{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:JB5RHSCDB4H2DARHB5ZWRIU6JG","short_pith_number":"pith:JB5RHSCD","canonical_record":{"source":{"id":"1105.0039","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-04-30T01:18:07Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"b355b57ccdbe365e1c507c96db76136f0e060b2ac014b9cc44fd0dad2f800a3b","abstract_canon_sha256":"395ae368c1795097d7813eb93c5d5743a398b7d7ae8a9cc36ca7ac54255ad6fd"},"schema_version":"1.0"},"canonical_sha256":"487b13c8430f0fa182270f7368a29e4984726c29835cd0e387fad6b2a4e9cc25","source":{"kind":"arxiv","id":"1105.0039","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1105.0039","created_at":"2026-05-18T03:23:34Z"},{"alias_kind":"arxiv_version","alias_value":"1105.0039v2","created_at":"2026-05-18T03:23:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.0039","created_at":"2026-05-18T03:23:34Z"},{"alias_kind":"pith_short_12","alias_value":"JB5RHSCDB4H2","created_at":"2026-05-18T12:26:32Z"},{"alias_kind":"pith_short_16","alias_value":"JB5RHSCDB4H2DARH","created_at":"2026-05-18T12:26:32Z"},{"alias_kind":"pith_short_8","alias_value":"JB5RHSCD","created_at":"2026-05-18T12:26:32Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:JB5RHSCDB4H2DARHB5ZWRIU6JG","target":"record","payload":{"canonical_record":{"source":{"id":"1105.0039","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-04-30T01:18:07Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"b355b57ccdbe365e1c507c96db76136f0e060b2ac014b9cc44fd0dad2f800a3b","abstract_canon_sha256":"395ae368c1795097d7813eb93c5d5743a398b7d7ae8a9cc36ca7ac54255ad6fd"},"schema_version":"1.0"},"canonical_sha256":"487b13c8430f0fa182270f7368a29e4984726c29835cd0e387fad6b2a4e9cc25","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:23:34.480506Z","signature_b64":"XWIzzDnt8f0vyXqOHMuKKWD7hZLF9sxxMW/sPu/lWoHcjCgiq2/p4sgq8Fvmk3b17gUid8k7n8ltI2qUAjj+Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"487b13c8430f0fa182270f7368a29e4984726c29835cd0e387fad6b2a4e9cc25","last_reissued_at":"2026-05-18T03:23:34.479771Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:23:34.479771Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1105.0039","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":"2026-05-18T03:23:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hqeuULX4NLRQsMkEGI+e7hwgOwKvMfp6wv6dxeWNN3kpzp11BVt7IOaDEPg2YFUDo+EI2BkSvALgKaUCFkZmBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T03:32:58.776637Z"},"content_sha256":"9846e3e9dda87d8c67c54785829af1b3284e405c8939c5bf1305c1a77647afbd","schema_version":"1.0","event_id":"sha256:9846e3e9dda87d8c67c54785829af1b3284e405c8939c5bf1305c1a77647afbd"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:JB5RHSCDB4H2DARHB5ZWRIU6JG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Higgs Properties in the Fourth Generation MSSM: Boosted Signals Over the 3G Plan","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"A. Ismail, J.L. Hewett, M.-P.Le, R.C. Cotta, T.G. Rizzo","submitted_at":"2011-04-30T01:18:07Z","abstract_excerpt":"The generalization of the MSSM to the case of four chiral fermion generations (4GMSSM) can lead to significant changes in the phenomenology of the otherwise familiar Higgs sector. In most of the 3GMSSM parameter space, the lighter CP-even $h$ is $\\sim 115-125$ GeV and mostly Standard Model-like while $H,A,H^\\pm$ are all relatively heavy. Furthermore, the ratio of Higgs vevs, $\\tan \\beta$, is relatively unconstrained. In contrast to this, in the 4GMSSM, heavy fourth generation fermion loops drive the masses of $h,H,H^\\pm$ to large values while the CP-odd boson, $A$, can remain relatively light "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.0039","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":"2026-05-18T03:23:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"MMyKd6i9DiaLFVfYrPXehdpEXPoOtHHQpcdJu4/DKlCluOEIUo5ObCX3Kb2Q+2L49oisXrrXZmjcWnT/5ZoECg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T03:32:58.777366Z"},"content_sha256":"23b286307408bd29803700c4263b78ed73910a82fa9c5dec4f1a257af795043c","schema_version":"1.0","event_id":"sha256:23b286307408bd29803700c4263b78ed73910a82fa9c5dec4f1a257af795043c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JB5RHSCDB4H2DARHB5ZWRIU6JG/bundle.json","state_url":"https://pith.science/pith/JB5RHSCDB4H2DARHB5ZWRIU6JG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JB5RHSCDB4H2DARHB5ZWRIU6JG/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":"2026-05-26T03:32:58Z","links":{"resolver":"https://pith.science/pith/JB5RHSCDB4H2DARHB5ZWRIU6JG","bundle":"https://pith.science/pith/JB5RHSCDB4H2DARHB5ZWRIU6JG/bundle.json","state":"https://pith.science/pith/JB5RHSCDB4H2DARHB5ZWRIU6JG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JB5RHSCDB4H2DARHB5ZWRIU6JG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:JB5RHSCDB4H2DARHB5ZWRIU6JG","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":"395ae368c1795097d7813eb93c5d5743a398b7d7ae8a9cc36ca7ac54255ad6fd","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-04-30T01:18:07Z","title_canon_sha256":"b355b57ccdbe365e1c507c96db76136f0e060b2ac014b9cc44fd0dad2f800a3b"},"schema_version":"1.0","source":{"id":"1105.0039","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1105.0039","created_at":"2026-05-18T03:23:34Z"},{"alias_kind":"arxiv_version","alias_value":"1105.0039v2","created_at":"2026-05-18T03:23:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.0039","created_at":"2026-05-18T03:23:34Z"},{"alias_kind":"pith_short_12","alias_value":"JB5RHSCDB4H2","created_at":"2026-05-18T12:26:32Z"},{"alias_kind":"pith_short_16","alias_value":"JB5RHSCDB4H2DARH","created_at":"2026-05-18T12:26:32Z"},{"alias_kind":"pith_short_8","alias_value":"JB5RHSCD","created_at":"2026-05-18T12:26:32Z"}],"graph_snapshots":[{"event_id":"sha256:23b286307408bd29803700c4263b78ed73910a82fa9c5dec4f1a257af795043c","target":"graph","created_at":"2026-05-18T03:23:34Z","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 generalization of the MSSM to the case of four chiral fermion generations (4GMSSM) can lead to significant changes in the phenomenology of the otherwise familiar Higgs sector. In most of the 3GMSSM parameter space, the lighter CP-even $h$ is $\\sim 115-125$ GeV and mostly Standard Model-like while $H,A,H^\\pm$ are all relatively heavy. Furthermore, the ratio of Higgs vevs, $\\tan \\beta$, is relatively unconstrained. In contrast to this, in the 4GMSSM, heavy fourth generation fermion loops drive the masses of $h,H,H^\\pm$ to large values while the CP-odd boson, $A$, can remain relatively light ","authors_text":"A. Ismail, J.L. Hewett, M.-P.Le, R.C. Cotta, T.G. Rizzo","cross_cats":["hep-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-04-30T01:18:07Z","title":"Higgs Properties in the Fourth Generation MSSM: Boosted Signals Over the 3G Plan"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.0039","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":"sha256:9846e3e9dda87d8c67c54785829af1b3284e405c8939c5bf1305c1a77647afbd","target":"record","created_at":"2026-05-18T03:23:34Z","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":"395ae368c1795097d7813eb93c5d5743a398b7d7ae8a9cc36ca7ac54255ad6fd","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-04-30T01:18:07Z","title_canon_sha256":"b355b57ccdbe365e1c507c96db76136f0e060b2ac014b9cc44fd0dad2f800a3b"},"schema_version":"1.0","source":{"id":"1105.0039","kind":"arxiv","version":2}},"canonical_sha256":"487b13c8430f0fa182270f7368a29e4984726c29835cd0e387fad6b2a4e9cc25","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"487b13c8430f0fa182270f7368a29e4984726c29835cd0e387fad6b2a4e9cc25","first_computed_at":"2026-05-18T03:23:34.479771Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:23:34.479771Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"XWIzzDnt8f0vyXqOHMuKKWD7hZLF9sxxMW/sPu/lWoHcjCgiq2/p4sgq8Fvmk3b17gUid8k7n8ltI2qUAjj+Ag==","signature_status":"signed_v1","signed_at":"2026-05-18T03:23:34.480506Z","signed_message":"canonical_sha256_bytes"},"source_id":"1105.0039","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9846e3e9dda87d8c67c54785829af1b3284e405c8939c5bf1305c1a77647afbd","sha256:23b286307408bd29803700c4263b78ed73910a82fa9c5dec4f1a257af795043c"],"state_sha256":"c9a04eeed9d187a15ee9b2ddf02afc30ee05e2bd2b4817593539a5e811e6a8dd"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HE9vfbFRI67WF0WmMRkymZgYyKAlB8P1zXWzM9Effz/AEuIV+Byf9o/xIcMWTKCxuUGSNV2VIl5Mpj0+hBX1AA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T03:32:58.781087Z","bundle_sha256":"97bf03ffdc9382ff82be6b1926471df705c47133ad157d6823ebf9c79490ca1d"}}