{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:VPU3MCAZWE4OIVJOKNBFO6F7FW","short_pith_number":"pith:VPU3MCAZ","schema_version":"1.0","canonical_sha256":"abe9b60819b138e4552e53425778bf2dacd80ea4db977c757f7c2d91c593ff7f","source":{"kind":"arxiv","id":"1312.5233","version":1},"attestation_state":"computed","paper":{"title":"Implications of Improved Higgs Mass Calculations for Supersymmetric Models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"G. Weiglein, H. Rzehak, J. Ellis, J. Marrouche, K. A. Olive, K. de Vries, M.J. Dolan, O. Buchmueller, S. Heinemeyer, T. Hahn, W. Hollik","submitted_at":"2013-12-18T17:31:50Z","abstract_excerpt":"We discuss the allowed parameter spaces of supersymmetric scenarios in light of improved Higgs mass predictions provided by FeynHiggs 2.10.0. The Higgs mass predictions combine Feynman-diagrammatic results with a resummation of leading and subleading logarithmic corrections from the stop/top sector, which yield a significant improvement in the region of large stop masses. Scans in the pMSSM parameter space show that, for given values of the soft supersymmetry-breaking parameters, the new logarithmic contributions beyond the two-loop order implemented in FeynHiggs tend to give larger values of "},"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":"1312.5233","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-12-18T17:31:50Z","cross_cats_sorted":[],"title_canon_sha256":"14a2c540f2008ac12bbf09c66e37993770169b407230ca66092352adbafbe828","abstract_canon_sha256":"007760d37c2c07ea86c09d69096de4e16d063d9115e601614a3cfabe8ad4000b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:45:44.539788Z","signature_b64":"XldA+JlmEzyYicIa+LHfxBb2eYBJYBIa7EETEvf9XlU5Vih2oOxjhWvYFYBFJEV00AoMdUteUgizpHPFf3eGCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"abe9b60819b138e4552e53425778bf2dacd80ea4db977c757f7c2d91c593ff7f","last_reissued_at":"2026-05-18T01:45:44.539243Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:45:44.539243Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Implications of Improved Higgs Mass Calculations for Supersymmetric Models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"G. Weiglein, H. Rzehak, J. Ellis, J. Marrouche, K. A. Olive, K. de Vries, M.J. Dolan, O. Buchmueller, S. Heinemeyer, T. Hahn, W. Hollik","submitted_at":"2013-12-18T17:31:50Z","abstract_excerpt":"We discuss the allowed parameter spaces of supersymmetric scenarios in light of improved Higgs mass predictions provided by FeynHiggs 2.10.0. The Higgs mass predictions combine Feynman-diagrammatic results with a resummation of leading and subleading logarithmic corrections from the stop/top sector, which yield a significant improvement in the region of large stop masses. Scans in the pMSSM parameter space show that, for given values of the soft supersymmetry-breaking parameters, the new logarithmic contributions beyond the two-loop order implemented in FeynHiggs tend to give larger values of "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.5233","kind":"arxiv","version":1},"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":"1312.5233","created_at":"2026-05-18T01:45:44.539328+00:00"},{"alias_kind":"arxiv_version","alias_value":"1312.5233v1","created_at":"2026-05-18T01:45:44.539328+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.5233","created_at":"2026-05-18T01:45:44.539328+00:00"},{"alias_kind":"pith_short_12","alias_value":"VPU3MCAZWE4O","created_at":"2026-05-18T12:28:04.890932+00:00"},{"alias_kind":"pith_short_16","alias_value":"VPU3MCAZWE4OIVJO","created_at":"2026-05-18T12:28:04.890932+00:00"},{"alias_kind":"pith_short_8","alias_value":"VPU3MCAZ","created_at":"2026-05-18T12:28:04.890932+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/VPU3MCAZWE4OIVJOKNBFO6F7FW","json":"https://pith.science/pith/VPU3MCAZWE4OIVJOKNBFO6F7FW.json","graph_json":"https://pith.science/api/pith-number/VPU3MCAZWE4OIVJOKNBFO6F7FW/graph.json","events_json":"https://pith.science/api/pith-number/VPU3MCAZWE4OIVJOKNBFO6F7FW/events.json","paper":"https://pith.science/paper/VPU3MCAZ"},"agent_actions":{"view_html":"https://pith.science/pith/VPU3MCAZWE4OIVJOKNBFO6F7FW","download_json":"https://pith.science/pith/VPU3MCAZWE4OIVJOKNBFO6F7FW.json","view_paper":"https://pith.science/paper/VPU3MCAZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1312.5233&json=true","fetch_graph":"https://pith.science/api/pith-number/VPU3MCAZWE4OIVJOKNBFO6F7FW/graph.json","fetch_events":"https://pith.science/api/pith-number/VPU3MCAZWE4OIVJOKNBFO6F7FW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VPU3MCAZWE4OIVJOKNBFO6F7FW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VPU3MCAZWE4OIVJOKNBFO6F7FW/action/storage_attestation","attest_author":"https://pith.science/pith/VPU3MCAZWE4OIVJOKNBFO6F7FW/action/author_attestation","sign_citation":"https://pith.science/pith/VPU3MCAZWE4OIVJOKNBFO6F7FW/action/citation_signature","submit_replication":"https://pith.science/pith/VPU3MCAZWE4OIVJOKNBFO6F7FW/action/replication_record"}},"created_at":"2026-05-18T01:45:44.539328+00:00","updated_at":"2026-05-18T01:45:44.539328+00:00"}