{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:I5FKZE4PGCG4O6CO7CLMQNSB5R","short_pith_number":"pith:I5FKZE4P","schema_version":"1.0","canonical_sha256":"474aac938f308dc7784ef896c83641ec7e01ed28f93fa369fbc84f50868acdba","source":{"kind":"arxiv","id":"1409.6954","version":2},"attestation_state":"computed","paper":{"title":"Compact x-ray source based on burst-mode inverse Compton scattering at 100 kHz","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"B. Khaykovich, D.E. Moncton, E. A. Nanni, E. Ihloff, F.X. K\\\"artner, G. Resta, H. Lin, J. Bessuille, K.-H. Hong, K. Murari, L.E. Zapata, P. Brown, S. Carbajo, S. Tantawi, V. Dolgashev, W. S. Graves","submitted_at":"2014-09-24T13:31:32Z","abstract_excerpt":"A design for a compact x-ray light source (CXLS) with flux and brilliance orders of magnitude beyond existing laboratory scale sources is presented. The source is based on inverse Compton scattering of a high brightness electron bunch on a picosecond laser pulse. The accelerator is a novel high-efficiency standing-wave linac and RF photoinjector powered by a single ultrastable RF transmitter at x-band RF frequency. The high efficiency permits operation at repetition rates up to 1 kHz, which is further boosted to 100 kHz by operating with trains of 100 bunches of 100 pC charge, each separated b"},"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":"1409.6954","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.acc-ph","submitted_at":"2014-09-24T13:31:32Z","cross_cats_sorted":[],"title_canon_sha256":"564e8601261f523358c20eb4f8a21cb70e6bd169fc06a587f2b34de9294454b2","abstract_canon_sha256":"f6f07c1b48397b229c35525779c4af0e6b0dc80a44e5227d6a184f748f4a82fb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:44:23.312578Z","signature_b64":"qdjfzRRnbkJkVlJjlCVRXPm0XWatra89n0OgEuzAT0HRyPvVEg8xoqlfMaRy6Q87A20S5MYYeBfBpHJ4MiqUBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"474aac938f308dc7784ef896c83641ec7e01ed28f93fa369fbc84f50868acdba","last_reissued_at":"2026-05-17T23:44:23.311899Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:44:23.311899Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Compact x-ray source based on burst-mode inverse Compton scattering at 100 kHz","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"B. Khaykovich, D.E. Moncton, E. A. Nanni, E. Ihloff, F.X. K\\\"artner, G. Resta, H. Lin, J. Bessuille, K.-H. Hong, K. Murari, L.E. Zapata, P. Brown, S. Carbajo, S. Tantawi, V. Dolgashev, W. S. Graves","submitted_at":"2014-09-24T13:31:32Z","abstract_excerpt":"A design for a compact x-ray light source (CXLS) with flux and brilliance orders of magnitude beyond existing laboratory scale sources is presented. The source is based on inverse Compton scattering of a high brightness electron bunch on a picosecond laser pulse. The accelerator is a novel high-efficiency standing-wave linac and RF photoinjector powered by a single ultrastable RF transmitter at x-band RF frequency. The high efficiency permits operation at repetition rates up to 1 kHz, which is further boosted to 100 kHz by operating with trains of 100 bunches of 100 pC charge, each separated b"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.6954","kind":"arxiv","version":2},"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":"1409.6954","created_at":"2026-05-17T23:44:23.312000+00:00"},{"alias_kind":"arxiv_version","alias_value":"1409.6954v2","created_at":"2026-05-17T23:44:23.312000+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.6954","created_at":"2026-05-17T23:44:23.312000+00:00"},{"alias_kind":"pith_short_12","alias_value":"I5FKZE4PGCG4","created_at":"2026-05-18T12:28:33.132498+00:00"},{"alias_kind":"pith_short_16","alias_value":"I5FKZE4PGCG4O6CO","created_at":"2026-05-18T12:28:33.132498+00:00"},{"alias_kind":"pith_short_8","alias_value":"I5FKZE4P","created_at":"2026-05-18T12:28:33.132498+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/I5FKZE4PGCG4O6CO7CLMQNSB5R","json":"https://pith.science/pith/I5FKZE4PGCG4O6CO7CLMQNSB5R.json","graph_json":"https://pith.science/api/pith-number/I5FKZE4PGCG4O6CO7CLMQNSB5R/graph.json","events_json":"https://pith.science/api/pith-number/I5FKZE4PGCG4O6CO7CLMQNSB5R/events.json","paper":"https://pith.science/paper/I5FKZE4P"},"agent_actions":{"view_html":"https://pith.science/pith/I5FKZE4PGCG4O6CO7CLMQNSB5R","download_json":"https://pith.science/pith/I5FKZE4PGCG4O6CO7CLMQNSB5R.json","view_paper":"https://pith.science/paper/I5FKZE4P","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1409.6954&json=true","fetch_graph":"https://pith.science/api/pith-number/I5FKZE4PGCG4O6CO7CLMQNSB5R/graph.json","fetch_events":"https://pith.science/api/pith-number/I5FKZE4PGCG4O6CO7CLMQNSB5R/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/I5FKZE4PGCG4O6CO7CLMQNSB5R/action/timestamp_anchor","attest_storage":"https://pith.science/pith/I5FKZE4PGCG4O6CO7CLMQNSB5R/action/storage_attestation","attest_author":"https://pith.science/pith/I5FKZE4PGCG4O6CO7CLMQNSB5R/action/author_attestation","sign_citation":"https://pith.science/pith/I5FKZE4PGCG4O6CO7CLMQNSB5R/action/citation_signature","submit_replication":"https://pith.science/pith/I5FKZE4PGCG4O6CO7CLMQNSB5R/action/replication_record"}},"created_at":"2026-05-17T23:44:23.312000+00:00","updated_at":"2026-05-17T23:44:23.312000+00:00"}