{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2004:PVLNYZ3LGZHSCIF2HIRNDDXAAC","short_pith_number":"pith:PVLNYZ3L","canonical_record":{"source":{"id":"cond-mat/0408104","kind":"arxiv","version":4},"metadata":{"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2004-08-04T23:06:11Z","cross_cats_sorted":["cond-mat.quant-gas","cond-mat.str-el","cond-mat.supr-con"],"title_canon_sha256":"a5ffcca953888c6dcd0f6be48b288beec2d0cafd36ec2368bdd729b0a8fa136e","abstract_canon_sha256":"c4bc37501029b94ee2b46608d0d827c516dce0856d7cbfc52cc81d8e24d7b47f"},"schema_version":"1.0"},"canonical_sha256":"7d56dc676b364f2120ba3a22d18ee000a62d5e5d457c64259f6e8a4c755fc1b0","source":{"kind":"arxiv","id":"cond-mat/0408104","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0408104","created_at":"2026-05-18T04:13:37Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0408104v4","created_at":"2026-05-18T04:13:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0408104","created_at":"2026-05-18T04:13:37Z"},{"alias_kind":"pith_short_12","alias_value":"PVLNYZ3LGZHS","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"PVLNYZ3LGZHSCIF2","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"PVLNYZ3L","created_at":"2026-05-18T12:25:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2004:PVLNYZ3LGZHSCIF2HIRNDDXAAC","target":"record","payload":{"canonical_record":{"source":{"id":"cond-mat/0408104","kind":"arxiv","version":4},"metadata":{"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2004-08-04T23:06:11Z","cross_cats_sorted":["cond-mat.quant-gas","cond-mat.str-el","cond-mat.supr-con"],"title_canon_sha256":"a5ffcca953888c6dcd0f6be48b288beec2d0cafd36ec2368bdd729b0a8fa136e","abstract_canon_sha256":"c4bc37501029b94ee2b46608d0d827c516dce0856d7cbfc52cc81d8e24d7b47f"},"schema_version":"1.0"},"canonical_sha256":"7d56dc676b364f2120ba3a22d18ee000a62d5e5d457c64259f6e8a4c755fc1b0","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:13:37.270691Z","signature_b64":"6xALDCqZX5w/bhubzbB814HOUSMEVift0aUTTmfjvjFBBkuALaiIDQ8gL1m1cmqXf3FO+qQN4yw//Q/H39aHDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7d56dc676b364f2120ba3a22d18ee000a62d5e5d457c64259f6e8a4c755fc1b0","last_reissued_at":"2026-05-18T04:13:37.270140Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:13:37.270140Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"cond-mat/0408104","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:13:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bC1IwuejZ1NSlreM73twNBkZrFqcUjlgE4POG/cvXd44qUTwLmTFBEC6++G9K0J/vhB3YbOSt+XUA5yAbhh2Cg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T17:01:35.480472Z"},"content_sha256":"af69491f3785337c98ef3068d7c547836e967ad174c27d25c98191993b3ef0a2","schema_version":"1.0","event_id":"sha256:af69491f3785337c98ef3068d7c547836e967ad174c27d25c98191993b3ef0a2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2004:PVLNYZ3LGZHSCIF2HIRNDDXAAC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Density Profiles of Strongly Interacting Trapped Fermi Gases","license":"","headline":"","cross_cats":["cond-mat.quant-gas","cond-mat.str-el","cond-mat.supr-con"],"primary_cat":"cond-mat.stat-mech","authors_text":"Jelena Stajic, Kathryn Levin, Qijin Chen","submitted_at":"2004-08-04T23:06:11Z","abstract_excerpt":"We study density profiles in trapped fermionic gases, near Feshbach resonances, at all $T \\leq T_c$ and in the near-BEC and unitary regimes. For the latter, we quantify and characterize the generally neglected contribution from noncondensed Cooper pairs. As a consequence of these pairs, our profiles are rather well fit to a Thomas-Fermi (TF) functional form, and equally well fit to experimental data. Our work lends support to the notion that TF fits can be used in an experimental context to obtain information about the temperature."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0408104","kind":"arxiv","version":4},"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":"2026-05-18T04:13:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"O+11uk6JqMU8Nt9TkmBpgzXNHw605LbkEhv36olLMrMmwuaplEFivSpExs3wciuCvLuh7gQmu3wVU9hSSBovCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T17:01:35.480823Z"},"content_sha256":"a395544add7a3165e8b705b193541b03c1a4bd9635804fd46245181ecf719907","schema_version":"1.0","event_id":"sha256:a395544add7a3165e8b705b193541b03c1a4bd9635804fd46245181ecf719907"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PVLNYZ3LGZHSCIF2HIRNDDXAAC/bundle.json","state_url":"https://pith.science/pith/PVLNYZ3LGZHSCIF2HIRNDDXAAC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PVLNYZ3LGZHSCIF2HIRNDDXAAC/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":"2026-06-01T17:01:35Z","links":{"resolver":"https://pith.science/pith/PVLNYZ3LGZHSCIF2HIRNDDXAAC","bundle":"https://pith.science/pith/PVLNYZ3LGZHSCIF2HIRNDDXAAC/bundle.json","state":"https://pith.science/pith/PVLNYZ3LGZHSCIF2HIRNDDXAAC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PVLNYZ3LGZHSCIF2HIRNDDXAAC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2004:PVLNYZ3LGZHSCIF2HIRNDDXAAC","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":"c4bc37501029b94ee2b46608d0d827c516dce0856d7cbfc52cc81d8e24d7b47f","cross_cats_sorted":["cond-mat.quant-gas","cond-mat.str-el","cond-mat.supr-con"],"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2004-08-04T23:06:11Z","title_canon_sha256":"a5ffcca953888c6dcd0f6be48b288beec2d0cafd36ec2368bdd729b0a8fa136e"},"schema_version":"1.0","source":{"id":"cond-mat/0408104","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0408104","created_at":"2026-05-18T04:13:37Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0408104v4","created_at":"2026-05-18T04:13:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0408104","created_at":"2026-05-18T04:13:37Z"},{"alias_kind":"pith_short_12","alias_value":"PVLNYZ3LGZHS","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"PVLNYZ3LGZHSCIF2","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"PVLNYZ3L","created_at":"2026-05-18T12:25:52Z"}],"graph_snapshots":[{"event_id":"sha256:a395544add7a3165e8b705b193541b03c1a4bd9635804fd46245181ecf719907","target":"graph","created_at":"2026-05-18T04:13:37Z","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 study density profiles in trapped fermionic gases, near Feshbach resonances, at all $T \\leq T_c$ and in the near-BEC and unitary regimes. For the latter, we quantify and characterize the generally neglected contribution from noncondensed Cooper pairs. As a consequence of these pairs, our profiles are rather well fit to a Thomas-Fermi (TF) functional form, and equally well fit to experimental data. Our work lends support to the notion that TF fits can be used in an experimental context to obtain information about the temperature.","authors_text":"Jelena Stajic, Kathryn Levin, Qijin Chen","cross_cats":["cond-mat.quant-gas","cond-mat.str-el","cond-mat.supr-con"],"headline":"","license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2004-08-04T23:06:11Z","title":"Density Profiles of Strongly Interacting Trapped Fermi Gases"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0408104","kind":"arxiv","version":4},"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:af69491f3785337c98ef3068d7c547836e967ad174c27d25c98191993b3ef0a2","target":"record","created_at":"2026-05-18T04:13:37Z","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":"c4bc37501029b94ee2b46608d0d827c516dce0856d7cbfc52cc81d8e24d7b47f","cross_cats_sorted":["cond-mat.quant-gas","cond-mat.str-el","cond-mat.supr-con"],"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2004-08-04T23:06:11Z","title_canon_sha256":"a5ffcca953888c6dcd0f6be48b288beec2d0cafd36ec2368bdd729b0a8fa136e"},"schema_version":"1.0","source":{"id":"cond-mat/0408104","kind":"arxiv","version":4}},"canonical_sha256":"7d56dc676b364f2120ba3a22d18ee000a62d5e5d457c64259f6e8a4c755fc1b0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7d56dc676b364f2120ba3a22d18ee000a62d5e5d457c64259f6e8a4c755fc1b0","first_computed_at":"2026-05-18T04:13:37.270140Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:13:37.270140Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"6xALDCqZX5w/bhubzbB814HOUSMEVift0aUTTmfjvjFBBkuALaiIDQ8gL1m1cmqXf3FO+qQN4yw//Q/H39aHDg==","signature_status":"signed_v1","signed_at":"2026-05-18T04:13:37.270691Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/0408104","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:af69491f3785337c98ef3068d7c547836e967ad174c27d25c98191993b3ef0a2","sha256:a395544add7a3165e8b705b193541b03c1a4bd9635804fd46245181ecf719907"],"state_sha256":"5b948f9bdefb27a1b36bc1210df0b5804189a762006aebf3e9524c6d3c336686"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zlmursvJ5zOzOC2MLg+/KDrMcxmpu2NGUQW+6cERoHsfuNAKLEQbcBSY/OveKjONmSGQL6VBtuSHxCcpJaFUDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T17:01:35.482820Z","bundle_sha256":"6c6641e77884028cba3f349e132a193326e6c40c27bdf6904e8210c5cf30ccc5"}}