{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:NBAEMFWTYZGYR5BTNVATDHZTXC","short_pith_number":"pith:NBAEMFWT","schema_version":"1.0","canonical_sha256":"68404616d3c64d88f4336d41319f33b8bb3835e00c8cdf3d8a9ae5185335d5d0","source":{"kind":"arxiv","id":"1005.3998","version":3},"attestation_state":"computed","paper":{"title":"Electroweak Limits on General New Vector Bosons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"F. del Aguila, J. de Blas, M. Perez-Victoria","submitted_at":"2010-05-21T16:25:48Z","abstract_excerpt":"We study extensions of the Standard Model with general new vector bosons. The full Standard Model gauge symmetry is used to classify the extra vectors and constrain their couplings. We derive the corresponding effective Lagrangian, valid at energies lower than the mass of the extra vectors, and use it to extract limits from electroweak precision observables, including LEP 2 data. We consider both universal and nonuniversal couplings to fermions. We study the interplay of several extra vectors, which can have the effect of opening new regions in parameter space. In particular, it allows to expl"},"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":"1005.3998","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-05-21T16:25:48Z","cross_cats_sorted":[],"title_canon_sha256":"caaf6f4b20d3c7d49dd69833e75962f4c4468ea4d79e1b887e1a58af3ef43567","abstract_canon_sha256":"b4938548397ad1164d690237932c9aaf05ee5f410fb8882f05af93b868270775"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:08:57.465886Z","signature_b64":"hX9g8I23GMphHVn+RW8BVnjoAVdhQ9HvxvnTRiF/21oROoh5arpxerPQeCodiIAH7v+pBxG3W1EJj5u+iWI8Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"68404616d3c64d88f4336d41319f33b8bb3835e00c8cdf3d8a9ae5185335d5d0","last_reissued_at":"2026-07-05T10:08:57.465373Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:08:57.465373Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electroweak Limits on General New Vector Bosons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"F. del Aguila, J. de Blas, M. Perez-Victoria","submitted_at":"2010-05-21T16:25:48Z","abstract_excerpt":"We study extensions of the Standard Model with general new vector bosons. The full Standard Model gauge symmetry is used to classify the extra vectors and constrain their couplings. We derive the corresponding effective Lagrangian, valid at energies lower than the mass of the extra vectors, and use it to extract limits from electroweak precision observables, including LEP 2 data. We consider both universal and nonuniversal couplings to fermions. We study the interplay of several extra vectors, which can have the effect of opening new regions in parameter space. In particular, it allows to expl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1005.3998","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1005.3998/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"1005.3998","created_at":"2026-07-05T10:08:57.465448+00:00"},{"alias_kind":"arxiv_version","alias_value":"1005.3998v3","created_at":"2026-07-05T10:08:57.465448+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1005.3998","created_at":"2026-07-05T10:08:57.465448+00:00"},{"alias_kind":"pith_short_12","alias_value":"NBAEMFWTYZGY","created_at":"2026-07-05T10:08:57.465448+00:00"},{"alias_kind":"pith_short_16","alias_value":"NBAEMFWTYZGYR5BT","created_at":"2026-07-05T10:08:57.465448+00:00"},{"alias_kind":"pith_short_8","alias_value":"NBAEMFWT","created_at":"2026-07-05T10:08:57.465448+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":6,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.06753","citing_title":"Phenomenology of Leptophilic Gauge Interactions at Future $e^+e^-$ Colliders","ref_index":33,"is_internal_anchor":true},{"citing_arxiv_id":"2606.19293","citing_title":"The $Z'$-boson of the $B-L$ Supersymmetric Standard Model and its Large Hadron Collider Searches","ref_index":33,"is_internal_anchor":false},{"citing_arxiv_id":"2605.29031","citing_title":"Twilight of the WIMP: Comprehensive Phenomenology of Electroweak Triplet Dark Matter","ref_index":59,"is_internal_anchor":false},{"citing_arxiv_id":"2412.14253","citing_title":"From the EFT to the UV: the complete SMEFT one-loop dictionary","ref_index":15,"is_internal_anchor":false},{"citing_arxiv_id":"2605.03014","citing_title":"Searching for UFOs from the early universe: direct detection prospects for relativistically decoupling dark matter","ref_index":70,"is_internal_anchor":false},{"citing_arxiv_id":"2604.16599","citing_title":"The effect of the two-loop SMEFT RGEs at future colliders","ref_index":26,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NBAEMFWTYZGYR5BTNVATDHZTXC","json":"https://pith.science/pith/NBAEMFWTYZGYR5BTNVATDHZTXC.json","graph_json":"https://pith.science/api/pith-number/NBAEMFWTYZGYR5BTNVATDHZTXC/graph.json","events_json":"https://pith.science/api/pith-number/NBAEMFWTYZGYR5BTNVATDHZTXC/events.json","paper":"https://pith.science/paper/NBAEMFWT"},"agent_actions":{"view_html":"https://pith.science/pith/NBAEMFWTYZGYR5BTNVATDHZTXC","download_json":"https://pith.science/pith/NBAEMFWTYZGYR5BTNVATDHZTXC.json","view_paper":"https://pith.science/paper/NBAEMFWT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1005.3998&json=true","fetch_graph":"https://pith.science/api/pith-number/NBAEMFWTYZGYR5BTNVATDHZTXC/graph.json","fetch_events":"https://pith.science/api/pith-number/NBAEMFWTYZGYR5BTNVATDHZTXC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NBAEMFWTYZGYR5BTNVATDHZTXC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NBAEMFWTYZGYR5BTNVATDHZTXC/action/storage_attestation","attest_author":"https://pith.science/pith/NBAEMFWTYZGYR5BTNVATDHZTXC/action/author_attestation","sign_citation":"https://pith.science/pith/NBAEMFWTYZGYR5BTNVATDHZTXC/action/citation_signature","submit_replication":"https://pith.science/pith/NBAEMFWTYZGYR5BTNVATDHZTXC/action/replication_record"}},"created_at":"2026-07-05T10:08:57.465448+00:00","updated_at":"2026-07-05T10:08:57.465448+00:00"}