{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:GV5T2XBC6J7JCQ4FTBRSHW3E7U","short_pith_number":"pith:GV5T2XBC","schema_version":"1.0","canonical_sha256":"357b3d5c22f27e914385986323db64fd308836b601a03f803f25c69e11ec2547","source":{"kind":"arxiv","id":"1401.7874","version":1},"attestation_state":"computed","paper":{"title":"Multi-Pulse Laser Wakefield Acceleration: A New Route to Efficient, High-Repetition-Rate Plasma Accelerators and High Flux Radiation Sources","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.plasm-ph"],"primary_cat":"physics.acc-ph","authors_text":"A. Seryi, A. T\\\"unnermann, J. Limpert, L. Corner, R. Bartolini, R. Walczak, S. M. Hooker, S. P. D. Mangles","submitted_at":"2014-01-30T15:13:01Z","abstract_excerpt":"Laser-driven plasma accelerators can generate accelerating gradients three orders of magnitude larger than radio-frequency accelerators and have achieved beam energies above 1 GeV in centimetre long stages. However, the pulse repetition rate and wall-plug efficiency of plasma accelerators is limited by the driving laser to less than approximately 1 Hz and 0.1% respectively. Here we investigate the prospects for exciting the plasma wave with trains of low-energy laser pulses rather than a single high-energy pulse. Resonantly exciting the wakefield in this way would enable the use of different t"},"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":"1401.7874","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.acc-ph","submitted_at":"2014-01-30T15:13:01Z","cross_cats_sorted":["physics.plasm-ph"],"title_canon_sha256":"80af2094efd509672052cbe82a436f89bf724bf374a488d041f88ea8a90f455d","abstract_canon_sha256":"f71d63117414c50a89e60df3be9242fb5c62fb265bc467b4d7d33b0c6662e7b9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:44:54.484955Z","signature_b64":"UbcYiERqUXH6nw66zeCNcT1bIQfVjVBN7I61sOXCD8KduFGgfHnV+NZMRkHZqp3IVQ3FK4tpYG1KFzh6jBOICw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"357b3d5c22f27e914385986323db64fd308836b601a03f803f25c69e11ec2547","last_reissued_at":"2026-05-18T01:44:54.484480Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:44:54.484480Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Multi-Pulse Laser Wakefield Acceleration: A New Route to Efficient, High-Repetition-Rate Plasma Accelerators and High Flux Radiation Sources","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.plasm-ph"],"primary_cat":"physics.acc-ph","authors_text":"A. Seryi, A. T\\\"unnermann, J. Limpert, L. Corner, R. Bartolini, R. Walczak, S. M. Hooker, S. P. D. Mangles","submitted_at":"2014-01-30T15:13:01Z","abstract_excerpt":"Laser-driven plasma accelerators can generate accelerating gradients three orders of magnitude larger than radio-frequency accelerators and have achieved beam energies above 1 GeV in centimetre long stages. However, the pulse repetition rate and wall-plug efficiency of plasma accelerators is limited by the driving laser to less than approximately 1 Hz and 0.1% respectively. Here we investigate the prospects for exciting the plasma wave with trains of low-energy laser pulses rather than a single high-energy pulse. Resonantly exciting the wakefield in this way would enable the use of different t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.7874","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":""},"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":"1401.7874","created_at":"2026-05-18T01:44:54.484552+00:00"},{"alias_kind":"arxiv_version","alias_value":"1401.7874v1","created_at":"2026-05-18T01:44:54.484552+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.7874","created_at":"2026-05-18T01:44:54.484552+00:00"},{"alias_kind":"pith_short_12","alias_value":"GV5T2XBC6J7J","created_at":"2026-05-18T12:28:30.664211+00:00"},{"alias_kind":"pith_short_16","alias_value":"GV5T2XBC6J7JCQ4F","created_at":"2026-05-18T12:28:30.664211+00:00"},{"alias_kind":"pith_short_8","alias_value":"GV5T2XBC","created_at":"2026-05-18T12:28:30.664211+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/GV5T2XBC6J7JCQ4FTBRSHW3E7U","json":"https://pith.science/pith/GV5T2XBC6J7JCQ4FTBRSHW3E7U.json","graph_json":"https://pith.science/api/pith-number/GV5T2XBC6J7JCQ4FTBRSHW3E7U/graph.json","events_json":"https://pith.science/api/pith-number/GV5T2XBC6J7JCQ4FTBRSHW3E7U/events.json","paper":"https://pith.science/paper/GV5T2XBC"},"agent_actions":{"view_html":"https://pith.science/pith/GV5T2XBC6J7JCQ4FTBRSHW3E7U","download_json":"https://pith.science/pith/GV5T2XBC6J7JCQ4FTBRSHW3E7U.json","view_paper":"https://pith.science/paper/GV5T2XBC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1401.7874&json=true","fetch_graph":"https://pith.science/api/pith-number/GV5T2XBC6J7JCQ4FTBRSHW3E7U/graph.json","fetch_events":"https://pith.science/api/pith-number/GV5T2XBC6J7JCQ4FTBRSHW3E7U/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GV5T2XBC6J7JCQ4FTBRSHW3E7U/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GV5T2XBC6J7JCQ4FTBRSHW3E7U/action/storage_attestation","attest_author":"https://pith.science/pith/GV5T2XBC6J7JCQ4FTBRSHW3E7U/action/author_attestation","sign_citation":"https://pith.science/pith/GV5T2XBC6J7JCQ4FTBRSHW3E7U/action/citation_signature","submit_replication":"https://pith.science/pith/GV5T2XBC6J7JCQ4FTBRSHW3E7U/action/replication_record"}},"created_at":"2026-05-18T01:44:54.484552+00:00","updated_at":"2026-05-18T01:44:54.484552+00:00"}