{"record":{"author":{"account_ref":null,"orcid":null},"builds_on":[],"content_schema":"pubphys.content.topic/1","content_sha256":"71a74a22782e6f718410642a55948d3130fb9d5619706e7b094edf78e57f9d16","created":"2026-10-03T07:17:51Z","files":[],"origin":{"assisted_by":[],"kind":"seed"},"parents":[],"salt":"dc0a1dc2bc8ac5fef408217d4cfa5dd57ee8b3b898393a045463486fbc485c82","schema":"pubphys.record/2","site":"pubphys.com","target":null,"type":"topic"},"content":{"external_id":"cm.strange-metals","field":"cm","n":"1","review_cite":"P. W. Phillips, N. E. Hussey, P. Abbamonte, Stranger than metals, Science, 2022","review_link":"https://doi.org/10.1126/science.abh4273","review_verified":"true","summary":"In many correlated metals the electrical resistance grows in exact proportion to temperature down to the lowest temperatures, which standard metal theory does not allow. The electrons seem to scatter at a rate set only by temperature and Planck's constant, called the Planckian rate.","title":"Strange metals and Planckian dissipation","topic_ref":null,"why":"Strange-metal behavior appears above the superconducting dome in cuprates, heavy fermions, iron pnictides, nickelates and twisted graphene, so its explanation is tied to that of high-temperature superconductivity."},"attested":{"attestation":{"batch":null,"client_id":null,"id_token_sha256":null,"kind":"platform"},"record_hash":"bfd78216bee7da77225ac2973e7d9a78ff7a1c51ad977d9d7c3327e70d7ac174","schema":"pubphys.attested/1"},"envelope":{"attested_hash":"43a29b7f00608d80c967db5ad64f860da8f1fa970664f99d66d0c8df72b8738f","platform_signature":{"key_id":"c6afc19b31429869751f06879c75cd64ea92654423d15b44be775bf1310a60da","sig":"DVd5fIxJFaNvy5DtQ4JNfEZMgp8j00_wzzjYPNlXorxOiaDXdC6rvRnagzJO83FX6GdY719rSSn--NyJo6UiDA"},"schema":"pubphys.envelope/1"},"record_hash":"bfd78216bee7da77225ac2973e7d9a78ff7a1c51ad977d9d7c3327e70d7ac174","leaf_index":174}