{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:AH3KHDL3RLW33ZQJD7EYAU5BVJ","short_pith_number":"pith:AH3KHDL3","schema_version":"1.0","canonical_sha256":"01f6a38d7b8aedbde6091fc98053a1aa7a7ec699415f1f82451337019264ee67","source":{"kind":"arxiv","id":"1811.08720","version":1},"attestation_state":"computed","paper":{"title":"Collider phenomenology of vector resonances in WZ scattering processes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A.Dobado, C.Garcia-Garcia, D.Espriu, J.J.Sanz-Cillero, M.J.Herrero, Rafael L. Delgado, X.Marcano","submitted_at":"2018-11-21T13:33:27Z","abstract_excerpt":"We study the production of vector resonances at the LHC via $WZ$ scattering processes and explore the sensitivities to these resonances for the expected future LHC luminosities. The electroweak chiral Lagrangian and the Inverse Amplitude Method (IAM) are used for analyzing a dynamically generated vector resonance, whose origin would be the (hypothetically strong) self interactions of the longitudinal gauge bosons, $W_L$ and $Z_L$. We implement the unitarized scattering amplitudes into a single model, the IAM-MC, that has been adapted to MadGraph~5. It is written in terms of the electroweak chi"},"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":"1811.08720","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-11-21T13:33:27Z","cross_cats_sorted":[],"title_canon_sha256":"bed53a50fdc14b5b4a505936a8c4b86ce60cd86cf248afa04998f7e2fd340874","abstract_canon_sha256":"2cdf76b27c4a850c0fa3235f0786531bcc7e889f0c9a53092b20edc5b20724f2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:54:58.688125Z","signature_b64":"5ji8g3bBLBQW6137QImtQZMmgqcygepo6ibsHUyDQ4BPLcgHrzyLbcu5+6jChVAwdqdota9ex3MQ8o6D2ckyCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"01f6a38d7b8aedbde6091fc98053a1aa7a7ec699415f1f82451337019264ee67","last_reissued_at":"2026-05-17T23:54:58.687528Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:54:58.687528Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Collider phenomenology of vector resonances in WZ scattering processes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A.Dobado, C.Garcia-Garcia, D.Espriu, J.J.Sanz-Cillero, M.J.Herrero, Rafael L. Delgado, X.Marcano","submitted_at":"2018-11-21T13:33:27Z","abstract_excerpt":"We study the production of vector resonances at the LHC via $WZ$ scattering processes and explore the sensitivities to these resonances for the expected future LHC luminosities. The electroweak chiral Lagrangian and the Inverse Amplitude Method (IAM) are used for analyzing a dynamically generated vector resonance, whose origin would be the (hypothetically strong) self interactions of the longitudinal gauge bosons, $W_L$ and $Z_L$. We implement the unitarized scattering amplitudes into a single model, the IAM-MC, that has been adapted to MadGraph~5. It is written in terms of the electroweak chi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.08720","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":"1811.08720","created_at":"2026-05-17T23:54:58.687644+00:00"},{"alias_kind":"arxiv_version","alias_value":"1811.08720v1","created_at":"2026-05-17T23:54:58.687644+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.08720","created_at":"2026-05-17T23:54:58.687644+00:00"},{"alias_kind":"pith_short_12","alias_value":"AH3KHDL3RLW3","created_at":"2026-05-18T12:32:13.499390+00:00"},{"alias_kind":"pith_short_16","alias_value":"AH3KHDL3RLW33ZQJ","created_at":"2026-05-18T12:32:13.499390+00:00"},{"alias_kind":"pith_short_8","alias_value":"AH3KHDL3","created_at":"2026-05-18T12:32:13.499390+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/AH3KHDL3RLW33ZQJD7EYAU5BVJ","json":"https://pith.science/pith/AH3KHDL3RLW33ZQJD7EYAU5BVJ.json","graph_json":"https://pith.science/api/pith-number/AH3KHDL3RLW33ZQJD7EYAU5BVJ/graph.json","events_json":"https://pith.science/api/pith-number/AH3KHDL3RLW33ZQJD7EYAU5BVJ/events.json","paper":"https://pith.science/paper/AH3KHDL3"},"agent_actions":{"view_html":"https://pith.science/pith/AH3KHDL3RLW33ZQJD7EYAU5BVJ","download_json":"https://pith.science/pith/AH3KHDL3RLW33ZQJD7EYAU5BVJ.json","view_paper":"https://pith.science/paper/AH3KHDL3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1811.08720&json=true","fetch_graph":"https://pith.science/api/pith-number/AH3KHDL3RLW33ZQJD7EYAU5BVJ/graph.json","fetch_events":"https://pith.science/api/pith-number/AH3KHDL3RLW33ZQJD7EYAU5BVJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AH3KHDL3RLW33ZQJD7EYAU5BVJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AH3KHDL3RLW33ZQJD7EYAU5BVJ/action/storage_attestation","attest_author":"https://pith.science/pith/AH3KHDL3RLW33ZQJD7EYAU5BVJ/action/author_attestation","sign_citation":"https://pith.science/pith/AH3KHDL3RLW33ZQJD7EYAU5BVJ/action/citation_signature","submit_replication":"https://pith.science/pith/AH3KHDL3RLW33ZQJD7EYAU5BVJ/action/replication_record"}},"created_at":"2026-05-17T23:54:58.687644+00:00","updated_at":"2026-05-17T23:54:58.687644+00:00"}