{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2002:XOWR6UTHUIEJJRGXKI3J55EM7U","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":"0354ce5955f97465470c62afb43174488c976d1606fcb7778e1cf4fb942f1bc9","cross_cats_sorted":["nucl-th","physics.atom-ph"],"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2002-10-09T21:42:06Z","title_canon_sha256":"186e1e84b7f34c3e91c69add15ee1d0597cd108c08d166c15a32b30a8a8f052d"},"schema_version":"1.0","source":{"id":"cond-mat/0210217","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0210217","created_at":"2026-07-04T14:19:32Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0210217v2","created_at":"2026-07-04T14:19:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0210217","created_at":"2026-07-04T14:19:32Z"},{"alias_kind":"pith_short_12","alias_value":"XOWR6UTHUIEJ","created_at":"2026-07-04T14:19:32Z"},{"alias_kind":"pith_short_16","alias_value":"XOWR6UTHUIEJJRGX","created_at":"2026-07-04T14:19:32Z"},{"alias_kind":"pith_short_8","alias_value":"XOWR6UTH","created_at":"2026-07-04T14:19:32Z"}],"graph_snapshots":[{"event_id":"sha256:e0ddcc499fce2443d648a5833424cd6052873089c7c79dfe54245436d5032f01","target":"graph","created_at":"2026-07-04T14:19:32Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/cond-mat/0210217/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We show that in the limit of large and positive atom--atom scattering length the properties of an atomic--molecular Bose--Einstein Condensate (amBEC) are determined by an universal energy density functional (EDF). We find that the optimal conditions for the formation of a stable amBEC are in the regime where there are no shallow trimers and the atom--dimer scattering length is negative and comparable in magnitude with the atom--atom scattering length. At temperatures lower than $T_c$ the chemical potentials for the atoms and molecules can be specified independently. Besides three--body recombi","authors_text":"Aurel Bulgac, Paulo F. Bedaque","cross_cats":["nucl-th","physics.atom-ph"],"headline":"","license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2002-10-09T21:42:06Z","title":"Atomic-Molecular Condensates with Large Positive Scattering Length"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0210217","kind":"arxiv","version":2},"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":"sha256:1ff2a5757ad2f58110b10d634575eba1124cd0d37327e6972bae3970ec8b5596","target":"record","created_at":"2026-07-04T14:19:32Z","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":"0354ce5955f97465470c62afb43174488c976d1606fcb7778e1cf4fb942f1bc9","cross_cats_sorted":["nucl-th","physics.atom-ph"],"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2002-10-09T21:42:06Z","title_canon_sha256":"186e1e84b7f34c3e91c69add15ee1d0597cd108c08d166c15a32b30a8a8f052d"},"schema_version":"1.0","source":{"id":"cond-mat/0210217","kind":"arxiv","version":2}},"canonical_sha256":"bbad1f5267a20894c4d752369ef48cfd229cd13febcf3fadf134c47dbb47d9a4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"bbad1f5267a20894c4d752369ef48cfd229cd13febcf3fadf134c47dbb47d9a4","first_computed_at":"2026-07-04T14:19:32.238999Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T14:19:32.238999Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"tje5TqRPqrEzaE1IWOOUBc3rD4CaNmQChjpbMpm6rfWm6EdnfBSXhxhH7Y7rnNMGVqplArg5OoO8thqhNaR3CA==","signature_status":"signed_v1","signed_at":"2026-07-04T14:19:32.239349Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/0210217","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1ff2a5757ad2f58110b10d634575eba1124cd0d37327e6972bae3970ec8b5596","sha256:e0ddcc499fce2443d648a5833424cd6052873089c7c79dfe54245436d5032f01"],"state_sha256":"ed688141d8507d2f0c0838e49cf6dc1478377f8438e6f5f2abfaa1c67c5666d6"}