{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:AM56HCH2Z55WILSYTOYXL3L52F","short_pith_number":"pith:AM56HCH2","schema_version":"1.0","canonical_sha256":"033be388facf7b642e589bb175ed7dd14da44dcfb9aabc67c0090be389783a1e","source":{"kind":"arxiv","id":"1701.08187","version":2},"attestation_state":"computed","paper":{"title":"Analysis and Measurement of the Transfer Matrix of a 9-cell 1.3-GHz Superconducting Cavity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"A. Halavanau, A. Lunin, A. Romanov, D. Edstrom, E. Harms, J. Ruan, N. Eddy, N. Solyak, P. Piot, V. Shiltsev","submitted_at":"2017-01-27T20:46:03Z","abstract_excerpt":"Superconducting linacs are capable of producing intense, stable, high-quality electron beams that have found widespread applications in science and industry. The 9-cell 1.3-GHz superconducting standing-wave accelerating RF cavity originally developed for $e^+/e^-$ linear-collider applications [B. Aunes, {\\em et al.} Phys. Rev. ST Accel. Beams {\\bf 3}, 092001 (2000)] has been broadly employed in various superconducting-linac designs. In this paper we discuss the transfer matrix of such a cavity and present its measurement performed at the Fermilab Accelerator Science and Technology (FAST) facil"},"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":"1701.08187","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.acc-ph","submitted_at":"2017-01-27T20:46:03Z","cross_cats_sorted":[],"title_canon_sha256":"d9f9f19c84e8323892ef71ce084874f6130d5f75a5f3d16c1af355dfe0cf07ba","abstract_canon_sha256":"c31ed3a7fece0a313887e488a69e948e2fdb67056a28fca24360027c4df39570"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:45:58.292069Z","signature_b64":"zbMAEtLTn6SuhGES+wiLy56LAzwk2IQdDwtecJrjY/mIWrB2F4vXpUxbGEoJwuiCZOsQZHl/RbQwbuGN9WhNDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"033be388facf7b642e589bb175ed7dd14da44dcfb9aabc67c0090be389783a1e","last_reissued_at":"2026-05-18T00:45:58.291633Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:45:58.291633Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Analysis and Measurement of the Transfer Matrix of a 9-cell 1.3-GHz Superconducting Cavity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"A. Halavanau, A. Lunin, A. Romanov, D. Edstrom, E. Harms, J. Ruan, N. Eddy, N. Solyak, P. Piot, V. Shiltsev","submitted_at":"2017-01-27T20:46:03Z","abstract_excerpt":"Superconducting linacs are capable of producing intense, stable, high-quality electron beams that have found widespread applications in science and industry. The 9-cell 1.3-GHz superconducting standing-wave accelerating RF cavity originally developed for $e^+/e^-$ linear-collider applications [B. Aunes, {\\em et al.} Phys. Rev. ST Accel. Beams {\\bf 3}, 092001 (2000)] has been broadly employed in various superconducting-linac designs. In this paper we discuss the transfer matrix of such a cavity and present its measurement performed at the Fermilab Accelerator Science and Technology (FAST) facil"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.08187","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":"1701.08187","created_at":"2026-05-18T00:45:58.291703+00:00"},{"alias_kind":"arxiv_version","alias_value":"1701.08187v2","created_at":"2026-05-18T00:45:58.291703+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1701.08187","created_at":"2026-05-18T00:45:58.291703+00:00"},{"alias_kind":"pith_short_12","alias_value":"AM56HCH2Z55W","created_at":"2026-05-18T12:31:05.417338+00:00"},{"alias_kind":"pith_short_16","alias_value":"AM56HCH2Z55WILSY","created_at":"2026-05-18T12:31:05.417338+00:00"},{"alias_kind":"pith_short_8","alias_value":"AM56HCH2","created_at":"2026-05-18T12:31:05.417338+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/AM56HCH2Z55WILSYTOYXL3L52F","json":"https://pith.science/pith/AM56HCH2Z55WILSYTOYXL3L52F.json","graph_json":"https://pith.science/api/pith-number/AM56HCH2Z55WILSYTOYXL3L52F/graph.json","events_json":"https://pith.science/api/pith-number/AM56HCH2Z55WILSYTOYXL3L52F/events.json","paper":"https://pith.science/paper/AM56HCH2"},"agent_actions":{"view_html":"https://pith.science/pith/AM56HCH2Z55WILSYTOYXL3L52F","download_json":"https://pith.science/pith/AM56HCH2Z55WILSYTOYXL3L52F.json","view_paper":"https://pith.science/paper/AM56HCH2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1701.08187&json=true","fetch_graph":"https://pith.science/api/pith-number/AM56HCH2Z55WILSYTOYXL3L52F/graph.json","fetch_events":"https://pith.science/api/pith-number/AM56HCH2Z55WILSYTOYXL3L52F/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AM56HCH2Z55WILSYTOYXL3L52F/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AM56HCH2Z55WILSYTOYXL3L52F/action/storage_attestation","attest_author":"https://pith.science/pith/AM56HCH2Z55WILSYTOYXL3L52F/action/author_attestation","sign_citation":"https://pith.science/pith/AM56HCH2Z55WILSYTOYXL3L52F/action/citation_signature","submit_replication":"https://pith.science/pith/AM56HCH2Z55WILSYTOYXL3L52F/action/replication_record"}},"created_at":"2026-05-18T00:45:58.291703+00:00","updated_at":"2026-05-18T00:45:58.291703+00:00"}