{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:ZZNYQGSIJU2KPY2QAPM3MCQQZP","short_pith_number":"pith:ZZNYQGSI","canonical_record":{"source":{"id":"1307.6813","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2013-07-25T17:04:32Z","cross_cats_sorted":["math-ph","math.MP","nucl-th","quant-ph"],"title_canon_sha256":"f5d10c19d33f4d445228aed17c21086a47bb15eee0254812d00004f3568e8492","abstract_canon_sha256":"34b4b57b5dbdd21a25b9c7b54c78b33f579e45cbb76fc6365f3f920ce48de914"},"schema_version":"1.0"},"canonical_sha256":"ce5b881a484d34a7e35003d9b60a10cbdc05575bf242e009410bcf83a86ebea7","source":{"kind":"arxiv","id":"1307.6813","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1307.6813","created_at":"2026-05-18T03:00:37Z"},{"alias_kind":"arxiv_version","alias_value":"1307.6813v2","created_at":"2026-05-18T03:00:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1307.6813","created_at":"2026-05-18T03:00:37Z"},{"alias_kind":"pith_short_12","alias_value":"ZZNYQGSIJU2K","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_16","alias_value":"ZZNYQGSIJU2KPY2Q","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_8","alias_value":"ZZNYQGSI","created_at":"2026-05-18T12:28:09Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:ZZNYQGSIJU2KPY2QAPM3MCQQZP","target":"record","payload":{"canonical_record":{"source":{"id":"1307.6813","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2013-07-25T17:04:32Z","cross_cats_sorted":["math-ph","math.MP","nucl-th","quant-ph"],"title_canon_sha256":"f5d10c19d33f4d445228aed17c21086a47bb15eee0254812d00004f3568e8492","abstract_canon_sha256":"34b4b57b5dbdd21a25b9c7b54c78b33f579e45cbb76fc6365f3f920ce48de914"},"schema_version":"1.0"},"canonical_sha256":"ce5b881a484d34a7e35003d9b60a10cbdc05575bf242e009410bcf83a86ebea7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:00:37.182956Z","signature_b64":"42P2/aEtduAOojaWNQfvDzp2AFixan2Ch5v8GH/ZEPqkzo5bwQakXyX83NqVaR7ilr2HetXqvofvNAPrj2VyAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ce5b881a484d34a7e35003d9b60a10cbdc05575bf242e009410bcf83a86ebea7","last_reissued_at":"2026-05-18T03:00:37.182198Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:00:37.182198Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1307.6813","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":"2026-05-18T03:00:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0nExFVBiZ2z7CxWBmrrrGrXXCdqFsypZw3+nNbWCpmvKkL9KAaZUcnGRne98Sbh1rCsY4YOavonTJwItEA5+AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T22:26:11.091867Z"},"content_sha256":"196f9e3d7686d903b1d0f3b03869ed511e459bd0dcdfbac8507c864c1f7696dc","schema_version":"1.0","event_id":"sha256:196f9e3d7686d903b1d0f3b03869ed511e459bd0dcdfbac8507c864c1f7696dc"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:ZZNYQGSIJU2KPY2QAPM3MCQQZP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Contact parameters in two dimensions for general three-body systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP","nucl-th","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"A. S. Jensen, D. V. Fedorov, F. F. Bellotti, M. T. Yamashita, N. T. Zinner, T. Frederico","submitted_at":"2013-07-25T17:04:32Z","abstract_excerpt":"We study the two dimensional three-body problem in the general case of three distinguishable particles interacting through zero-range potentials. The Faddeev decomposition is used to write the momentum-space wave function. We show that the large-momentum asymptotic spectator function has the same functional form as derived previously for three identical particles. We derive analytic relations between the three different Faddeev components for three distinguishable particles. We investigate the one-body momentum distributions both analytically and numerically and analyze the tail of the distrib"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1307.6813","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":"2026-05-18T03:00:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PI0ShGgQMjDNuGhqpgIPbE++EZNUPXFshgucPDjXEgea1U0ekphk9c9oLCJ9pLB8Og1O+7lVbX/nnEkO7i+jAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T22:26:11.092506Z"},"content_sha256":"ce8704a3ec7579cc7b865f0f8b0f73dc08cc2f77d98f06f9bf596d1d773e1fc8","schema_version":"1.0","event_id":"sha256:ce8704a3ec7579cc7b865f0f8b0f73dc08cc2f77d98f06f9bf596d1d773e1fc8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZZNYQGSIJU2KPY2QAPM3MCQQZP/bundle.json","state_url":"https://pith.science/pith/ZZNYQGSIJU2KPY2QAPM3MCQQZP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZZNYQGSIJU2KPY2QAPM3MCQQZP/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":"2026-05-25T22:26:11Z","links":{"resolver":"https://pith.science/pith/ZZNYQGSIJU2KPY2QAPM3MCQQZP","bundle":"https://pith.science/pith/ZZNYQGSIJU2KPY2QAPM3MCQQZP/bundle.json","state":"https://pith.science/pith/ZZNYQGSIJU2KPY2QAPM3MCQQZP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZZNYQGSIJU2KPY2QAPM3MCQQZP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:ZZNYQGSIJU2KPY2QAPM3MCQQZP","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":"34b4b57b5dbdd21a25b9c7b54c78b33f579e45cbb76fc6365f3f920ce48de914","cross_cats_sorted":["math-ph","math.MP","nucl-th","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2013-07-25T17:04:32Z","title_canon_sha256":"f5d10c19d33f4d445228aed17c21086a47bb15eee0254812d00004f3568e8492"},"schema_version":"1.0","source":{"id":"1307.6813","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1307.6813","created_at":"2026-05-18T03:00:37Z"},{"alias_kind":"arxiv_version","alias_value":"1307.6813v2","created_at":"2026-05-18T03:00:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1307.6813","created_at":"2026-05-18T03:00:37Z"},{"alias_kind":"pith_short_12","alias_value":"ZZNYQGSIJU2K","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_16","alias_value":"ZZNYQGSIJU2KPY2Q","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_8","alias_value":"ZZNYQGSI","created_at":"2026-05-18T12:28:09Z"}],"graph_snapshots":[{"event_id":"sha256:ce8704a3ec7579cc7b865f0f8b0f73dc08cc2f77d98f06f9bf596d1d773e1fc8","target":"graph","created_at":"2026-05-18T03:00:37Z","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 two dimensional three-body problem in the general case of three distinguishable particles interacting through zero-range potentials. The Faddeev decomposition is used to write the momentum-space wave function. We show that the large-momentum asymptotic spectator function has the same functional form as derived previously for three identical particles. We derive analytic relations between the three different Faddeev components for three distinguishable particles. We investigate the one-body momentum distributions both analytically and numerically and analyze the tail of the distrib","authors_text":"A. S. Jensen, D. V. Fedorov, F. F. Bellotti, M. T. Yamashita, N. T. Zinner, T. Frederico","cross_cats":["math-ph","math.MP","nucl-th","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2013-07-25T17:04:32Z","title":"Contact parameters in two dimensions for general three-body systems"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1307.6813","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":"sha256:196f9e3d7686d903b1d0f3b03869ed511e459bd0dcdfbac8507c864c1f7696dc","target":"record","created_at":"2026-05-18T03:00:37Z","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":"34b4b57b5dbdd21a25b9c7b54c78b33f579e45cbb76fc6365f3f920ce48de914","cross_cats_sorted":["math-ph","math.MP","nucl-th","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2013-07-25T17:04:32Z","title_canon_sha256":"f5d10c19d33f4d445228aed17c21086a47bb15eee0254812d00004f3568e8492"},"schema_version":"1.0","source":{"id":"1307.6813","kind":"arxiv","version":2}},"canonical_sha256":"ce5b881a484d34a7e35003d9b60a10cbdc05575bf242e009410bcf83a86ebea7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ce5b881a484d34a7e35003d9b60a10cbdc05575bf242e009410bcf83a86ebea7","first_computed_at":"2026-05-18T03:00:37.182198Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:00:37.182198Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"42P2/aEtduAOojaWNQfvDzp2AFixan2Ch5v8GH/ZEPqkzo5bwQakXyX83NqVaR7ilr2HetXqvofvNAPrj2VyAw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:00:37.182956Z","signed_message":"canonical_sha256_bytes"},"source_id":"1307.6813","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:196f9e3d7686d903b1d0f3b03869ed511e459bd0dcdfbac8507c864c1f7696dc","sha256:ce8704a3ec7579cc7b865f0f8b0f73dc08cc2f77d98f06f9bf596d1d773e1fc8"],"state_sha256":"5b67044402683f691a46b3d953377a4c9e5ab76b81b6645ca43dcccc9f961fc3"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"L8V61OOL28tVM0OzaNRGxCm5i7hXRhAbNebJfILSvXyCc74t6Cg4BTHEuq8S3TUD9NgIpnXvPmZjnxf1kjn5Ag==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T22:26:11.095713Z","bundle_sha256":"2858a8350d83efcc97d0375c95992d473f392905dc2221b0e73f5f8def352a36"}}