{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:QKNMPVH5PWUDBE4ZEWYF4R32GG","short_pith_number":"pith:QKNMPVH5","schema_version":"1.0","canonical_sha256":"829ac7d4fd7da830939925b05e477a31a3ad0b0fe2ccd7b1d7f4817b47bc2d2b","source":{"kind":"arxiv","id":"1806.09249","version":1},"attestation_state":"computed","paper":{"title":"T0 Fan-out for Back-n White Neutron Facility at CSNS","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["eess.SP"],"primary_cat":"physics.ins-det","authors_text":"B. Li, C.J. Ning, C.Q. Feng, G.H. Zhang, G.Y. Luan, G.Z. He, H.Q. Tang, H. Sun, H.X. Huang, H.Y. Bai, H. Yi, H.Y. Jiang, H.Y. Jing, J. Bao, J. Ren, J. Wen, J.Y. Tang, J. Zhang, K.J. Zhu, L. Kang, L.K. Xie, L. Li, L. Yu, L.Y. Zhang, L. Zhou, M.H. Gu, P. Cao, P.C. Wang, P.J. Cheng, Q. An, Q.B. Wu, Q. Li, Q.M. Zhang, Q.P. Zhong, Q. Wang, Q.W. Zhang, R. Liu, R.R. Fan, S.B. Liu, T.F. Wang, T. Yu, W. Jiang, W.L. Huang, X.C. Ruan, X.G. Wu, X. Li, X.L. Ji, X.P. Zhang, X.R. Huang, X. Wu, X.Y. Ji, X.Y. Liu, X.Y. Sun, Y.C. He, Y.F. He, Y.F. Wang, Y.H. Chen, Y.J. Yu, Y. Li, Y.L. Ma, Y.T. Zhao, Y.W. Yang, Z.H. Song, Z.H. Wang, Z.J. Han, Z.J. Sun, Z.Q. Cui, Z. Wang, Z.W. Wen, Z.X. Tan, Z.Y. Zhou","submitted_at":"2018-06-25T01:50:28Z","abstract_excerpt":"the main physics goal for Back-n white neutron facility at China Spallation Neutron Source (CSNS) is to measure nuclear data. The energy of neutrons is one of the most important parameters for measuring nuclear data. Method of time of flight (TOF) is used to obtain the energy of neutrons. The time when proton bunches hit the thick tungsten target is considered as the start point of TOF. T0 signal, generated from the CSNS accelerator, represents this start time. Besides, the T0 signal is also used as the gate control signal that triggers the readout electronics. Obviously, the timing precision "},"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":"1806.09249","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2018-06-25T01:50:28Z","cross_cats_sorted":["eess.SP"],"title_canon_sha256":"be7755b20e7aff7fcd611c20064e65446e185beffb8e6d1905323ce0370b2dc0","abstract_canon_sha256":"47bf356ebb3e46f3a6bae2af3fea0c7917a675f19d957f43937f5256a686a7ae"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:12:29.882096Z","signature_b64":"ZJICW489YaijpJcc1VzubDbwOoNVaQRL6UmpRbh8v4c2PiIG9W2IvKQw7vjOybljVYVmJsQbCIvOJcLOKv0mBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"829ac7d4fd7da830939925b05e477a31a3ad0b0fe2ccd7b1d7f4817b47bc2d2b","last_reissued_at":"2026-05-18T00:12:29.881287Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:12:29.881287Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"T0 Fan-out for Back-n White Neutron Facility at CSNS","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["eess.SP"],"primary_cat":"physics.ins-det","authors_text":"B. Li, C.J. Ning, C.Q. Feng, G.H. Zhang, G.Y. Luan, G.Z. He, H.Q. Tang, H. Sun, H.X. Huang, H.Y. Bai, H. Yi, H.Y. Jiang, H.Y. Jing, J. Bao, J. Ren, J. Wen, J.Y. Tang, J. Zhang, K.J. Zhu, L. Kang, L.K. Xie, L. Li, L. Yu, L.Y. Zhang, L. Zhou, M.H. Gu, P. Cao, P.C. Wang, P.J. Cheng, Q. An, Q.B. Wu, Q. Li, Q.M. Zhang, Q.P. Zhong, Q. Wang, Q.W. Zhang, R. Liu, R.R. Fan, S.B. Liu, T.F. Wang, T. Yu, W. Jiang, W.L. Huang, X.C. Ruan, X.G. Wu, X. Li, X.L. Ji, X.P. Zhang, X.R. Huang, X. Wu, X.Y. Ji, X.Y. Liu, X.Y. Sun, Y.C. He, Y.F. He, Y.F. Wang, Y.H. Chen, Y.J. Yu, Y. Li, Y.L. Ma, Y.T. Zhao, Y.W. Yang, Z.H. Song, Z.H. Wang, Z.J. Han, Z.J. Sun, Z.Q. Cui, Z. Wang, Z.W. Wen, Z.X. Tan, Z.Y. Zhou","submitted_at":"2018-06-25T01:50:28Z","abstract_excerpt":"the main physics goal for Back-n white neutron facility at China Spallation Neutron Source (CSNS) is to measure nuclear data. The energy of neutrons is one of the most important parameters for measuring nuclear data. Method of time of flight (TOF) is used to obtain the energy of neutrons. The time when proton bunches hit the thick tungsten target is considered as the start point of TOF. T0 signal, generated from the CSNS accelerator, represents this start time. Besides, the T0 signal is also used as the gate control signal that triggers the readout electronics. Obviously, the timing precision "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1806.09249","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":"1806.09249","created_at":"2026-05-18T00:12:29.881426+00:00"},{"alias_kind":"arxiv_version","alias_value":"1806.09249v1","created_at":"2026-05-18T00:12:29.881426+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1806.09249","created_at":"2026-05-18T00:12:29.881426+00:00"},{"alias_kind":"pith_short_12","alias_value":"QKNMPVH5PWUD","created_at":"2026-05-18T12:32:46.962924+00:00"},{"alias_kind":"pith_short_16","alias_value":"QKNMPVH5PWUDBE4Z","created_at":"2026-05-18T12:32:46.962924+00:00"},{"alias_kind":"pith_short_8","alias_value":"QKNMPVH5","created_at":"2026-05-18T12:32:46.962924+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/QKNMPVH5PWUDBE4ZEWYF4R32GG","json":"https://pith.science/pith/QKNMPVH5PWUDBE4ZEWYF4R32GG.json","graph_json":"https://pith.science/api/pith-number/QKNMPVH5PWUDBE4ZEWYF4R32GG/graph.json","events_json":"https://pith.science/api/pith-number/QKNMPVH5PWUDBE4ZEWYF4R32GG/events.json","paper":"https://pith.science/paper/QKNMPVH5"},"agent_actions":{"view_html":"https://pith.science/pith/QKNMPVH5PWUDBE4ZEWYF4R32GG","download_json":"https://pith.science/pith/QKNMPVH5PWUDBE4ZEWYF4R32GG.json","view_paper":"https://pith.science/paper/QKNMPVH5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1806.09249&json=true","fetch_graph":"https://pith.science/api/pith-number/QKNMPVH5PWUDBE4ZEWYF4R32GG/graph.json","fetch_events":"https://pith.science/api/pith-number/QKNMPVH5PWUDBE4ZEWYF4R32GG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QKNMPVH5PWUDBE4ZEWYF4R32GG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QKNMPVH5PWUDBE4ZEWYF4R32GG/action/storage_attestation","attest_author":"https://pith.science/pith/QKNMPVH5PWUDBE4ZEWYF4R32GG/action/author_attestation","sign_citation":"https://pith.science/pith/QKNMPVH5PWUDBE4ZEWYF4R32GG/action/citation_signature","submit_replication":"https://pith.science/pith/QKNMPVH5PWUDBE4ZEWYF4R32GG/action/replication_record"}},"created_at":"2026-05-18T00:12:29.881426+00:00","updated_at":"2026-05-18T00:12:29.881426+00:00"}