{"record":{"author":{"account_ref":null,"orcid":null},"builds_on":[],"content_schema":"pubphys.content.topic/1","content_sha256":"da81c459af799351087f6e50f9b5b39ce84db4a0b6cabe48455317201cd3902a","created":"2026-10-03T07:17:49Z","files":[],"origin":{"assisted_by":[],"kind":"seed"},"parents":[],"salt":"8055521197e68571fcb31c8aac969314276c04888da014b7a667b5bdfca783c1","schema":"pubphys.record/2","site":"pubphys.com","target":null,"type":"topic"},"content":{"external_id":"amo.anderson-localization-3d","field":"amo","n":"1","review_cite":"A. Yamilov, S. E. Skipetrov, T. W. Hughes, M. Minkov, Z. Yu and H. Cao, Anderson localization of electromagnetic waves in three dimensions, Nature Physics, 2023","review_link":"https://doi.org/10.1038/s41567-023-02091-7","review_verified":"true","summary":"In a strongly disordered material, waves scattered along many paths can interfere so that they stop spreading and stay trapped, an effect called Anderson localization. In three dimensions this needs disorder above a threshold, and for light it has never been shown beyond doubt.","title":"Anderson localization of waves in three dimensions","topic_ref":null,"why":"It tests whether interference alone can halt wave transport and measures the universal behavior of the three-dimensional metal-insulator transition with clean, noninteracting waves."},"attested":{"attestation":{"batch":null,"client_id":null,"id_token_sha256":null,"kind":"platform"},"record_hash":"bc11afe41898d1fca110e69c7ca3a2305936041c4a0223c9dc11cbf47acacf74","schema":"pubphys.attested/1"},"envelope":{"attested_hash":"50fb68b547777574187c36b78613217b5a9a75b0fe1c87b49280552b5dc97d30","platform_signature":{"key_id":"c6afc19b31429869751f06879c75cd64ea92654423d15b44be775bf1310a60da","sig":"oLizVgJDEpqiImP2NxdA-0DD0dQpsDtMo15je0wcJHJd4x0zYDU4icF2nPgrw47m542Bu2WVb1tB0mD5WVSlAQ"},"schema":"pubphys.envelope/1"},"record_hash":"bc11afe41898d1fca110e69c7ca3a2305936041c4a0223c9dc11cbf47acacf74","leaf_index":2}