{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:7ZIY4KFNWLA7YSW5EBJ2O3TDY5","short_pith_number":"pith:7ZIY4KFN","canonical_record":{"source":{"id":"1105.1189","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2011-05-05T22:44:52Z","cross_cats_sorted":["physics.atom-ph","quant-ph"],"title_canon_sha256":"cb8d8408cbe820ea861acd46c044ec1eca3b62d287847ce3955f095854130ab0","abstract_canon_sha256":"f1c81690a191b8841105cba3758d271ac0a8f533fb237fafa5a5433fd9fcd52b"},"schema_version":"1.0"},"canonical_sha256":"fe518e28adb2c1fc4add2053a76e63c7551e9fffe6c2773798a7497dbf36afa4","source":{"kind":"arxiv","id":"1105.1189","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1105.1189","created_at":"2026-05-18T04:07:07Z"},{"alias_kind":"arxiv_version","alias_value":"1105.1189v1","created_at":"2026-05-18T04:07:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.1189","created_at":"2026-05-18T04:07:07Z"},{"alias_kind":"pith_short_12","alias_value":"7ZIY4KFNWLA7","created_at":"2026-05-18T12:26:22Z"},{"alias_kind":"pith_short_16","alias_value":"7ZIY4KFNWLA7YSW5","created_at":"2026-05-18T12:26:22Z"},{"alias_kind":"pith_short_8","alias_value":"7ZIY4KFN","created_at":"2026-05-18T12:26:22Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:7ZIY4KFNWLA7YSW5EBJ2O3TDY5","target":"record","payload":{"canonical_record":{"source":{"id":"1105.1189","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2011-05-05T22:44:52Z","cross_cats_sorted":["physics.atom-ph","quant-ph"],"title_canon_sha256":"cb8d8408cbe820ea861acd46c044ec1eca3b62d287847ce3955f095854130ab0","abstract_canon_sha256":"f1c81690a191b8841105cba3758d271ac0a8f533fb237fafa5a5433fd9fcd52b"},"schema_version":"1.0"},"canonical_sha256":"fe518e28adb2c1fc4add2053a76e63c7551e9fffe6c2773798a7497dbf36afa4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:07:07.891556Z","signature_b64":"HtmxxJsoK9VugRnBeUMJcnQV5QAg8m7K68LWnKwFIA+vVcnTa3ICo1B7i1/l/oyxmtKUApDbeWf7IpPSF9FKDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fe518e28adb2c1fc4add2053a76e63c7551e9fffe6c2773798a7497dbf36afa4","last_reissued_at":"2026-05-18T04:07:07.890852Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:07:07.890852Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1105.1189","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":"2026-05-18T04:07:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IjuRI4giwlUjIFrNtKk/mQBNWNWWdMVggt+5KwPbAQ/WBkKMOBzvjCRerfI1qswYS2wRJrvmRWaQluYdIP0xCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T07:09:47.169005Z"},"content_sha256":"1fd01be0be848b3d438fef65878d1d17c5ff95cc78b86c133514712135bb29b3","schema_version":"1.0","event_id":"sha256:1fd01be0be848b3d438fef65878d1d17c5ff95cc78b86c133514712135bb29b3"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:7ZIY4KFNWLA7YSW5EBJ2O3TDY5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Suppression of Kelvon-induced decay of quantized vortices in oblate Bose-Einstein Condensates","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":"A. S. Bradley, B. P. Anderson, P. B. Blakie, S. J. Rooney","submitted_at":"2011-05-05T22:44:52Z","abstract_excerpt":"We study the Kelvin mode excitations on a vortex line in a three-dimensional trapped Bose-Einstein condensate at finite temperature. Our stochastic Gross-Pitaevskii simulations show that the activation of these modes can be suppressed by tightening the confinement along the direction of the vortex line, leading to a strong suppression in the vortex decay rate as the system enters a regime of two-dimensional vortex dynamics. As the system approaches the condensation transition temperature we find that the vortex decay rate is strongly sensitive to dimensionality and temperature, observing a lar"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.1189","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":"2026-05-18T04:07:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3O2itqMVKZMEpsMA849gyp+HFmfP4Ve1tUe6zsMlwwlGqW4CUygAzQsZN5OakdcNG7sgbAxhd+xN4OlwSwYYCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T07:09:47.169713Z"},"content_sha256":"63dd87366554187b584fc6c17afc7f3078952bf101a4cc55662aae89886c8147","schema_version":"1.0","event_id":"sha256:63dd87366554187b584fc6c17afc7f3078952bf101a4cc55662aae89886c8147"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7ZIY4KFNWLA7YSW5EBJ2O3TDY5/bundle.json","state_url":"https://pith.science/pith/7ZIY4KFNWLA7YSW5EBJ2O3TDY5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7ZIY4KFNWLA7YSW5EBJ2O3TDY5/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":"2026-05-27T07:09:47Z","links":{"resolver":"https://pith.science/pith/7ZIY4KFNWLA7YSW5EBJ2O3TDY5","bundle":"https://pith.science/pith/7ZIY4KFNWLA7YSW5EBJ2O3TDY5/bundle.json","state":"https://pith.science/pith/7ZIY4KFNWLA7YSW5EBJ2O3TDY5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7ZIY4KFNWLA7YSW5EBJ2O3TDY5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:7ZIY4KFNWLA7YSW5EBJ2O3TDY5","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":"f1c81690a191b8841105cba3758d271ac0a8f533fb237fafa5a5433fd9fcd52b","cross_cats_sorted":["physics.atom-ph","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2011-05-05T22:44:52Z","title_canon_sha256":"cb8d8408cbe820ea861acd46c044ec1eca3b62d287847ce3955f095854130ab0"},"schema_version":"1.0","source":{"id":"1105.1189","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1105.1189","created_at":"2026-05-18T04:07:07Z"},{"alias_kind":"arxiv_version","alias_value":"1105.1189v1","created_at":"2026-05-18T04:07:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.1189","created_at":"2026-05-18T04:07:07Z"},{"alias_kind":"pith_short_12","alias_value":"7ZIY4KFNWLA7","created_at":"2026-05-18T12:26:22Z"},{"alias_kind":"pith_short_16","alias_value":"7ZIY4KFNWLA7YSW5","created_at":"2026-05-18T12:26:22Z"},{"alias_kind":"pith_short_8","alias_value":"7ZIY4KFN","created_at":"2026-05-18T12:26:22Z"}],"graph_snapshots":[{"event_id":"sha256:63dd87366554187b584fc6c17afc7f3078952bf101a4cc55662aae89886c8147","target":"graph","created_at":"2026-05-18T04:07:07Z","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 the Kelvin mode excitations on a vortex line in a three-dimensional trapped Bose-Einstein condensate at finite temperature. Our stochastic Gross-Pitaevskii simulations show that the activation of these modes can be suppressed by tightening the confinement along the direction of the vortex line, leading to a strong suppression in the vortex decay rate as the system enters a regime of two-dimensional vortex dynamics. As the system approaches the condensation transition temperature we find that the vortex decay rate is strongly sensitive to dimensionality and temperature, observing a lar","authors_text":"A. S. Bradley, B. P. Anderson, P. B. Blakie, S. J. Rooney","cross_cats":["physics.atom-ph","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2011-05-05T22:44:52Z","title":"Suppression of Kelvon-induced decay of quantized vortices in oblate Bose-Einstein Condensates"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.1189","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":"sha256:1fd01be0be848b3d438fef65878d1d17c5ff95cc78b86c133514712135bb29b3","target":"record","created_at":"2026-05-18T04:07:07Z","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":"f1c81690a191b8841105cba3758d271ac0a8f533fb237fafa5a5433fd9fcd52b","cross_cats_sorted":["physics.atom-ph","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2011-05-05T22:44:52Z","title_canon_sha256":"cb8d8408cbe820ea861acd46c044ec1eca3b62d287847ce3955f095854130ab0"},"schema_version":"1.0","source":{"id":"1105.1189","kind":"arxiv","version":1}},"canonical_sha256":"fe518e28adb2c1fc4add2053a76e63c7551e9fffe6c2773798a7497dbf36afa4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"fe518e28adb2c1fc4add2053a76e63c7551e9fffe6c2773798a7497dbf36afa4","first_computed_at":"2026-05-18T04:07:07.890852Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:07:07.890852Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"HtmxxJsoK9VugRnBeUMJcnQV5QAg8m7K68LWnKwFIA+vVcnTa3ICo1B7i1/l/oyxmtKUApDbeWf7IpPSF9FKDA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:07:07.891556Z","signed_message":"canonical_sha256_bytes"},"source_id":"1105.1189","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1fd01be0be848b3d438fef65878d1d17c5ff95cc78b86c133514712135bb29b3","sha256:63dd87366554187b584fc6c17afc7f3078952bf101a4cc55662aae89886c8147"],"state_sha256":"d9f192be984af5e699a2672c10040de8468bb4e9348d96b974e0ddc9b1278079"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"H7ixD2v9kiGO+/8/WJ66fIcp7C7TYKRH9B5yp3jsi6Tx479d9TAXczE7FngUBjJYKKmsHRISI10cpHeTbZwNDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T07:09:47.173162Z","bundle_sha256":"33e49cba9ecb84c2c458de5ee5fe5c57632d372de76a493ce3e2a9e14aff369b"}}