{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:AL2WKLA7VJPANYAN4ZMPCPF765","short_pith_number":"pith:AL2WKLA7","schema_version":"1.0","canonical_sha256":"02f5652c1faa5e06e00de658f13cbff7498826ea98e451b7155ecd4307197177","source":{"kind":"arxiv","id":"1304.6092","version":2},"attestation_state":"computed","paper":{"title":"The Higgs Mass and the Emergence of New Physics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Djordje Minic, Tatsu Takeuchi, Ufuk Aydemir","submitted_at":"2013-04-22T20:00:22Z","abstract_excerpt":"We investigate the physical implications of formulating the electroweak (EW) part of the Standard Model (SM) in terms of a superconnection involving the supergroup SU(2/1). In particular, we relate the observed Higgs mass to new physics at around 4 TeV. The ultraviolet incompleteness of the superconnection approach points to its emergent nature. The new physics beyond the SM is associated with the emergent supergroup SU(2/2), which is natural from the point of view of the Pati-Salam model. Given that the Pati-Salam group is robust in certain constructions of string vacua, these results suggest"},"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":"1304.6092","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-04-22T20:00:22Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"f5c191df2f0403eb5a921d841005f7b287eb676d2ec61a2db3a8dcd367c2a07e","abstract_canon_sha256":"e668dfa2734fe1ea7922981e85c13bcd6aafadad4dddbc908d5d92d73e5f3caa"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:19:04.043382Z","signature_b64":"+GXUav63hvq0//MPPaMOpdeJVD9G3p5EVZesu2rCLjAdbS2ZXjoam8t9/3PSbt0l0p3sR4Dl3CJlFBcD4h9jDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"02f5652c1faa5e06e00de658f13cbff7498826ea98e451b7155ecd4307197177","last_reissued_at":"2026-05-18T03:19:04.042642Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:19:04.042642Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Higgs Mass and the Emergence of New Physics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Djordje Minic, Tatsu Takeuchi, Ufuk Aydemir","submitted_at":"2013-04-22T20:00:22Z","abstract_excerpt":"We investigate the physical implications of formulating the electroweak (EW) part of the Standard Model (SM) in terms of a superconnection involving the supergroup SU(2/1). In particular, we relate the observed Higgs mass to new physics at around 4 TeV. The ultraviolet incompleteness of the superconnection approach points to its emergent nature. The new physics beyond the SM is associated with the emergent supergroup SU(2/2), which is natural from the point of view of the Pati-Salam model. Given that the Pati-Salam group is robust in certain constructions of string vacua, these results suggest"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1304.6092","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":""},"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":"1304.6092","created_at":"2026-05-18T03:19:04.042751+00:00"},{"alias_kind":"arxiv_version","alias_value":"1304.6092v2","created_at":"2026-05-18T03:19:04.042751+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1304.6092","created_at":"2026-05-18T03:19:04.042751+00:00"},{"alias_kind":"pith_short_12","alias_value":"AL2WKLA7VJPA","created_at":"2026-05-18T12:27:38.830355+00:00"},{"alias_kind":"pith_short_16","alias_value":"AL2WKLA7VJPANYAN","created_at":"2026-05-18T12:27:38.830355+00:00"},{"alias_kind":"pith_short_8","alias_value":"AL2WKLA7","created_at":"2026-05-18T12:27:38.830355+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1906.09583","citing_title":"Spectral Noncommutative Geometry, Standard Model and all that","ref_index":18,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/AL2WKLA7VJPANYAN4ZMPCPF765","json":"https://pith.science/pith/AL2WKLA7VJPANYAN4ZMPCPF765.json","graph_json":"https://pith.science/api/pith-number/AL2WKLA7VJPANYAN4ZMPCPF765/graph.json","events_json":"https://pith.science/api/pith-number/AL2WKLA7VJPANYAN4ZMPCPF765/events.json","paper":"https://pith.science/paper/AL2WKLA7"},"agent_actions":{"view_html":"https://pith.science/pith/AL2WKLA7VJPANYAN4ZMPCPF765","download_json":"https://pith.science/pith/AL2WKLA7VJPANYAN4ZMPCPF765.json","view_paper":"https://pith.science/paper/AL2WKLA7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1304.6092&json=true","fetch_graph":"https://pith.science/api/pith-number/AL2WKLA7VJPANYAN4ZMPCPF765/graph.json","fetch_events":"https://pith.science/api/pith-number/AL2WKLA7VJPANYAN4ZMPCPF765/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AL2WKLA7VJPANYAN4ZMPCPF765/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AL2WKLA7VJPANYAN4ZMPCPF765/action/storage_attestation","attest_author":"https://pith.science/pith/AL2WKLA7VJPANYAN4ZMPCPF765/action/author_attestation","sign_citation":"https://pith.science/pith/AL2WKLA7VJPANYAN4ZMPCPF765/action/citation_signature","submit_replication":"https://pith.science/pith/AL2WKLA7VJPANYAN4ZMPCPF765/action/replication_record"}},"created_at":"2026-05-18T03:19:04.042751+00:00","updated_at":"2026-05-18T03:19:04.042751+00:00"}