{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:GM73GPXRE5DHBMWXG2U4DZUKDC","short_pith_number":"pith:GM73GPXR","canonical_record":{"source":{"id":"1210.4936","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-10-17T20:01:35Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"4decccc3bdf0dee0410ade0db947c4d70f84595361879886f01b8883229f3bf0","abstract_canon_sha256":"d1144b297494c7c0524b2260c958592b2a92d06239c03efd7112e17a101395a3"},"schema_version":"1.0"},"canonical_sha256":"333fb33ef1274670b2d736a9c1e68a18950a84d4fe311532c785997212fa66f3","source":{"kind":"arxiv","id":"1210.4936","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1210.4936","created_at":"2026-05-18T03:09:59Z"},{"alias_kind":"arxiv_version","alias_value":"1210.4936v2","created_at":"2026-05-18T03:09:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.4936","created_at":"2026-05-18T03:09:59Z"},{"alias_kind":"pith_short_12","alias_value":"GM73GPXRE5DH","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_16","alias_value":"GM73GPXRE5DHBMWX","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_8","alias_value":"GM73GPXR","created_at":"2026-05-18T12:27:06Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:GM73GPXRE5DHBMWXG2U4DZUKDC","target":"record","payload":{"canonical_record":{"source":{"id":"1210.4936","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-10-17T20:01:35Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"4decccc3bdf0dee0410ade0db947c4d70f84595361879886f01b8883229f3bf0","abstract_canon_sha256":"d1144b297494c7c0524b2260c958592b2a92d06239c03efd7112e17a101395a3"},"schema_version":"1.0"},"canonical_sha256":"333fb33ef1274670b2d736a9c1e68a18950a84d4fe311532c785997212fa66f3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:09:59.791065Z","signature_b64":"gc6bPavvuo+rWQi3I+YO6vlOstP45oMFCvzSuquzd3NCwT5SGGV6sArVZVUr1UL9d5BBPSo/uWrZR6WLeM92Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"333fb33ef1274670b2d736a9c1e68a18950a84d4fe311532c785997212fa66f3","last_reissued_at":"2026-05-18T03:09:59.790641Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:09:59.790641Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1210.4936","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":"2026-05-18T03:09:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qxpcX3kniyk/1hBRrMYpjlWjhJaK1JN7+z3dn3+wzANsYkMwOtoqI1wbvEw3F7BmIygepDa5+uN4QJSxzXB9BQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T19:28:47.514355Z"},"content_sha256":"e96799a8b0383d40cf9c5bafcca2f40d8a2871dd9f2b9fa850438ee8d8dd654e","schema_version":"1.0","event_id":"sha256:e96799a8b0383d40cf9c5bafcca2f40d8a2871dd9f2b9fa850438ee8d8dd654e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:GM73GPXRE5DHBMWXG2U4DZUKDC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"R-symmetric High Scale Supersymmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"James Unwin","submitted_at":"2012-10-17T20:01:35Z","abstract_excerpt":"Introducing an R-symmetry to models of high scale supersymmetry (SUSY) can have interesting consequences, and we focus on two aspects. If Majorana masses are forbidden by an R-symmetry and the main source of electroweak gaugino masses are Dirac terms, then the Higgs quartic coupling vanishing at the SUSY scale and the Higgs boson mass will be near 125 GeV. Moreover, using an R-symmetry, models with only one Higgs doublet in the UV can be constructed and we argue that, since we desire only a single Higgs at the weak scale, this scenario is more aesthetic than existing models. We subsequently pr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.4936","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":"2026-05-18T03:09:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fBbyo0C3Lcc94rshlvncKb+/5RYlyDyzSUW7mhYuLNZQtTbvALuJun8b/kBSWGPimPM1V9ZBwhUsn4RKfw/8Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T19:28:47.514806Z"},"content_sha256":"ede34bc0ad7269c3151f75a15a408acb603e78e809c1495d0e28e296c7b5866a","schema_version":"1.0","event_id":"sha256:ede34bc0ad7269c3151f75a15a408acb603e78e809c1495d0e28e296c7b5866a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GM73GPXRE5DHBMWXG2U4DZUKDC/bundle.json","state_url":"https://pith.science/pith/GM73GPXRE5DHBMWXG2U4DZUKDC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GM73GPXRE5DHBMWXG2U4DZUKDC/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":"2026-08-03T19:28:47Z","links":{"resolver":"https://pith.science/pith/GM73GPXRE5DHBMWXG2U4DZUKDC","bundle":"https://pith.science/pith/GM73GPXRE5DHBMWXG2U4DZUKDC/bundle.json","state":"https://pith.science/pith/GM73GPXRE5DHBMWXG2U4DZUKDC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GM73GPXRE5DHBMWXG2U4DZUKDC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:GM73GPXRE5DHBMWXG2U4DZUKDC","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":"d1144b297494c7c0524b2260c958592b2a92d06239c03efd7112e17a101395a3","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-10-17T20:01:35Z","title_canon_sha256":"4decccc3bdf0dee0410ade0db947c4d70f84595361879886f01b8883229f3bf0"},"schema_version":"1.0","source":{"id":"1210.4936","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1210.4936","created_at":"2026-05-18T03:09:59Z"},{"alias_kind":"arxiv_version","alias_value":"1210.4936v2","created_at":"2026-05-18T03:09:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.4936","created_at":"2026-05-18T03:09:59Z"},{"alias_kind":"pith_short_12","alias_value":"GM73GPXRE5DH","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_16","alias_value":"GM73GPXRE5DHBMWX","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_8","alias_value":"GM73GPXR","created_at":"2026-05-18T12:27:06Z"}],"graph_snapshots":[{"event_id":"sha256:ede34bc0ad7269c3151f75a15a408acb603e78e809c1495d0e28e296c7b5866a","target":"graph","created_at":"2026-05-18T03:09:59Z","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":"Introducing an R-symmetry to models of high scale supersymmetry (SUSY) can have interesting consequences, and we focus on two aspects. If Majorana masses are forbidden by an R-symmetry and the main source of electroweak gaugino masses are Dirac terms, then the Higgs quartic coupling vanishing at the SUSY scale and the Higgs boson mass will be near 125 GeV. Moreover, using an R-symmetry, models with only one Higgs doublet in the UV can be constructed and we argue that, since we desire only a single Higgs at the weak scale, this scenario is more aesthetic than existing models. We subsequently pr","authors_text":"James Unwin","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-10-17T20:01:35Z","title":"R-symmetric High Scale Supersymmetry"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.4936","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:e96799a8b0383d40cf9c5bafcca2f40d8a2871dd9f2b9fa850438ee8d8dd654e","target":"record","created_at":"2026-05-18T03:09:59Z","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":"d1144b297494c7c0524b2260c958592b2a92d06239c03efd7112e17a101395a3","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-10-17T20:01:35Z","title_canon_sha256":"4decccc3bdf0dee0410ade0db947c4d70f84595361879886f01b8883229f3bf0"},"schema_version":"1.0","source":{"id":"1210.4936","kind":"arxiv","version":2}},"canonical_sha256":"333fb33ef1274670b2d736a9c1e68a18950a84d4fe311532c785997212fa66f3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"333fb33ef1274670b2d736a9c1e68a18950a84d4fe311532c785997212fa66f3","first_computed_at":"2026-05-18T03:09:59.790641Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:09:59.790641Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"gc6bPavvuo+rWQi3I+YO6vlOstP45oMFCvzSuquzd3NCwT5SGGV6sArVZVUr1UL9d5BBPSo/uWrZR6WLeM92Cg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:09:59.791065Z","signed_message":"canonical_sha256_bytes"},"source_id":"1210.4936","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e96799a8b0383d40cf9c5bafcca2f40d8a2871dd9f2b9fa850438ee8d8dd654e","sha256:ede34bc0ad7269c3151f75a15a408acb603e78e809c1495d0e28e296c7b5866a"],"state_sha256":"885ddff8a9694b0c0f8c852c14e069d40fceb88c90ad7edc9e7e3de92f5a7e49"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bX9+0S7NQOPkedAUN0oDJTHLJgatI1d4f34GsaA5xXZYbAOMdIo0w7tERXFBgwwnSMZFEIAw8Fju4bT05Y9kCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-03T19:28:47.519170Z","bundle_sha256":"943f4b6c01669cfb37e02c47307c732be9718baa912481ff994e5a8031083a8d"}}