{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:WR37USP5ZJNKHAJYSW426765I2","short_pith_number":"pith:WR37USP5","schema_version":"1.0","canonical_sha256":"b477fa49fdca5aa3813895b9af7fdd4695d962cc2a446dba884bbf11baf79cd3","source":{"kind":"arxiv","id":"2209.06690","version":1},"attestation_state":"computed","paper":{"title":"Longitudinally resolved measurement of energy-transfer efficiency in a plasma-wakefield accelerator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"B. Hidding, C. A. Lindstr{\\o}m, F. Pe\\~na, G. Loisch, J. Beinortaite, J. Bj\\\"orklund Svensson, J. C. Wood, J. M. Garland, J. Osterhoff, K. P\\~oder, L. Boulton, P. Gonz\\'alez Caminal, R. D'Arcy, S. Schr\\\"oder, S. Wesch","submitted_at":"2022-09-14T14:47:57Z","abstract_excerpt":"Energy-transfer efficiency is an important quantity in plasma-wakefield acceleration, especially for applications that demand high average power. Conventionally, the efficiency is measured using an electron spectrometer; an invasive method that provides an energy-transfer efficiency averaged over the full length of the plasma accelerator. Here, we experimentally demonstrate a novel diagnostic utilizing the excess light emitted by the plasma after a beam-plasma interaction, which yields noninvasive, longitudinally resolved measurements of the local energy-transfer efficiency from the wake to th"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2209.06690","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.acc-ph","submitted_at":"2022-09-14T14:47:57Z","cross_cats_sorted":[],"title_canon_sha256":"c02f0db816e8a541cd05dfdc5d1e0c22b0ae9d3c7bcfe9e5d61d3bffaa4ccdac","abstract_canon_sha256":"c9fb82ab2fafcdb38dbb84de13aa3f968ce27e38c3618674cc491bb8488e6284"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-11T01:09:06.774983Z","signature_b64":"sMA3o5B+ZyTXCXgUCA1V3csWxDt8hHs4eP5d23wdza178RBJxyUkKD5d48WsZLFfCeJ4vHJ61DHzQwcNepeMAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b477fa49fdca5aa3813895b9af7fdd4695d962cc2a446dba884bbf11baf79cd3","last_reissued_at":"2026-06-11T01:09:06.774006Z","signature_status":"signed_v1","first_computed_at":"2026-06-11T01:09:06.774006Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Longitudinally resolved measurement of energy-transfer efficiency in a plasma-wakefield accelerator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"B. Hidding, C. A. Lindstr{\\o}m, F. Pe\\~na, G. Loisch, J. Beinortaite, J. Bj\\\"orklund Svensson, J. C. Wood, J. M. Garland, J. Osterhoff, K. P\\~oder, L. Boulton, P. Gonz\\'alez Caminal, R. D'Arcy, S. Schr\\\"oder, S. Wesch","submitted_at":"2022-09-14T14:47:57Z","abstract_excerpt":"Energy-transfer efficiency is an important quantity in plasma-wakefield acceleration, especially for applications that demand high average power. Conventionally, the efficiency is measured using an electron spectrometer; an invasive method that provides an energy-transfer efficiency averaged over the full length of the plasma accelerator. Here, we experimentally demonstrate a novel diagnostic utilizing the excess light emitted by the plasma after a beam-plasma interaction, which yields noninvasive, longitudinally resolved measurements of the local energy-transfer efficiency from the wake to th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2209.06690","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2209.06690/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2209.06690","created_at":"2026-06-11T01:09:06.774127+00:00"},{"alias_kind":"arxiv_version","alias_value":"2209.06690v1","created_at":"2026-06-11T01:09:06.774127+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2209.06690","created_at":"2026-06-11T01:09:06.774127+00:00"},{"alias_kind":"pith_short_12","alias_value":"WR37USP5ZJNK","created_at":"2026-06-11T01:09:06.774127+00:00"},{"alias_kind":"pith_short_16","alias_value":"WR37USP5ZJNKHAJY","created_at":"2026-06-11T01:09:06.774127+00:00"},{"alias_kind":"pith_short_8","alias_value":"WR37USP5","created_at":"2026-06-11T01:09:06.774127+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WR37USP5ZJNKHAJYSW426765I2","json":"https://pith.science/pith/WR37USP5ZJNKHAJYSW426765I2.json","graph_json":"https://pith.science/api/pith-number/WR37USP5ZJNKHAJYSW426765I2/graph.json","events_json":"https://pith.science/api/pith-number/WR37USP5ZJNKHAJYSW426765I2/events.json","paper":"https://pith.science/paper/WR37USP5"},"agent_actions":{"view_html":"https://pith.science/pith/WR37USP5ZJNKHAJYSW426765I2","download_json":"https://pith.science/pith/WR37USP5ZJNKHAJYSW426765I2.json","view_paper":"https://pith.science/paper/WR37USP5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2209.06690&json=true","fetch_graph":"https://pith.science/api/pith-number/WR37USP5ZJNKHAJYSW426765I2/graph.json","fetch_events":"https://pith.science/api/pith-number/WR37USP5ZJNKHAJYSW426765I2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WR37USP5ZJNKHAJYSW426765I2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WR37USP5ZJNKHAJYSW426765I2/action/storage_attestation","attest_author":"https://pith.science/pith/WR37USP5ZJNKHAJYSW426765I2/action/author_attestation","sign_citation":"https://pith.science/pith/WR37USP5ZJNKHAJYSW426765I2/action/citation_signature","submit_replication":"https://pith.science/pith/WR37USP5ZJNKHAJYSW426765I2/action/replication_record"}},"created_at":"2026-06-11T01:09:06.774127+00:00","updated_at":"2026-06-11T01:09:06.774127+00:00"}