{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:MV3PFR6WRSQDFKRYX5RU4XZR4C","short_pith_number":"pith:MV3PFR6W","canonical_record":{"source":{"id":"1711.06470","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-17T09:43:11Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"ee971629b114b22588669094d581cd072504c039633f6f5471cdcb76e1f82e4b","abstract_canon_sha256":"093a66eb2522f6612c33f8c2bbf9e578d926c2a79db0665805ed6a24ab3cc285"},"schema_version":"1.0"},"canonical_sha256":"6576f2c7d68ca032aa38bf634e5f31e080103de7f27fae6c6cc158f7539e312f","source":{"kind":"arxiv","id":"1711.06470","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.06470","created_at":"2026-05-18T00:00:13Z"},{"alias_kind":"arxiv_version","alias_value":"1711.06470v2","created_at":"2026-05-18T00:00:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.06470","created_at":"2026-05-18T00:00:13Z"},{"alias_kind":"pith_short_12","alias_value":"MV3PFR6WRSQD","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_16","alias_value":"MV3PFR6WRSQDFKRY","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_8","alias_value":"MV3PFR6W","created_at":"2026-05-18T12:31:31Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:MV3PFR6WRSQDFKRYX5RU4XZR4C","target":"record","payload":{"canonical_record":{"source":{"id":"1711.06470","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-17T09:43:11Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"ee971629b114b22588669094d581cd072504c039633f6f5471cdcb76e1f82e4b","abstract_canon_sha256":"093a66eb2522f6612c33f8c2bbf9e578d926c2a79db0665805ed6a24ab3cc285"},"schema_version":"1.0"},"canonical_sha256":"6576f2c7d68ca032aa38bf634e5f31e080103de7f27fae6c6cc158f7539e312f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:00:13.508104Z","signature_b64":"lI2vhm5dI/KyfQ3ch+CrfLV+FpMLAe66rHlvCjLYAX76NBJ1uH5vJ9ugFQZmBBh4QFvkK1fSz87P/pGrL0ODBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6576f2c7d68ca032aa38bf634e5f31e080103de7f27fae6c6cc158f7539e312f","last_reissued_at":"2026-05-18T00:00:13.507418Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:00:13.507418Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1711.06470","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":"2026-05-18T00:00:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ipw+W3Y2KWhbrfWHzZ0jt0RsHLyuvRsIHJXcgLMahwOR2bS20F+rwY1e19ZodBVRHThSdCM8QoVdXTU+2fLwDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T05:10:51.201044Z"},"content_sha256":"7e57ecca3aa7f98871dafab658a245728aeac4211e260b1ccf6f703e0fa15800","schema_version":"1.0","event_id":"sha256:7e57ecca3aa7f98871dafab658a245728aeac4211e260b1ccf6f703e0fa15800"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:MV3PFR6WRSQDFKRYX5RU4XZR4C","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Scattering of charmed baryons on nucleons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"G. Krein, J. Haidenbauer","submitted_at":"2017-11-17T09:43:11Z","abstract_excerpt":"Chiral effective field theory is utilized for extrapolating results on the $\\Lambda_c N$ interaction, obtained in lattice QCD at unphysical (large) quark masses, to the physical point. The pion-mass dependence of the components that constitute the $\\Lambda_c N$ potential up to next-to-leading order (pion-exchange diagrams and four-baryon contact terms) is fixed by information from lattice QCD simulations. No recourse to SU(3) or SU(4) flavor symmetry is made. It is found that the results of the HAL QCD Collaboration for quark masses corresponding to $m_\\pi = 410$--$570$ MeV imply a moderately "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.06470","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":"2026-05-18T00:00:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"K3UWOBVflhe+tNMbdRWz4yVCkLrYChmjO4I+pHV9m8xXrkgcEtkVYn5x9vGI1yvY40X3i7ES0Eu+F4cNXghWDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T05:10:51.201405Z"},"content_sha256":"d0bffcebb64c8506485d5a8870808cec524438b0b9db672514c138390cd3cabe","schema_version":"1.0","event_id":"sha256:d0bffcebb64c8506485d5a8870808cec524438b0b9db672514c138390cd3cabe"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MV3PFR6WRSQDFKRYX5RU4XZR4C/bundle.json","state_url":"https://pith.science/pith/MV3PFR6WRSQDFKRYX5RU4XZR4C/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MV3PFR6WRSQDFKRYX5RU4XZR4C/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":"2026-06-02T05:10:51Z","links":{"resolver":"https://pith.science/pith/MV3PFR6WRSQDFKRYX5RU4XZR4C","bundle":"https://pith.science/pith/MV3PFR6WRSQDFKRYX5RU4XZR4C/bundle.json","state":"https://pith.science/pith/MV3PFR6WRSQDFKRYX5RU4XZR4C/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MV3PFR6WRSQDFKRYX5RU4XZR4C/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:MV3PFR6WRSQDFKRYX5RU4XZR4C","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":"093a66eb2522f6612c33f8c2bbf9e578d926c2a79db0665805ed6a24ab3cc285","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-17T09:43:11Z","title_canon_sha256":"ee971629b114b22588669094d581cd072504c039633f6f5471cdcb76e1f82e4b"},"schema_version":"1.0","source":{"id":"1711.06470","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.06470","created_at":"2026-05-18T00:00:13Z"},{"alias_kind":"arxiv_version","alias_value":"1711.06470v2","created_at":"2026-05-18T00:00:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.06470","created_at":"2026-05-18T00:00:13Z"},{"alias_kind":"pith_short_12","alias_value":"MV3PFR6WRSQD","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_16","alias_value":"MV3PFR6WRSQDFKRY","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_8","alias_value":"MV3PFR6W","created_at":"2026-05-18T12:31:31Z"}],"graph_snapshots":[{"event_id":"sha256:d0bffcebb64c8506485d5a8870808cec524438b0b9db672514c138390cd3cabe","target":"graph","created_at":"2026-05-18T00:00:13Z","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":"Chiral effective field theory is utilized for extrapolating results on the $\\Lambda_c N$ interaction, obtained in lattice QCD at unphysical (large) quark masses, to the physical point. The pion-mass dependence of the components that constitute the $\\Lambda_c N$ potential up to next-to-leading order (pion-exchange diagrams and four-baryon contact terms) is fixed by information from lattice QCD simulations. No recourse to SU(3) or SU(4) flavor symmetry is made. It is found that the results of the HAL QCD Collaboration for quark masses corresponding to $m_\\pi = 410$--$570$ MeV imply a moderately ","authors_text":"G. Krein, J. Haidenbauer","cross_cats":["nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-17T09:43:11Z","title":"Scattering of charmed baryons on nucleons"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.06470","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":"sha256:7e57ecca3aa7f98871dafab658a245728aeac4211e260b1ccf6f703e0fa15800","target":"record","created_at":"2026-05-18T00:00:13Z","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":"093a66eb2522f6612c33f8c2bbf9e578d926c2a79db0665805ed6a24ab3cc285","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-17T09:43:11Z","title_canon_sha256":"ee971629b114b22588669094d581cd072504c039633f6f5471cdcb76e1f82e4b"},"schema_version":"1.0","source":{"id":"1711.06470","kind":"arxiv","version":2}},"canonical_sha256":"6576f2c7d68ca032aa38bf634e5f31e080103de7f27fae6c6cc158f7539e312f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6576f2c7d68ca032aa38bf634e5f31e080103de7f27fae6c6cc158f7539e312f","first_computed_at":"2026-05-18T00:00:13.507418Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:00:13.507418Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"lI2vhm5dI/KyfQ3ch+CrfLV+FpMLAe66rHlvCjLYAX76NBJ1uH5vJ9ugFQZmBBh4QFvkK1fSz87P/pGrL0ODBw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:00:13.508104Z","signed_message":"canonical_sha256_bytes"},"source_id":"1711.06470","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7e57ecca3aa7f98871dafab658a245728aeac4211e260b1ccf6f703e0fa15800","sha256:d0bffcebb64c8506485d5a8870808cec524438b0b9db672514c138390cd3cabe"],"state_sha256":"a4c7813b41cad34fcf9298e9fb89aeab052efde004befe4e7b6355390bf6bff8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WnMWRXIdWRNA7F1y4BsjxItzjs1ZtPiMbRSuqp0Ph2ypMpdNRmPM8ABiwTITay+A/l+GavdYlFm+oWBAAuLCAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T05:10:51.203364Z","bundle_sha256":"d0a20f0af4d644256b274de479d2c91c056373f7e2f5686712f9fe22c543dcfc"}}