{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:PTGRBYKBAGNVIG6MHJFMKFNS7G","short_pith_number":"pith:PTGRBYKB","schema_version":"1.0","canonical_sha256":"7ccd10e141019b541bcc3a4ac515b2f9a63017ecea3f7aa1ae6f0bb08db75707","source":{"kind":"arxiv","id":"1512.04281","version":2},"attestation_state":"computed","paper":{"title":"Discovery Prospects of a Light Scalar in the NMSSM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Matias Rodriguez-Vazquez, Ulrich Ellwanger","submitted_at":"2015-12-14T12:37:52Z","abstract_excerpt":"We study a region in the NMSSM parameter space in which the mass of the SM-like Higgs boson is uplifted by ~4-17 GeV, allowing for stop masses and |A_t| <= 1 TeV alleviating the little fine tuning problem of the MSSM. An uplift of the mass of the SM-like Higgs boson is possible in two distinct regions in the NMSSM parameter space: Either for large lambda and small tan(beta) or, through singlet-doublet mixing, for small lambda and large tan(beta). For a mostly singlet-like Higgs state H_S with a mass below 125 GeV we investigate possible direct or indirect search channels at the run II of the L"},"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":"1512.04281","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-12-14T12:37:52Z","cross_cats_sorted":[],"title_canon_sha256":"21db941343575cbfc3d24edb494d35c8fb3369fc7f2355c8475a5eb13285f23e","abstract_canon_sha256":"5b485897be0a8edd3c1e54c6a80737837db6b4c3212c5d1253662bf9206689ba"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:18:39.110874Z","signature_b64":"4ugW9lHg/9opc2E3Ht51VWqzU2voNiFMNEew8roICP+rlyk1Bo9O8PXzTXmYt+ASGZ8aWD76wpA/zB8WgduXAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7ccd10e141019b541bcc3a4ac515b2f9a63017ecea3f7aa1ae6f0bb08db75707","last_reissued_at":"2026-05-18T01:18:39.110326Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:18:39.110326Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Discovery Prospects of a Light Scalar in the NMSSM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Matias Rodriguez-Vazquez, Ulrich Ellwanger","submitted_at":"2015-12-14T12:37:52Z","abstract_excerpt":"We study a region in the NMSSM parameter space in which the mass of the SM-like Higgs boson is uplifted by ~4-17 GeV, allowing for stop masses and |A_t| <= 1 TeV alleviating the little fine tuning problem of the MSSM. An uplift of the mass of the SM-like Higgs boson is possible in two distinct regions in the NMSSM parameter space: Either for large lambda and small tan(beta) or, through singlet-doublet mixing, for small lambda and large tan(beta). For a mostly singlet-like Higgs state H_S with a mass below 125 GeV we investigate possible direct or indirect search channels at the run II of the L"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.04281","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":"1512.04281","created_at":"2026-05-18T01:18:39.110412+00:00"},{"alias_kind":"arxiv_version","alias_value":"1512.04281v2","created_at":"2026-05-18T01:18:39.110412+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.04281","created_at":"2026-05-18T01:18:39.110412+00:00"},{"alias_kind":"pith_short_12","alias_value":"PTGRBYKBAGNV","created_at":"2026-05-18T12:29:37.295048+00:00"},{"alias_kind":"pith_short_16","alias_value":"PTGRBYKBAGNVIG6M","created_at":"2026-05-18T12:29:37.295048+00:00"},{"alias_kind":"pith_short_8","alias_value":"PTGRBYKB","created_at":"2026-05-18T12:29:37.295048+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/PTGRBYKBAGNVIG6MHJFMKFNS7G","json":"https://pith.science/pith/PTGRBYKBAGNVIG6MHJFMKFNS7G.json","graph_json":"https://pith.science/api/pith-number/PTGRBYKBAGNVIG6MHJFMKFNS7G/graph.json","events_json":"https://pith.science/api/pith-number/PTGRBYKBAGNVIG6MHJFMKFNS7G/events.json","paper":"https://pith.science/paper/PTGRBYKB"},"agent_actions":{"view_html":"https://pith.science/pith/PTGRBYKBAGNVIG6MHJFMKFNS7G","download_json":"https://pith.science/pith/PTGRBYKBAGNVIG6MHJFMKFNS7G.json","view_paper":"https://pith.science/paper/PTGRBYKB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1512.04281&json=true","fetch_graph":"https://pith.science/api/pith-number/PTGRBYKBAGNVIG6MHJFMKFNS7G/graph.json","fetch_events":"https://pith.science/api/pith-number/PTGRBYKBAGNVIG6MHJFMKFNS7G/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PTGRBYKBAGNVIG6MHJFMKFNS7G/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PTGRBYKBAGNVIG6MHJFMKFNS7G/action/storage_attestation","attest_author":"https://pith.science/pith/PTGRBYKBAGNVIG6MHJFMKFNS7G/action/author_attestation","sign_citation":"https://pith.science/pith/PTGRBYKBAGNVIG6MHJFMKFNS7G/action/citation_signature","submit_replication":"https://pith.science/pith/PTGRBYKBAGNVIG6MHJFMKFNS7G/action/replication_record"}},"created_at":"2026-05-18T01:18:39.110412+00:00","updated_at":"2026-05-18T01:18:39.110412+00:00"}