{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:EWBEUIASRUWJOZ54OCNRINVQN3","short_pith_number":"pith:EWBEUIAS","schema_version":"1.0","canonical_sha256":"25824a20128d2c9767bc709b1436b06ec2feb0f8585c869222b3a0c673c0c31d","source":{"kind":"arxiv","id":"1303.3876","version":4},"attestation_state":"computed","paper":{"title":"Effective Lagrangian for a light Higgs-like scalar","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Christophe Grojean, Margarete Muhlleitner, Margherita Ghezzi, Michael Spira, Roberto Contino","submitted_at":"2013-03-15T19:34:02Z","abstract_excerpt":"We reconsider the effective Lagrangian that describes a light Higgs-like boson and better clarify a few issues which were not exhaustively addressed in the previous literature. In particular we highlight the strategy to determine whether the dynamics responsible for the electroweak symmetry breaking is weakly or strongly interacting. We also discuss how the effective Lagrangian can be implemented into automatic tools for the calculation of Higgs decay rates and production cross sections."},"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":"1303.3876","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-03-15T19:34:02Z","cross_cats_sorted":[],"title_canon_sha256":"bb3d082316af48518237bde2efac5813b4d6da501db42e0f4e051a07c656646c","abstract_canon_sha256":"f8b777c9c28ac8962d957a776dd12084f59e47ec1728803bc45bc76437f15bd8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:56:32.760462Z","signature_b64":"L4qXJYzSmX6NvagE3l6rSVWScdq6ptKw/0Hi7iJiis+mm0FY6/V9zc+Z/sZQu6ZtP/d1s4aEz5/pbYeNsx+7DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"25824a20128d2c9767bc709b1436b06ec2feb0f8585c869222b3a0c673c0c31d","last_reissued_at":"2026-05-18T02:56:32.759681Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:56:32.759681Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effective Lagrangian for a light Higgs-like scalar","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Christophe Grojean, Margarete Muhlleitner, Margherita Ghezzi, Michael Spira, Roberto Contino","submitted_at":"2013-03-15T19:34:02Z","abstract_excerpt":"We reconsider the effective Lagrangian that describes a light Higgs-like boson and better clarify a few issues which were not exhaustively addressed in the previous literature. In particular we highlight the strategy to determine whether the dynamics responsible for the electroweak symmetry breaking is weakly or strongly interacting. We also discuss how the effective Lagrangian can be implemented into automatic tools for the calculation of Higgs decay rates and production cross sections."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.3876","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":"1303.3876","created_at":"2026-05-18T02:56:32.759808+00:00"},{"alias_kind":"arxiv_version","alias_value":"1303.3876v4","created_at":"2026-05-18T02:56:32.759808+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.3876","created_at":"2026-05-18T02:56:32.759808+00:00"},{"alias_kind":"pith_short_12","alias_value":"EWBEUIASRUWJ","created_at":"2026-05-18T12:27:43.054852+00:00"},{"alias_kind":"pith_short_16","alias_value":"EWBEUIASRUWJOZ54","created_at":"2026-05-18T12:27:43.054852+00:00"},{"alias_kind":"pith_short_8","alias_value":"EWBEUIAS","created_at":"2026-05-18T12:27:43.054852+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2511.23410","citing_title":"The Art of Counting: a reappraisal of the HEFT expansion","ref_index":124,"is_internal_anchor":true},{"citing_arxiv_id":"2604.00107","citing_title":"Full positivity bounds for anomalous quartic gauge couplings in SMEFT","ref_index":6,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EWBEUIASRUWJOZ54OCNRINVQN3","json":"https://pith.science/pith/EWBEUIASRUWJOZ54OCNRINVQN3.json","graph_json":"https://pith.science/api/pith-number/EWBEUIASRUWJOZ54OCNRINVQN3/graph.json","events_json":"https://pith.science/api/pith-number/EWBEUIASRUWJOZ54OCNRINVQN3/events.json","paper":"https://pith.science/paper/EWBEUIAS"},"agent_actions":{"view_html":"https://pith.science/pith/EWBEUIASRUWJOZ54OCNRINVQN3","download_json":"https://pith.science/pith/EWBEUIASRUWJOZ54OCNRINVQN3.json","view_paper":"https://pith.science/paper/EWBEUIAS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1303.3876&json=true","fetch_graph":"https://pith.science/api/pith-number/EWBEUIASRUWJOZ54OCNRINVQN3/graph.json","fetch_events":"https://pith.science/api/pith-number/EWBEUIASRUWJOZ54OCNRINVQN3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EWBEUIASRUWJOZ54OCNRINVQN3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EWBEUIASRUWJOZ54OCNRINVQN3/action/storage_attestation","attest_author":"https://pith.science/pith/EWBEUIASRUWJOZ54OCNRINVQN3/action/author_attestation","sign_citation":"https://pith.science/pith/EWBEUIASRUWJOZ54OCNRINVQN3/action/citation_signature","submit_replication":"https://pith.science/pith/EWBEUIASRUWJOZ54OCNRINVQN3/action/replication_record"}},"created_at":"2026-05-18T02:56:32.759808+00:00","updated_at":"2026-05-18T02:56:32.759808+00:00"}