{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:LQJMJ2GF5IDKX3E6XILUV3T6XF","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":"c63e40131d7ec460bda64c9b4df9108bbacd106edda700d6b441d31309361526","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-09-05T17:29:51Z","title_canon_sha256":"1b11e3d648e96494c712afb6e8e09b8404154712794462ee38a1042413544b1f"},"schema_version":"1.0","source":{"id":"1909.02542","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1909.02542","created_at":"2026-07-05T00:56:31Z"},{"alias_kind":"arxiv_version","alias_value":"1909.02542v1","created_at":"2026-07-05T00:56:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1909.02542","created_at":"2026-07-05T00:56:31Z"},{"alias_kind":"pith_short_12","alias_value":"LQJMJ2GF5IDK","created_at":"2026-07-05T00:56:31Z"},{"alias_kind":"pith_short_16","alias_value":"LQJMJ2GF5IDKX3E6","created_at":"2026-07-05T00:56:31Z"},{"alias_kind":"pith_short_8","alias_value":"LQJMJ2GF","created_at":"2026-07-05T00:56:31Z"}],"graph_snapshots":[{"event_id":"sha256:8a8c89b72cf2958b8823f012e948504d6f76254756005bb6158151de2cb4baa5","target":"graph","created_at":"2026-07-05T00:56:31Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/1909.02542/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present the first crossed beam scattering experiment using a Zeeman decelerated molecular beam. The narrow velocity spreads of Zeeman decelerated NO ($X ^2\\Pi_{3/2}, j=3/2$) radicals result in high-resolution scattering images, thereby fully resolving quantum diffraction oscillations in the angular scattering distribution for inelastic NO-Ne collisions, and product-pair correlations in the radial scattering distribution for inelastic NO-O$_2$ collisions. These measurements demonstrate similar resolution and sensitivity as in experiments using Stark decelerators, opening up possibilities for","authors_text":"Matthieu Besemer, Sebastiaan Y.T. van de Meerakker, Theo Cremers, Vikram Plomp, Zhi Gao","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-09-05T17:29:51Z","title":"High-resolution imaging of molecular collisions using a Zeeman decelerator"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1909.02542","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":"sha256:6f7386f39d887542130204de2bb814df9970911d3e27f86f595ed9a214f6d909","target":"record","created_at":"2026-07-05T00:56:31Z","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":"c63e40131d7ec460bda64c9b4df9108bbacd106edda700d6b441d31309361526","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-09-05T17:29:51Z","title_canon_sha256":"1b11e3d648e96494c712afb6e8e09b8404154712794462ee38a1042413544b1f"},"schema_version":"1.0","source":{"id":"1909.02542","kind":"arxiv","version":1}},"canonical_sha256":"5c12c4e8c5ea06abec9eba174aee7eb95926b340aa9e629659b1cc4aa30e42ed","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5c12c4e8c5ea06abec9eba174aee7eb95926b340aa9e629659b1cc4aa30e42ed","first_computed_at":"2026-07-05T00:56:31.134436Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T00:56:31.134436Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"rd+17U/N9fqPNh/+VQiYk5P/HYmf77lpuYj3hUA2dQbcG5ByqlT3bcfyO4oBbDQLTmAo5DbJi8jtZVDOWTwGCQ==","signature_status":"signed_v1","signed_at":"2026-07-05T00:56:31.134928Z","signed_message":"canonical_sha256_bytes"},"source_id":"1909.02542","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6f7386f39d887542130204de2bb814df9970911d3e27f86f595ed9a214f6d909","sha256:8a8c89b72cf2958b8823f012e948504d6f76254756005bb6158151de2cb4baa5"],"state_sha256":"2d67c77116640d20362f7118f5287c24a500c5702515076c7773ac2ef467b368"}