{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:ZICWB45QQ7O5KRLJSFDSKPN5A4","short_pith_number":"pith:ZICWB45Q","schema_version":"1.0","canonical_sha256":"ca0560f3b087ddd545699147253dbd07271bb8781468dde36bf01f4df57b15b5","source":{"kind":"arxiv","id":"1811.12595","version":1},"attestation_state":"computed","paper":{"title":"Experimental Investigation of the Transition Energy $\\gamma_t$ in the Isochronous Mode of the HIRFL-CSRe","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"B. Wu, C. Y. Fu, D. Y. Yin, G. D. Shen, G. Wang, H. Du, H. F. Li, H. Zhao, J. C. Yang, J. H. Liu, J. Yang, L. J. Mao, M. Wang, M. Z. Sun, P. Shuai, P. Zhang, Q. Zeng, R. J. Chen, S. Litvinov, S. Ruan, T. Bao, W. H. Zheng, W. J. Huang, W. W. Ge, X. C. Chen, X. L. Yan, X. N. Li, X. Xu, X. Zhou, Y. H. Zhang, Y. J. Yuan, Y. M. Xing, Yu. A. Litvinov, Z. S. Li","submitted_at":"2018-11-30T03:17:01Z","abstract_excerpt":"The Isochronous Mass Spectrometry (IMS) based on storage rings is a powerful technique for mass measurement of short-lived exotic nuclei. The transition energy $\\gamma_t$ of the storage ring is a vital parameter of the IMS technique. It is difficult to measure the $\\gamma_t$ and its relation to momentum spread or circulating length, especially to monitor the variation of $\\gamma_t$ during experiments. An experimental investigation on the $\\gamma_t$ has been performed for the IMS experiment at the Cooler Storage Ring of the Heavy Ion Research Facility in Lanzhou (HIRFL-CSRe). With the velocity "},"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":"1811.12595","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.acc-ph","submitted_at":"2018-11-30T03:17:01Z","cross_cats_sorted":[],"title_canon_sha256":"dac74a84e3493f5a21f738566cf059d392ab3fa00f74fd5bf2d1adf1486fa10c","abstract_canon_sha256":"c6cd35fd929a6a0f28f4c53ff60c0979f0bf76d5684e65c2d7ab5a3fef0b4009"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:59:29.128917Z","signature_b64":"B9TKKhuNHabZPzqy7lVTi4zOnpf4v2ar4Tnfc/U4zMnqJoatxoaQiiLBMU1lTgh+DLMHe+pg/UfsG5EuN7nvDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ca0560f3b087ddd545699147253dbd07271bb8781468dde36bf01f4df57b15b5","last_reissued_at":"2026-05-17T23:59:29.128269Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:59:29.128269Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Experimental Investigation of the Transition Energy $\\gamma_t$ in the Isochronous Mode of the HIRFL-CSRe","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"B. Wu, C. Y. Fu, D. Y. Yin, G. D. Shen, G. Wang, H. Du, H. F. Li, H. Zhao, J. C. Yang, J. H. Liu, J. Yang, L. J. Mao, M. Wang, M. Z. Sun, P. Shuai, P. Zhang, Q. Zeng, R. J. Chen, S. Litvinov, S. Ruan, T. Bao, W. H. Zheng, W. J. Huang, W. W. Ge, X. C. Chen, X. L. Yan, X. N. Li, X. Xu, X. Zhou, Y. H. Zhang, Y. J. Yuan, Y. M. Xing, Yu. A. Litvinov, Z. S. Li","submitted_at":"2018-11-30T03:17:01Z","abstract_excerpt":"The Isochronous Mass Spectrometry (IMS) based on storage rings is a powerful technique for mass measurement of short-lived exotic nuclei. The transition energy $\\gamma_t$ of the storage ring is a vital parameter of the IMS technique. It is difficult to measure the $\\gamma_t$ and its relation to momentum spread or circulating length, especially to monitor the variation of $\\gamma_t$ during experiments. An experimental investigation on the $\\gamma_t$ has been performed for the IMS experiment at the Cooler Storage Ring of the Heavy Ion Research Facility in Lanzhou (HIRFL-CSRe). With the velocity "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.12595","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":"1811.12595","created_at":"2026-05-17T23:59:29.128387+00:00"},{"alias_kind":"arxiv_version","alias_value":"1811.12595v1","created_at":"2026-05-17T23:59:29.128387+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.12595","created_at":"2026-05-17T23:59:29.128387+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZICWB45QQ7O5","created_at":"2026-05-18T12:33:07.085635+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZICWB45QQ7O5KRLJ","created_at":"2026-05-18T12:33:07.085635+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZICWB45Q","created_at":"2026-05-18T12:33:07.085635+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/ZICWB45QQ7O5KRLJSFDSKPN5A4","json":"https://pith.science/pith/ZICWB45QQ7O5KRLJSFDSKPN5A4.json","graph_json":"https://pith.science/api/pith-number/ZICWB45QQ7O5KRLJSFDSKPN5A4/graph.json","events_json":"https://pith.science/api/pith-number/ZICWB45QQ7O5KRLJSFDSKPN5A4/events.json","paper":"https://pith.science/paper/ZICWB45Q"},"agent_actions":{"view_html":"https://pith.science/pith/ZICWB45QQ7O5KRLJSFDSKPN5A4","download_json":"https://pith.science/pith/ZICWB45QQ7O5KRLJSFDSKPN5A4.json","view_paper":"https://pith.science/paper/ZICWB45Q","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1811.12595&json=true","fetch_graph":"https://pith.science/api/pith-number/ZICWB45QQ7O5KRLJSFDSKPN5A4/graph.json","fetch_events":"https://pith.science/api/pith-number/ZICWB45QQ7O5KRLJSFDSKPN5A4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZICWB45QQ7O5KRLJSFDSKPN5A4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZICWB45QQ7O5KRLJSFDSKPN5A4/action/storage_attestation","attest_author":"https://pith.science/pith/ZICWB45QQ7O5KRLJSFDSKPN5A4/action/author_attestation","sign_citation":"https://pith.science/pith/ZICWB45QQ7O5KRLJSFDSKPN5A4/action/citation_signature","submit_replication":"https://pith.science/pith/ZICWB45QQ7O5KRLJSFDSKPN5A4/action/replication_record"}},"created_at":"2026-05-17T23:59:29.128387+00:00","updated_at":"2026-05-17T23:59:29.128387+00:00"}