{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:ZOTTOWVZEODNQHMU7YOIL7Y2AH","short_pith_number":"pith:ZOTTOWVZ","canonical_record":{"source":{"id":"1207.1999","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2012-07-09T10:21:40Z","cross_cats_sorted":["physics.atom-ph","quant-ph"],"title_canon_sha256":"f13b6d541af59ddb2ddbea55feff6fbfaf301c05d2cd3fcb157a718474102055","abstract_canon_sha256":"d00139c9658530b2bf0fbc353060cd05f397a53229ca89e72aca5868636f5e21"},"schema_version":"1.0"},"canonical_sha256":"cba7375ab92386d81d94fe1c85ff1a01d6b4944f09f745644fbb1911bd0ad959","source":{"kind":"arxiv","id":"1207.1999","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1207.1999","created_at":"2026-05-18T03:48:13Z"},{"alias_kind":"arxiv_version","alias_value":"1207.1999v3","created_at":"2026-05-18T03:48:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.1999","created_at":"2026-05-18T03:48:13Z"},{"alias_kind":"pith_short_12","alias_value":"ZOTTOWVZEODN","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_16","alias_value":"ZOTTOWVZEODNQHMU","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_8","alias_value":"ZOTTOWVZ","created_at":"2026-05-18T12:27:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:ZOTTOWVZEODNQHMU7YOIL7Y2AH","target":"record","payload":{"canonical_record":{"source":{"id":"1207.1999","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2012-07-09T10:21:40Z","cross_cats_sorted":["physics.atom-ph","quant-ph"],"title_canon_sha256":"f13b6d541af59ddb2ddbea55feff6fbfaf301c05d2cd3fcb157a718474102055","abstract_canon_sha256":"d00139c9658530b2bf0fbc353060cd05f397a53229ca89e72aca5868636f5e21"},"schema_version":"1.0"},"canonical_sha256":"cba7375ab92386d81d94fe1c85ff1a01d6b4944f09f745644fbb1911bd0ad959","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:48:13.130067Z","signature_b64":"yUufVxSLfVfN3zz5epbiAUjEmeyy3aFxFCG8mBY0Wc0JYG3wUFd8sR3BCPx/Hws0/Z/xAX1BGo7myq20nRjtAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cba7375ab92386d81d94fe1c85ff1a01d6b4944f09f745644fbb1911bd0ad959","last_reissued_at":"2026-05-18T03:48:13.129401Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:48:13.129401Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1207.1999","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:48:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"J+LXf1cxRLUGt0lJfd+ErqH//4cnto97r/MUIcE1Ia1zCbbuNC1uqSU2CmdNsCDfO1vG9RUqC5Mn26ChCKkkCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T09:55:25.544558Z"},"content_sha256":"d108f9467f7e12c811a6ef3f7a92a046163345d35cbd369ff10c0158ceb9e1cc","schema_version":"1.0","event_id":"sha256:d108f9467f7e12c811a6ef3f7a92a046163345d35cbd369ff10c0158ceb9e1cc"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:ZOTTOWVZEODNQHMU7YOIL7Y2AH","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Faraday patterns in coupled one-dimensional dipolar 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":"Kazimierz {\\L}akomy, Luis Santos, Rejish Nath","submitted_at":"2012-07-09T10:21:40Z","abstract_excerpt":"We study Faraday patterns in quasi-one-dimensional dipolar Bose-Einstein condensates with parametrically driven dipolar interactions. We show that in the presence of a roton minimum in the excitation spectrum, the emergent Faraday waves differ substantially in two- and one-dimensional geometries, providing a clear example of the key role of confinement dimensionality in dipolar gases. Moreover, Faraday patterns constitute an excellent tool to study non-local effects in polar gases, as we illustrate for two parallel quasi-one-dimensional dipolar condensates. Non-local interactions between the c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.1999","kind":"arxiv","version":3},"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":"2026-05-18T03:48:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"I8/WGZbGPgC5uujX/i7OHKvm1DjGsdnaGTg/pBL7Evyt3EbyFAHySnpoQ0CVX4hiOkgcJ+Zm959m7RHbBRGXAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T09:55:25.544935Z"},"content_sha256":"db98ceb9c3442dde6ff2852944e5e83173b66ceb4834797c2feaedb5fad822d3","schema_version":"1.0","event_id":"sha256:db98ceb9c3442dde6ff2852944e5e83173b66ceb4834797c2feaedb5fad822d3"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZOTTOWVZEODNQHMU7YOIL7Y2AH/bundle.json","state_url":"https://pith.science/pith/ZOTTOWVZEODNQHMU7YOIL7Y2AH/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZOTTOWVZEODNQHMU7YOIL7Y2AH/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":"2026-06-03T09:55:25Z","links":{"resolver":"https://pith.science/pith/ZOTTOWVZEODNQHMU7YOIL7Y2AH","bundle":"https://pith.science/pith/ZOTTOWVZEODNQHMU7YOIL7Y2AH/bundle.json","state":"https://pith.science/pith/ZOTTOWVZEODNQHMU7YOIL7Y2AH/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZOTTOWVZEODNQHMU7YOIL7Y2AH/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:ZOTTOWVZEODNQHMU7YOIL7Y2AH","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":"d00139c9658530b2bf0fbc353060cd05f397a53229ca89e72aca5868636f5e21","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":"2012-07-09T10:21:40Z","title_canon_sha256":"f13b6d541af59ddb2ddbea55feff6fbfaf301c05d2cd3fcb157a718474102055"},"schema_version":"1.0","source":{"id":"1207.1999","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1207.1999","created_at":"2026-05-18T03:48:13Z"},{"alias_kind":"arxiv_version","alias_value":"1207.1999v3","created_at":"2026-05-18T03:48:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.1999","created_at":"2026-05-18T03:48:13Z"},{"alias_kind":"pith_short_12","alias_value":"ZOTTOWVZEODN","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_16","alias_value":"ZOTTOWVZEODNQHMU","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_8","alias_value":"ZOTTOWVZ","created_at":"2026-05-18T12:27:30Z"}],"graph_snapshots":[{"event_id":"sha256:db98ceb9c3442dde6ff2852944e5e83173b66ceb4834797c2feaedb5fad822d3","target":"graph","created_at":"2026-05-18T03:48:13Z","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 Faraday patterns in quasi-one-dimensional dipolar Bose-Einstein condensates with parametrically driven dipolar interactions. We show that in the presence of a roton minimum in the excitation spectrum, the emergent Faraday waves differ substantially in two- and one-dimensional geometries, providing a clear example of the key role of confinement dimensionality in dipolar gases. Moreover, Faraday patterns constitute an excellent tool to study non-local effects in polar gases, as we illustrate for two parallel quasi-one-dimensional dipolar condensates. Non-local interactions between the c","authors_text":"Kazimierz {\\L}akomy, Luis Santos, Rejish Nath","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":"2012-07-09T10:21:40Z","title":"Faraday patterns in coupled one-dimensional dipolar condensates"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.1999","kind":"arxiv","version":3},"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:d108f9467f7e12c811a6ef3f7a92a046163345d35cbd369ff10c0158ceb9e1cc","target":"record","created_at":"2026-05-18T03:48:13Z","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":"d00139c9658530b2bf0fbc353060cd05f397a53229ca89e72aca5868636f5e21","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":"2012-07-09T10:21:40Z","title_canon_sha256":"f13b6d541af59ddb2ddbea55feff6fbfaf301c05d2cd3fcb157a718474102055"},"schema_version":"1.0","source":{"id":"1207.1999","kind":"arxiv","version":3}},"canonical_sha256":"cba7375ab92386d81d94fe1c85ff1a01d6b4944f09f745644fbb1911bd0ad959","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"cba7375ab92386d81d94fe1c85ff1a01d6b4944f09f745644fbb1911bd0ad959","first_computed_at":"2026-05-18T03:48:13.129401Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:48:13.129401Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"yUufVxSLfVfN3zz5epbiAUjEmeyy3aFxFCG8mBY0Wc0JYG3wUFd8sR3BCPx/Hws0/Z/xAX1BGo7myq20nRjtAw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:48:13.130067Z","signed_message":"canonical_sha256_bytes"},"source_id":"1207.1999","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d108f9467f7e12c811a6ef3f7a92a046163345d35cbd369ff10c0158ceb9e1cc","sha256:db98ceb9c3442dde6ff2852944e5e83173b66ceb4834797c2feaedb5fad822d3"],"state_sha256":"b9582f65e9311268a94ce19e22f4b7aae42e73c6fbabb37550e3ad11c0e72eb2"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"F9FL4Wr2Q5oebfr/59aRYgHKt6MhfcyWm7PKCVHcUZyQgyxHtlNT5MUD0SljckbYzfKD4pNktfZ4O8jCf1/fCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T09:55:25.546942Z","bundle_sha256":"817db6f03b36daacb2be05fbc574be070340df4de7d104b4a2c32ff3f01d38c3"}}