{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:C6XWXDPBQSGVOLVU472FWD3KMH","short_pith_number":"pith:C6XWXDPB","canonical_record":{"source":{"id":"1201.0149","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-12-30T16:19:19Z","cross_cats_sorted":["hep-ex","hep-lat","nucl-ex","nucl-th"],"title_canon_sha256":"a1701687d7117d16f2fb7bf88a526c60fa84ac5ba01cf16c46c3fb020c3b6982","abstract_canon_sha256":"42619bdfb0d73c02d1585c395811111e0ae1196ca2d8ced9c750a420823cbe18"},"schema_version":"1.0"},"canonical_sha256":"17af6b8de1848d572eb4e7f45b0f6a61d63dece35f9f3b70d4bbba2f16dd48a3","source":{"kind":"arxiv","id":"1201.0149","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.0149","created_at":"2026-05-18T01:58:59Z"},{"alias_kind":"arxiv_version","alias_value":"1201.0149v2","created_at":"2026-05-18T01:58:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.0149","created_at":"2026-05-18T01:58:59Z"},{"alias_kind":"pith_short_12","alias_value":"C6XWXDPBQSGV","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_16","alias_value":"C6XWXDPBQSGVOLVU","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_8","alias_value":"C6XWXDPB","created_at":"2026-05-18T12:26:24Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:C6XWXDPBQSGVOLVU472FWD3KMH","target":"record","payload":{"canonical_record":{"source":{"id":"1201.0149","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-12-30T16:19:19Z","cross_cats_sorted":["hep-ex","hep-lat","nucl-ex","nucl-th"],"title_canon_sha256":"a1701687d7117d16f2fb7bf88a526c60fa84ac5ba01cf16c46c3fb020c3b6982","abstract_canon_sha256":"42619bdfb0d73c02d1585c395811111e0ae1196ca2d8ced9c750a420823cbe18"},"schema_version":"1.0"},"canonical_sha256":"17af6b8de1848d572eb4e7f45b0f6a61d63dece35f9f3b70d4bbba2f16dd48a3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:58:59.360358Z","signature_b64":"ZQjMCa8UHB8HISrqxJ0nw9UHNUH1LD1yhFtfdjNjlPCH3avhxYbtR5tUo3zDiZte2M29+fCfnn7kyOByxtTFCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"17af6b8de1848d572eb4e7f45b0f6a61d63dece35f9f3b70d4bbba2f16dd48a3","last_reissued_at":"2026-05-18T01:58:59.359820Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:58:59.359820Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1201.0149","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":"2026-05-18T01:58:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xOxSctK6LeCsLD7alqS41FpfMSYi8S5VKH3Znp9Ip0xDJVhU4jHneS+55PQGqA05NCdQGTL/X6UPK8RQO6Z/Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T20:06:11.464080Z"},"content_sha256":"c53fc7ba4aa1ca93ea9443a360bfa9d798ffd29a107fd2348bf6e170cce03592","schema_version":"1.0","event_id":"sha256:c53fc7ba4aa1ca93ea9443a360bfa9d798ffd29a107fd2348bf6e170cce03592"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:C6XWXDPBQSGVOLVU472FWD3KMH","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The $DN$, $\\pi \\Sigma_c$ interaction in finite volume and the $\\Lambda_c(2595)$ resonance","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"E. Oset, Ju-Jun Xie","submitted_at":"2011-12-30T16:19:19Z","abstract_excerpt":"In this work the interaction of the coupled channels $DN$ and $\\pi \\Sigma_c$ in an SU(4) extrapolation of the chiral unitary theory, where the $\\Lambda_c(2595)$ resonance appears as dynamically generated from that interaction, is extended to produce results in finite volume. Energy levels in the finite box are evaluated and, assuming that they would correspond to lattice results, the inverse problem of determining the phase shifts in the infinite volume from the lattice results is solved. We observe that it is possible to obtain accurate $\\pi \\Sigma_c$ phase shifts and the position of the $\\La"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.0149","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":"2026-05-18T01:58:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+iW9qQYBNmWkMtXSaOma6JSqGpbhXT7qLPGANBdhhwsZkRF0/5Qr9Amd7D2gB0nRkKsLlAAghTM+lf0LicBlAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T20:06:11.464459Z"},"content_sha256":"38d985a628da977b213d282f54141142a2397ad21736f00f953f835b58e8fdaa","schema_version":"1.0","event_id":"sha256:38d985a628da977b213d282f54141142a2397ad21736f00f953f835b58e8fdaa"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/C6XWXDPBQSGVOLVU472FWD3KMH/bundle.json","state_url":"https://pith.science/pith/C6XWXDPBQSGVOLVU472FWD3KMH/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/C6XWXDPBQSGVOLVU472FWD3KMH/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":"2026-05-20T20:06:11Z","links":{"resolver":"https://pith.science/pith/C6XWXDPBQSGVOLVU472FWD3KMH","bundle":"https://pith.science/pith/C6XWXDPBQSGVOLVU472FWD3KMH/bundle.json","state":"https://pith.science/pith/C6XWXDPBQSGVOLVU472FWD3KMH/state.json","well_known_bundle":"https://pith.science/.well-known/pith/C6XWXDPBQSGVOLVU472FWD3KMH/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:C6XWXDPBQSGVOLVU472FWD3KMH","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":"42619bdfb0d73c02d1585c395811111e0ae1196ca2d8ced9c750a420823cbe18","cross_cats_sorted":["hep-ex","hep-lat","nucl-ex","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-12-30T16:19:19Z","title_canon_sha256":"a1701687d7117d16f2fb7bf88a526c60fa84ac5ba01cf16c46c3fb020c3b6982"},"schema_version":"1.0","source":{"id":"1201.0149","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.0149","created_at":"2026-05-18T01:58:59Z"},{"alias_kind":"arxiv_version","alias_value":"1201.0149v2","created_at":"2026-05-18T01:58:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.0149","created_at":"2026-05-18T01:58:59Z"},{"alias_kind":"pith_short_12","alias_value":"C6XWXDPBQSGV","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_16","alias_value":"C6XWXDPBQSGVOLVU","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_8","alias_value":"C6XWXDPB","created_at":"2026-05-18T12:26:24Z"}],"graph_snapshots":[{"event_id":"sha256:38d985a628da977b213d282f54141142a2397ad21736f00f953f835b58e8fdaa","target":"graph","created_at":"2026-05-18T01:58:59Z","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 work the interaction of the coupled channels $DN$ and $\\pi \\Sigma_c$ in an SU(4) extrapolation of the chiral unitary theory, where the $\\Lambda_c(2595)$ resonance appears as dynamically generated from that interaction, is extended to produce results in finite volume. Energy levels in the finite box are evaluated and, assuming that they would correspond to lattice results, the inverse problem of determining the phase shifts in the infinite volume from the lattice results is solved. We observe that it is possible to obtain accurate $\\pi \\Sigma_c$ phase shifts and the position of the $\\La","authors_text":"E. Oset, Ju-Jun Xie","cross_cats":["hep-ex","hep-lat","nucl-ex","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-12-30T16:19:19Z","title":"The $DN$, $\\pi \\Sigma_c$ interaction in finite volume and the $\\Lambda_c(2595)$ resonance"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.0149","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:c53fc7ba4aa1ca93ea9443a360bfa9d798ffd29a107fd2348bf6e170cce03592","target":"record","created_at":"2026-05-18T01:58:59Z","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":"42619bdfb0d73c02d1585c395811111e0ae1196ca2d8ced9c750a420823cbe18","cross_cats_sorted":["hep-ex","hep-lat","nucl-ex","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-12-30T16:19:19Z","title_canon_sha256":"a1701687d7117d16f2fb7bf88a526c60fa84ac5ba01cf16c46c3fb020c3b6982"},"schema_version":"1.0","source":{"id":"1201.0149","kind":"arxiv","version":2}},"canonical_sha256":"17af6b8de1848d572eb4e7f45b0f6a61d63dece35f9f3b70d4bbba2f16dd48a3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"17af6b8de1848d572eb4e7f45b0f6a61d63dece35f9f3b70d4bbba2f16dd48a3","first_computed_at":"2026-05-18T01:58:59.359820Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:58:59.359820Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ZQjMCa8UHB8HISrqxJ0nw9UHNUH1LD1yhFtfdjNjlPCH3avhxYbtR5tUo3zDiZte2M29+fCfnn7kyOByxtTFCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:58:59.360358Z","signed_message":"canonical_sha256_bytes"},"source_id":"1201.0149","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c53fc7ba4aa1ca93ea9443a360bfa9d798ffd29a107fd2348bf6e170cce03592","sha256:38d985a628da977b213d282f54141142a2397ad21736f00f953f835b58e8fdaa"],"state_sha256":"cf1474bad171399ae5be671f6c153c140e9c1d95da7d43a7e6da0a5da341c478"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+B7FAfHkF/7NOU0FylYVDVL37E7N8i5sdO9dWc5MOBwv/1fe+LshCfsXu0TsYD0FZg7VCD7Pe2KIS1UZjfASDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-20T20:06:11.466627Z","bundle_sha256":"43af28a912d33d12715d92febd1f3a84f34918ea86fb2cdfaa111af780db7d26"}}