{"record":{"author":{"account_ref":null,"orcid":null},"builds_on":[],"content_schema":"pubphys.content.topic/1","content_sha256":"6094392aa015407a9b4b824e515a9df97311276cff35219da0eb36100df2e210","created":"2026-10-03T07:17:50Z","files":[],"origin":{"assisted_by":[],"kind":"seed"},"parents":[],"salt":"1d3ae24eef96bf7487660bfe65aa58cd3ddf1b2a241cdbc08e84137fc0a6014b","schema":"pubphys.record/2","site":"pubphys.com","target":null,"type":"topic"},"content":{"external_id":"cm.deconfined-criticality","field":"cm","n":"1","review_cite":"T. Senthil, Deconfined quantum critical points: a review, arXiv, 2023","review_link":"https://arxiv.org/abs/2306.12638","review_verified":"true","summary":"Normally a material can switch between two unrelated ordered patterns only through a sudden jump or an intermediate phase. Deconfined criticality predicts a smooth switch between magnetic order and a pattern of paired spins, driven by fractional particles that exist only at the transition.","title":"Deconfined quantum criticality","topic_ref":null,"why":"It would be a phase transition outside the Landau symmetry-breaking framework, described by emergent gauge fields and fractional particles."},"attested":{"attestation":{"batch":null,"client_id":null,"id_token_sha256":null,"kind":"platform"},"record_hash":"2349550dc7ce2650de0f02331c77da4c02e3e4166a157a99e1d2814209a4678f","schema":"pubphys.attested/1"},"envelope":{"attested_hash":"02271593f5473eda2860ecaf6d1e9f40addb65ab9fb3c4286688da6eb0b393b1","platform_signature":{"key_id":"c6afc19b31429869751f06879c75cd64ea92654423d15b44be775bf1310a60da","sig":"cP33xP9WJFhLRegsXY2ui4SwNKbK_F7qVxJRJQcFZG_sGaes2s7J0e6op9R0J4rI9eN64IovBrpbinZCw4uNCg"},"schema":"pubphys.envelope/1"},"record_hash":"2349550dc7ce2650de0f02331c77da4c02e3e4166a157a99e1d2814209a4678f","leaf_index":123}