{"record":{"author":{"account_ref":null,"orcid":null},"builds_on":[],"content_schema":"pubphys.content.topic/1","content_sha256":"0a933df8a9fe261d376efb6e049f35147daf6c1cf80aa96f92efd10d21d09190","created":"2026-10-03T07:17:52Z","files":[],"origin":{"assisted_by":[],"kind":"seed"},"parents":[],"salt":"350a90fea99010ca01831d0e03bc89ba23eb856cdf2a06ead15ad21aaaadf0ea","schema":"pubphys.record/2","site":"pubphys.com","target":null,"type":"topic"},"content":{"external_id":"hep.higgs-potential","field":"hep","n":"1","review_cite":"D. Buttazzo, G. Degrassi, P. P. Giardino, G. F. Giudice, F. Sala, A. Salvio, A. Strumia, Investigating the near-criticality of the Higgs boson, JHEP, 2013","review_link":"https://arxiv.org/abs/1307.3536","review_verified":"true","summary":"The shape of the Higgs field's energy curve decides whether our vacuum is permanent or could one day decay. That shape is set by how strongly the Higgs interacts with itself, which has barely been measured.","title":"Higgs self-coupling and electroweak vacuum stability","topic_ref":null,"why":"It decides the fate of the vacuum and whether the early universe had an abrupt electroweak phase transition."},"attested":{"attestation":{"batch":null,"client_id":null,"id_token_sha256":null,"kind":"platform"},"record_hash":"7cc87e9a0f125c6a08907b134b87f69c6cd9e45b624b6e55e2b4dc1ba9882691","schema":"pubphys.attested/1"},"envelope":{"attested_hash":"c455699b1279d0a53387ee467296d080d683c8e76a795d7c4629fe840e07c433","platform_signature":{"key_id":"c6afc19b31429869751f06879c75cd64ea92654423d15b44be775bf1310a60da","sig":"NB617wpeQHAIHmKDSAmaVckyCkxM_kU9HTxtqoKH9UfbsuC763_eH6W9Ggh2Mtr6VYFy87kI3b_MkmPNvTcyBw"},"schema":"pubphys.envelope/1"},"record_hash":"7cc87e9a0f125c6a08907b134b87f69c6cd9e45b624b6e55e2b4dc1ba9882691","leaf_index":246}