{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:PYXWBUCZYUEISKD33VTU64MEKA","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":"9bda74ba19c9c360aea0ad6964a03e1e2fa250d8cb4eee674ee62e3f28d1982a","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-07-11T12:17:45Z","title_canon_sha256":"3d5b5f698ea26e2cd7d021a21dedc5b6aad2fc62e61492336947f4286770cf50"},"schema_version":"1.0","source":{"id":"1707.03239","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1707.03239","created_at":"2026-05-18T00:33:49Z"},{"alias_kind":"arxiv_version","alias_value":"1707.03239v1","created_at":"2026-05-18T00:33:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.03239","created_at":"2026-05-18T00:33:49Z"},{"alias_kind":"pith_short_12","alias_value":"PYXWBUCZYUEI","created_at":"2026-05-18T12:31:37Z"},{"alias_kind":"pith_short_16","alias_value":"PYXWBUCZYUEISKD3","created_at":"2026-05-18T12:31:37Z"},{"alias_kind":"pith_short_8","alias_value":"PYXWBUCZ","created_at":"2026-05-18T12:31:37Z"}],"graph_snapshots":[{"event_id":"sha256:f8e73972d24193d1c41ccf683190099335fdf574789dee2cf9663e893bf31fdd","target":"graph","created_at":"2026-05-18T00:33:49Z","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":"We investigate the electric field shielding of ultracold collisions of dipolar rotors, initially in their first rotational excited state, using an adimensional approach. We establish a map of good and bad candidates for efficient evaporative cooling based on this shielding mechanism, by presenting the ratio of elastic over quenching processes as a function of a rescaled rotational constant $\\tilde{B} = B/s_{E_3}$ and a rescaled electric field $\\tilde{F} = dF/B$. $B, d, F, s_{E_3}$ are respectively the rotational constant, the full electric dipole moment of the molecules, the applied electric f","authors_text":"Goulven Qu\\'em\\'ener, John L. Bohn, Maykel L. Gonz\\'alez-Mart\\'inez","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-07-11T12:17:45Z","title":"Adimensional theory of shielding in ultracold collisions of dipolar rotors"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.03239","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":"sha256:52122c85883d285f6e42988c2e707049d98ac38775446a92c3b9c38fd402bdc1","target":"record","created_at":"2026-05-18T00:33:49Z","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":"9bda74ba19c9c360aea0ad6964a03e1e2fa250d8cb4eee674ee62e3f28d1982a","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-07-11T12:17:45Z","title_canon_sha256":"3d5b5f698ea26e2cd7d021a21dedc5b6aad2fc62e61492336947f4286770cf50"},"schema_version":"1.0","source":{"id":"1707.03239","kind":"arxiv","version":1}},"canonical_sha256":"7e2f60d059c50889287bdd674f71845008355659f888e0a9ff8269c7b41af20a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7e2f60d059c50889287bdd674f71845008355659f888e0a9ff8269c7b41af20a","first_computed_at":"2026-05-18T00:33:49.172268Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:33:49.172268Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Q7UU8G5O6k8t2FYQGIN2hpHvRxcaQ06K4r9wr6LN5D7pipBT6yZgEZtMjySvnzPSdMzl57CQQrJaCPF1v25EBw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:33:49.172759Z","signed_message":"canonical_sha256_bytes"},"source_id":"1707.03239","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:52122c85883d285f6e42988c2e707049d98ac38775446a92c3b9c38fd402bdc1","sha256:f8e73972d24193d1c41ccf683190099335fdf574789dee2cf9663e893bf31fdd"],"state_sha256":"0223ce181ece9f3410d8ce3ceddf24d687efbfe8b068f63cf9ca8b3ecffe471b"}