{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:W7DS2N3R2A7CILMN6J2KYHOPVE","short_pith_number":"pith:W7DS2N3R","canonical_record":{"source":{"id":"1107.4516","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2011-07-22T13:43:52Z","cross_cats_sorted":[],"title_canon_sha256":"d102fd5a99b388017229d77d885b349e4183c2c04bb88b528378c7de0d520b2c","abstract_canon_sha256":"362a31e19131fce215c07c14959660df859618aaf46f1c99c774ed63b4a0c148"},"schema_version":"1.0"},"canonical_sha256":"b7c72d3771d03e242d8df274ac1dcfa908723c3820116e7beaf92264ce35d55f","source":{"kind":"arxiv","id":"1107.4516","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1107.4516","created_at":"2026-05-18T04:07:06Z"},{"alias_kind":"arxiv_version","alias_value":"1107.4516v1","created_at":"2026-05-18T04:07:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1107.4516","created_at":"2026-05-18T04:07:06Z"},{"alias_kind":"pith_short_12","alias_value":"W7DS2N3R2A7C","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_16","alias_value":"W7DS2N3R2A7CILMN","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_8","alias_value":"W7DS2N3R","created_at":"2026-05-18T12:26:44Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:W7DS2N3R2A7CILMN6J2KYHOPVE","target":"record","payload":{"canonical_record":{"source":{"id":"1107.4516","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2011-07-22T13:43:52Z","cross_cats_sorted":[],"title_canon_sha256":"d102fd5a99b388017229d77d885b349e4183c2c04bb88b528378c7de0d520b2c","abstract_canon_sha256":"362a31e19131fce215c07c14959660df859618aaf46f1c99c774ed63b4a0c148"},"schema_version":"1.0"},"canonical_sha256":"b7c72d3771d03e242d8df274ac1dcfa908723c3820116e7beaf92264ce35d55f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:07:06.563355Z","signature_b64":"Q+m1T7Gs+PRh9WMB+0pJVj7PCpAH7puw1CLr1BdfKtEueviax+3WPVRNPTCW/jP1mq/x+so0pNuPvkGPx/C5Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b7c72d3771d03e242d8df274ac1dcfa908723c3820116e7beaf92264ce35d55f","last_reissued_at":"2026-05-18T04:07:06.562702Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:07:06.562702Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1107.4516","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":"2026-05-18T04:07:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zcw5iK1J5CZO64fpUwkzpX66aTCtjscKsVUFhzF38SsdO5ZXv7JDysjfISRqiIzdT1irsLmJzvZ/5l85W3jgCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T23:18:45.926474Z"},"content_sha256":"31078cfd27bf890333823a4be2a39c0ab9423cdf877f011a4822570284766b08","schema_version":"1.0","event_id":"sha256:31078cfd27bf890333823a4be2a39c0ab9423cdf877f011a4822570284766b08"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:W7DS2N3R2A7CILMN6J2KYHOPVE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Three-body correlation functions and recombination rates for bosons in three and one dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"Elmar Haller, Guido Pupillo, Hanns-Christoph N\\\"agerl, Johann G. Danzl, Katharina Lauber, Manfred J. Mark, Mohamed Rabie, Russell Hart","submitted_at":"2011-07-22T13:43:52Z","abstract_excerpt":"We investigate local three-body correlations for bosonic particles in three and one dimensions as a function of the interaction strength. The three-body correlation function g(3) is determined by measuring the three-body recombination rate in an ultracold gas of Cs atoms. In three dimensions, we measure the dependence of g(3) on the gas parameter in a BEC, finding good agreement with the theoretical prediction accounting for beyond-mean-field effects. In one dimension, we observe a reduction of g(3) by several orders of magnitude upon increasing interactions from the weakly interacting BEC to "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1107.4516","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":"2026-05-18T04:07:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cd76plsxEkcZLwIMN5gq1uY5ouzjPQLakBkHKtsL5AbwLS5DTpYcs+D96FuCNklXtN4QoStSAwOtyqS1iqE1BQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T23:18:45.927091Z"},"content_sha256":"820c164e61fdbb342b1a35be4ff996906e399eeedb3037253e1b88e050c824fe","schema_version":"1.0","event_id":"sha256:820c164e61fdbb342b1a35be4ff996906e399eeedb3037253e1b88e050c824fe"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/W7DS2N3R2A7CILMN6J2KYHOPVE/bundle.json","state_url":"https://pith.science/pith/W7DS2N3R2A7CILMN6J2KYHOPVE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/W7DS2N3R2A7CILMN6J2KYHOPVE/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":"2026-05-27T23:18:45Z","links":{"resolver":"https://pith.science/pith/W7DS2N3R2A7CILMN6J2KYHOPVE","bundle":"https://pith.science/pith/W7DS2N3R2A7CILMN6J2KYHOPVE/bundle.json","state":"https://pith.science/pith/W7DS2N3R2A7CILMN6J2KYHOPVE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/W7DS2N3R2A7CILMN6J2KYHOPVE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:W7DS2N3R2A7CILMN6J2KYHOPVE","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":"362a31e19131fce215c07c14959660df859618aaf46f1c99c774ed63b4a0c148","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2011-07-22T13:43:52Z","title_canon_sha256":"d102fd5a99b388017229d77d885b349e4183c2c04bb88b528378c7de0d520b2c"},"schema_version":"1.0","source":{"id":"1107.4516","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1107.4516","created_at":"2026-05-18T04:07:06Z"},{"alias_kind":"arxiv_version","alias_value":"1107.4516v1","created_at":"2026-05-18T04:07:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1107.4516","created_at":"2026-05-18T04:07:06Z"},{"alias_kind":"pith_short_12","alias_value":"W7DS2N3R2A7C","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_16","alias_value":"W7DS2N3R2A7CILMN","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_8","alias_value":"W7DS2N3R","created_at":"2026-05-18T12:26:44Z"}],"graph_snapshots":[{"event_id":"sha256:820c164e61fdbb342b1a35be4ff996906e399eeedb3037253e1b88e050c824fe","target":"graph","created_at":"2026-05-18T04:07:06Z","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 local three-body correlations for bosonic particles in three and one dimensions as a function of the interaction strength. The three-body correlation function g(3) is determined by measuring the three-body recombination rate in an ultracold gas of Cs atoms. In three dimensions, we measure the dependence of g(3) on the gas parameter in a BEC, finding good agreement with the theoretical prediction accounting for beyond-mean-field effects. In one dimension, we observe a reduction of g(3) by several orders of magnitude upon increasing interactions from the weakly interacting BEC to ","authors_text":"Elmar Haller, Guido Pupillo, Hanns-Christoph N\\\"agerl, Johann G. Danzl, Katharina Lauber, Manfred J. Mark, Mohamed Rabie, Russell Hart","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2011-07-22T13:43:52Z","title":"Three-body correlation functions and recombination rates for bosons in three and one dimensions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1107.4516","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":"sha256:31078cfd27bf890333823a4be2a39c0ab9423cdf877f011a4822570284766b08","target":"record","created_at":"2026-05-18T04:07:06Z","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":"362a31e19131fce215c07c14959660df859618aaf46f1c99c774ed63b4a0c148","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2011-07-22T13:43:52Z","title_canon_sha256":"d102fd5a99b388017229d77d885b349e4183c2c04bb88b528378c7de0d520b2c"},"schema_version":"1.0","source":{"id":"1107.4516","kind":"arxiv","version":1}},"canonical_sha256":"b7c72d3771d03e242d8df274ac1dcfa908723c3820116e7beaf92264ce35d55f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b7c72d3771d03e242d8df274ac1dcfa908723c3820116e7beaf92264ce35d55f","first_computed_at":"2026-05-18T04:07:06.562702Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:07:06.562702Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Q+m1T7Gs+PRh9WMB+0pJVj7PCpAH7puw1CLr1BdfKtEueviax+3WPVRNPTCW/jP1mq/x+so0pNuPvkGPx/C5Aw==","signature_status":"signed_v1","signed_at":"2026-05-18T04:07:06.563355Z","signed_message":"canonical_sha256_bytes"},"source_id":"1107.4516","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:31078cfd27bf890333823a4be2a39c0ab9423cdf877f011a4822570284766b08","sha256:820c164e61fdbb342b1a35be4ff996906e399eeedb3037253e1b88e050c824fe"],"state_sha256":"cd5a16d1a837e95f9efaf1bf11de689e945cd08f38c6253f6bae4a1598f84a3d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"r2FHGDEt1YY7dgU7GfYafFgbeWZHMl9uEO2JEKJSef+YAOuhr3l/fvyGTOjKgdeQLBvZNSf2sx25VzYihpd8AQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T23:18:45.930348Z","bundle_sha256":"23b0684f8ecb77fff515686d9f2d0dea83a4f7b419726dc8a9faebae6a2f2c26"}}