{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:PZVDWTK2MR334XMNGUC6A3PZ3A","short_pith_number":"pith:PZVDWTK2","canonical_record":{"source":{"id":"1003.5873","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2010-03-30T17:30:58Z","cross_cats_sorted":["math-ph","math.MP","quant-ph"],"title_canon_sha256":"5480712c8170b3975768b8b489318d93af8c0acd288ea16c93c7adec2f9f0846","abstract_canon_sha256":"2003efb58a5b2203b1511b9f1758840271322c99a8ac3f6d5589451256466122"},"schema_version":"1.0"},"canonical_sha256":"7e6a3b4d5a6477be5d8d3505e06df9d82ff050107d6b04c9bf8744aaf1c8764e","source":{"kind":"arxiv","id":"1003.5873","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1003.5873","created_at":"2026-05-18T02:24:26Z"},{"alias_kind":"arxiv_version","alias_value":"1003.5873v2","created_at":"2026-05-18T02:24:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1003.5873","created_at":"2026-05-18T02:24:26Z"},{"alias_kind":"pith_short_12","alias_value":"PZVDWTK2MR33","created_at":"2026-05-18T12:26:12Z"},{"alias_kind":"pith_short_16","alias_value":"PZVDWTK2MR334XMN","created_at":"2026-05-18T12:26:12Z"},{"alias_kind":"pith_short_8","alias_value":"PZVDWTK2","created_at":"2026-05-18T12:26:12Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:PZVDWTK2MR334XMNGUC6A3PZ3A","target":"record","payload":{"canonical_record":{"source":{"id":"1003.5873","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2010-03-30T17:30:58Z","cross_cats_sorted":["math-ph","math.MP","quant-ph"],"title_canon_sha256":"5480712c8170b3975768b8b489318d93af8c0acd288ea16c93c7adec2f9f0846","abstract_canon_sha256":"2003efb58a5b2203b1511b9f1758840271322c99a8ac3f6d5589451256466122"},"schema_version":"1.0"},"canonical_sha256":"7e6a3b4d5a6477be5d8d3505e06df9d82ff050107d6b04c9bf8744aaf1c8764e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:24:26.017174Z","signature_b64":"AGCT2j6FVExJfmVZUwVrOty6vowBPxWypCCz+4s/kQRF/EakpA3sSCs6W2GV896eOkfUrhxhAGsoSOYsrq5uBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7e6a3b4d5a6477be5d8d3505e06df9d82ff050107d6b04c9bf8744aaf1c8764e","last_reissued_at":"2026-05-18T02:24:26.016405Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:24:26.016405Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1003.5873","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:24:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RwZwh3ar7RS2Rb1iW0oLRlyLWnqLf+V8ptP88xaoYSkKpTHiaUXtfTCtdN0bYD7suER2qXoX6PyBbBKqMSQ/BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T18:47:45.320537Z"},"content_sha256":"b8a96e68c226a0cf08178b924bf658fcf4ce486f641041e3d657a67939272ee5","schema_version":"1.0","event_id":"sha256:b8a96e68c226a0cf08178b924bf658fcf4ce486f641041e3d657a67939272ee5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:PZVDWTK2MR334XMNGUC6A3PZ3A","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Bound States and Universality in Layers of Cold Polar Molecules","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"A. S. Jensen, D. V. Fedorov, J. R. Armstrong, N. T. Zinner","submitted_at":"2010-03-30T17:30:58Z","abstract_excerpt":"The recent experimental realization of cold polar molecules in the rotational and vibrational ground state opens the door to the study of a wealth of phenomena involving long-range interactions. By applying an optical lattice to a gas of cold polar molecules one can create a layered system of planar traps. Due to the long-range dipole-dipole interaction one expects a rich structure of bound complexes in this geometry. We study the bilayer case and determine the two-body bound state properties as a function of the interaction strength. The results clearly show that a least one bound state will "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1003.5873","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:24:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yBvMy4B1aNw4FwBbMBx0qiWQt8wpForB97qpTkuNfqF2gNq+PUWGQaluyY8AZ8uUSAR38G0EuaESrzWIc3FGAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T18:47:45.321291Z"},"content_sha256":"8b176ae29e85f22651ced39d56c298f42f91c7654b55f845546bcffd3c21ddff","schema_version":"1.0","event_id":"sha256:8b176ae29e85f22651ced39d56c298f42f91c7654b55f845546bcffd3c21ddff"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PZVDWTK2MR334XMNGUC6A3PZ3A/bundle.json","state_url":"https://pith.science/pith/PZVDWTK2MR334XMNGUC6A3PZ3A/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PZVDWTK2MR334XMNGUC6A3PZ3A/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":"2026-05-25T18:47:45Z","links":{"resolver":"https://pith.science/pith/PZVDWTK2MR334XMNGUC6A3PZ3A","bundle":"https://pith.science/pith/PZVDWTK2MR334XMNGUC6A3PZ3A/bundle.json","state":"https://pith.science/pith/PZVDWTK2MR334XMNGUC6A3PZ3A/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PZVDWTK2MR334XMNGUC6A3PZ3A/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:PZVDWTK2MR334XMNGUC6A3PZ3A","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":"2003efb58a5b2203b1511b9f1758840271322c99a8ac3f6d5589451256466122","cross_cats_sorted":["math-ph","math.MP","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2010-03-30T17:30:58Z","title_canon_sha256":"5480712c8170b3975768b8b489318d93af8c0acd288ea16c93c7adec2f9f0846"},"schema_version":"1.0","source":{"id":"1003.5873","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1003.5873","created_at":"2026-05-18T02:24:26Z"},{"alias_kind":"arxiv_version","alias_value":"1003.5873v2","created_at":"2026-05-18T02:24:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1003.5873","created_at":"2026-05-18T02:24:26Z"},{"alias_kind":"pith_short_12","alias_value":"PZVDWTK2MR33","created_at":"2026-05-18T12:26:12Z"},{"alias_kind":"pith_short_16","alias_value":"PZVDWTK2MR334XMN","created_at":"2026-05-18T12:26:12Z"},{"alias_kind":"pith_short_8","alias_value":"PZVDWTK2","created_at":"2026-05-18T12:26:12Z"}],"graph_snapshots":[{"event_id":"sha256:8b176ae29e85f22651ced39d56c298f42f91c7654b55f845546bcffd3c21ddff","target":"graph","created_at":"2026-05-18T02:24:26Z","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":"The recent experimental realization of cold polar molecules in the rotational and vibrational ground state opens the door to the study of a wealth of phenomena involving long-range interactions. By applying an optical lattice to a gas of cold polar molecules one can create a layered system of planar traps. Due to the long-range dipole-dipole interaction one expects a rich structure of bound complexes in this geometry. We study the bilayer case and determine the two-body bound state properties as a function of the interaction strength. The results clearly show that a least one bound state will ","authors_text":"A. S. Jensen, D. V. Fedorov, J. R. Armstrong, N. T. Zinner","cross_cats":["math-ph","math.MP","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2010-03-30T17:30:58Z","title":"Bound States and Universality in Layers of Cold Polar Molecules"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1003.5873","kind":"arxiv","version":2},"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:b8a96e68c226a0cf08178b924bf658fcf4ce486f641041e3d657a67939272ee5","target":"record","created_at":"2026-05-18T02:24:26Z","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":"2003efb58a5b2203b1511b9f1758840271322c99a8ac3f6d5589451256466122","cross_cats_sorted":["math-ph","math.MP","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2010-03-30T17:30:58Z","title_canon_sha256":"5480712c8170b3975768b8b489318d93af8c0acd288ea16c93c7adec2f9f0846"},"schema_version":"1.0","source":{"id":"1003.5873","kind":"arxiv","version":2}},"canonical_sha256":"7e6a3b4d5a6477be5d8d3505e06df9d82ff050107d6b04c9bf8744aaf1c8764e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7e6a3b4d5a6477be5d8d3505e06df9d82ff050107d6b04c9bf8744aaf1c8764e","first_computed_at":"2026-05-18T02:24:26.016405Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:24:26.016405Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"AGCT2j6FVExJfmVZUwVrOty6vowBPxWypCCz+4s/kQRF/EakpA3sSCs6W2GV896eOkfUrhxhAGsoSOYsrq5uBA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:24:26.017174Z","signed_message":"canonical_sha256_bytes"},"source_id":"1003.5873","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b8a96e68c226a0cf08178b924bf658fcf4ce486f641041e3d657a67939272ee5","sha256:8b176ae29e85f22651ced39d56c298f42f91c7654b55f845546bcffd3c21ddff"],"state_sha256":"f0caa092dd3223bef92071534536ff815e5671666ffd63d2824110acb03b9bab"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ig3n3heCK6Ud2HUaacyvSaw7DV18ddms/IXZdN9BdPJvcnGhjRCVxTN3YOYyH8kFOb0bR+njY1XhgDB+rdGMDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T18:47:45.325069Z","bundle_sha256":"b44e8c6f95d4c4895e9a249f489e92fe652079c25523cd0bb36eabbd0e4a671c"}}