{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:HBKUQ2NBHIML2RRHJDQC54XEZV","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":"bc8b70b25ec5ee7318cc079c1da6a5a4ad8f0a461138a7c31684aaba80ae55fb","cross_cats_sorted":["cond-mat.quant-gas","physics.chem-ph","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-05-04T08:31:41Z","title_canon_sha256":"fad50f88de227b0ac1ca6067d671bdaeb5b4634e94a529ebb10649873611815d"},"schema_version":"1.0","source":{"id":"1105.0761","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1105.0761","created_at":"2026-05-18T04:22:40Z"},{"alias_kind":"arxiv_version","alias_value":"1105.0761v1","created_at":"2026-05-18T04:22:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.0761","created_at":"2026-05-18T04:22:40Z"},{"alias_kind":"pith_short_12","alias_value":"HBKUQ2NBHIML","created_at":"2026-05-18T12:26:30Z"},{"alias_kind":"pith_short_16","alias_value":"HBKUQ2NBHIML2RRH","created_at":"2026-05-18T12:26:30Z"},{"alias_kind":"pith_short_8","alias_value":"HBKUQ2NB","created_at":"2026-05-18T12:26:30Z"}],"graph_snapshots":[{"event_id":"sha256:16eff9e407f2abf581723d3eed233b25f950e39638fb849e0f406dc4bb610eee","target":"graph","created_at":"2026-05-18T04:22:40Z","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":"A (diatomic) shape resonance is a metastable state of a pair of colliding atoms quasi-bound by the centrifugal barrier imposed by the angular momentum involved in the collision. The temporary trapping of the atoms' scattering wavefunction corresponds to an enhanced atom pair density at low interatomic separations. This leads to larger overlap of the wavefunctions involved in a molecule formation process such as photoassociation, rendering the process more efficient. However, for an ensemble of atoms, the atom pair density will only be enhanced if the energy of the resonance comes close to the ","authors_text":"Bretislav Friedrich, Christiane P. Koch, Mikhail Lemeshko, Rosario Gonz\\'alez-F\\'erez, Ruzin Aganoglu","cross_cats":["cond-mat.quant-gas","physics.chem-ph","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-05-04T08:31:41Z","title":"Controlling a diatomic shape resonance with non-resonant light"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.0761","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":"sha256:328ecdd50979dadc1f9456ad7bfb110c2f7952b59e2137763c1a5b2fa3acafae","target":"record","created_at":"2026-05-18T04:22:40Z","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":"bc8b70b25ec5ee7318cc079c1da6a5a4ad8f0a461138a7c31684aaba80ae55fb","cross_cats_sorted":["cond-mat.quant-gas","physics.chem-ph","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-05-04T08:31:41Z","title_canon_sha256":"fad50f88de227b0ac1ca6067d671bdaeb5b4634e94a529ebb10649873611815d"},"schema_version":"1.0","source":{"id":"1105.0761","kind":"arxiv","version":1}},"canonical_sha256":"38554869a13a18bd462748e02ef2e4cd71b8707a59f960194f932432bc8d5e31","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"38554869a13a18bd462748e02ef2e4cd71b8707a59f960194f932432bc8d5e31","first_computed_at":"2026-05-18T04:22:40.989816Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:22:40.989816Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Mp6ax+Qfm5OufkWjPU/GclBVzl9GBCY5CQxF+78FZOdAQgMycWLkJ3aOAQLlWMGdWMelZb0ohD/p3am1X4lLCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T04:22:40.990397Z","signed_message":"canonical_sha256_bytes"},"source_id":"1105.0761","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:328ecdd50979dadc1f9456ad7bfb110c2f7952b59e2137763c1a5b2fa3acafae","sha256:16eff9e407f2abf581723d3eed233b25f950e39638fb849e0f406dc4bb610eee"],"state_sha256":"898c88ac2ffce8fc5fcee7c45338d9c656d99e5525e9eb91501105cddf1c0949"}