{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1995:O7D2VYJYTIAUBVYUULRMWGR3JV","short_pith_number":"pith:O7D2VYJY","canonical_record":{"source":{"id":"hep-ph/9505428","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1995-06-01T06:22:17Z","cross_cats_sorted":[],"title_canon_sha256":"79556b7bd2338b92631bd94a7c46bb28e56f68af4408120fb7afb897adb548e9","abstract_canon_sha256":"42423e963d3c854b9c82ab73240cf2cfa9b5981624974e391d64dd95ed291ba5"},"schema_version":"1.0"},"canonical_sha256":"77c7aae1389a0140d714a2e2cb1a3b4d4364450dc2aa0c76da04665c2c68808e","source":{"kind":"arxiv","id":"hep-ph/9505428","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9505428","created_at":"2026-05-18T04:30:37Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9505428v1","created_at":"2026-05-18T04:30:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9505428","created_at":"2026-05-18T04:30:37Z"},{"alias_kind":"pith_short_12","alias_value":"O7D2VYJYTIAU","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_16","alias_value":"O7D2VYJYTIAUBVYU","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_8","alias_value":"O7D2VYJY","created_at":"2026-05-18T12:25:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1995:O7D2VYJYTIAUBVYUULRMWGR3JV","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9505428","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1995-06-01T06:22:17Z","cross_cats_sorted":[],"title_canon_sha256":"79556b7bd2338b92631bd94a7c46bb28e56f68af4408120fb7afb897adb548e9","abstract_canon_sha256":"42423e963d3c854b9c82ab73240cf2cfa9b5981624974e391d64dd95ed291ba5"},"schema_version":"1.0"},"canonical_sha256":"77c7aae1389a0140d714a2e2cb1a3b4d4364450dc2aa0c76da04665c2c68808e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:30:37.757899Z","signature_b64":"8ClbfxKkn1NubLVfM1ZDlLgGTY5uxUQ67qQBBSyh+bNY49rH03rdyTHML3VYK9ueIvGevuc4X5/9gZcHM++3Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"77c7aae1389a0140d714a2e2cb1a3b4d4364450dc2aa0c76da04665c2c68808e","last_reissued_at":"2026-05-18T04:30:37.757071Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:30:37.757071Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9505428","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":"2026-05-18T04:30:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jvFdHhayNe2Novo2YvlIATRMGgNh/07kxUZBlnj5drSQX4DWJoDacKYZBkWNbyeEA5aFUtBo/OgcqqfSpXuBDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-30T22:42:52.973608Z"},"content_sha256":"d2b81ec0918d32b6ef86df19b4758d415f776a4a7b5646f546f92da6c0fa74ab","schema_version":"1.0","event_id":"sha256:d2b81ec0918d32b6ef86df19b4758d415f776a4a7b5646f546f92da6c0fa74ab"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1995:O7D2VYJYTIAUBVYUULRMWGR3JV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The Unified Minimal Supersymmetric Model with Large Yukawa Couplings","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"R. Rattazzi (Rutgers), U. Sarid (Stanford)","submitted_at":"1995-06-01T06:22:17Z","abstract_excerpt":"The consequences of assuming the third-generation Yukawa couplings are all large and comparable are studied in the context of the minimal supersymmetric extension of the standard model. General aspects of the RG evolution of the parameters, theoretical constraints needed to ensure proper electroweak symmetry breaking, and experimental and cosmological bounds on low-energy parameters are presented. We also present complete and exact semi-analytic solutions to the 1-loop RG equations. Focusing on SU(5) or SO(10) unification, we analyze the relationship between the top and bottom masses and the s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9505428","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":"2026-05-18T04:30:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7988JNMsTFyvG7fyZB8S4bL84Yh+bKcZc7JRRaRG/Vc1sJSA+4NhG7vO6gR5OGEeGnNmS4HDPRhUiVDn2AbLAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-30T22:42:52.973952Z"},"content_sha256":"3af2d78c99b8545d855d99f1882997ca5053f93332f58db80da05b8d26d8df51","schema_version":"1.0","event_id":"sha256:3af2d78c99b8545d855d99f1882997ca5053f93332f58db80da05b8d26d8df51"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/O7D2VYJYTIAUBVYUULRMWGR3JV/bundle.json","state_url":"https://pith.science/pith/O7D2VYJYTIAUBVYUULRMWGR3JV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/O7D2VYJYTIAUBVYUULRMWGR3JV/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":"2026-06-30T22:42:52Z","links":{"resolver":"https://pith.science/pith/O7D2VYJYTIAUBVYUULRMWGR3JV","bundle":"https://pith.science/pith/O7D2VYJYTIAUBVYUULRMWGR3JV/bundle.json","state":"https://pith.science/pith/O7D2VYJYTIAUBVYUULRMWGR3JV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/O7D2VYJYTIAUBVYUULRMWGR3JV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1995:O7D2VYJYTIAUBVYUULRMWGR3JV","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":"42423e963d3c854b9c82ab73240cf2cfa9b5981624974e391d64dd95ed291ba5","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1995-06-01T06:22:17Z","title_canon_sha256":"79556b7bd2338b92631bd94a7c46bb28e56f68af4408120fb7afb897adb548e9"},"schema_version":"1.0","source":{"id":"hep-ph/9505428","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9505428","created_at":"2026-05-18T04:30:37Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9505428v1","created_at":"2026-05-18T04:30:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9505428","created_at":"2026-05-18T04:30:37Z"},{"alias_kind":"pith_short_12","alias_value":"O7D2VYJYTIAU","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_16","alias_value":"O7D2VYJYTIAUBVYU","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_8","alias_value":"O7D2VYJY","created_at":"2026-05-18T12:25:47Z"}],"graph_snapshots":[{"event_id":"sha256:3af2d78c99b8545d855d99f1882997ca5053f93332f58db80da05b8d26d8df51","target":"graph","created_at":"2026-05-18T04:30:37Z","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":"The consequences of assuming the third-generation Yukawa couplings are all large and comparable are studied in the context of the minimal supersymmetric extension of the standard model. General aspects of the RG evolution of the parameters, theoretical constraints needed to ensure proper electroweak symmetry breaking, and experimental and cosmological bounds on low-energy parameters are presented. We also present complete and exact semi-analytic solutions to the 1-loop RG equations. Focusing on SU(5) or SO(10) unification, we analyze the relationship between the top and bottom masses and the s","authors_text":"R. Rattazzi (Rutgers), U. Sarid (Stanford)","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1995-06-01T06:22:17Z","title":"The Unified Minimal Supersymmetric Model with Large Yukawa Couplings"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9505428","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:d2b81ec0918d32b6ef86df19b4758d415f776a4a7b5646f546f92da6c0fa74ab","target":"record","created_at":"2026-05-18T04:30:37Z","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":"42423e963d3c854b9c82ab73240cf2cfa9b5981624974e391d64dd95ed291ba5","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1995-06-01T06:22:17Z","title_canon_sha256":"79556b7bd2338b92631bd94a7c46bb28e56f68af4408120fb7afb897adb548e9"},"schema_version":"1.0","source":{"id":"hep-ph/9505428","kind":"arxiv","version":1}},"canonical_sha256":"77c7aae1389a0140d714a2e2cb1a3b4d4364450dc2aa0c76da04665c2c68808e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"77c7aae1389a0140d714a2e2cb1a3b4d4364450dc2aa0c76da04665c2c68808e","first_computed_at":"2026-05-18T04:30:37.757071Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:30:37.757071Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"8ClbfxKkn1NubLVfM1ZDlLgGTY5uxUQ67qQBBSyh+bNY49rH03rdyTHML3VYK9ueIvGevuc4X5/9gZcHM++3Cg==","signature_status":"signed_v1","signed_at":"2026-05-18T04:30:37.757899Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9505428","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d2b81ec0918d32b6ef86df19b4758d415f776a4a7b5646f546f92da6c0fa74ab","sha256:3af2d78c99b8545d855d99f1882997ca5053f93332f58db80da05b8d26d8df51"],"state_sha256":"91d5c210f7870228b57d43507efce7f4be2533051c2ed3d4d0ed50d3553989bc"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XT57tm2okwxNfcw/c2C+dueP1NXxWLiL6wCHAfJD3U2Mau4uDz1o1ojKLhVyEeonuu5LogwqKqrTuthKV96dCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-30T22:42:52.975926Z","bundle_sha256":"49fc1beceaeb883b4ea93192c9b40f8d6764eb8ec37fa6ab800cee202442c4ef"}}