{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:DMR22TOO6JWJTSU6UJ7CXTWLKD","short_pith_number":"pith:DMR22TOO","schema_version":"1.0","canonical_sha256":"1b23ad4dcef26c99ca9ea27e2bcecb50d7e12dc07a2b0ffb95c524115df110d6","source":{"kind":"arxiv","id":"1206.5028","version":2},"attestation_state":"computed","paper":{"title":"Constrained Exceptional Supersymmetric Standard Model with a Higgs Near 125 GeV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"D. J. Miller, P. Athron, R. Nevzorov, S. F. King, S. Moretti","submitted_at":"2012-06-21T22:33:07Z","abstract_excerpt":"We study the parameter space of the constrained exceptional supersymmetric standard model (cE6SSM) consistent with a Higgs signal near 125 GeV and the LHC searches for squarks, gluinos and Z'. The cE6SSM parameter space consistent with correct electroweak symmetry breaking, is represented by scans in the (m0, M1/2) plane for fixed Z' mass and tan beta, with squark, gluino and Higgs masses plotted as contours in this plane. We find that a 125 GeV Higgs mass only arises for a sufficiently large Z' mass, mostly above current limits, and for particular regions of squark and gluino masses correspon"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1206.5028","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-06-21T22:33:07Z","cross_cats_sorted":[],"title_canon_sha256":"b3cb47a32797653b33acff884c4057a79addf49800c99ad7950fea543799990c","abstract_canon_sha256":"0461333d9071d09ba443e7542564aedf213ccbeb7fa34d312788c334185daaa0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:22:39.928839Z","signature_b64":"ZZdWWcljO1M7fdP0rVbmGuoWf2NBPdrfKpoblbFB5rqHQGHoBKTAhOaWVyqlSZ1eaBD5NDI6HXMxbiJJgKXMCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1b23ad4dcef26c99ca9ea27e2bcecb50d7e12dc07a2b0ffb95c524115df110d6","last_reissued_at":"2026-05-18T03:22:39.928085Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:22:39.928085Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Constrained Exceptional Supersymmetric Standard Model with a Higgs Near 125 GeV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"D. J. Miller, P. Athron, R. Nevzorov, S. F. King, S. Moretti","submitted_at":"2012-06-21T22:33:07Z","abstract_excerpt":"We study the parameter space of the constrained exceptional supersymmetric standard model (cE6SSM) consistent with a Higgs signal near 125 GeV and the LHC searches for squarks, gluinos and Z'. The cE6SSM parameter space consistent with correct electroweak symmetry breaking, is represented by scans in the (m0, M1/2) plane for fixed Z' mass and tan beta, with squark, gluino and Higgs masses plotted as contours in this plane. We find that a 125 GeV Higgs mass only arises for a sufficiently large Z' mass, mostly above current limits, and for particular regions of squark and gluino masses correspon"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1206.5028","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1206.5028","created_at":"2026-05-18T03:22:39.928211+00:00"},{"alias_kind":"arxiv_version","alias_value":"1206.5028v2","created_at":"2026-05-18T03:22:39.928211+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1206.5028","created_at":"2026-05-18T03:22:39.928211+00:00"},{"alias_kind":"pith_short_12","alias_value":"DMR22TOO6JWJ","created_at":"2026-05-18T12:27:04.183437+00:00"},{"alias_kind":"pith_short_16","alias_value":"DMR22TOO6JWJTSU6","created_at":"2026-05-18T12:27:04.183437+00:00"},{"alias_kind":"pith_short_8","alias_value":"DMR22TOO","created_at":"2026-05-18T12:27:04.183437+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/DMR22TOO6JWJTSU6UJ7CXTWLKD","json":"https://pith.science/pith/DMR22TOO6JWJTSU6UJ7CXTWLKD.json","graph_json":"https://pith.science/api/pith-number/DMR22TOO6JWJTSU6UJ7CXTWLKD/graph.json","events_json":"https://pith.science/api/pith-number/DMR22TOO6JWJTSU6UJ7CXTWLKD/events.json","paper":"https://pith.science/paper/DMR22TOO"},"agent_actions":{"view_html":"https://pith.science/pith/DMR22TOO6JWJTSU6UJ7CXTWLKD","download_json":"https://pith.science/pith/DMR22TOO6JWJTSU6UJ7CXTWLKD.json","view_paper":"https://pith.science/paper/DMR22TOO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1206.5028&json=true","fetch_graph":"https://pith.science/api/pith-number/DMR22TOO6JWJTSU6UJ7CXTWLKD/graph.json","fetch_events":"https://pith.science/api/pith-number/DMR22TOO6JWJTSU6UJ7CXTWLKD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DMR22TOO6JWJTSU6UJ7CXTWLKD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DMR22TOO6JWJTSU6UJ7CXTWLKD/action/storage_attestation","attest_author":"https://pith.science/pith/DMR22TOO6JWJTSU6UJ7CXTWLKD/action/author_attestation","sign_citation":"https://pith.science/pith/DMR22TOO6JWJTSU6UJ7CXTWLKD/action/citation_signature","submit_replication":"https://pith.science/pith/DMR22TOO6JWJTSU6UJ7CXTWLKD/action/replication_record"}},"created_at":"2026-05-18T03:22:39.928211+00:00","updated_at":"2026-05-18T03:22:39.928211+00:00"}