{"record":{"author":{"account_ref":null,"orcid":null},"builds_on":[],"content_schema":"pubphys.content.topic/1","content_sha256":"5a4cc5a0f76b7695c7966019dc7361f14db8f5b700b96bc9584725770d13898f","created":"2026-10-03T07:17:53Z","files":[],"origin":{"assisted_by":[],"kind":"seed"},"parents":[],"salt":"3fc49bf94cc51b9dfc0548e75ecf419b59343c19f959738a7c142fd71ca2921f","schema":"pubphys.record/2","site":"pubphys.com","target":null,"type":"topic"},"content":{"external_id":"stat.ising-3d","field":"stat","n":"1","review_cite":"A. Pelissetto, E. Vicari, Critical phenomena and renormalization-group theory, Physics Reports, 2002","review_link":"https://arxiv.org/abs/cond-mat/0012164","review_verified":"true","summary":"The Ising model is the simplest model of a magnet, with spins that point only up or down. It was solved exactly in two dimensions in 1944, but in three dimensions its behavior at the critical temperature is known only from numerics.","title":"Critical behavior of the 3D Ising model","topic_ref":null,"why":"Its critical exponents also describe liquid-gas critical points and binary liquid mixtures, making it the most tested universality class in nature."},"attested":{"attestation":{"batch":null,"client_id":null,"id_token_sha256":null,"kind":"platform"},"record_hash":"19afc80a045932b8aeafee2d78656bd6c97eb566258215dd3cc140a709804606","schema":"pubphys.attested/1"},"envelope":{"attested_hash":"beb0858ea9dfc311da2f06e70e43f99819665583a1c407808dc06085504f7ba3","platform_signature":{"key_id":"c6afc19b31429869751f06879c75cd64ea92654423d15b44be775bf1310a60da","sig":"hM2Sz_Na6-wejQmZk6lBUPhMJlCGz4ganOHvjYPPb7nBKsOjPqoDvjcjgwP5mtgXbv3IdI2IcaOhG2ho6yV5AQ"},"schema":"pubphys.envelope/1"},"record_hash":"19afc80a045932b8aeafee2d78656bd6c97eb566258215dd3cc140a709804606","leaf_index":353}