{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:NWKTS5CIMEG5RPGMSNRQR7MYSA","short_pith_number":"pith:NWKTS5CI","canonical_record":{"source":{"id":"1511.08744","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-11-27T17:03:49Z","cross_cats_sorted":["cond-mat.quant-gas","nlin.CD"],"title_canon_sha256":"84358171032117c8db4cd5f6af76219095a3f38290502b36744229854a5b8ed0","abstract_canon_sha256":"738a9f37595cd799b54e5cc762bc835ea499057296b9ea6ddf97c4356032ecce"},"schema_version":"1.0"},"canonical_sha256":"6d95397448610dd8bccc936308fd98901099114bb5e7b09d21031165cccfb18a","source":{"kind":"arxiv","id":"1511.08744","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1511.08744","created_at":"2026-05-18T01:13:16Z"},{"alias_kind":"arxiv_version","alias_value":"1511.08744v2","created_at":"2026-05-18T01:13:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.08744","created_at":"2026-05-18T01:13:16Z"},{"alias_kind":"pith_short_12","alias_value":"NWKTS5CIMEG5","created_at":"2026-05-18T12:29:34Z"},{"alias_kind":"pith_short_16","alias_value":"NWKTS5CIMEG5RPGM","created_at":"2026-05-18T12:29:34Z"},{"alias_kind":"pith_short_8","alias_value":"NWKTS5CI","created_at":"2026-05-18T12:29:34Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:NWKTS5CIMEG5RPGMSNRQR7MYSA","target":"record","payload":{"canonical_record":{"source":{"id":"1511.08744","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-11-27T17:03:49Z","cross_cats_sorted":["cond-mat.quant-gas","nlin.CD"],"title_canon_sha256":"84358171032117c8db4cd5f6af76219095a3f38290502b36744229854a5b8ed0","abstract_canon_sha256":"738a9f37595cd799b54e5cc762bc835ea499057296b9ea6ddf97c4356032ecce"},"schema_version":"1.0"},"canonical_sha256":"6d95397448610dd8bccc936308fd98901099114bb5e7b09d21031165cccfb18a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:13:16.179996Z","signature_b64":"UBInvA4Lpm0Ex70TXTEgVuhrqn7R7DMQ+9Zmhkj7letEUFwkg3b01c7PzaSIygEDbLzNfzYa9+3EtABgg6m7DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6d95397448610dd8bccc936308fd98901099114bb5e7b09d21031165cccfb18a","last_reissued_at":"2026-05-18T01:13:16.179481Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:13:16.179481Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1511.08744","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":"2026-05-18T01:13:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BpSuUJgJ4Ly7jMS2LJMgo2l8OIiFLVqQKYDi7H0KJ8qo3qulufmeFIuWHtg/DGJk9JDLR0SlzNbi/zzL6n+mBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T05:51:15.488721Z"},"content_sha256":"b7947da4290c0c960589446c72b18a166964ce07fe2e78c74b08dd2bb18335af","schema_version":"1.0","event_id":"sha256:b7947da4290c0c960589446c72b18a166964ce07fe2e78c74b08dd2bb18335af"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:NWKTS5CIMEG5RPGMSNRQR7MYSA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The approach to chaos in ultracold atomic and molecular physics: statistics of near-threshold bound states for Li+CaH and Li+CaF","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","nlin.CD"],"primary_cat":"physics.atom-ph","authors_text":"Christophe L. Vaillant, Dermot G. Green, Jeremy M. Hutson, Masato Morita, Matthew D. Frye","submitted_at":"2015-11-27T17:03:49Z","abstract_excerpt":"We calculate near-threshold bound states and Feshbach resonance positions for atom + rigid-rotor models of the highly anisotropic systems Li+CaH and Li+CaF. We perform statistical analysis on the resonance positions to compare with the predictions of random matrix theory. For Li+CaH with total angular momentum $J=0$ we find fully chaotic behavior in both the nearest-neighbor spacing distribution and the level number variance. However, for $J>0$ we find different behavior due to the presence of a nearly conserved quantum number. Li+CaF ($J=0$) also shows apparently reduced levels of chaotic beh"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.08744","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":"2026-05-18T01:13:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yLi4shevzdjKgqE8cMV7EVFSVCHMRuVfwjiqdLLkPzHU+Jq1s7v9rd8DaGqMqK+LsJCYQaktkVhPR3yVtmOpBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T05:51:15.489069Z"},"content_sha256":"b74205a6ecd84efa686cb221e04764fcb155ffe3ba00ba8283ead7d668af1890","schema_version":"1.0","event_id":"sha256:b74205a6ecd84efa686cb221e04764fcb155ffe3ba00ba8283ead7d668af1890"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/NWKTS5CIMEG5RPGMSNRQR7MYSA/bundle.json","state_url":"https://pith.science/pith/NWKTS5CIMEG5RPGMSNRQR7MYSA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/NWKTS5CIMEG5RPGMSNRQR7MYSA/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":"2026-06-03T05:51:15Z","links":{"resolver":"https://pith.science/pith/NWKTS5CIMEG5RPGMSNRQR7MYSA","bundle":"https://pith.science/pith/NWKTS5CIMEG5RPGMSNRQR7MYSA/bundle.json","state":"https://pith.science/pith/NWKTS5CIMEG5RPGMSNRQR7MYSA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/NWKTS5CIMEG5RPGMSNRQR7MYSA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:NWKTS5CIMEG5RPGMSNRQR7MYSA","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":"738a9f37595cd799b54e5cc762bc835ea499057296b9ea6ddf97c4356032ecce","cross_cats_sorted":["cond-mat.quant-gas","nlin.CD"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-11-27T17:03:49Z","title_canon_sha256":"84358171032117c8db4cd5f6af76219095a3f38290502b36744229854a5b8ed0"},"schema_version":"1.0","source":{"id":"1511.08744","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1511.08744","created_at":"2026-05-18T01:13:16Z"},{"alias_kind":"arxiv_version","alias_value":"1511.08744v2","created_at":"2026-05-18T01:13:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.08744","created_at":"2026-05-18T01:13:16Z"},{"alias_kind":"pith_short_12","alias_value":"NWKTS5CIMEG5","created_at":"2026-05-18T12:29:34Z"},{"alias_kind":"pith_short_16","alias_value":"NWKTS5CIMEG5RPGM","created_at":"2026-05-18T12:29:34Z"},{"alias_kind":"pith_short_8","alias_value":"NWKTS5CI","created_at":"2026-05-18T12:29:34Z"}],"graph_snapshots":[{"event_id":"sha256:b74205a6ecd84efa686cb221e04764fcb155ffe3ba00ba8283ead7d668af1890","target":"graph","created_at":"2026-05-18T01:13:16Z","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 calculate near-threshold bound states and Feshbach resonance positions for atom + rigid-rotor models of the highly anisotropic systems Li+CaH and Li+CaF. We perform statistical analysis on the resonance positions to compare with the predictions of random matrix theory. For Li+CaH with total angular momentum $J=0$ we find fully chaotic behavior in both the nearest-neighbor spacing distribution and the level number variance. However, for $J>0$ we find different behavior due to the presence of a nearly conserved quantum number. Li+CaF ($J=0$) also shows apparently reduced levels of chaotic beh","authors_text":"Christophe L. Vaillant, Dermot G. Green, Jeremy M. Hutson, Masato Morita, Matthew D. Frye","cross_cats":["cond-mat.quant-gas","nlin.CD"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-11-27T17:03:49Z","title":"The approach to chaos in ultracold atomic and molecular physics: statistics of near-threshold bound states for Li+CaH and Li+CaF"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.08744","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:b7947da4290c0c960589446c72b18a166964ce07fe2e78c74b08dd2bb18335af","target":"record","created_at":"2026-05-18T01:13:16Z","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":"738a9f37595cd799b54e5cc762bc835ea499057296b9ea6ddf97c4356032ecce","cross_cats_sorted":["cond-mat.quant-gas","nlin.CD"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-11-27T17:03:49Z","title_canon_sha256":"84358171032117c8db4cd5f6af76219095a3f38290502b36744229854a5b8ed0"},"schema_version":"1.0","source":{"id":"1511.08744","kind":"arxiv","version":2}},"canonical_sha256":"6d95397448610dd8bccc936308fd98901099114bb5e7b09d21031165cccfb18a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6d95397448610dd8bccc936308fd98901099114bb5e7b09d21031165cccfb18a","first_computed_at":"2026-05-18T01:13:16.179481Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:13:16.179481Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"UBInvA4Lpm0Ex70TXTEgVuhrqn7R7DMQ+9Zmhkj7letEUFwkg3b01c7PzaSIygEDbLzNfzYa9+3EtABgg6m7DA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:13:16.179996Z","signed_message":"canonical_sha256_bytes"},"source_id":"1511.08744","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b7947da4290c0c960589446c72b18a166964ce07fe2e78c74b08dd2bb18335af","sha256:b74205a6ecd84efa686cb221e04764fcb155ffe3ba00ba8283ead7d668af1890"],"state_sha256":"00dd5280dd2941fbb2634ea061fce4afea919f5c27ae339568592f37384a326b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JqxPTfRQKht+kTAx0oA83ernxOvxRdeVigIuODWu2wMEPISVV8v3lE2vddziXqCKAlM2yuBCiYBtlpZAzRnjBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T05:51:15.491253Z","bundle_sha256":"eac8d9b1e10d48e8f09cd5c94ec1ccbb33c07669ac95e80216a30e221b8c826e"}}