{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:VDJLL5SQYLB3IXHISKQFSOVJFH","short_pith_number":"pith:VDJLL5SQ","schema_version":"1.0","canonical_sha256":"a8d2b5f650c2c3b45ce892a0593aa929d6d538e2679363de0bcaeddca80f09ca","source":{"kind":"arxiv","id":"1210.0033","version":2},"attestation_state":"computed","paper":{"title":"Collective Excitation Interferometry with a Toroidal Bose-Einstein Condensate","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"Dan M. Stamper-Kurn, G. Edward Marti, Ryan Olf","submitted_at":"2012-09-28T20:48:11Z","abstract_excerpt":"The precision of compact inertial sensing schemes using trapped- and guided-atom interferometers has been limited by uncontrolled phase errors caused by trapping potentials and interactions. Here, we propose an acoustic interferometer that uses sound waves in a toroidal Bose-Einstein condensate to measure rotation, and we demonstrate experimentally several key aspects of this type of interferometer. We use spatially patterned light beams to excite counter-propagating sound waves within the condensate and use \\emph{in situ} absorption imaging to characterize their evolution. We present an analy"},"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":"1210.0033","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2012-09-28T20:48:11Z","cross_cats_sorted":["physics.atom-ph","quant-ph"],"title_canon_sha256":"da91cd7f3ab3d4884bf847924c7a5a78f65b606e535ed318b6b3a4ed8b8f5ac9","abstract_canon_sha256":"817f73d7bd612e673e03200c4e559a8b2db808ef55404dbe709ac8b02e7397b5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:28:48.414881Z","signature_b64":"VVpyWM90y4CgLGgEm2Q36ruvMzcYBDjiNWDxqyhbaZi8KOW2uFjvHDOdfTSyQRt9rGn0v1DDRQdpjhCF+QwVBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a8d2b5f650c2c3b45ce892a0593aa929d6d538e2679363de0bcaeddca80f09ca","last_reissued_at":"2026-05-18T02:28:48.414517Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:28:48.414517Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Collective Excitation Interferometry with a Toroidal Bose-Einstein Condensate","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"Dan M. Stamper-Kurn, G. Edward Marti, Ryan Olf","submitted_at":"2012-09-28T20:48:11Z","abstract_excerpt":"The precision of compact inertial sensing schemes using trapped- and guided-atom interferometers has been limited by uncontrolled phase errors caused by trapping potentials and interactions. Here, we propose an acoustic interferometer that uses sound waves in a toroidal Bose-Einstein condensate to measure rotation, and we demonstrate experimentally several key aspects of this type of interferometer. We use spatially patterned light beams to excite counter-propagating sound waves within the condensate and use \\emph{in situ} absorption imaging to characterize their evolution. We present an analy"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.0033","kind":"arxiv","version":2},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1210.0033","created_at":"2026-05-18T02:28:48.414576+00:00"},{"alias_kind":"arxiv_version","alias_value":"1210.0033v2","created_at":"2026-05-18T02:28:48.414576+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.0033","created_at":"2026-05-18T02:28:48.414576+00:00"},{"alias_kind":"pith_short_12","alias_value":"VDJLL5SQYLB3","created_at":"2026-05-18T12:27:25.539911+00:00"},{"alias_kind":"pith_short_16","alias_value":"VDJLL5SQYLB3IXHI","created_at":"2026-05-18T12:27:25.539911+00:00"},{"alias_kind":"pith_short_8","alias_value":"VDJLL5SQ","created_at":"2026-05-18T12:27:25.539911+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/VDJLL5SQYLB3IXHISKQFSOVJFH","json":"https://pith.science/pith/VDJLL5SQYLB3IXHISKQFSOVJFH.json","graph_json":"https://pith.science/api/pith-number/VDJLL5SQYLB3IXHISKQFSOVJFH/graph.json","events_json":"https://pith.science/api/pith-number/VDJLL5SQYLB3IXHISKQFSOVJFH/events.json","paper":"https://pith.science/paper/VDJLL5SQ"},"agent_actions":{"view_html":"https://pith.science/pith/VDJLL5SQYLB3IXHISKQFSOVJFH","download_json":"https://pith.science/pith/VDJLL5SQYLB3IXHISKQFSOVJFH.json","view_paper":"https://pith.science/paper/VDJLL5SQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1210.0033&json=true","fetch_graph":"https://pith.science/api/pith-number/VDJLL5SQYLB3IXHISKQFSOVJFH/graph.json","fetch_events":"https://pith.science/api/pith-number/VDJLL5SQYLB3IXHISKQFSOVJFH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VDJLL5SQYLB3IXHISKQFSOVJFH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VDJLL5SQYLB3IXHISKQFSOVJFH/action/storage_attestation","attest_author":"https://pith.science/pith/VDJLL5SQYLB3IXHISKQFSOVJFH/action/author_attestation","sign_citation":"https://pith.science/pith/VDJLL5SQYLB3IXHISKQFSOVJFH/action/citation_signature","submit_replication":"https://pith.science/pith/VDJLL5SQYLB3IXHISKQFSOVJFH/action/replication_record"}},"created_at":"2026-05-18T02:28:48.414576+00:00","updated_at":"2026-05-18T02:28:48.414576+00:00"}