{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:ENLMRDPPB7GS5H6TTN7NI4ZSAQ","short_pith_number":"pith:ENLMRDPP","schema_version":"1.0","canonical_sha256":"2356c88def0fcd2e9fd39b7ed47332040a56868103875a899485590b46755441","source":{"kind":"arxiv","id":"1010.6169","version":1},"attestation_state":"computed","paper":{"title":"Effects of a potential fourth fermion generation on the Higgs boson mass bounds","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"J. Kallarackal, K. Jansen, P. Gerhold","submitted_at":"2010-10-29T10:03:42Z","abstract_excerpt":"We study the effect of a potential fourth fermion generation on the upper and lower Higgs boson mass bounds. This investigation is based on the numerical evaluation of a chirally invariant lattice Higgs-Yukawa model emulating the same Higgs-fermion coupling structure as in the Higgs sector of the electroweak Standard Model. In particular, the considered model obeys a Ginsparg-Wilson version of the underlying $SU(2)_L\\times U(1)_Y$ symmetry, being a global symmetry here due to the neglection of gauge fields in this model. We present our results on the modification of the upper and lower Higgs b"},"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":"1010.6169","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2010-10-29T10:03:42Z","cross_cats_sorted":[],"title_canon_sha256":"5ca24e5e48e00f5ed668e9942b91801c3618d1e8c57676eefa00c2c733903840","abstract_canon_sha256":"d218774181722713e1d013bb6ddd7482c21474b672a789a16a29eb0ad16e5d50"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:38:07.353484Z","signature_b64":"MEfFsxTuCPCDTNu0mtH8zImB0X1RCYH9Y4UbwP2msx5eKJ6MrXz+hErZiukBJQYm6TGt2r54CGBck31189fzCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2356c88def0fcd2e9fd39b7ed47332040a56868103875a899485590b46755441","last_reissued_at":"2026-05-18T04:38:07.353055Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:38:07.353055Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effects of a potential fourth fermion generation on the Higgs boson mass bounds","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"J. Kallarackal, K. Jansen, P. Gerhold","submitted_at":"2010-10-29T10:03:42Z","abstract_excerpt":"We study the effect of a potential fourth fermion generation on the upper and lower Higgs boson mass bounds. This investigation is based on the numerical evaluation of a chirally invariant lattice Higgs-Yukawa model emulating the same Higgs-fermion coupling structure as in the Higgs sector of the electroweak Standard Model. In particular, the considered model obeys a Ginsparg-Wilson version of the underlying $SU(2)_L\\times U(1)_Y$ symmetry, being a global symmetry here due to the neglection of gauge fields in this model. We present our results on the modification of the upper and lower Higgs b"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.6169","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":"1010.6169","created_at":"2026-05-18T04:38:07.353112+00:00"},{"alias_kind":"arxiv_version","alias_value":"1010.6169v1","created_at":"2026-05-18T04:38:07.353112+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.6169","created_at":"2026-05-18T04:38:07.353112+00:00"},{"alias_kind":"pith_short_12","alias_value":"ENLMRDPPB7GS","created_at":"2026-05-18T12:26:06.534383+00:00"},{"alias_kind":"pith_short_16","alias_value":"ENLMRDPPB7GS5H6T","created_at":"2026-05-18T12:26:06.534383+00:00"},{"alias_kind":"pith_short_8","alias_value":"ENLMRDPP","created_at":"2026-05-18T12:26:06.534383+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/ENLMRDPPB7GS5H6TTN7NI4ZSAQ","json":"https://pith.science/pith/ENLMRDPPB7GS5H6TTN7NI4ZSAQ.json","graph_json":"https://pith.science/api/pith-number/ENLMRDPPB7GS5H6TTN7NI4ZSAQ/graph.json","events_json":"https://pith.science/api/pith-number/ENLMRDPPB7GS5H6TTN7NI4ZSAQ/events.json","paper":"https://pith.science/paper/ENLMRDPP"},"agent_actions":{"view_html":"https://pith.science/pith/ENLMRDPPB7GS5H6TTN7NI4ZSAQ","download_json":"https://pith.science/pith/ENLMRDPPB7GS5H6TTN7NI4ZSAQ.json","view_paper":"https://pith.science/paper/ENLMRDPP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1010.6169&json=true","fetch_graph":"https://pith.science/api/pith-number/ENLMRDPPB7GS5H6TTN7NI4ZSAQ/graph.json","fetch_events":"https://pith.science/api/pith-number/ENLMRDPPB7GS5H6TTN7NI4ZSAQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ENLMRDPPB7GS5H6TTN7NI4ZSAQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ENLMRDPPB7GS5H6TTN7NI4ZSAQ/action/storage_attestation","attest_author":"https://pith.science/pith/ENLMRDPPB7GS5H6TTN7NI4ZSAQ/action/author_attestation","sign_citation":"https://pith.science/pith/ENLMRDPPB7GS5H6TTN7NI4ZSAQ/action/citation_signature","submit_replication":"https://pith.science/pith/ENLMRDPPB7GS5H6TTN7NI4ZSAQ/action/replication_record"}},"created_at":"2026-05-18T04:38:07.353112+00:00","updated_at":"2026-05-18T04:38:07.353112+00:00"}