{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:CEWLYQIL3IOZXARTA3WVR4HJZJ","short_pith_number":"pith:CEWLYQIL","schema_version":"1.0","canonical_sha256":"112cbc410bda1d9b823306ed58f0e9ca59c31221fb665c12e06b0e67dd9a3145","source":{"kind":"arxiv","id":"hep-ph/9608269","version":2},"attestation_state":"computed","paper":{"title":"Coloron Phenomenology","license":"","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"E. H. Simmons","submitted_at":"1996-08-08T15:32:12Z","abstract_excerpt":"A flavor-universal extension of the strong interactions was recently proposed in response to the apparent excess of high-$E_T$ jets in the inclusive jet spectrum measured at the Tevatron. This paper studies the color octet of massive gauge bosons (`colorons') that is present in the low-energy spectrum of the model's Higgs phase. Constraints from searches for new particles decaying to dijets and from measurements of the weak-interaction $\\rho$ parameter imply that the colorons must have masses greater than 870-1000 GeV. The implications of recent Tevatron data and the prospective input from fut"},"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":"hep-ph/9608269","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1996-08-08T15:32:12Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"0525199903a348f49a4bdff3ff98407a827ac014772a6e21804e3a0def03eced","abstract_canon_sha256":"2d4991cc6bf82dd9d933234c629d2ff722b09fa3f758539978d1f59a675954da"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:08:05.642088Z","signature_b64":"qNZXRPRsDe6yueZn0L6WHCqGVh6meF4qOvlrLI0koczX3c2JuB316fx/p3NcIkKc58atDQqxJTDxI/PQ8Ig3Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"112cbc410bda1d9b823306ed58f0e9ca59c31221fb665c12e06b0e67dd9a3145","last_reissued_at":"2026-05-18T01:08:05.641720Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:08:05.641720Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Coloron Phenomenology","license":"","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"E. H. Simmons","submitted_at":"1996-08-08T15:32:12Z","abstract_excerpt":"A flavor-universal extension of the strong interactions was recently proposed in response to the apparent excess of high-$E_T$ jets in the inclusive jet spectrum measured at the Tevatron. This paper studies the color octet of massive gauge bosons (`colorons') that is present in the low-energy spectrum of the model's Higgs phase. Constraints from searches for new particles decaying to dijets and from measurements of the weak-interaction $\\rho$ parameter imply that the colorons must have masses greater than 870-1000 GeV. The implications of recent Tevatron data and the prospective input from fut"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9608269","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":"hep-ph/9608269","created_at":"2026-05-18T01:08:05.641786+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9608269v2","created_at":"2026-05-18T01:08:05.641786+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9608269","created_at":"2026-05-18T01:08:05.641786+00:00"},{"alias_kind":"pith_short_12","alias_value":"CEWLYQIL3IOZ","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_16","alias_value":"CEWLYQIL3IOZXART","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_8","alias_value":"CEWLYQIL","created_at":"2026-05-18T12:25:47.700082+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2510.21641","citing_title":"Search for dijet resonances with data scouting in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","ref_index":6,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CEWLYQIL3IOZXARTA3WVR4HJZJ","json":"https://pith.science/pith/CEWLYQIL3IOZXARTA3WVR4HJZJ.json","graph_json":"https://pith.science/api/pith-number/CEWLYQIL3IOZXARTA3WVR4HJZJ/graph.json","events_json":"https://pith.science/api/pith-number/CEWLYQIL3IOZXARTA3WVR4HJZJ/events.json","paper":"https://pith.science/paper/CEWLYQIL"},"agent_actions":{"view_html":"https://pith.science/pith/CEWLYQIL3IOZXARTA3WVR4HJZJ","download_json":"https://pith.science/pith/CEWLYQIL3IOZXARTA3WVR4HJZJ.json","view_paper":"https://pith.science/paper/CEWLYQIL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9608269&json=true","fetch_graph":"https://pith.science/api/pith-number/CEWLYQIL3IOZXARTA3WVR4HJZJ/graph.json","fetch_events":"https://pith.science/api/pith-number/CEWLYQIL3IOZXARTA3WVR4HJZJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CEWLYQIL3IOZXARTA3WVR4HJZJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CEWLYQIL3IOZXARTA3WVR4HJZJ/action/storage_attestation","attest_author":"https://pith.science/pith/CEWLYQIL3IOZXARTA3WVR4HJZJ/action/author_attestation","sign_citation":"https://pith.science/pith/CEWLYQIL3IOZXARTA3WVR4HJZJ/action/citation_signature","submit_replication":"https://pith.science/pith/CEWLYQIL3IOZXARTA3WVR4HJZJ/action/replication_record"}},"created_at":"2026-05-18T01:08:05.641786+00:00","updated_at":"2026-05-18T01:08:05.641786+00:00"}