{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:WDQAUMXRYNVD4M6PSIBJKXN6JN","short_pith_number":"pith:WDQAUMXR","canonical_record":{"source":{"id":"1805.09580","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-05-24T09:52:36Z","cross_cats_sorted":["hep-ex","hep-lat","nucl-th"],"title_canon_sha256":"effde059563392cd4d1164108232ba711f8f2ee3cfa62572b8adfb5b3161c5ea","abstract_canon_sha256":"c42135a96881293b7c933fc9e0a331bce2474a8d21d2230b359fd76e78cf54c3"},"schema_version":"1.0"},"canonical_sha256":"b0e00a32f1c36a3e33cf9202955dbe4b40eaa33d1f28ac9ecb3f4ddf0d293c8f","source":{"kind":"arxiv","id":"1805.09580","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1805.09580","created_at":"2026-05-18T00:00:19Z"},{"alias_kind":"arxiv_version","alias_value":"1805.09580v2","created_at":"2026-05-18T00:00:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.09580","created_at":"2026-05-18T00:00:19Z"},{"alias_kind":"pith_short_12","alias_value":"WDQAUMXRYNVD","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_16","alias_value":"WDQAUMXRYNVD4M6P","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_8","alias_value":"WDQAUMXR","created_at":"2026-05-18T12:32:59Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:WDQAUMXRYNVD4M6PSIBJKXN6JN","target":"record","payload":{"canonical_record":{"source":{"id":"1805.09580","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-05-24T09:52:36Z","cross_cats_sorted":["hep-ex","hep-lat","nucl-th"],"title_canon_sha256":"effde059563392cd4d1164108232ba711f8f2ee3cfa62572b8adfb5b3161c5ea","abstract_canon_sha256":"c42135a96881293b7c933fc9e0a331bce2474a8d21d2230b359fd76e78cf54c3"},"schema_version":"1.0"},"canonical_sha256":"b0e00a32f1c36a3e33cf9202955dbe4b40eaa33d1f28ac9ecb3f4ddf0d293c8f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:00:19.442308Z","signature_b64":"DZAz09E9LsjOuYk8nsVfJYmGGeWqZixoiqJWFoWYD6JJBtf1/QpVg2G+hyHXColapFMHINh8F6z+w24ZwbSBBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b0e00a32f1c36a3e33cf9202955dbe4b40eaa33d1f28ac9ecb3f4ddf0d293c8f","last_reissued_at":"2026-05-18T00:00:19.441827Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:00:19.441827Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1805.09580","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":"2026-05-18T00:00:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7H7P6BHEXcnP6j6lWjdiDyYrG/NtyCuIXlQ6pJI0aBOGZpD3FInqC14lFTXh68/L2Nz4/PagfaT7nZKuLnGRDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T05:08:09.785690Z"},"content_sha256":"584a140dc0706c9770d0ce11c9338d9470f2fd3ea00191367b8524bef3122dce","schema_version":"1.0","event_id":"sha256:584a140dc0706c9770d0ce11c9338d9470f2fd3ea00191367b8524bef3122dce"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:WDQAUMXRYNVD4M6PSIBJKXN6JN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Magnetic moments of the spin-${3\\over 2}$ singly heavy baryons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"Chang-Zhi Leng, Guang-Juan Wang, Lu Meng, Shi-Lin Zhu, Zhan-Wei Liu","submitted_at":"2018-05-24T09:52:36Z","abstract_excerpt":"We calculate the magnetic moments of spin-$3\\over 2$ singly charmed baryons in the heavy baryon chiral perturbation theory (HBChPT). The analytical expressions are given up to $\\mathcal{O}(p^3)$. The heavy quark symmetry is used to reduce the number of low energy constants (LECs). With the lattice QCD simulation data as the magnetic moments of the charmed baryons, the numerical results are given up to $\\mathcal{O}(p^3)$ in three scenarios. In the first scenario, we use the results in the quark model as the leading order input. In the second scenario, we use the heavy quark symmetry and neglect"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.09580","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":"2026-05-18T00:00:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dYp1bSDSghvRwCqtUcNSYJGufK+vSWL9rLuqiBOTmkWVoAuWRTWx2fEmE0mtMO0U1W0w8dSqDCrxQBugIIqDDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T05:08:09.786383Z"},"content_sha256":"96b0dbdeccf57394fbb6a399c5695079dcae3ac8da3beff79b05ed13f166773d","schema_version":"1.0","event_id":"sha256:96b0dbdeccf57394fbb6a399c5695079dcae3ac8da3beff79b05ed13f166773d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/WDQAUMXRYNVD4M6PSIBJKXN6JN/bundle.json","state_url":"https://pith.science/pith/WDQAUMXRYNVD4M6PSIBJKXN6JN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/WDQAUMXRYNVD4M6PSIBJKXN6JN/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":"2026-05-23T05:08:09Z","links":{"resolver":"https://pith.science/pith/WDQAUMXRYNVD4M6PSIBJKXN6JN","bundle":"https://pith.science/pith/WDQAUMXRYNVD4M6PSIBJKXN6JN/bundle.json","state":"https://pith.science/pith/WDQAUMXRYNVD4M6PSIBJKXN6JN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/WDQAUMXRYNVD4M6PSIBJKXN6JN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:WDQAUMXRYNVD4M6PSIBJKXN6JN","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":"c42135a96881293b7c933fc9e0a331bce2474a8d21d2230b359fd76e78cf54c3","cross_cats_sorted":["hep-ex","hep-lat","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-05-24T09:52:36Z","title_canon_sha256":"effde059563392cd4d1164108232ba711f8f2ee3cfa62572b8adfb5b3161c5ea"},"schema_version":"1.0","source":{"id":"1805.09580","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1805.09580","created_at":"2026-05-18T00:00:19Z"},{"alias_kind":"arxiv_version","alias_value":"1805.09580v2","created_at":"2026-05-18T00:00:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.09580","created_at":"2026-05-18T00:00:19Z"},{"alias_kind":"pith_short_12","alias_value":"WDQAUMXRYNVD","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_16","alias_value":"WDQAUMXRYNVD4M6P","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_8","alias_value":"WDQAUMXR","created_at":"2026-05-18T12:32:59Z"}],"graph_snapshots":[{"event_id":"sha256:96b0dbdeccf57394fbb6a399c5695079dcae3ac8da3beff79b05ed13f166773d","target":"graph","created_at":"2026-05-18T00:00:19Z","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 the magnetic moments of spin-$3\\over 2$ singly charmed baryons in the heavy baryon chiral perturbation theory (HBChPT). The analytical expressions are given up to $\\mathcal{O}(p^3)$. The heavy quark symmetry is used to reduce the number of low energy constants (LECs). With the lattice QCD simulation data as the magnetic moments of the charmed baryons, the numerical results are given up to $\\mathcal{O}(p^3)$ in three scenarios. In the first scenario, we use the results in the quark model as the leading order input. In the second scenario, we use the heavy quark symmetry and neglect","authors_text":"Chang-Zhi Leng, Guang-Juan Wang, Lu Meng, Shi-Lin Zhu, Zhan-Wei Liu","cross_cats":["hep-ex","hep-lat","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-05-24T09:52:36Z","title":"Magnetic moments of the spin-${3\\over 2}$ singly heavy baryons"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.09580","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":"sha256:584a140dc0706c9770d0ce11c9338d9470f2fd3ea00191367b8524bef3122dce","target":"record","created_at":"2026-05-18T00:00:19Z","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":"c42135a96881293b7c933fc9e0a331bce2474a8d21d2230b359fd76e78cf54c3","cross_cats_sorted":["hep-ex","hep-lat","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-05-24T09:52:36Z","title_canon_sha256":"effde059563392cd4d1164108232ba711f8f2ee3cfa62572b8adfb5b3161c5ea"},"schema_version":"1.0","source":{"id":"1805.09580","kind":"arxiv","version":2}},"canonical_sha256":"b0e00a32f1c36a3e33cf9202955dbe4b40eaa33d1f28ac9ecb3f4ddf0d293c8f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b0e00a32f1c36a3e33cf9202955dbe4b40eaa33d1f28ac9ecb3f4ddf0d293c8f","first_computed_at":"2026-05-18T00:00:19.441827Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:00:19.441827Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"DZAz09E9LsjOuYk8nsVfJYmGGeWqZixoiqJWFoWYD6JJBtf1/QpVg2G+hyHXColapFMHINh8F6z+w24ZwbSBBw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:00:19.442308Z","signed_message":"canonical_sha256_bytes"},"source_id":"1805.09580","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:584a140dc0706c9770d0ce11c9338d9470f2fd3ea00191367b8524bef3122dce","sha256:96b0dbdeccf57394fbb6a399c5695079dcae3ac8da3beff79b05ed13f166773d"],"state_sha256":"f5b47930bbac7c02411442d03c64b8f290ef2e015c60c9455a58eda3d99ea597"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iz9WkJMQpd5NCEYkEMSo4hDvKglSOe0umzEXUqmYSoudaTn7kWeVGGA+j+hH6aD1MDdPHhV7AUQl1m7nJpSRDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-23T05:08:09.790444Z","bundle_sha256":"6ef6e68ef402d12e78387c45ea478aaf56c67d280137c1dd26ef660d54a4f52a"}}