{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:J43AL6OSZMC2P5ULLNGSBNXG4G","short_pith_number":"pith:J43AL6OS","schema_version":"1.0","canonical_sha256":"4f3605f9d2cb05a7f68b5b4d20b6e6e1a275009a291e3a3fb337b20cd40ad5ef","source":{"kind":"arxiv","id":"1601.01905","version":1},"attestation_state":"computed","paper":{"title":"Magnetic dipole excitations of $^{50}$Cr","license":"http://creativecommons.org/publicdomain/zero/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"nucl-ex","authors_text":"A. Repko, A. Zilges, B. Loher, C. Romig, D. Savran, G. Martinez-Pinedo, H. Pai, J. Beller, J. Isaak, J. Kvasil, J. Wilhelmy, L. Mertes, M. Bhike, M. Zweidinger, N. Pietralla, P. C. Ries, P.-G. Reinhard, R. Beyer, R. Schwengner, T. Beck, U. Gayer, V. Derya, V. O. Nesterenko, V. Werner, V. Yu. Ponomarev, W. Tornow","submitted_at":"2016-01-08T15:28:00Z","abstract_excerpt":"The low-lying $M1$-strength of the open-shell nucleus $^{50}$Cr has been studied with the method of nuclear resonance fluorescence up to 9.7 MeV, using bremsstrahlung at the superconducting Darmstadt linear electron accelerator S-DALINAC and Compton backscattered photons at the High Intensity $\\gamma$-ray Source (HI$\\gamma$S) facility between 6 and 9.7 MeV of the initial photon energy. Fifteen $1^{+}$ states have been observed between 3.6 and 9.7 MeV. Following our analysis, the lowest $1^{+}$ state at 3.6 MeV can be considered as an isovector orbital mode with some spin admixture. The obtaine"},"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":"1601.01905","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/publicdomain/zero/1.0/","primary_cat":"nucl-ex","submitted_at":"2016-01-08T15:28:00Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"382dd9c0351c5424991ed10a6f20ff7fd8e562ecccae8d1617d6cbaff5ce0cea","abstract_canon_sha256":"782b60af41f6b809fe21b4737a47ce93e5caacb7c9288716e540714a0d6fbd87"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:20:32.317557Z","signature_b64":"S8vPKjH6TGs8faC87sr3fKwNpuaYEehiwZWBlPE0LSzbHdO4sEZRFSHCRxVTwMqt48dzHiUUqO54LOKaKmyUAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4f3605f9d2cb05a7f68b5b4d20b6e6e1a275009a291e3a3fb337b20cd40ad5ef","last_reissued_at":"2026-05-18T01:20:32.317081Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:20:32.317081Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Magnetic dipole excitations of $^{50}$Cr","license":"http://creativecommons.org/publicdomain/zero/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"nucl-ex","authors_text":"A. Repko, A. Zilges, B. Loher, C. Romig, D. Savran, G. Martinez-Pinedo, H. Pai, J. Beller, J. Isaak, J. Kvasil, J. Wilhelmy, L. Mertes, M. Bhike, M. Zweidinger, N. Pietralla, P. C. Ries, P.-G. Reinhard, R. Beyer, R. Schwengner, T. Beck, U. Gayer, V. Derya, V. O. Nesterenko, V. Werner, V. Yu. Ponomarev, W. Tornow","submitted_at":"2016-01-08T15:28:00Z","abstract_excerpt":"The low-lying $M1$-strength of the open-shell nucleus $^{50}$Cr has been studied with the method of nuclear resonance fluorescence up to 9.7 MeV, using bremsstrahlung at the superconducting Darmstadt linear electron accelerator S-DALINAC and Compton backscattered photons at the High Intensity $\\gamma$-ray Source (HI$\\gamma$S) facility between 6 and 9.7 MeV of the initial photon energy. Fifteen $1^{+}$ states have been observed between 3.6 and 9.7 MeV. Following our analysis, the lowest $1^{+}$ state at 3.6 MeV can be considered as an isovector orbital mode with some spin admixture. The obtaine"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1601.01905","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":"1601.01905","created_at":"2026-05-18T01:20:32.317147+00:00"},{"alias_kind":"arxiv_version","alias_value":"1601.01905v1","created_at":"2026-05-18T01:20:32.317147+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1601.01905","created_at":"2026-05-18T01:20:32.317147+00:00"},{"alias_kind":"pith_short_12","alias_value":"J43AL6OSZMC2","created_at":"2026-05-18T12:30:22.444734+00:00"},{"alias_kind":"pith_short_16","alias_value":"J43AL6OSZMC2P5UL","created_at":"2026-05-18T12:30:22.444734+00:00"},{"alias_kind":"pith_short_8","alias_value":"J43AL6OS","created_at":"2026-05-18T12:30:22.444734+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/J43AL6OSZMC2P5ULLNGSBNXG4G","json":"https://pith.science/pith/J43AL6OSZMC2P5ULLNGSBNXG4G.json","graph_json":"https://pith.science/api/pith-number/J43AL6OSZMC2P5ULLNGSBNXG4G/graph.json","events_json":"https://pith.science/api/pith-number/J43AL6OSZMC2P5ULLNGSBNXG4G/events.json","paper":"https://pith.science/paper/J43AL6OS"},"agent_actions":{"view_html":"https://pith.science/pith/J43AL6OSZMC2P5ULLNGSBNXG4G","download_json":"https://pith.science/pith/J43AL6OSZMC2P5ULLNGSBNXG4G.json","view_paper":"https://pith.science/paper/J43AL6OS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1601.01905&json=true","fetch_graph":"https://pith.science/api/pith-number/J43AL6OSZMC2P5ULLNGSBNXG4G/graph.json","fetch_events":"https://pith.science/api/pith-number/J43AL6OSZMC2P5ULLNGSBNXG4G/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/J43AL6OSZMC2P5ULLNGSBNXG4G/action/timestamp_anchor","attest_storage":"https://pith.science/pith/J43AL6OSZMC2P5ULLNGSBNXG4G/action/storage_attestation","attest_author":"https://pith.science/pith/J43AL6OSZMC2P5ULLNGSBNXG4G/action/author_attestation","sign_citation":"https://pith.science/pith/J43AL6OSZMC2P5ULLNGSBNXG4G/action/citation_signature","submit_replication":"https://pith.science/pith/J43AL6OSZMC2P5ULLNGSBNXG4G/action/replication_record"}},"created_at":"2026-05-18T01:20:32.317147+00:00","updated_at":"2026-05-18T01:20:32.317147+00:00"}