{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:LC6BH66BXBTGGPAUABG3GUDHNJ","short_pith_number":"pith:LC6BH66B","schema_version":"1.0","canonical_sha256":"58bc13fbc1b866633c14004db350676a57fdaa677e3621be70ecff4241e08990","source":{"kind":"arxiv","id":"cond-mat/0208567","version":1},"attestation_state":"computed","paper":{"title":"Transverse modes of a cigar-shaped Bose-Einstein condensate","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"B. Jackson, E. Zaremba","submitted_at":"2002-08-28T19:11:56Z","abstract_excerpt":"We discuss the collective modes in a harmonically trapped, highly-elongated Bose condensed gas. The transverse breathing mode exhibits a number of interesting features, such as the insensitivity of the condensate mode frequency to the interaction strength, and the closeness of the frequency to that of the non-condensed thermal cloud in the collisionless limit. Using finite temperature simulations, we show that these features are responsible for the very small damping rate observed experimentally. Our results for the temperature dependence of the damping rate and frequency shift are in excellen"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"cond-mat/0208567","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2002-08-28T19:11:56Z","cross_cats_sorted":[],"title_canon_sha256":"dc8a72d6f91d8161c58ee3dcdd984f60c9a004f75bf0a498b48864f52b7d557b","abstract_canon_sha256":"06e181e3fe4788136a900b033edee6882da834c321082f5fa668c4009f63a08f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:19:26.726117Z","signature_b64":"ksAI5Lj2WzTx9jBjj/EMo88a76B8/0NKzEUWdDpQPuzPMLmAI8WAEkOpcQQWmFzOL14KluF+i+UP+p04VvFGDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"58bc13fbc1b866633c14004db350676a57fdaa677e3621be70ecff4241e08990","last_reissued_at":"2026-07-04T14:19:26.725673Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:19:26.725673Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Transverse modes of a cigar-shaped Bose-Einstein condensate","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"B. Jackson, E. Zaremba","submitted_at":"2002-08-28T19:11:56Z","abstract_excerpt":"We discuss the collective modes in a harmonically trapped, highly-elongated Bose condensed gas. The transverse breathing mode exhibits a number of interesting features, such as the insensitivity of the condensate mode frequency to the interaction strength, and the closeness of the frequency to that of the non-condensed thermal cloud in the collisionless limit. Using finite temperature simulations, we show that these features are responsible for the very small damping rate observed experimentally. Our results for the temperature dependence of the damping rate and frequency shift are in excellen"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0208567","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/cond-mat/0208567/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0208567","created_at":"2026-07-04T14:19:26.725733+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0208567v1","created_at":"2026-07-04T14:19:26.725733+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0208567","created_at":"2026-07-04T14:19:26.725733+00:00"},{"alias_kind":"pith_short_12","alias_value":"LC6BH66BXBTG","created_at":"2026-07-04T14:19:26.725733+00:00"},{"alias_kind":"pith_short_16","alias_value":"LC6BH66BXBTGGPAU","created_at":"2026-07-04T14:19:26.725733+00:00"},{"alias_kind":"pith_short_8","alias_value":"LC6BH66B","created_at":"2026-07-04T14:19:26.725733+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LC6BH66BXBTGGPAUABG3GUDHNJ","json":"https://pith.science/pith/LC6BH66BXBTGGPAUABG3GUDHNJ.json","graph_json":"https://pith.science/api/pith-number/LC6BH66BXBTGGPAUABG3GUDHNJ/graph.json","events_json":"https://pith.science/api/pith-number/LC6BH66BXBTGGPAUABG3GUDHNJ/events.json","paper":"https://pith.science/paper/LC6BH66B"},"agent_actions":{"view_html":"https://pith.science/pith/LC6BH66BXBTGGPAUABG3GUDHNJ","download_json":"https://pith.science/pith/LC6BH66BXBTGGPAUABG3GUDHNJ.json","view_paper":"https://pith.science/paper/LC6BH66B","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/0208567&json=true","fetch_graph":"https://pith.science/api/pith-number/LC6BH66BXBTGGPAUABG3GUDHNJ/graph.json","fetch_events":"https://pith.science/api/pith-number/LC6BH66BXBTGGPAUABG3GUDHNJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LC6BH66BXBTGGPAUABG3GUDHNJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LC6BH66BXBTGGPAUABG3GUDHNJ/action/storage_attestation","attest_author":"https://pith.science/pith/LC6BH66BXBTGGPAUABG3GUDHNJ/action/author_attestation","sign_citation":"https://pith.science/pith/LC6BH66BXBTGGPAUABG3GUDHNJ/action/citation_signature","submit_replication":"https://pith.science/pith/LC6BH66BXBTGGPAUABG3GUDHNJ/action/replication_record"}},"created_at":"2026-07-04T14:19:26.725733+00:00","updated_at":"2026-07-04T14:19:26.725733+00:00"}