{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:7VNZG4HZTPSWFXJFNQ2PJEMVA6","short_pith_number":"pith:7VNZG4HZ","canonical_record":{"source":{"id":"1407.2814","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-10T14:50:02Z","cross_cats_sorted":[],"title_canon_sha256":"2596ea73ce3e78d414f220d74e4d93261fab91c75109f087ae946d380ced6188","abstract_canon_sha256":"5d7efb80b961f48eecf4ab0b95bdea0fad4ecd0c83433f12aa0505a6541f114c"},"schema_version":"1.0"},"canonical_sha256":"fd5b9370f99be562dd256c34f4919507a90c76046fbd96c608259a1ebc9e4faa","source":{"kind":"arxiv","id":"1407.2814","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.2814","created_at":"2026-05-18T01:32:34Z"},{"alias_kind":"arxiv_version","alias_value":"1407.2814v4","created_at":"2026-05-18T01:32:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.2814","created_at":"2026-05-18T01:32:34Z"},{"alias_kind":"pith_short_12","alias_value":"7VNZG4HZTPSW","created_at":"2026-05-18T12:28:19Z"},{"alias_kind":"pith_short_16","alias_value":"7VNZG4HZTPSWFXJF","created_at":"2026-05-18T12:28:19Z"},{"alias_kind":"pith_short_8","alias_value":"7VNZG4HZ","created_at":"2026-05-18T12:28:19Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:7VNZG4HZTPSWFXJFNQ2PJEMVA6","target":"record","payload":{"canonical_record":{"source":{"id":"1407.2814","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-10T14:50:02Z","cross_cats_sorted":[],"title_canon_sha256":"2596ea73ce3e78d414f220d74e4d93261fab91c75109f087ae946d380ced6188","abstract_canon_sha256":"5d7efb80b961f48eecf4ab0b95bdea0fad4ecd0c83433f12aa0505a6541f114c"},"schema_version":"1.0"},"canonical_sha256":"fd5b9370f99be562dd256c34f4919507a90c76046fbd96c608259a1ebc9e4faa","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:32:34.760386Z","signature_b64":"Ffwz+imMRTggwus9t1FX45bc51ZOrLApRZ8G0ORxRnL95GUB8mLHF+kr8B0hff3CsuRVesFS9Tb0CgfbXsTxBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fd5b9370f99be562dd256c34f4919507a90c76046fbd96c608259a1ebc9e4faa","last_reissued_at":"2026-05-18T01:32:34.759746Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:32:34.759746Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1407.2814","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:32:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"huiaJOM2OM4atKCy5HnvjefoWJKTMplL8Eoe+UUb+R38ICDDCzVrb98pWEm5csiGFcf/vayh87CVw0VrpOuZBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T20:12:44.475506Z"},"content_sha256":"bde408ef34cd96b2c3b590ce8216d81e6def000aedaa058f2be62e0a4f0ff4d2","schema_version":"1.0","event_id":"sha256:bde408ef34cd96b2c3b590ce8216d81e6def000aedaa058f2be62e0a4f0ff4d2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:7VNZG4HZTPSWFXJFNQ2PJEMVA6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Vacuum stability of the effective Higgs potential in the Minimal Supersymmetric Standard Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Guillaume Chalons, Markus Bobrowski, Ulrich Nierste, Wolfgang G. Hollik","submitted_at":"2014-07-10T14:50:02Z","abstract_excerpt":"The parameters of the Higgs potential of the Minimal Supersymmetric Standard Model (MSSM) receive large radiative corrections which lift the mass of the lightest Higgs boson to the measured value of 126 GeV. Depending on the MSSM parameters, these radiative corrections may also lead to the situation that the local minimum corresponding to the electroweak vacuum state is not the global minimum of the Higgs potential. We analyze the stability of the vacuum for the case of heavy squark masses as favored by current LHC data. To this end we first consider an effective Lagrangian obtained by integra"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.2814","kind":"arxiv","version":4},"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":"2026-05-18T01:32:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oSXP+kGghkXD988iGdEILEUL5Daf7yg4yxWDD7brXKLN7PQgCWWRYz85/q16xkpe8/Kh/X3Yj7Du27F5e02CBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T20:12:44.475859Z"},"content_sha256":"93c18423fb71e26f863bd2c0bea81fdf04ec526ca07cacd0a8eef8aa7b2d6f3f","schema_version":"1.0","event_id":"sha256:93c18423fb71e26f863bd2c0bea81fdf04ec526ca07cacd0a8eef8aa7b2d6f3f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7VNZG4HZTPSWFXJFNQ2PJEMVA6/bundle.json","state_url":"https://pith.science/pith/7VNZG4HZTPSWFXJFNQ2PJEMVA6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7VNZG4HZTPSWFXJFNQ2PJEMVA6/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":"2026-05-28T20:12:44Z","links":{"resolver":"https://pith.science/pith/7VNZG4HZTPSWFXJFNQ2PJEMVA6","bundle":"https://pith.science/pith/7VNZG4HZTPSWFXJFNQ2PJEMVA6/bundle.json","state":"https://pith.science/pith/7VNZG4HZTPSWFXJFNQ2PJEMVA6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7VNZG4HZTPSWFXJFNQ2PJEMVA6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:7VNZG4HZTPSWFXJFNQ2PJEMVA6","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":"5d7efb80b961f48eecf4ab0b95bdea0fad4ecd0c83433f12aa0505a6541f114c","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-10T14:50:02Z","title_canon_sha256":"2596ea73ce3e78d414f220d74e4d93261fab91c75109f087ae946d380ced6188"},"schema_version":"1.0","source":{"id":"1407.2814","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.2814","created_at":"2026-05-18T01:32:34Z"},{"alias_kind":"arxiv_version","alias_value":"1407.2814v4","created_at":"2026-05-18T01:32:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.2814","created_at":"2026-05-18T01:32:34Z"},{"alias_kind":"pith_short_12","alias_value":"7VNZG4HZTPSW","created_at":"2026-05-18T12:28:19Z"},{"alias_kind":"pith_short_16","alias_value":"7VNZG4HZTPSWFXJF","created_at":"2026-05-18T12:28:19Z"},{"alias_kind":"pith_short_8","alias_value":"7VNZG4HZ","created_at":"2026-05-18T12:28:19Z"}],"graph_snapshots":[{"event_id":"sha256:93c18423fb71e26f863bd2c0bea81fdf04ec526ca07cacd0a8eef8aa7b2d6f3f","target":"graph","created_at":"2026-05-18T01:32:34Z","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 parameters of the Higgs potential of the Minimal Supersymmetric Standard Model (MSSM) receive large radiative corrections which lift the mass of the lightest Higgs boson to the measured value of 126 GeV. Depending on the MSSM parameters, these radiative corrections may also lead to the situation that the local minimum corresponding to the electroweak vacuum state is not the global minimum of the Higgs potential. We analyze the stability of the vacuum for the case of heavy squark masses as favored by current LHC data. To this end we first consider an effective Lagrangian obtained by integra","authors_text":"Guillaume Chalons, Markus Bobrowski, Ulrich Nierste, Wolfgang G. Hollik","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-10T14:50:02Z","title":"Vacuum stability of the effective Higgs potential in the Minimal Supersymmetric Standard Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.2814","kind":"arxiv","version":4},"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:bde408ef34cd96b2c3b590ce8216d81e6def000aedaa058f2be62e0a4f0ff4d2","target":"record","created_at":"2026-05-18T01:32:34Z","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":"5d7efb80b961f48eecf4ab0b95bdea0fad4ecd0c83433f12aa0505a6541f114c","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-10T14:50:02Z","title_canon_sha256":"2596ea73ce3e78d414f220d74e4d93261fab91c75109f087ae946d380ced6188"},"schema_version":"1.0","source":{"id":"1407.2814","kind":"arxiv","version":4}},"canonical_sha256":"fd5b9370f99be562dd256c34f4919507a90c76046fbd96c608259a1ebc9e4faa","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"fd5b9370f99be562dd256c34f4919507a90c76046fbd96c608259a1ebc9e4faa","first_computed_at":"2026-05-18T01:32:34.759746Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:32:34.759746Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Ffwz+imMRTggwus9t1FX45bc51ZOrLApRZ8G0ORxRnL95GUB8mLHF+kr8B0hff3CsuRVesFS9Tb0CgfbXsTxBg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:32:34.760386Z","signed_message":"canonical_sha256_bytes"},"source_id":"1407.2814","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:bde408ef34cd96b2c3b590ce8216d81e6def000aedaa058f2be62e0a4f0ff4d2","sha256:93c18423fb71e26f863bd2c0bea81fdf04ec526ca07cacd0a8eef8aa7b2d6f3f"],"state_sha256":"0e2417205069590084cabcadb412cebc73ea436fd304fbb410fcddd933041101"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/q8nQL8Zm1doxnTewrtL/qsHsocqNvXgTWAWAl8sVe2W+aAhtkpIzpBOe9Y1lbQGjHlYmphCiDREu4pXqVh+Dw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T20:12:44.477808Z","bundle_sha256":"cd42d9c423b6044cf57bc1ab160cca089011968084aeb502621cb3e1587d4711"}}