{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:QVMVPD5VY4PU5DF7ACUL5Y7Q3S","short_pith_number":"pith:QVMVPD5V","schema_version":"1.0","canonical_sha256":"8559578fb5c71f4e8cbf00a8bee3f0dc8d3487bd7cb78f24b0df0d18664d3817","source":{"kind":"arxiv","id":"1108.5986","version":1},"attestation_state":"computed","paper":{"title":"Potential of the FLASH FEL technology for the construction of a kW-scale light source for the next generation lithography","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"E.A. Schneidmiller, H. Weise, M.V. Yurkov, V.F. Vogel","submitted_at":"2011-08-30T15:39:07Z","abstract_excerpt":"The driving engine of the Free Electron Laser in Hamburg (FLASH) is an L-band superconducting accelerator. It is designed to operate in burst mode with 800 microsecond pulse duration at a repetition rate of 10 Hz. The maximum accelerated beam current during the macropulse is 9 mA. Our analysis shows that the FLASH technology has great potential since it is possible to construct a FLASH like free electron laser operating at the wavelength of 13.5 and 6.8 nanometer with an average power up to 2.6 kW. Such a source meets the physical requirements for the light source for the next generation litho"},"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":"1108.5986","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.acc-ph","submitted_at":"2011-08-30T15:39:07Z","cross_cats_sorted":[],"title_canon_sha256":"1065de93ce40f91deecb6e6ee86a4f90bc5569afbeeacbd3cd8c365c8f1ade1c","abstract_canon_sha256":"086e78b8ee224e7a36f910b440a787ecb68175eb4142aadfa1db6d117b901084"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:14:28.078372Z","signature_b64":"fsyqXfh8B7z8Ex+1THLUam5UWIu54oIdrc9n58mjQ48WfS62h/Wudm+HoY7EJ7IxWVxKerhCCcKZJB3O7bcZAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8559578fb5c71f4e8cbf00a8bee3f0dc8d3487bd7cb78f24b0df0d18664d3817","last_reissued_at":"2026-05-18T04:14:28.077864Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:14:28.077864Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Potential of the FLASH FEL technology for the construction of a kW-scale light source for the next generation lithography","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"E.A. Schneidmiller, H. Weise, M.V. Yurkov, V.F. Vogel","submitted_at":"2011-08-30T15:39:07Z","abstract_excerpt":"The driving engine of the Free Electron Laser in Hamburg (FLASH) is an L-band superconducting accelerator. It is designed to operate in burst mode with 800 microsecond pulse duration at a repetition rate of 10 Hz. The maximum accelerated beam current during the macropulse is 9 mA. Our analysis shows that the FLASH technology has great potential since it is possible to construct a FLASH like free electron laser operating at the wavelength of 13.5 and 6.8 nanometer with an average power up to 2.6 kW. Such a source meets the physical requirements for the light source for the next generation litho"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1108.5986","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":"1108.5986","created_at":"2026-05-18T04:14:28.077940+00:00"},{"alias_kind":"arxiv_version","alias_value":"1108.5986v1","created_at":"2026-05-18T04:14:28.077940+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1108.5986","created_at":"2026-05-18T04:14:28.077940+00:00"},{"alias_kind":"pith_short_12","alias_value":"QVMVPD5VY4PU","created_at":"2026-05-18T12:26:39.201973+00:00"},{"alias_kind":"pith_short_16","alias_value":"QVMVPD5VY4PU5DF7","created_at":"2026-05-18T12:26:39.201973+00:00"},{"alias_kind":"pith_short_8","alias_value":"QVMVPD5V","created_at":"2026-05-18T12:26:39.201973+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/QVMVPD5VY4PU5DF7ACUL5Y7Q3S","json":"https://pith.science/pith/QVMVPD5VY4PU5DF7ACUL5Y7Q3S.json","graph_json":"https://pith.science/api/pith-number/QVMVPD5VY4PU5DF7ACUL5Y7Q3S/graph.json","events_json":"https://pith.science/api/pith-number/QVMVPD5VY4PU5DF7ACUL5Y7Q3S/events.json","paper":"https://pith.science/paper/QVMVPD5V"},"agent_actions":{"view_html":"https://pith.science/pith/QVMVPD5VY4PU5DF7ACUL5Y7Q3S","download_json":"https://pith.science/pith/QVMVPD5VY4PU5DF7ACUL5Y7Q3S.json","view_paper":"https://pith.science/paper/QVMVPD5V","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1108.5986&json=true","fetch_graph":"https://pith.science/api/pith-number/QVMVPD5VY4PU5DF7ACUL5Y7Q3S/graph.json","fetch_events":"https://pith.science/api/pith-number/QVMVPD5VY4PU5DF7ACUL5Y7Q3S/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QVMVPD5VY4PU5DF7ACUL5Y7Q3S/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QVMVPD5VY4PU5DF7ACUL5Y7Q3S/action/storage_attestation","attest_author":"https://pith.science/pith/QVMVPD5VY4PU5DF7ACUL5Y7Q3S/action/author_attestation","sign_citation":"https://pith.science/pith/QVMVPD5VY4PU5DF7ACUL5Y7Q3S/action/citation_signature","submit_replication":"https://pith.science/pith/QVMVPD5VY4PU5DF7ACUL5Y7Q3S/action/replication_record"}},"created_at":"2026-05-18T04:14:28.077940+00:00","updated_at":"2026-05-18T04:14:28.077940+00:00"}