{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:DGELDLMECZN3IEKAQUR5BP236D","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"04da08d544ef02aae46cfab71c0fa9a5e4047afd3f36243a88871078e396ab1c","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2017-11-09T13:39:51Z","title_canon_sha256":"2c94d880757c6d50058a18762b8c460dab86d9e670dda1ec865ade53df6c22f5"},"schema_version":"1.0","source":{"id":"1711.03374","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.03374","created_at":"2026-05-18T00:23:29Z"},{"alias_kind":"arxiv_version","alias_value":"1711.03374v1","created_at":"2026-05-18T00:23:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.03374","created_at":"2026-05-18T00:23:29Z"},{"alias_kind":"pith_short_12","alias_value":"DGELDLMECZN3","created_at":"2026-05-18T12:31:10Z"},{"alias_kind":"pith_short_16","alias_value":"DGELDLMECZN3IEKA","created_at":"2026-05-18T12:31:10Z"},{"alias_kind":"pith_short_8","alias_value":"DGELDLME","created_at":"2026-05-18T12:31:10Z"}],"graph_snapshots":[{"event_id":"sha256:44385a3267d7fd5c8be21e65d857a6de511d5df0af1b29f3074f2594635c0cb7","target":"graph","created_at":"2026-05-18T00:23:29Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"The current deuteron beam polarimetry at Nuclotron is provided by the Internal Target polarimeter based on the use of the asymmetry in dp- elastic scattering at large angles in the cms at 270 MeV. The upgraded deuteron beam polarimeter has been used obtain the vector and tensor polarization during 2016/2017 runs for the DSS experimental program. The polarimeter has been used also for tuning of the polarized ion source parameters for 6 different spin modes.","authors_text":"A.A.Terekhin, A.N.Khrenov, A.N.Livanov, A.S.Belov, A.V.Averyanov, A.V.Tishevsky, A.Yu.Isupov, D.Enache, D.O.Krivenkov, E.V.Chernykh, J.-T.Karachuk, M.Janek, P.K.Kurilkin, S.G.Reznikov, S.M.Piyadin, V.P.Ladygin, V.V.Fimushkin, Ya.T.Skhomenko, Yu.V.Gurchin","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2017-11-09T13:39:51Z","title":"Measurement of the deuteron beam polarization at internal target at Nuclotron for DSS experiment"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.03374","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:aec9901def40d412b8e72c957aa9c2079a8b9767dc5f75e86ef03364b52ecd69","target":"record","created_at":"2026-05-18T00:23:29Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"04da08d544ef02aae46cfab71c0fa9a5e4047afd3f36243a88871078e396ab1c","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2017-11-09T13:39:51Z","title_canon_sha256":"2c94d880757c6d50058a18762b8c460dab86d9e670dda1ec865ade53df6c22f5"},"schema_version":"1.0","source":{"id":"1711.03374","kind":"arxiv","version":1}},"canonical_sha256":"1988b1ad84165bb411408523d0bf5bf0eb0ac80c1cc6ff5daf9fa4a819b1a68f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1988b1ad84165bb411408523d0bf5bf0eb0ac80c1cc6ff5daf9fa4a819b1a68f","first_computed_at":"2026-05-18T00:23:29.605850Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:23:29.605850Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"aSKAXMSGoDAc/f4JPYzyZpnsgayQx5g2K/Op3t7VGMCQwH8HJutH2kVz4rGfqUikPSvIbstZleMeF3N2PYMuBA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:23:29.606365Z","signed_message":"canonical_sha256_bytes"},"source_id":"1711.03374","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:aec9901def40d412b8e72c957aa9c2079a8b9767dc5f75e86ef03364b52ecd69","sha256:44385a3267d7fd5c8be21e65d857a6de511d5df0af1b29f3074f2594635c0cb7"],"state_sha256":"c4a28039371c22f43b220d6f9aabdcd75a851dd4ce7ff68cbf2480a582d6c0d1"}