{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:Y6VZVEDQVVTQLTSTHGE4GI4LX7","short_pith_number":"pith:Y6VZVEDQ","schema_version":"1.0","canonical_sha256":"c7ab9a9070ad6705ce533989c3238bbfc72415c0c1c18689b61e10ba63584269","source":{"kind":"arxiv","id":"1307.1064","version":4},"attestation_state":"computed","paper":{"title":"Constraints on the Scalar Sector of the Renormalizable Coloron Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Arsham Farzinnia, Elizabeth H. Simmons, Jing Ren, R. Sekhar Chivukula","submitted_at":"2013-07-03T16:16:59Z","abstract_excerpt":"The renormalizable coloron model is the minimal extension of the standard model color sector, in which the color gauge group is enlarged to SU(3)_{1c} x SU(3)_{2c}. In this paper we discuss the constraints on this model derived from the requirements of vacuum stability, tree-level unitarity, electroweak precision measurements, and from LHC measurements of the properties of the observed Higgs-like scalar boson. The combination of these theoretical and experimental considerations strongly constrains the allowed parameter space. (Erratum appended, March 2014.)"},"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":"1307.1064","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-07-03T16:16:59Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"4f50a0d6910c47fc50d594af08aa11689ca5fe7481c6299730be80b4fd6835bb","abstract_canon_sha256":"ba766e5844c768624fcbf4cc497c0696bd19bf482ea2764203c7248488b1e50e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:57:06.680350Z","signature_b64":"xaLqT9/Mh0RHMOnWFYxisMUaWu736P5lm5cjOEw50x0Vq2KzdPv5FgUiwb5kcSPDJZUl7zzuq4I9fhYrCHHGDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c7ab9a9070ad6705ce533989c3238bbfc72415c0c1c18689b61e10ba63584269","last_reissued_at":"2026-05-18T02:57:06.679504Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:57:06.679504Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Constraints on the Scalar Sector of the Renormalizable Coloron Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Arsham Farzinnia, Elizabeth H. Simmons, Jing Ren, R. Sekhar Chivukula","submitted_at":"2013-07-03T16:16:59Z","abstract_excerpt":"The renormalizable coloron model is the minimal extension of the standard model color sector, in which the color gauge group is enlarged to SU(3)_{1c} x SU(3)_{2c}. In this paper we discuss the constraints on this model derived from the requirements of vacuum stability, tree-level unitarity, electroweak precision measurements, and from LHC measurements of the properties of the observed Higgs-like scalar boson. The combination of these theoretical and experimental considerations strongly constrains the allowed parameter space. (Erratum appended, March 2014.)"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1307.1064","kind":"arxiv","version":4},"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":"1307.1064","created_at":"2026-05-18T02:57:06.679611+00:00"},{"alias_kind":"arxiv_version","alias_value":"1307.1064v4","created_at":"2026-05-18T02:57:06.679611+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1307.1064","created_at":"2026-05-18T02:57:06.679611+00:00"},{"alias_kind":"pith_short_12","alias_value":"Y6VZVEDQVVTQ","created_at":"2026-05-18T12:28:06.772260+00:00"},{"alias_kind":"pith_short_16","alias_value":"Y6VZVEDQVVTQLTST","created_at":"2026-05-18T12:28:06.772260+00:00"},{"alias_kind":"pith_short_8","alias_value":"Y6VZVEDQ","created_at":"2026-05-18T12:28:06.772260+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2511.09632","citing_title":"Octet scalars shaping LHC distributions in 4-jet final states","ref_index":9,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/Y6VZVEDQVVTQLTSTHGE4GI4LX7","json":"https://pith.science/pith/Y6VZVEDQVVTQLTSTHGE4GI4LX7.json","graph_json":"https://pith.science/api/pith-number/Y6VZVEDQVVTQLTSTHGE4GI4LX7/graph.json","events_json":"https://pith.science/api/pith-number/Y6VZVEDQVVTQLTSTHGE4GI4LX7/events.json","paper":"https://pith.science/paper/Y6VZVEDQ"},"agent_actions":{"view_html":"https://pith.science/pith/Y6VZVEDQVVTQLTSTHGE4GI4LX7","download_json":"https://pith.science/pith/Y6VZVEDQVVTQLTSTHGE4GI4LX7.json","view_paper":"https://pith.science/paper/Y6VZVEDQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1307.1064&json=true","fetch_graph":"https://pith.science/api/pith-number/Y6VZVEDQVVTQLTSTHGE4GI4LX7/graph.json","fetch_events":"https://pith.science/api/pith-number/Y6VZVEDQVVTQLTSTHGE4GI4LX7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Y6VZVEDQVVTQLTSTHGE4GI4LX7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Y6VZVEDQVVTQLTSTHGE4GI4LX7/action/storage_attestation","attest_author":"https://pith.science/pith/Y6VZVEDQVVTQLTSTHGE4GI4LX7/action/author_attestation","sign_citation":"https://pith.science/pith/Y6VZVEDQVVTQLTSTHGE4GI4LX7/action/citation_signature","submit_replication":"https://pith.science/pith/Y6VZVEDQVVTQLTSTHGE4GI4LX7/action/replication_record"}},"created_at":"2026-05-18T02:57:06.679611+00:00","updated_at":"2026-05-18T02:57:06.679611+00:00"}