{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:V7IHPMU3G2GR5WMHXIMJ7N2LM4","short_pith_number":"pith:V7IHPMU3","canonical_record":{"source":{"id":"1102.0549","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-02-02T20:34:57Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"f745f0f2df4b15802d90a80a813d61ba647744355b269d04e3a5eddc8a7dd71b","abstract_canon_sha256":"61e6d5379de4c8e08981ba57747e12ea3fcce819fec294c08a3975140f342da7"},"schema_version":"1.0"},"canonical_sha256":"afd077b29b368d1ed987ba189fb74b672922bf87693d87cdf1d2b5da91152f34","source":{"kind":"arxiv","id":"1102.0549","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1102.0549","created_at":"2026-05-18T04:17:02Z"},{"alias_kind":"arxiv_version","alias_value":"1102.0549v1","created_at":"2026-05-18T04:17:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1102.0549","created_at":"2026-05-18T04:17:02Z"},{"alias_kind":"pith_short_12","alias_value":"V7IHPMU3G2GR","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_16","alias_value":"V7IHPMU3G2GR5WMH","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_8","alias_value":"V7IHPMU3","created_at":"2026-05-18T12:26:42Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:V7IHPMU3G2GR5WMHXIMJ7N2LM4","target":"record","payload":{"canonical_record":{"source":{"id":"1102.0549","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-02-02T20:34:57Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"f745f0f2df4b15802d90a80a813d61ba647744355b269d04e3a5eddc8a7dd71b","abstract_canon_sha256":"61e6d5379de4c8e08981ba57747e12ea3fcce819fec294c08a3975140f342da7"},"schema_version":"1.0"},"canonical_sha256":"afd077b29b368d1ed987ba189fb74b672922bf87693d87cdf1d2b5da91152f34","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:17:02.807396Z","signature_b64":"zRc84mXH5+rzY7a+pWv+l56i/5BPhtgXTnUHd++xAmTI+elGal+zSKtmLPMyQ2HCj8GZV0IrrqJj/qO14DsEAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"afd077b29b368d1ed987ba189fb74b672922bf87693d87cdf1d2b5da91152f34","last_reissued_at":"2026-05-18T04:17:02.806615Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:17:02.806615Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1102.0549","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":"2026-05-18T04:17:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BSAdMBc0NRPkxoU0eM9zkjQgYUXK218KQs1XO+lxTsZv68SHqy235i9fXSbx8zIX8g+hmLQKyThAdXgHjSEQAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T02:29:23.315657Z"},"content_sha256":"1cdf01c1651549e075fb623f6d6304e1cdcaa37f6d6e6e91dcb7c41e7f8280ba","schema_version":"1.0","event_id":"sha256:1cdf01c1651549e075fb623f6d6304e1cdcaa37f6d6e6e91dcb7c41e7f8280ba"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:V7IHPMU3G2GR5WMHXIMJ7N2LM4","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Potential splitting approach to multichannel Coulomb scattering: the driven Schr\\\"odinger equation formulation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"physics.atom-ph","authors_text":"E.A. Yarevsky, M.V. Volkov, N. Elander, S.L. Yakovlev","submitted_at":"2011-02-02T20:34:57Z","abstract_excerpt":"In this paper we suggest a new approach for the multichannel Coulomb scattering problem. The Schr\\\"{o}dinger equation for the problem is reformulated in the form of a set of inhomogeneous equations with a finite-range driving term. The boundary conditions at infinity for this set of equations have been proven to be purely outgoing waves. The formulation {presented here} is based on splitting the interaction potential into a finite range core part and a long range tail part. The conventional matching procedure coupled with the integral Lippmann-Schwinger equations technique are used in the form"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1102.0549","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":"2026-05-18T04:17:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"F2Lu3haASYb0O7+rnOu7kUeNxRTyKrUJTsZXxDuv7VPkFj18ZRpTgN5upGDDtcva0aw0tCSNJdhwMhVinpHYAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T02:29:23.316371Z"},"content_sha256":"e9ab7dac993548f678e0a530fec5669b86017871e2039834d8ae3197fa37278c","schema_version":"1.0","event_id":"sha256:e9ab7dac993548f678e0a530fec5669b86017871e2039834d8ae3197fa37278c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/V7IHPMU3G2GR5WMHXIMJ7N2LM4/bundle.json","state_url":"https://pith.science/pith/V7IHPMU3G2GR5WMHXIMJ7N2LM4/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/V7IHPMU3G2GR5WMHXIMJ7N2LM4/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":"2026-05-31T02:29:23Z","links":{"resolver":"https://pith.science/pith/V7IHPMU3G2GR5WMHXIMJ7N2LM4","bundle":"https://pith.science/pith/V7IHPMU3G2GR5WMHXIMJ7N2LM4/bundle.json","state":"https://pith.science/pith/V7IHPMU3G2GR5WMHXIMJ7N2LM4/state.json","well_known_bundle":"https://pith.science/.well-known/pith/V7IHPMU3G2GR5WMHXIMJ7N2LM4/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:V7IHPMU3G2GR5WMHXIMJ7N2LM4","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":"61e6d5379de4c8e08981ba57747e12ea3fcce819fec294c08a3975140f342da7","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-02-02T20:34:57Z","title_canon_sha256":"f745f0f2df4b15802d90a80a813d61ba647744355b269d04e3a5eddc8a7dd71b"},"schema_version":"1.0","source":{"id":"1102.0549","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1102.0549","created_at":"2026-05-18T04:17:02Z"},{"alias_kind":"arxiv_version","alias_value":"1102.0549v1","created_at":"2026-05-18T04:17:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1102.0549","created_at":"2026-05-18T04:17:02Z"},{"alias_kind":"pith_short_12","alias_value":"V7IHPMU3G2GR","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_16","alias_value":"V7IHPMU3G2GR5WMH","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_8","alias_value":"V7IHPMU3","created_at":"2026-05-18T12:26:42Z"}],"graph_snapshots":[{"event_id":"sha256:e9ab7dac993548f678e0a530fec5669b86017871e2039834d8ae3197fa37278c","target":"graph","created_at":"2026-05-18T04:17:02Z","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":"In this paper we suggest a new approach for the multichannel Coulomb scattering problem. The Schr\\\"{o}dinger equation for the problem is reformulated in the form of a set of inhomogeneous equations with a finite-range driving term. The boundary conditions at infinity for this set of equations have been proven to be purely outgoing waves. The formulation {presented here} is based on splitting the interaction potential into a finite range core part and a long range tail part. The conventional matching procedure coupled with the integral Lippmann-Schwinger equations technique are used in the form","authors_text":"E.A. Yarevsky, M.V. Volkov, N. Elander, S.L. Yakovlev","cross_cats":["nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-02-02T20:34:57Z","title":"Potential splitting approach to multichannel Coulomb scattering: the driven Schr\\\"odinger equation formulation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1102.0549","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":"sha256:1cdf01c1651549e075fb623f6d6304e1cdcaa37f6d6e6e91dcb7c41e7f8280ba","target":"record","created_at":"2026-05-18T04:17:02Z","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":"61e6d5379de4c8e08981ba57747e12ea3fcce819fec294c08a3975140f342da7","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-02-02T20:34:57Z","title_canon_sha256":"f745f0f2df4b15802d90a80a813d61ba647744355b269d04e3a5eddc8a7dd71b"},"schema_version":"1.0","source":{"id":"1102.0549","kind":"arxiv","version":1}},"canonical_sha256":"afd077b29b368d1ed987ba189fb74b672922bf87693d87cdf1d2b5da91152f34","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"afd077b29b368d1ed987ba189fb74b672922bf87693d87cdf1d2b5da91152f34","first_computed_at":"2026-05-18T04:17:02.806615Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:17:02.806615Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"zRc84mXH5+rzY7a+pWv+l56i/5BPhtgXTnUHd++xAmTI+elGal+zSKtmLPMyQ2HCj8GZV0IrrqJj/qO14DsEAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T04:17:02.807396Z","signed_message":"canonical_sha256_bytes"},"source_id":"1102.0549","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1cdf01c1651549e075fb623f6d6304e1cdcaa37f6d6e6e91dcb7c41e7f8280ba","sha256:e9ab7dac993548f678e0a530fec5669b86017871e2039834d8ae3197fa37278c"],"state_sha256":"23fb5f0e0d70292704aa782b7464a4231a4e5db8fcc2a23a3a2a8cecc979905b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9m/Kq556UVDTs0jXzOYlwrtV8+qHGHVBBQzKkLy4yKqXI9HLWb1Sd5K2hhJI5vzKO7id+i200uI9vZJEYgyaBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T02:29:23.320034Z","bundle_sha256":"7af60bfef9e266d9fd745fc93520ed5edb69a9cd6c783908596a9629c569d8f0"}}