{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:LIYSCNBHD6U4MH4WZGU6CDKLYX","short_pith_number":"pith:LIYSCNBH","schema_version":"1.0","canonical_sha256":"5a312134271fa9c61f96c9a9e10d4bc5c5cf08ba2efb96d2f95d09186812fbde","source":{"kind":"arxiv","id":"2507.21910","version":2},"attestation_state":"computed","paper":{"title":"BSM: Extended Scalar Sectors","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Rui Santos, Tania Robens","submitted_at":"2025-07-29T15:25:02Z","abstract_excerpt":"In particle physics the world is described by a function, the Lagrangian. Each of its sectors characterizes the interactions between the particles of the Standard Model (SM). The addition of hypothetical new particles is done by including new terms in the Lagrangian. The scalar or Higgs sector of the SM is built with only one scalar complex field and it is extended by including new spin zero fields. This can help to solve questions that cannot be answered by the SM alone, like introducing dark matter candidates or new sources of CP-violation required to explain the matter-antimatter asymmetry "},"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":"2507.21910","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-07-29T15:25:02Z","cross_cats_sorted":[],"title_canon_sha256":"113ddfba305c080c4f7d81a39881e38c4417babce7f45eb013eb66d93150caa5","abstract_canon_sha256":"f3a0cc4c4519d42400e1735b7b625e0ab9652923326662b3a06a7387e2dbabc1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:55:20.672526Z","signature_b64":"1FlaEBH0SG2UbS54jtiqNo3F0WEOFNFNyjeaIgYypL5d64fYHZJU1SVDiiRM/vfJqbF3XQ3aG5XylZDGa6iBBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5a312134271fa9c61f96c9a9e10d4bc5c5cf08ba2efb96d2f95d09186812fbde","last_reissued_at":"2026-07-05T11:55:20.672021Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:55:20.672021Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"BSM: Extended Scalar Sectors","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Rui Santos, Tania Robens","submitted_at":"2025-07-29T15:25:02Z","abstract_excerpt":"In particle physics the world is described by a function, the Lagrangian. Each of its sectors characterizes the interactions between the particles of the Standard Model (SM). The addition of hypothetical new particles is done by including new terms in the Lagrangian. The scalar or Higgs sector of the SM is built with only one scalar complex field and it is extended by including new spin zero fields. This can help to solve questions that cannot be answered by the SM alone, like introducing dark matter candidates or new sources of CP-violation required to explain the matter-antimatter asymmetry "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2507.21910","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2507.21910/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":"2507.21910","created_at":"2026-07-05T11:55:20.672079+00:00"},{"alias_kind":"arxiv_version","alias_value":"2507.21910v2","created_at":"2026-07-05T11:55:20.672079+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2507.21910","created_at":"2026-07-05T11:55:20.672079+00:00"},{"alias_kind":"pith_short_12","alias_value":"LIYSCNBHD6U4","created_at":"2026-07-05T11:55:20.672079+00:00"},{"alias_kind":"pith_short_16","alias_value":"LIYSCNBHD6U4MH4W","created_at":"2026-07-05T11:55:20.672079+00:00"},{"alias_kind":"pith_short_8","alias_value":"LIYSCNBH","created_at":"2026-07-05T11:55:20.672079+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.04826","citing_title":"Kinematic Riffs and Interference Effects in Triple Higgs Production in the N2HDM","ref_index":25,"is_internal_anchor":false},{"citing_arxiv_id":"2604.27541","citing_title":"Low mass scalars at $e^+e^-$ colliders","ref_index":4,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LIYSCNBHD6U4MH4WZGU6CDKLYX","json":"https://pith.science/pith/LIYSCNBHD6U4MH4WZGU6CDKLYX.json","graph_json":"https://pith.science/api/pith-number/LIYSCNBHD6U4MH4WZGU6CDKLYX/graph.json","events_json":"https://pith.science/api/pith-number/LIYSCNBHD6U4MH4WZGU6CDKLYX/events.json","paper":"https://pith.science/paper/LIYSCNBH"},"agent_actions":{"view_html":"https://pith.science/pith/LIYSCNBHD6U4MH4WZGU6CDKLYX","download_json":"https://pith.science/pith/LIYSCNBHD6U4MH4WZGU6CDKLYX.json","view_paper":"https://pith.science/paper/LIYSCNBH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2507.21910&json=true","fetch_graph":"https://pith.science/api/pith-number/LIYSCNBHD6U4MH4WZGU6CDKLYX/graph.json","fetch_events":"https://pith.science/api/pith-number/LIYSCNBHD6U4MH4WZGU6CDKLYX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LIYSCNBHD6U4MH4WZGU6CDKLYX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LIYSCNBHD6U4MH4WZGU6CDKLYX/action/storage_attestation","attest_author":"https://pith.science/pith/LIYSCNBHD6U4MH4WZGU6CDKLYX/action/author_attestation","sign_citation":"https://pith.science/pith/LIYSCNBHD6U4MH4WZGU6CDKLYX/action/citation_signature","submit_replication":"https://pith.science/pith/LIYSCNBHD6U4MH4WZGU6CDKLYX/action/replication_record"}},"created_at":"2026-07-05T11:55:20.672079+00:00","updated_at":"2026-07-05T11:55:20.672079+00:00"}