{"record":{"author":{"account_ref":null,"orcid":null},"builds_on":[],"content_schema":"pubphys.content.topic/1","content_sha256":"5bf7aa5ccde1368e8cb70898a3274fbbfd7fa05b05739385c4683701ae6be2e7","created":"2026-10-03T07:17:50Z","files":[],"origin":{"assisted_by":[],"kind":"seed"},"parents":[],"salt":"09f85a2e698e1ccdd9a51a49935e65d729556869c6519b497b9ec15c80aac5ff","schema":"pubphys.record/2","site":"pubphys.com","target":null,"type":"topic"},"content":{"external_id":"beams.advanced-structures","field":"beams","n":"1","review_cite":"R. J. England, R. J. Noble, K. Bane et al., Dielectric laser accelerators, Reviews of Modern Physics, 2014","review_link":"https://doi.org/10.1103/RevModPhys.86.1337","review_verified":"true","summary":"Instead of microwaves, small dielectric tubes can be driven by an intense electron bunch, or tiny glass structures by a laser, to reach much higher accelerating fields. The open questions are how efficient, stable and scalable such accelerators can be.","title":"Structure wakefield and dielectric laser accelerators","topic_ref":null,"why":"They are candidates for compact linacs and for multi-TeV colliders far shorter than present designs."},"attested":{"attestation":{"batch":null,"client_id":null,"id_token_sha256":null,"kind":"platform"},"record_hash":"b7298016c1710150668f62e56e87b36d9f62eb89c17a03f22442da1d6e9f7f80","schema":"pubphys.attested/1"},"envelope":{"attested_hash":"1571a755c5affbd8e891bed4646b73c6683ab079a11ec384485f0c4d9c3515c5","platform_signature":{"key_id":"c6afc19b31429869751f06879c75cd64ea92654423d15b44be775bf1310a60da","sig":"M84vrdqNyWQBbFt-nMIH7_DETcEoyffmiiJSatIwy9Fshlg5URSRTQkv5HLKZShv9SIBvRofDnFBIZe4r3dDDw"},"schema":"pubphys.envelope/1"},"record_hash":"b7298016c1710150668f62e56e87b36d9f62eb89c17a03f22442da1d6e9f7f80","leaf_index":60}