{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:DACDGVVUW4CMF7PCBXSTPWOAL6","short_pith_number":"pith:DACDGVVU","schema_version":"1.0","canonical_sha256":"18043356b4b704c2fde20de537d9c05f88c8f0bef088b7ed3b84756a4eda131f","source":{"kind":"arxiv","id":"1305.3761","version":1},"attestation_state":"computed","paper":{"title":"One-loop calculation of the oblique S and T parameters within strongly-coupled scenarios with a light Higgs-like boson","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ignasi Rosell","submitted_at":"2013-05-16T11:25:37Z","abstract_excerpt":"We present a one-loop calculation of the oblique S and T parameters within strongly-coupled models of electroweak symmetry breaking with a light Higgs-like boson. We use a general effective Lagrangian, implementing the chiral symmetry breaking SU(2)_L x SU(2)_R -> SU(2)_{L+R} with Goldstones, gauge bosons, the Higgs-like scalar and one multiplet of vector and axial-vector massive resonance states. The estimation is based on the short-distance constraints and a dispersive approach. The experimentally allowed range forces the vector and axial-vector states to be heavy, with masses above the TeV "},"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":"1305.3761","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-05-16T11:25:37Z","cross_cats_sorted":[],"title_canon_sha256":"b189d49d4830981b6513818e1a16da65c913ea53cdc01183f0d1af0996c2db32","abstract_canon_sha256":"326ad1a27ebe5fbf40c691612429e0f281c715b700da58068878d032a3602afd"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:25:34.000081Z","signature_b64":"srndLhTgpChxiFWldJeUPNI/23crDNIgDLwDLbmjJiGQZALDrkVEfHif1aY8X+D6glhrFQOLQaWdiUvLf90DDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"18043356b4b704c2fde20de537d9c05f88c8f0bef088b7ed3b84756a4eda131f","last_reissued_at":"2026-05-18T03:25:33.999693Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:25:33.999693Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"One-loop calculation of the oblique S and T parameters within strongly-coupled scenarios with a light Higgs-like boson","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ignasi Rosell","submitted_at":"2013-05-16T11:25:37Z","abstract_excerpt":"We present a one-loop calculation of the oblique S and T parameters within strongly-coupled models of electroweak symmetry breaking with a light Higgs-like boson. We use a general effective Lagrangian, implementing the chiral symmetry breaking SU(2)_L x SU(2)_R -> SU(2)_{L+R} with Goldstones, gauge bosons, the Higgs-like scalar and one multiplet of vector and axial-vector massive resonance states. The estimation is based on the short-distance constraints and a dispersive approach. The experimentally allowed range forces the vector and axial-vector states to be heavy, with masses above the TeV "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1305.3761","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":"1305.3761","created_at":"2026-05-18T03:25:33.999751+00:00"},{"alias_kind":"arxiv_version","alias_value":"1305.3761v1","created_at":"2026-05-18T03:25:33.999751+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1305.3761","created_at":"2026-05-18T03:25:33.999751+00:00"},{"alias_kind":"pith_short_12","alias_value":"DACDGVVUW4CM","created_at":"2026-05-18T12:27:40.988391+00:00"},{"alias_kind":"pith_short_16","alias_value":"DACDGVVUW4CMF7PC","created_at":"2026-05-18T12:27:40.988391+00:00"},{"alias_kind":"pith_short_8","alias_value":"DACDGVVU","created_at":"2026-05-18T12:27:40.988391+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/DACDGVVUW4CMF7PCBXSTPWOAL6","json":"https://pith.science/pith/DACDGVVUW4CMF7PCBXSTPWOAL6.json","graph_json":"https://pith.science/api/pith-number/DACDGVVUW4CMF7PCBXSTPWOAL6/graph.json","events_json":"https://pith.science/api/pith-number/DACDGVVUW4CMF7PCBXSTPWOAL6/events.json","paper":"https://pith.science/paper/DACDGVVU"},"agent_actions":{"view_html":"https://pith.science/pith/DACDGVVUW4CMF7PCBXSTPWOAL6","download_json":"https://pith.science/pith/DACDGVVUW4CMF7PCBXSTPWOAL6.json","view_paper":"https://pith.science/paper/DACDGVVU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1305.3761&json=true","fetch_graph":"https://pith.science/api/pith-number/DACDGVVUW4CMF7PCBXSTPWOAL6/graph.json","fetch_events":"https://pith.science/api/pith-number/DACDGVVUW4CMF7PCBXSTPWOAL6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DACDGVVUW4CMF7PCBXSTPWOAL6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DACDGVVUW4CMF7PCBXSTPWOAL6/action/storage_attestation","attest_author":"https://pith.science/pith/DACDGVVUW4CMF7PCBXSTPWOAL6/action/author_attestation","sign_citation":"https://pith.science/pith/DACDGVVUW4CMF7PCBXSTPWOAL6/action/citation_signature","submit_replication":"https://pith.science/pith/DACDGVVUW4CMF7PCBXSTPWOAL6/action/replication_record"}},"created_at":"2026-05-18T03:25:33.999751+00:00","updated_at":"2026-05-18T03:25:33.999751+00:00"}