{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:5463MNKLL2BTYNNPYW3SWZYMGN","short_pith_number":"pith:5463MNKL","canonical_record":{"source":{"id":"1010.3245","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2010-10-15T19:02:46Z","cross_cats_sorted":["cond-mat.quant-gas"],"title_canon_sha256":"0cc3cc029959f2bdf13d0142df212005f3a9a15216c5711092a8fff259df5b27","abstract_canon_sha256":"f20e68c032647c49756dd32019192fa6628606fced8b4c81f6f1579e741cb3d7"},"schema_version":"1.0"},"canonical_sha256":"ef3db6354b5e833c35afc5b72b670c3343a51a1b36d7c110fbedcf4ef109121f","source":{"kind":"arxiv","id":"1010.3245","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1010.3245","created_at":"2026-05-18T04:31:32Z"},{"alias_kind":"arxiv_version","alias_value":"1010.3245v1","created_at":"2026-05-18T04:31:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.3245","created_at":"2026-05-18T04:31:32Z"},{"alias_kind":"pith_short_12","alias_value":"5463MNKLL2BT","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_16","alias_value":"5463MNKLL2BTYNNP","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_8","alias_value":"5463MNKL","created_at":"2026-05-18T12:26:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:5463MNKLL2BTYNNPYW3SWZYMGN","target":"record","payload":{"canonical_record":{"source":{"id":"1010.3245","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2010-10-15T19:02:46Z","cross_cats_sorted":["cond-mat.quant-gas"],"title_canon_sha256":"0cc3cc029959f2bdf13d0142df212005f3a9a15216c5711092a8fff259df5b27","abstract_canon_sha256":"f20e68c032647c49756dd32019192fa6628606fced8b4c81f6f1579e741cb3d7"},"schema_version":"1.0"},"canonical_sha256":"ef3db6354b5e833c35afc5b72b670c3343a51a1b36d7c110fbedcf4ef109121f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:31:32.088569Z","signature_b64":"9LRiIm39/CiwToDq3b5T44x8CO7xKAsolonOjLD76NVw6WCX4wHKkpQaPHCNKYZvlVoqBaCY74tfJQ8F9mW9AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ef3db6354b5e833c35afc5b72b670c3343a51a1b36d7c110fbedcf4ef109121f","last_reissued_at":"2026-05-18T04:31:32.088177Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:31:32.088177Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1010.3245","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:31:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"aJp0cwCSDNxWDKsHChPL+tzAvGjFLa4+uBd2NJ34IloWgMIzzgXMkgPE+7Wd70yyZXqJVCBXEQpTo0zN1khZAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T12:40:29.002953Z"},"content_sha256":"37e89c2f0b5d34c82455e54df11440ea2195d0261e57340dbbcc11f48a053067","schema_version":"1.0","event_id":"sha256:37e89c2f0b5d34c82455e54df11440ea2195d0261e57340dbbcc11f48a053067"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:5463MNKLL2BTYNNPYW3SWZYMGN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dynamics of ultracold molecules in confined geometry and electric field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas"],"primary_cat":"physics.atom-ph","authors_text":"Goulven Qu\\'em\\'ener, John L. Bohn","submitted_at":"2010-10-15T19:02:46Z","abstract_excerpt":"We present a time-independent quantum formalism to describe the dynamics of molecules with permanent electric dipole moments in a two-dimensional confined geometry such as a one-dimensional optical lattice, in the presence of an electric field. Bose/Fermi statistics and selection rules play a crucial role in the dynamics. As examples, we compare the dynamics of confined fermionic and bosonic polar KRb molecules under different confinements and electric fields. We show how chemical reactions can be suppressed, either by a \"statistical suppression\" which applies for fermions at small electric fi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.3245","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:31:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"w149tL7TqZSR+ZzlPECZBl12QtOt+kL3oHJ7F+42kRbStluL9s0bZX67FgcLEypjb9+tfKwdg/pTdA9IjdusCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T12:40:29.003681Z"},"content_sha256":"025aa9b3c40999cb5c60f8aaede31cf8c2d489f5ecadbc1aaa2b512382b5c04d","schema_version":"1.0","event_id":"sha256:025aa9b3c40999cb5c60f8aaede31cf8c2d489f5ecadbc1aaa2b512382b5c04d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5463MNKLL2BTYNNPYW3SWZYMGN/bundle.json","state_url":"https://pith.science/pith/5463MNKLL2BTYNNPYW3SWZYMGN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5463MNKLL2BTYNNPYW3SWZYMGN/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-26T12:40:29Z","links":{"resolver":"https://pith.science/pith/5463MNKLL2BTYNNPYW3SWZYMGN","bundle":"https://pith.science/pith/5463MNKLL2BTYNNPYW3SWZYMGN/bundle.json","state":"https://pith.science/pith/5463MNKLL2BTYNNPYW3SWZYMGN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5463MNKLL2BTYNNPYW3SWZYMGN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:5463MNKLL2BTYNNPYW3SWZYMGN","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":"f20e68c032647c49756dd32019192fa6628606fced8b4c81f6f1579e741cb3d7","cross_cats_sorted":["cond-mat.quant-gas"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2010-10-15T19:02:46Z","title_canon_sha256":"0cc3cc029959f2bdf13d0142df212005f3a9a15216c5711092a8fff259df5b27"},"schema_version":"1.0","source":{"id":"1010.3245","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1010.3245","created_at":"2026-05-18T04:31:32Z"},{"alias_kind":"arxiv_version","alias_value":"1010.3245v1","created_at":"2026-05-18T04:31:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.3245","created_at":"2026-05-18T04:31:32Z"},{"alias_kind":"pith_short_12","alias_value":"5463MNKLL2BT","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_16","alias_value":"5463MNKLL2BTYNNP","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_8","alias_value":"5463MNKL","created_at":"2026-05-18T12:26:04Z"}],"graph_snapshots":[{"event_id":"sha256:025aa9b3c40999cb5c60f8aaede31cf8c2d489f5ecadbc1aaa2b512382b5c04d","target":"graph","created_at":"2026-05-18T04:31:32Z","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 present a time-independent quantum formalism to describe the dynamics of molecules with permanent electric dipole moments in a two-dimensional confined geometry such as a one-dimensional optical lattice, in the presence of an electric field. Bose/Fermi statistics and selection rules play a crucial role in the dynamics. As examples, we compare the dynamics of confined fermionic and bosonic polar KRb molecules under different confinements and electric fields. We show how chemical reactions can be suppressed, either by a \"statistical suppression\" which applies for fermions at small electric fi","authors_text":"Goulven Qu\\'em\\'ener, John L. Bohn","cross_cats":["cond-mat.quant-gas"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2010-10-15T19:02:46Z","title":"Dynamics of ultracold molecules in confined geometry and electric field"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.3245","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":"sha256:37e89c2f0b5d34c82455e54df11440ea2195d0261e57340dbbcc11f48a053067","target":"record","created_at":"2026-05-18T04:31:32Z","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":"f20e68c032647c49756dd32019192fa6628606fced8b4c81f6f1579e741cb3d7","cross_cats_sorted":["cond-mat.quant-gas"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2010-10-15T19:02:46Z","title_canon_sha256":"0cc3cc029959f2bdf13d0142df212005f3a9a15216c5711092a8fff259df5b27"},"schema_version":"1.0","source":{"id":"1010.3245","kind":"arxiv","version":1}},"canonical_sha256":"ef3db6354b5e833c35afc5b72b670c3343a51a1b36d7c110fbedcf4ef109121f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ef3db6354b5e833c35afc5b72b670c3343a51a1b36d7c110fbedcf4ef109121f","first_computed_at":"2026-05-18T04:31:32.088177Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:31:32.088177Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"9LRiIm39/CiwToDq3b5T44x8CO7xKAsolonOjLD76NVw6WCX4wHKkpQaPHCNKYZvlVoqBaCY74tfJQ8F9mW9AA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:31:32.088569Z","signed_message":"canonical_sha256_bytes"},"source_id":"1010.3245","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:37e89c2f0b5d34c82455e54df11440ea2195d0261e57340dbbcc11f48a053067","sha256:025aa9b3c40999cb5c60f8aaede31cf8c2d489f5ecadbc1aaa2b512382b5c04d"],"state_sha256":"89172157f176e657b85575d4c4ea82c74122b4ad1fc25b5e0826964268c656cf"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cpcUTmFdiZRbh056XtAxGqfk2H6F91JZNJqSgCHEF2TJ+ge1qRo3K50zPtg8ZdtKAvTCvQgchbFrxytz2PygDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T12:40:29.007839Z","bundle_sha256":"602ec48e6200b9b4a019f656a396653da5ab61c473847d68fa078b623bd83d9d"}}