{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:SMPE5XSPFZAMWICFN67SCNJUZ7","short_pith_number":"pith:SMPE5XSP","schema_version":"1.0","canonical_sha256":"931e4ede4f2e40cb20456fbf213534cfce75e546902a2952155654ae93d6e68d","source":{"kind":"arxiv","id":"1111.4904","version":1},"attestation_state":"computed","paper":{"title":"Effective chiral Lagrangians for new vector bosons to O(p^4) order","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Daniele Dominici, Francesco Bernardini, Francesco Coradeschi","submitted_at":"2011-11-21T15:47:55Z","abstract_excerpt":"If the SM Higgs boson does not exist, electroweak symmetry breaking may be realized via a strong interaction with a typical scale Lambda > 1 TeV. Resonances from the strong sector may help to unitarize WW scattering, which becomes strong in the absence of an Higgs field, and could be detected at the LHC. In this paper we describe such a scenario, in the minimal case in which only one new vector resonance is present, via a chiral SU(2) x SU(2)/SU(2) lagrangian also including all possible invariant terms up to O(p^4) order (assuming a parity symmetry in the strong sector). The O(p^4) invariants "},"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":"1111.4904","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-11-21T15:47:55Z","cross_cats_sorted":[],"title_canon_sha256":"b3ca38a73f66337502d85fdb055f02d2545f3a13dcea035feb8224e5ce2d16fa","abstract_canon_sha256":"d07ab5eb20d472b3cd8aa75c2d9c05b63657680f181fde49fab92f170e27fac5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:07:54.781914Z","signature_b64":"ha2NfM24DSQzfOSXWarMDAUFLXKQBcooCdObmR9NSVItcaxwnjZ027m2jJdD+q+Cjn2jKc5tFHavGvc2ikU+AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"931e4ede4f2e40cb20456fbf213534cfce75e546902a2952155654ae93d6e68d","last_reissued_at":"2026-05-18T04:07:54.781336Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:07:54.781336Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effective chiral Lagrangians for new vector bosons to O(p^4) order","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Daniele Dominici, Francesco Bernardini, Francesco Coradeschi","submitted_at":"2011-11-21T15:47:55Z","abstract_excerpt":"If the SM Higgs boson does not exist, electroweak symmetry breaking may be realized via a strong interaction with a typical scale Lambda > 1 TeV. Resonances from the strong sector may help to unitarize WW scattering, which becomes strong in the absence of an Higgs field, and could be detected at the LHC. In this paper we describe such a scenario, in the minimal case in which only one new vector resonance is present, via a chiral SU(2) x SU(2)/SU(2) lagrangian also including all possible invariant terms up to O(p^4) order (assuming a parity symmetry in the strong sector). The O(p^4) invariants "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1111.4904","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":"1111.4904","created_at":"2026-05-18T04:07:54.781433+00:00"},{"alias_kind":"arxiv_version","alias_value":"1111.4904v1","created_at":"2026-05-18T04:07:54.781433+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1111.4904","created_at":"2026-05-18T04:07:54.781433+00:00"},{"alias_kind":"pith_short_12","alias_value":"SMPE5XSPFZAM","created_at":"2026-05-18T12:26:41.206345+00:00"},{"alias_kind":"pith_short_16","alias_value":"SMPE5XSPFZAMWICF","created_at":"2026-05-18T12:26:41.206345+00:00"},{"alias_kind":"pith_short_8","alias_value":"SMPE5XSP","created_at":"2026-05-18T12:26:41.206345+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/SMPE5XSPFZAMWICFN67SCNJUZ7","json":"https://pith.science/pith/SMPE5XSPFZAMWICFN67SCNJUZ7.json","graph_json":"https://pith.science/api/pith-number/SMPE5XSPFZAMWICFN67SCNJUZ7/graph.json","events_json":"https://pith.science/api/pith-number/SMPE5XSPFZAMWICFN67SCNJUZ7/events.json","paper":"https://pith.science/paper/SMPE5XSP"},"agent_actions":{"view_html":"https://pith.science/pith/SMPE5XSPFZAMWICFN67SCNJUZ7","download_json":"https://pith.science/pith/SMPE5XSPFZAMWICFN67SCNJUZ7.json","view_paper":"https://pith.science/paper/SMPE5XSP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1111.4904&json=true","fetch_graph":"https://pith.science/api/pith-number/SMPE5XSPFZAMWICFN67SCNJUZ7/graph.json","fetch_events":"https://pith.science/api/pith-number/SMPE5XSPFZAMWICFN67SCNJUZ7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SMPE5XSPFZAMWICFN67SCNJUZ7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SMPE5XSPFZAMWICFN67SCNJUZ7/action/storage_attestation","attest_author":"https://pith.science/pith/SMPE5XSPFZAMWICFN67SCNJUZ7/action/author_attestation","sign_citation":"https://pith.science/pith/SMPE5XSPFZAMWICFN67SCNJUZ7/action/citation_signature","submit_replication":"https://pith.science/pith/SMPE5XSPFZAMWICFN67SCNJUZ7/action/replication_record"}},"created_at":"2026-05-18T04:07:54.781433+00:00","updated_at":"2026-05-18T04:07:54.781433+00:00"}