{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:E7BI6QQ4PXMGXLNES3WUOGPLFC","short_pith_number":"pith:E7BI6QQ4","canonical_record":{"source":{"id":"1412.4420","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2014-12-14T22:29:55Z","cross_cats_sorted":["physics.atom-ph","quant-ph"],"title_canon_sha256":"ef0ee2b4477621c057e77a4e0948b6da846228a68532014117b859546ad16194","abstract_canon_sha256":"0d7a5cb79ecc15894e84903e650a0ff173f902b150b072252260d75adc8d7d28"},"schema_version":"1.0"},"canonical_sha256":"27c28f421c7dd86bada496ed4719eb2894c5fadaeef96784fbe51f97b286ae1a","source":{"kind":"arxiv","id":"1412.4420","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.4420","created_at":"2026-05-18T01:02:46Z"},{"alias_kind":"arxiv_version","alias_value":"1412.4420v1","created_at":"2026-05-18T01:02:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.4420","created_at":"2026-05-18T01:02:46Z"},{"alias_kind":"pith_short_12","alias_value":"E7BI6QQ4PXMG","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_16","alias_value":"E7BI6QQ4PXMGXLNE","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_8","alias_value":"E7BI6QQ4","created_at":"2026-05-18T12:28:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:E7BI6QQ4PXMGXLNES3WUOGPLFC","target":"record","payload":{"canonical_record":{"source":{"id":"1412.4420","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2014-12-14T22:29:55Z","cross_cats_sorted":["physics.atom-ph","quant-ph"],"title_canon_sha256":"ef0ee2b4477621c057e77a4e0948b6da846228a68532014117b859546ad16194","abstract_canon_sha256":"0d7a5cb79ecc15894e84903e650a0ff173f902b150b072252260d75adc8d7d28"},"schema_version":"1.0"},"canonical_sha256":"27c28f421c7dd86bada496ed4719eb2894c5fadaeef96784fbe51f97b286ae1a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:02:46.021436Z","signature_b64":"D5HgiAp4M+QuK20SW9qnl7v/kc/KFaCSBus3KfDaZG5uu3k+e7JwZFWPuIpRgfT2KpD7NdXllmnmlg7M3ND4Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"27c28f421c7dd86bada496ed4719eb2894c5fadaeef96784fbe51f97b286ae1a","last_reissued_at":"2026-05-18T01:02:46.021020Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:02:46.021020Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1412.4420","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":"2026-05-18T01:02:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"e7kNp8HngL/C/byyE51HeCJ9vTUwnTZVb/hiANM5CeCTZpcQV/0FptjD1qVULZYEKJ1vi+12UqH2wvG2O1hEDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T07:42:01.867562Z"},"content_sha256":"613fb9c4499f7cf7793bc093a3ff1b91af2214841b5c5f19ea1f371a052ddb46","schema_version":"1.0","event_id":"sha256:613fb9c4499f7cf7793bc093a3ff1b91af2214841b5c5f19ea1f371a052ddb46"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:E7BI6QQ4PXMGXLNES3WUOGPLFC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"General ultracold scattering formalism with isotropic spin orbit coupling","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":"Chris H. Greene, Su-Ju Wang","submitted_at":"2014-12-14T22:29:55Z","abstract_excerpt":"A general treatment of ultracold two-body scattering in the presence of isotropic spin-orbit coupling (SOC) is presented. Owing to the mixing of different partial wave channels, scattering with SOC is in general a coupled multichannel problem. A systematic method is introduced to analytically solve a class of coupled differential equations by recasting the coupled channel problem as a simple eigenvalue problem. The exact Green's matrix in the presence of SOC is found, which readily gives the scattering solutions for any two identical particles in any total angular momentum subspace having negl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.4420","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":"2026-05-18T01:02:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/lFTTUbBf0VuJIK+jXoM+S10LXCTeIV94MxjwZSpBHNhrib+Gj3OudnMz7C9rHs6Z0pJolWJ0IMoiXRynxa+CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T07:42:01.868150Z"},"content_sha256":"accbc6f31b7f95706d380e9341727dc0eb2a6b636c94d902794f13949bff2574","schema_version":"1.0","event_id":"sha256:accbc6f31b7f95706d380e9341727dc0eb2a6b636c94d902794f13949bff2574"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/E7BI6QQ4PXMGXLNES3WUOGPLFC/bundle.json","state_url":"https://pith.science/pith/E7BI6QQ4PXMGXLNES3WUOGPLFC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/E7BI6QQ4PXMGXLNES3WUOGPLFC/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":"2026-05-30T07:42:01Z","links":{"resolver":"https://pith.science/pith/E7BI6QQ4PXMGXLNES3WUOGPLFC","bundle":"https://pith.science/pith/E7BI6QQ4PXMGXLNES3WUOGPLFC/bundle.json","state":"https://pith.science/pith/E7BI6QQ4PXMGXLNES3WUOGPLFC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/E7BI6QQ4PXMGXLNES3WUOGPLFC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:E7BI6QQ4PXMGXLNES3WUOGPLFC","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":"0d7a5cb79ecc15894e84903e650a0ff173f902b150b072252260d75adc8d7d28","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":"2014-12-14T22:29:55Z","title_canon_sha256":"ef0ee2b4477621c057e77a4e0948b6da846228a68532014117b859546ad16194"},"schema_version":"1.0","source":{"id":"1412.4420","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.4420","created_at":"2026-05-18T01:02:46Z"},{"alias_kind":"arxiv_version","alias_value":"1412.4420v1","created_at":"2026-05-18T01:02:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.4420","created_at":"2026-05-18T01:02:46Z"},{"alias_kind":"pith_short_12","alias_value":"E7BI6QQ4PXMG","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_16","alias_value":"E7BI6QQ4PXMGXLNE","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_8","alias_value":"E7BI6QQ4","created_at":"2026-05-18T12:28:25Z"}],"graph_snapshots":[{"event_id":"sha256:accbc6f31b7f95706d380e9341727dc0eb2a6b636c94d902794f13949bff2574","target":"graph","created_at":"2026-05-18T01:02:46Z","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":"A general treatment of ultracold two-body scattering in the presence of isotropic spin-orbit coupling (SOC) is presented. Owing to the mixing of different partial wave channels, scattering with SOC is in general a coupled multichannel problem. A systematic method is introduced to analytically solve a class of coupled differential equations by recasting the coupled channel problem as a simple eigenvalue problem. The exact Green's matrix in the presence of SOC is found, which readily gives the scattering solutions for any two identical particles in any total angular momentum subspace having negl","authors_text":"Chris H. Greene, Su-Ju Wang","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":"2014-12-14T22:29:55Z","title":"General ultracold scattering formalism with isotropic spin orbit coupling"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.4420","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":"sha256:613fb9c4499f7cf7793bc093a3ff1b91af2214841b5c5f19ea1f371a052ddb46","target":"record","created_at":"2026-05-18T01:02:46Z","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":"0d7a5cb79ecc15894e84903e650a0ff173f902b150b072252260d75adc8d7d28","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":"2014-12-14T22:29:55Z","title_canon_sha256":"ef0ee2b4477621c057e77a4e0948b6da846228a68532014117b859546ad16194"},"schema_version":"1.0","source":{"id":"1412.4420","kind":"arxiv","version":1}},"canonical_sha256":"27c28f421c7dd86bada496ed4719eb2894c5fadaeef96784fbe51f97b286ae1a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"27c28f421c7dd86bada496ed4719eb2894c5fadaeef96784fbe51f97b286ae1a","first_computed_at":"2026-05-18T01:02:46.021020Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:02:46.021020Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"D5HgiAp4M+QuK20SW9qnl7v/kc/KFaCSBus3KfDaZG5uu3k+e7JwZFWPuIpRgfT2KpD7NdXllmnmlg7M3ND4Bg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:02:46.021436Z","signed_message":"canonical_sha256_bytes"},"source_id":"1412.4420","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:613fb9c4499f7cf7793bc093a3ff1b91af2214841b5c5f19ea1f371a052ddb46","sha256:accbc6f31b7f95706d380e9341727dc0eb2a6b636c94d902794f13949bff2574"],"state_sha256":"4e77c7637c9248580e0b01de87f6e83e70761d20dcbb2930444f62b1bed97183"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UdBJ7UMLaWXlghkGKsbMnWz1fNJyZ8WOLJjMSurubldDlLeH5IZSGfykZrJE20vu7HUFCkVOeLvZeio1c8iFDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T07:42:01.870950Z","bundle_sha256":"70e753ab8e2ebbd33c7f01ea824be1be876410f0064c6536ede33fdff9e41cd6"}}