{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:EY4SZVWZGSC6RP4XWNLMGC2ES6","short_pith_number":"pith:EY4SZVWZ","schema_version":"1.0","canonical_sha256":"26392cd6d93485e8bf97b356c30b449797a8a0aaa0fb74b6cb65fd0ac5984b91","source":{"kind":"arxiv","id":"1503.08216","version":2},"attestation_state":"computed","paper":{"title":"Global fits of the two-loop renormalized Two-Higgs-Doublet model with soft $Z_2$ breaking","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Debtosh Chowdhury, Otto Eberhardt","submitted_at":"2015-03-27T20:00:53Z","abstract_excerpt":"We determine the next-to-leading order renormalization group equations for the Two-Higgs-Doublet model with a softly broken $Z_2$ symmetry and CP conservation in the scalar potential. We use them to identify the parameter regions which are stable up to the Planck scale and find that in this case the quartic couplings of the Higgs potential cannot be larger than 1 in magnitude and that the absolute values of the S-matrix eigenvalues cannot exceed 2.5 at the electroweak symmetry breaking scale. Interpreting the 125 GeV resonance as the light CP-even Higgs eigenstate, we combine stability constra"},"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":"1503.08216","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-03-27T20:00:53Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"f536a7532ffa9f2ccafc4101d2bb51b5d926256d8e2d7a1d8b842bfb51280c5d","abstract_canon_sha256":"601333e610ef65e07f048681be2b5317790bd86b0930a47d9e8fded854cee604"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:22:40.751508Z","signature_b64":"IyjJUvYEra/XLd1mO/D2rSo066pPEOXm1g7qeTz9jwcO4lQG1KokFjLx846vOzO7nefGNkVe5qeGupxzMBwpDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"26392cd6d93485e8bf97b356c30b449797a8a0aaa0fb74b6cb65fd0ac5984b91","last_reissued_at":"2026-05-18T01:22:40.751008Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:22:40.751008Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Global fits of the two-loop renormalized Two-Higgs-Doublet model with soft $Z_2$ breaking","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Debtosh Chowdhury, Otto Eberhardt","submitted_at":"2015-03-27T20:00:53Z","abstract_excerpt":"We determine the next-to-leading order renormalization group equations for the Two-Higgs-Doublet model with a softly broken $Z_2$ symmetry and CP conservation in the scalar potential. We use them to identify the parameter regions which are stable up to the Planck scale and find that in this case the quartic couplings of the Higgs potential cannot be larger than 1 in magnitude and that the absolute values of the S-matrix eigenvalues cannot exceed 2.5 at the electroweak symmetry breaking scale. Interpreting the 125 GeV resonance as the light CP-even Higgs eigenstate, we combine stability constra"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1503.08216","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":"1503.08216","created_at":"2026-05-18T01:22:40.751081+00:00"},{"alias_kind":"arxiv_version","alias_value":"1503.08216v2","created_at":"2026-05-18T01:22:40.751081+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1503.08216","created_at":"2026-05-18T01:22:40.751081+00:00"},{"alias_kind":"pith_short_12","alias_value":"EY4SZVWZGSC6","created_at":"2026-05-18T12:29:19.899920+00:00"},{"alias_kind":"pith_short_16","alias_value":"EY4SZVWZGSC6RP4X","created_at":"2026-05-18T12:29:19.899920+00:00"},{"alias_kind":"pith_short_8","alias_value":"EY4SZVWZ","created_at":"2026-05-18T12:29:19.899920+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/EY4SZVWZGSC6RP4XWNLMGC2ES6","json":"https://pith.science/pith/EY4SZVWZGSC6RP4XWNLMGC2ES6.json","graph_json":"https://pith.science/api/pith-number/EY4SZVWZGSC6RP4XWNLMGC2ES6/graph.json","events_json":"https://pith.science/api/pith-number/EY4SZVWZGSC6RP4XWNLMGC2ES6/events.json","paper":"https://pith.science/paper/EY4SZVWZ"},"agent_actions":{"view_html":"https://pith.science/pith/EY4SZVWZGSC6RP4XWNLMGC2ES6","download_json":"https://pith.science/pith/EY4SZVWZGSC6RP4XWNLMGC2ES6.json","view_paper":"https://pith.science/paper/EY4SZVWZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1503.08216&json=true","fetch_graph":"https://pith.science/api/pith-number/EY4SZVWZGSC6RP4XWNLMGC2ES6/graph.json","fetch_events":"https://pith.science/api/pith-number/EY4SZVWZGSC6RP4XWNLMGC2ES6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EY4SZVWZGSC6RP4XWNLMGC2ES6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EY4SZVWZGSC6RP4XWNLMGC2ES6/action/storage_attestation","attest_author":"https://pith.science/pith/EY4SZVWZGSC6RP4XWNLMGC2ES6/action/author_attestation","sign_citation":"https://pith.science/pith/EY4SZVWZGSC6RP4XWNLMGC2ES6/action/citation_signature","submit_replication":"https://pith.science/pith/EY4SZVWZGSC6RP4XWNLMGC2ES6/action/replication_record"}},"created_at":"2026-05-18T01:22:40.751081+00:00","updated_at":"2026-05-18T01:22:40.751081+00:00"}