{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:UMBEBHR4JWUYX6P6YBAB5TEW3A","short_pith_number":"pith:UMBEBHR4","canonical_record":{"source":{"id":"1303.3093","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2013-03-13T06:35:57Z","cross_cats_sorted":[],"title_canon_sha256":"86fe86e334a7bd3751c711a7f67609e03eba72a1cf60fecf45b514d02633ccaf","abstract_canon_sha256":"903bc332f203fca9743b2deb3604c793982dc43ca44d6b5cecc44dacc027c7b2"},"schema_version":"1.0"},"canonical_sha256":"a302409e3c4da98bf9fec0401ecc96d82892dca5c2281ecb0f7f623b611ed48c","source":{"kind":"arxiv","id":"1303.3093","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.3093","created_at":"2026-05-18T03:21:53Z"},{"alias_kind":"arxiv_version","alias_value":"1303.3093v2","created_at":"2026-05-18T03:21:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.3093","created_at":"2026-05-18T03:21:53Z"},{"alias_kind":"pith_short_12","alias_value":"UMBEBHR4JWUY","created_at":"2026-05-18T12:28:02Z"},{"alias_kind":"pith_short_16","alias_value":"UMBEBHR4JWUYX6P6","created_at":"2026-05-18T12:28:02Z"},{"alias_kind":"pith_short_8","alias_value":"UMBEBHR4","created_at":"2026-05-18T12:28:02Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:UMBEBHR4JWUYX6P6YBAB5TEW3A","target":"record","payload":{"canonical_record":{"source":{"id":"1303.3093","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2013-03-13T06:35:57Z","cross_cats_sorted":[],"title_canon_sha256":"86fe86e334a7bd3751c711a7f67609e03eba72a1cf60fecf45b514d02633ccaf","abstract_canon_sha256":"903bc332f203fca9743b2deb3604c793982dc43ca44d6b5cecc44dacc027c7b2"},"schema_version":"1.0"},"canonical_sha256":"a302409e3c4da98bf9fec0401ecc96d82892dca5c2281ecb0f7f623b611ed48c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:21:53.723539Z","signature_b64":"AquzAcq9eqx2466qzVcsrmWY2PEoKQjkj7zHqvHAFvasFir7yR7K2pTxKVNLs874k9NSsxRbieLlJLOJRAEGBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a302409e3c4da98bf9fec0401ecc96d82892dca5c2281ecb0f7f623b611ed48c","last_reissued_at":"2026-05-18T03:21:53.722985Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:21:53.722985Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1303.3093","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":"2026-05-18T03:21:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"j+NyYLrvqjUKymZ/xIcHmJaPvrfQxXmJSvcdC/2SyEJUd9XlftY0xxJHjHioF/fe+cmn25vHC+oXmohCwj9OBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T18:46:17.928542Z"},"content_sha256":"06688fd5e83d32fa0acc86a477fbb795be14cc0e1868798232b0c93eaef5321d","schema_version":"1.0","event_id":"sha256:06688fd5e83d32fa0acc86a477fbb795be14cc0e1868798232b0c93eaef5321d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:UMBEBHR4JWUYX6P6YBAB5TEW3A","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Charge transfer in the cold Yb$^+$ + Rb collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"Alexei A. Buchachenko, Andrey K. Belyaev, Elvira R. Sayfutyarova, Svetlana A. Yakovleva","submitted_at":"2013-03-13T06:35:57Z","abstract_excerpt":"Charge-transfer cold Yb$^+$ + Rb collision dynamics is investigated theoretically using high-level {\\it ab initio} potential energy curves, dipole moment functions and nonadiabatic coupling matrix elements. Within the scalar-relativistic approximation, the radiative transitions from the entrance $A^1\\Sigma^+$ to the ground $X^1\\Sigma^+$ state are found to be the only efficient charge-transfer pathway. The spin-orbit coupling does not open other efficient pathways, but alters the potential energy curves and the transition dipole moment for the $A-X$ pair of states. The radiative, as well as the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.3093","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":"2026-05-18T03:21:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ut6zzeYszzNwuhSQ0Jbr0BemyJWAS8lh/76f4avlT8O7eBIgAtBGZilPxXkTy4qyGbqY+lBe1zrrnvvtICowCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T18:46:17.928883Z"},"content_sha256":"f99ee9bdf79e8fa9fad8b861b54be9b27516f135788702f0892c88da2c81191d","schema_version":"1.0","event_id":"sha256:f99ee9bdf79e8fa9fad8b861b54be9b27516f135788702f0892c88da2c81191d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UMBEBHR4JWUYX6P6YBAB5TEW3A/bundle.json","state_url":"https://pith.science/pith/UMBEBHR4JWUYX6P6YBAB5TEW3A/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UMBEBHR4JWUYX6P6YBAB5TEW3A/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":"2026-06-24T18:46:17Z","links":{"resolver":"https://pith.science/pith/UMBEBHR4JWUYX6P6YBAB5TEW3A","bundle":"https://pith.science/pith/UMBEBHR4JWUYX6P6YBAB5TEW3A/bundle.json","state":"https://pith.science/pith/UMBEBHR4JWUYX6P6YBAB5TEW3A/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UMBEBHR4JWUYX6P6YBAB5TEW3A/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:UMBEBHR4JWUYX6P6YBAB5TEW3A","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":"903bc332f203fca9743b2deb3604c793982dc43ca44d6b5cecc44dacc027c7b2","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2013-03-13T06:35:57Z","title_canon_sha256":"86fe86e334a7bd3751c711a7f67609e03eba72a1cf60fecf45b514d02633ccaf"},"schema_version":"1.0","source":{"id":"1303.3093","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.3093","created_at":"2026-05-18T03:21:53Z"},{"alias_kind":"arxiv_version","alias_value":"1303.3093v2","created_at":"2026-05-18T03:21:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.3093","created_at":"2026-05-18T03:21:53Z"},{"alias_kind":"pith_short_12","alias_value":"UMBEBHR4JWUY","created_at":"2026-05-18T12:28:02Z"},{"alias_kind":"pith_short_16","alias_value":"UMBEBHR4JWUYX6P6","created_at":"2026-05-18T12:28:02Z"},{"alias_kind":"pith_short_8","alias_value":"UMBEBHR4","created_at":"2026-05-18T12:28:02Z"}],"graph_snapshots":[{"event_id":"sha256:f99ee9bdf79e8fa9fad8b861b54be9b27516f135788702f0892c88da2c81191d","target":"graph","created_at":"2026-05-18T03:21:53Z","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":"Charge-transfer cold Yb$^+$ + Rb collision dynamics is investigated theoretically using high-level {\\it ab initio} potential energy curves, dipole moment functions and nonadiabatic coupling matrix elements. Within the scalar-relativistic approximation, the radiative transitions from the entrance $A^1\\Sigma^+$ to the ground $X^1\\Sigma^+$ state are found to be the only efficient charge-transfer pathway. The spin-orbit coupling does not open other efficient pathways, but alters the potential energy curves and the transition dipole moment for the $A-X$ pair of states. The radiative, as well as the","authors_text":"Alexei A. Buchachenko, Andrey K. Belyaev, Elvira R. Sayfutyarova, Svetlana A. Yakovleva","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2013-03-13T06:35:57Z","title":"Charge transfer in the cold Yb$^+$ + Rb collisions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.3093","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":"sha256:06688fd5e83d32fa0acc86a477fbb795be14cc0e1868798232b0c93eaef5321d","target":"record","created_at":"2026-05-18T03:21:53Z","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":"903bc332f203fca9743b2deb3604c793982dc43ca44d6b5cecc44dacc027c7b2","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2013-03-13T06:35:57Z","title_canon_sha256":"86fe86e334a7bd3751c711a7f67609e03eba72a1cf60fecf45b514d02633ccaf"},"schema_version":"1.0","source":{"id":"1303.3093","kind":"arxiv","version":2}},"canonical_sha256":"a302409e3c4da98bf9fec0401ecc96d82892dca5c2281ecb0f7f623b611ed48c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a302409e3c4da98bf9fec0401ecc96d82892dca5c2281ecb0f7f623b611ed48c","first_computed_at":"2026-05-18T03:21:53.722985Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:21:53.722985Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"AquzAcq9eqx2466qzVcsrmWY2PEoKQjkj7zHqvHAFvasFir7yR7K2pTxKVNLs874k9NSsxRbieLlJLOJRAEGBw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:21:53.723539Z","signed_message":"canonical_sha256_bytes"},"source_id":"1303.3093","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:06688fd5e83d32fa0acc86a477fbb795be14cc0e1868798232b0c93eaef5321d","sha256:f99ee9bdf79e8fa9fad8b861b54be9b27516f135788702f0892c88da2c81191d"],"state_sha256":"e14dcd6f6ef17b1aba9da64c15963eedd9eb7f605605b94e98c3144a3a4c1182"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oWsveXqAad5cpb6HpVXYPWOMbEXvaXGsUZapbuX9vwDQI5MaGTubbHLucKpsq6ymRXYmFNm28i6J+yAt3nKeBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-24T18:46:17.930740Z","bundle_sha256":"1ff2d0739bac39fa936885b7235bb4c66ed5db8b44e92cf5af6ad33e73e18b26"}}