass comparable to that of the theor"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0308301","kind":"arxiv","version":3},"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":"2026-05-18T01:39:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ivq3ScFCApbqp6UhmTeIXhpXjGgtVUgBi2DPl3d0tKT9JHgGhWsa4mWLvUDfcLUISxSL6qSGchMqSQx8h44zDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T02:54:43.144761Z"},"content_sha256":"23ae4e1c0a37a42fa2d6359b83146355fadf4fb10eb110caa6176e494abcd5aa","schema_version":"1.0","event_id":"sha256:23ae4e1c0a37a42fa2d6359b83146355fadf4fb10eb110caa6176e494abcd5aa"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/BCVM4DDIN6X5BKYJNXR6X3CHUQ/bundle.json","state_url":"https://pith.science/pith/BCVM4DDIN6X5BKYJNXR6X3CHUQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/BCVM4DDIN6X5BKYJNXR6X3CHUQ/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":"2026-06-03T02:54:43Z","links":{"resolver":"https://pith.science/pith/BCVM4DDIN6X5BKYJNXR6X3CHUQ","bundle":"https://pith.science/pith/BCVM4DDIN6X5BKYJNXR6X3CHUQ/bundle.json","state":"https://pith.science/pith/BCVM4DDIN6X5BKYJNXR6X3CHUQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/BCVM4DDIN6X5BKYJNXR6X3CHUQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2003:BCVM4DDIN6X5BKYJNXR6X3CHUQ","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":"01f0de82e8c8f29216db36fd8b566274fb759e3f5f0f727c017e138859e11a9e","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2003-08-28T16:29:49Z","title_canon_sha256":"8daa954ad26a99266282d06a1d49ac003731ea47806f7ca2d6b6cc922c1a6dd3"},"schema_version":"1.0","source":{"id":"hep-ph/0308301","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0308301","created_at":"2026-05-18T01:39:06Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0308301v3","created_at":"2026-05-18T01:39:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0308301","created_at":"2026-05-18T01:39:06Z"},{"alias_kind":"pith_short_12","alias_value":"BCVM4DDIN6X5","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_16","alias_value":"BCVM4DDIN6X5BKYJ","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_8","alias_value":"BCVM4DDI","created_at":"2026-05-18T12:25:51Z"}],"graph_snapshots":[{"event_id":"sha256:23ae4e1c0a37a42fa2d6359b83146355fadf4fb10eb110caa6176e494abcd5aa","target":"graph","created_at":"2026-05-18T01:39:06Z","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":"In the absence of a tree-level scalar-field mass, renormalization-group (RG) methods permit the explicit summation of leading-logarithm contributions to all orders of the perturbative series for the effective-potential functions utilized in radiative symmetry breaking. For scalar-field electrodynamics, such a summation of leading logarithm contributions leads to upper bounds on the magnitudes of both gauge and scalar-field coupling constants, and suggests the possibility of an additional phase of spontaneous symmetry breaking characterized by a scalar-field mass comparable to that of the theor","authors_text":"D.G.C. McKeon, R.B. Mann, T.G. Steele, V. Elias","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2003-08-28T16:29:49Z","title":"Optimal Renormalization-Group Improvement of Two Radiatively-Broken Gauge Theories"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0308301","kind":"arxiv","version":3},"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":"sha256:715cf7f3d4ab8211b3453b9d9e55362d21f76f69669d8a22383074158e208a1a","target":"record","created_at":"2026-05-18T01:39:06Z","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":"01f0de82e8c8f29216db36fd8b566274fb759e3f5f0f727c017e138859e11a9e","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2003-08-28T16:29:49Z","title_canon_sha256":"8daa954ad26a99266282d06a1d49ac003731ea47806f7ca2d6b6cc922c1a6dd3"},"schema_version":"1.0","source":{"id":"hep-ph/0308301","kind":"arxiv","version":3}},"canonical_sha256":"08aace0c686fafd0ab096de3ebec47a420036dbf4a0badcaaed58e88acff6cde","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"08aace0c686fafd0ab096de3ebec47a420036dbf4a0badcaaed58e88acff6cde","first_computed_at":"2026-05-18T01:39:06.281866Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:39:06.281866Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Q/v1QgNDnby9/Bd4RhkeupuxnOMX++DehPZtDR9oKUcGxf3JW60GyQV4ieg5oO+uSF1eYx9JKSL6bj/kgJ8JAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:39:06.282349Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0308301","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:715cf7f3d4ab8211b3453b9d9e55362d21f76f69669d8a22383074158e208a1a","sha256:23ae4e1c0a37a42fa2d6359b83146355fadf4fb10eb110caa6176e494abcd5aa"],"state_sha256":"bd17b0050c99d447f8a7480d05460db6bdf206abef64e318ac8eed8e2b123d7f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9zn/xldc7NnJJMurG4fGWDFHig07W1nKgCSgZd5yWZMdLPIpCmm8EFTtmWjadTp9Uw+JivQrxEyAiGrARQRcBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T02:54:43.146958Z","bundle_sha256":"7547afccec6451057aa54004d91869921105c80efe5f39973f3fad295914cd27"}}