{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:XJCW3BHEXFV6FQJ6G5HBUPFXOG","short_pith_number":"pith:XJCW3BHE","schema_version":"1.0","canonical_sha256":"ba456d84e4b96be2c13e374e1a3cb771aff9c7153d78f82f6f1da33ac779686a","source":{"kind":"arxiv","id":"1807.02211","version":2},"attestation_state":"computed","paper":{"title":"Scalar resonance in a top partner model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alfonso Zerwekh, Juan Yepes, Sebasti\\'an Norero","submitted_at":"2018-07-06T00:56:27Z","abstract_excerpt":"The phenomenology entailed by a scalar resonance in a top partner model is analysed here in a $SO(5)$ Composite Higgs formalism. Heavy scalar resonances production and their decays modes are explored along a benchmark resonance mass range. The production of single-double partner final states has been scanned along the partner mass scale. QCD drives such production, as well as the SM gauge, Higgs, plus the intermediation of the scalar resonance. Non-zero contributions are induced as long as extra fermion-resonance effects are included. Finally, we have excluded regions of the parameter spaces u"},"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":"1807.02211","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-07-06T00:56:27Z","cross_cats_sorted":[],"title_canon_sha256":"5f0a4a93e87d689bcab4acaeb7acc03a361f882d277303321323bc1c2a67034c","abstract_canon_sha256":"8dde8e71d740339c3d9919cd98cef207d6227bf51e1c0309b8381e583e1a2cf1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:08:02.643725Z","signature_b64":"uXpWJon0cjExhXY6VcTlywQWM1sCJlMbVI10WymubFg0mBlsNsU5xlC1zVqdkCvjb4mL542VqFA2jSa1sjYPBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ba456d84e4b96be2c13e374e1a3cb771aff9c7153d78f82f6f1da33ac779686a","last_reissued_at":"2026-05-18T00:08:02.643077Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:08:02.643077Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Scalar resonance in a top partner model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alfonso Zerwekh, Juan Yepes, Sebasti\\'an Norero","submitted_at":"2018-07-06T00:56:27Z","abstract_excerpt":"The phenomenology entailed by a scalar resonance in a top partner model is analysed here in a $SO(5)$ Composite Higgs formalism. Heavy scalar resonances production and their decays modes are explored along a benchmark resonance mass range. The production of single-double partner final states has been scanned along the partner mass scale. QCD drives such production, as well as the SM gauge, Higgs, plus the intermediation of the scalar resonance. Non-zero contributions are induced as long as extra fermion-resonance effects are included. Finally, we have excluded regions of the parameter spaces u"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.02211","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":"1807.02211","created_at":"2026-05-18T00:08:02.643194+00:00"},{"alias_kind":"arxiv_version","alias_value":"1807.02211v2","created_at":"2026-05-18T00:08:02.643194+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.02211","created_at":"2026-05-18T00:08:02.643194+00:00"},{"alias_kind":"pith_short_12","alias_value":"XJCW3BHEXFV6","created_at":"2026-05-18T12:33:01.666342+00:00"},{"alias_kind":"pith_short_16","alias_value":"XJCW3BHEXFV6FQJ6","created_at":"2026-05-18T12:33:01.666342+00:00"},{"alias_kind":"pith_short_8","alias_value":"XJCW3BHE","created_at":"2026-05-18T12:33:01.666342+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/XJCW3BHEXFV6FQJ6G5HBUPFXOG","json":"https://pith.science/pith/XJCW3BHEXFV6FQJ6G5HBUPFXOG.json","graph_json":"https://pith.science/api/pith-number/XJCW3BHEXFV6FQJ6G5HBUPFXOG/graph.json","events_json":"https://pith.science/api/pith-number/XJCW3BHEXFV6FQJ6G5HBUPFXOG/events.json","paper":"https://pith.science/paper/XJCW3BHE"},"agent_actions":{"view_html":"https://pith.science/pith/XJCW3BHEXFV6FQJ6G5HBUPFXOG","download_json":"https://pith.science/pith/XJCW3BHEXFV6FQJ6G5HBUPFXOG.json","view_paper":"https://pith.science/paper/XJCW3BHE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1807.02211&json=true","fetch_graph":"https://pith.science/api/pith-number/XJCW3BHEXFV6FQJ6G5HBUPFXOG/graph.json","fetch_events":"https://pith.science/api/pith-number/XJCW3BHEXFV6FQJ6G5HBUPFXOG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XJCW3BHEXFV6FQJ6G5HBUPFXOG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XJCW3BHEXFV6FQJ6G5HBUPFXOG/action/storage_attestation","attest_author":"https://pith.science/pith/XJCW3BHEXFV6FQJ6G5HBUPFXOG/action/author_attestation","sign_citation":"https://pith.science/pith/XJCW3BHEXFV6FQJ6G5HBUPFXOG/action/citation_signature","submit_replication":"https://pith.science/pith/XJCW3BHEXFV6FQJ6G5HBUPFXOG/action/replication_record"}},"created_at":"2026-05-18T00:08:02.643194+00:00","updated_at":"2026-05-18T00:08:02.643194+00:00"}