{"record":{"author":{"account_ref":null,"orcid":null},"builds_on":[],"content_schema":"pubphys.content.topic/1","content_sha256":"617ae5a03bf3ff3dfbc3a4e755ac7176b33d79d02e7bf71502a3f9a49c3a134e","created":"2026-10-03T07:17:52Z","files":[],"origin":{"assisted_by":[],"kind":"seed"},"parents":[],"salt":"c8fdfcbc573c7d2d6c3b6b1bdf82dd187e9990baca48dc264a9c0639e9946467","schema":"pubphys.record/2","site":"pubphys.com","target":null,"type":"topic"},"content":{"external_id":"mathph.yang-mills","field":"mathph","n":"1","review_cite":"S. Chatterjee, Yang-Mills for probabilists, arXiv, 2018","review_link":"https://arxiv.org/abs/1803.01950","review_verified":"true","summary":"Quantum field theories describe particles as excitations of fields that fill space, but no interacting one has been built with full mathematical rigor in four-dimensional spacetime. The main test case is Yang-Mills theory, the theory of gluons, which should produce particles with a smallest nonzero mass.","title":"Yang-Mills theory and four-dimensional quantum fields","topic_ref":null,"why":"A construction would show that the framework of the Standard Model is mathematically consistent and would explain why the strong force has short range."},"attested":{"attestation":{"batch":null,"client_id":null,"id_token_sha256":null,"kind":"platform"},"record_hash":"c1a7c5336cf6e262c1ec8a96010ceec0183209142167af7077f763d0eba2c1d0","schema":"pubphys.attested/1"},"envelope":{"attested_hash":"0bdc51f8c3643ebe08f1fa6957e892ac3f2cc4abe9f7fd0903fbc8618f28bd78","platform_signature":{"key_id":"c6afc19b31429869751f06879c75cd64ea92654423d15b44be775bf1310a60da","sig":"N4UKD-QbZ80NtSNWNKB_RkbuIz7bRHmRR7__VMI99dIiFdNQ4XJxD40dA8YpFgJomtwrrXuimBanzp9TuH7jBA"},"schema":"pubphys.envelope/1"},"record_hash":"c1a7c5336cf6e262c1ec8a96010ceec0183209142167af7077f763d0eba2c1d0","leaf_index":267}