{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:2ZBPOK3HPYP4ET6B773HPGM5CZ","short_pith_number":"pith:2ZBPOK3H","canonical_record":{"source":{"id":"1710.04147","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2017-10-11T16:08:12Z","cross_cats_sorted":["nucl-th","physics.atom-ph","quant-ph"],"title_canon_sha256":"b57953cc92f3df96602dfd6e07a893f00cba8dca99387886a48903031ae40573","abstract_canon_sha256":"5fb2ffdf15bdb1bb428b70e58deae17bea1b3c1b2e6b86fea16007c16237b915"},"schema_version":"1.0"},"canonical_sha256":"d642f72b677e1fc24fc1fff677999d1678ea2a8260089f8c034924a317cf7727","source":{"kind":"arxiv","id":"1710.04147","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.04147","created_at":"2026-05-18T00:33:04Z"},{"alias_kind":"arxiv_version","alias_value":"1710.04147v1","created_at":"2026-05-18T00:33:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.04147","created_at":"2026-05-18T00:33:04Z"},{"alias_kind":"pith_short_12","alias_value":"2ZBPOK3HPYP4","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_16","alias_value":"2ZBPOK3HPYP4ET6B","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_8","alias_value":"2ZBPOK3H","created_at":"2026-05-18T12:30:55Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:2ZBPOK3HPYP4ET6B773HPGM5CZ","target":"record","payload":{"canonical_record":{"source":{"id":"1710.04147","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2017-10-11T16:08:12Z","cross_cats_sorted":["nucl-th","physics.atom-ph","quant-ph"],"title_canon_sha256":"b57953cc92f3df96602dfd6e07a893f00cba8dca99387886a48903031ae40573","abstract_canon_sha256":"5fb2ffdf15bdb1bb428b70e58deae17bea1b3c1b2e6b86fea16007c16237b915"},"schema_version":"1.0"},"canonical_sha256":"d642f72b677e1fc24fc1fff677999d1678ea2a8260089f8c034924a317cf7727","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:33:04.785074Z","signature_b64":"31eXC4w7Vk1JBtPQVsjo2lwCwXO7wAjgFm22AkC6Ux5zt1MeBg1auUnS7GMk5fli1MGPNwVqbyGeeycyM6HMCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d642f72b677e1fc24fc1fff677999d1678ea2a8260089f8c034924a317cf7727","last_reissued_at":"2026-05-18T00:33:04.784407Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:33:04.784407Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1710.04147","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":"2026-05-18T00:33:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UE1Ob0slYXUMxsPbjVK5H2ITzridZ50VW2EGiKjixxBcHwiCOiZOzJrlK82nsg6jiMdPP5f58EF697R+BpvxDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T15:13:24.485100Z"},"content_sha256":"57aec06e1b8eac110a8098e2dc69a58fa1ed2c13044db79f7f2f5e44c792bffc","schema_version":"1.0","event_id":"sha256:57aec06e1b8eac110a8098e2dc69a58fa1ed2c13044db79f7f2f5e44c792bffc"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:2ZBPOK3HPYP4ET6B773HPGM5CZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Three-body scattering hypervolumes of particles with short-range interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th","physics.atom-ph","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"Shangguo Zhu, Shina Tan","submitted_at":"2017-10-11T16:08:12Z","abstract_excerpt":"The low-energy scattering of three bosons or distinguishable particles with short-range interactions is characterized by a fundamental parameter, the three-body scattering hypervolume. Its imaginary part is directly related to the three-body recombination rate in a quantum gas consisting of such particles. We derive an analytical formula of it for weak interactions, and perform its first numerical calculations for bosons with a variable nonzero-range potential. For attractive interactions, we identify several three-body resonances at which the three-body scattering hypervolume becomes divergen"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.04147","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":"2026-05-18T00:33:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sMbcua4j2KOBOzexxH3m9k8ND+IRikcMPGloCyub86o2hyRfm7uIhDfslXHG6fMnZjmEFaNdxtNqhgTvfpwbDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T15:13:24.485740Z"},"content_sha256":"59ec1dd9295e96875450bad72b8a089046debfd9a929d71d753180141aa2abaa","schema_version":"1.0","event_id":"sha256:59ec1dd9295e96875450bad72b8a089046debfd9a929d71d753180141aa2abaa"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2ZBPOK3HPYP4ET6B773HPGM5CZ/bundle.json","state_url":"https://pith.science/pith/2ZBPOK3HPYP4ET6B773HPGM5CZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2ZBPOK3HPYP4ET6B773HPGM5CZ/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":"2026-05-21T15:13:24Z","links":{"resolver":"https://pith.science/pith/2ZBPOK3HPYP4ET6B773HPGM5CZ","bundle":"https://pith.science/pith/2ZBPOK3HPYP4ET6B773HPGM5CZ/bundle.json","state":"https://pith.science/pith/2ZBPOK3HPYP4ET6B773HPGM5CZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2ZBPOK3HPYP4ET6B773HPGM5CZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:2ZBPOK3HPYP4ET6B773HPGM5CZ","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":"5fb2ffdf15bdb1bb428b70e58deae17bea1b3c1b2e6b86fea16007c16237b915","cross_cats_sorted":["nucl-th","physics.atom-ph","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2017-10-11T16:08:12Z","title_canon_sha256":"b57953cc92f3df96602dfd6e07a893f00cba8dca99387886a48903031ae40573"},"schema_version":"1.0","source":{"id":"1710.04147","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.04147","created_at":"2026-05-18T00:33:04Z"},{"alias_kind":"arxiv_version","alias_value":"1710.04147v1","created_at":"2026-05-18T00:33:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.04147","created_at":"2026-05-18T00:33:04Z"},{"alias_kind":"pith_short_12","alias_value":"2ZBPOK3HPYP4","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_16","alias_value":"2ZBPOK3HPYP4ET6B","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_8","alias_value":"2ZBPOK3H","created_at":"2026-05-18T12:30:55Z"}],"graph_snapshots":[{"event_id":"sha256:59ec1dd9295e96875450bad72b8a089046debfd9a929d71d753180141aa2abaa","target":"graph","created_at":"2026-05-18T00:33:04Z","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 low-energy scattering of three bosons or distinguishable particles with short-range interactions is characterized by a fundamental parameter, the three-body scattering hypervolume. Its imaginary part is directly related to the three-body recombination rate in a quantum gas consisting of such particles. We derive an analytical formula of it for weak interactions, and perform its first numerical calculations for bosons with a variable nonzero-range potential. For attractive interactions, we identify several three-body resonances at which the three-body scattering hypervolume becomes divergen","authors_text":"Shangguo Zhu, Shina Tan","cross_cats":["nucl-th","physics.atom-ph","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2017-10-11T16:08:12Z","title":"Three-body scattering hypervolumes of particles with short-range interactions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.04147","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":"sha256:57aec06e1b8eac110a8098e2dc69a58fa1ed2c13044db79f7f2f5e44c792bffc","target":"record","created_at":"2026-05-18T00:33:04Z","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":"5fb2ffdf15bdb1bb428b70e58deae17bea1b3c1b2e6b86fea16007c16237b915","cross_cats_sorted":["nucl-th","physics.atom-ph","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2017-10-11T16:08:12Z","title_canon_sha256":"b57953cc92f3df96602dfd6e07a893f00cba8dca99387886a48903031ae40573"},"schema_version":"1.0","source":{"id":"1710.04147","kind":"arxiv","version":1}},"canonical_sha256":"d642f72b677e1fc24fc1fff677999d1678ea2a8260089f8c034924a317cf7727","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d642f72b677e1fc24fc1fff677999d1678ea2a8260089f8c034924a317cf7727","first_computed_at":"2026-05-18T00:33:04.784407Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:33:04.784407Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"31eXC4w7Vk1JBtPQVsjo2lwCwXO7wAjgFm22AkC6Ux5zt1MeBg1auUnS7GMk5fli1MGPNwVqbyGeeycyM6HMCw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:33:04.785074Z","signed_message":"canonical_sha256_bytes"},"source_id":"1710.04147","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:57aec06e1b8eac110a8098e2dc69a58fa1ed2c13044db79f7f2f5e44c792bffc","sha256:59ec1dd9295e96875450bad72b8a089046debfd9a929d71d753180141aa2abaa"],"state_sha256":"ad778dddc945c9a25b2d65e1e68e322f3b3a2ac3483f9eae8a358e9cb6253b50"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"EgrtkqrWiV9zwLVTgSxWNBbwfmo0OQE/vDVCYs9Mz3ux0ivJHE/qnvyeEhHaDiEbNnzBqWmqfFbm6eexmw1kDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-21T15:13:24.488677Z","bundle_sha256":"77e02b5d9f83c93fd29fb50b3ab22513963c815035cdf43f09c98361826846cd"}}