{"record":{"author":{"account_ref":null,"orcid":null},"builds_on":[],"content_schema":"pubphys.content.topic/1","content_sha256":"d15e6a94e05b0d11382f76289e89280854520ef5b14f2eaaa7af31d54b7a941b","created":"2026-10-03T07:17:51Z","files":[],"origin":{"assisted_by":[],"kind":"seed"},"parents":[],"salt":"1971ab7b92829d02bb96040820b304fe8d75509e5651618875f44d87cca48b54","schema":"pubphys.record/2","site":"pubphys.com","target":null,"type":"topic"},"content":{"external_id":"cm.majorana-zero-modes","field":"cm","n":"1","review_cite":"E. Prada et al., From Andreev to Majorana bound states in hybrid superconductor-semiconductor nanowires, Nature Reviews Physics, 2020","review_link":"https://arxiv.org/abs/1911.04512","review_verified":"true","summary":"A Majorana zero mode is half of an ordinary electron state, bound to the end of a special superconducting wire or to a vortex core; two separated halves store one quantum bit that local noise cannot easily disturb.","title":"Majorana zero modes and topological superconductors","topic_ref":null,"why":"Majorana modes are the basis of proposed topological qubits, and claims for them have repeatedly been challenged, so resolving them affects both physics and quantum-computing programs."},"attested":{"attestation":{"batch":null,"client_id":null,"id_token_sha256":null,"kind":"platform"},"record_hash":"22b1c284f405dca649b67435bdabcd2fe6cb89dca2e57c0dd9c49b870c73940e","schema":"pubphys.attested/1"},"envelope":{"attested_hash":"4b49ce1628b107ed7a09b307adaffa3b84a9554f5ad62f394026c1a6c6ab7de8","platform_signature":{"key_id":"c6afc19b31429869751f06879c75cd64ea92654423d15b44be775bf1310a60da","sig":"Y64QEPXTsiWFSTn4K07n7GaBZBU2BsksQke0qk-06za6SAde-ghqZtYRBbh8Hg62a3lOc8d7Wqz76nzcGw2ICw"},"schema":"pubphys.envelope/1"},"record_hash":"22b1c284f405dca649b67435bdabcd2fe6cb89dca2e57c0dd9c49b870c73940e","leaf_index":153}