{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:6QUYNY3YRW7AONJNW7XIHKIWD7","short_pith_number":"pith:6QUYNY3Y","canonical_record":{"source":{"id":"1208.0477","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-08-02T13:29:58Z","cross_cats_sorted":[],"title_canon_sha256":"dad3aa92ade406dc8c394e481d52be337345bc4fccaa0d13e305df605219367e","abstract_canon_sha256":"95a96dcfb894c749f986a16bb980fcb6d316e6090b0e1bb99ad77e29c5c92e7c"},"schema_version":"1.0"},"canonical_sha256":"f42986e3788dbe07352db7ee83a9161ffbb56ac7ba42fff5c40f9a7f7a6b67a2","source":{"kind":"arxiv","id":"1208.0477","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1208.0477","created_at":"2026-05-18T01:55:23Z"},{"alias_kind":"arxiv_version","alias_value":"1208.0477v1","created_at":"2026-05-18T01:55:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1208.0477","created_at":"2026-05-18T01:55:23Z"},{"alias_kind":"pith_short_12","alias_value":"6QUYNY3YRW7A","created_at":"2026-05-18T12:26:56Z"},{"alias_kind":"pith_short_16","alias_value":"6QUYNY3YRW7AONJN","created_at":"2026-05-18T12:26:56Z"},{"alias_kind":"pith_short_8","alias_value":"6QUYNY3Y","created_at":"2026-05-18T12:26:56Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:6QUYNY3YRW7AONJNW7XIHKIWD7","target":"record","payload":{"canonical_record":{"source":{"id":"1208.0477","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-08-02T13:29:58Z","cross_cats_sorted":[],"title_canon_sha256":"dad3aa92ade406dc8c394e481d52be337345bc4fccaa0d13e305df605219367e","abstract_canon_sha256":"95a96dcfb894c749f986a16bb980fcb6d316e6090b0e1bb99ad77e29c5c92e7c"},"schema_version":"1.0"},"canonical_sha256":"f42986e3788dbe07352db7ee83a9161ffbb56ac7ba42fff5c40f9a7f7a6b67a2","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:55:23.839897Z","signature_b64":"/qb3+k4HO8myR0TpqIPMiDTKirkoHh26cPZO8lWpajWyRWjUIDKWXkWRHLeKvRpS/i8cs5t3y2bP1kj8ge/xBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f42986e3788dbe07352db7ee83a9161ffbb56ac7ba42fff5c40f9a7f7a6b67a2","last_reissued_at":"2026-05-18T01:55:23.839376Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:55:23.839376Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1208.0477","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":"2026-05-18T01:55:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SjwPSh9Y0jgJ0/hmaKT2ZJx/XGXmnwAfP0BJM89Zvn4fw4r1O/GGf3kjHNnjw787uEzDuYYgPFnW6pdUPzEyBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T01:49:10.222342Z"},"content_sha256":"6dc2016d0d849480cb493dea1f9f5340db746f2e64f2f9077cff263bc0e87d0b","schema_version":"1.0","event_id":"sha256:6dc2016d0d849480cb493dea1f9f5340db746f2e64f2f9077cff263bc0e87d0b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:6QUYNY3YRW7AONJNW7XIHKIWD7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Magnetic moments of the low-lying $J^P=\\,1/2^-$, $3/2^-$ $\\Lambda$ resonances within the framework of the chiral quark model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"A. Mart\\'inez Torres, Harleen Dahiya, K. P. Khemchandani, Neetika Sharma","submitted_at":"2012-08-02T13:29:58Z","abstract_excerpt":"The magnetic moments of the low-lying spin-parity $J^P=$ $1/2^-$, $3/2^-$ $\\Lambda$ resonances, like, for example, $\\Lambda(1405)$ $1/2^-$, $\\Lambda(1520)$ $3/2^-$, as well as their transition magnetic moments, are calculated using the chiral quark model. The results found are compared with those obtained from the nonrelativistic quark model and those of unitary chiral theories, where some of these states are generated through the dynamics of two hadron coupled channels and their unitarization."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1208.0477","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":"2026-05-18T01:55:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LF2QgexazkVEj7mcGu7RgpF5TNGCpCcc6b0jHLC/dYKHtwD/NEqnkYK/NGajv/EDS4HoBllcLovKdVtHPs2LDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T01:49:10.223029Z"},"content_sha256":"2276fdb6888df47866fc606fd5529d34ab2ee6edc17fbc6aa86a2e6e44207d2a","schema_version":"1.0","event_id":"sha256:2276fdb6888df47866fc606fd5529d34ab2ee6edc17fbc6aa86a2e6e44207d2a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6QUYNY3YRW7AONJNW7XIHKIWD7/bundle.json","state_url":"https://pith.science/pith/6QUYNY3YRW7AONJNW7XIHKIWD7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6QUYNY3YRW7AONJNW7XIHKIWD7/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":"2026-06-05T01:49:10Z","links":{"resolver":"https://pith.science/pith/6QUYNY3YRW7AONJNW7XIHKIWD7","bundle":"https://pith.science/pith/6QUYNY3YRW7AONJNW7XIHKIWD7/bundle.json","state":"https://pith.science/pith/6QUYNY3YRW7AONJNW7XIHKIWD7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6QUYNY3YRW7AONJNW7XIHKIWD7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:6QUYNY3YRW7AONJNW7XIHKIWD7","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":"95a96dcfb894c749f986a16bb980fcb6d316e6090b0e1bb99ad77e29c5c92e7c","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-08-02T13:29:58Z","title_canon_sha256":"dad3aa92ade406dc8c394e481d52be337345bc4fccaa0d13e305df605219367e"},"schema_version":"1.0","source":{"id":"1208.0477","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1208.0477","created_at":"2026-05-18T01:55:23Z"},{"alias_kind":"arxiv_version","alias_value":"1208.0477v1","created_at":"2026-05-18T01:55:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1208.0477","created_at":"2026-05-18T01:55:23Z"},{"alias_kind":"pith_short_12","alias_value":"6QUYNY3YRW7A","created_at":"2026-05-18T12:26:56Z"},{"alias_kind":"pith_short_16","alias_value":"6QUYNY3YRW7AONJN","created_at":"2026-05-18T12:26:56Z"},{"alias_kind":"pith_short_8","alias_value":"6QUYNY3Y","created_at":"2026-05-18T12:26:56Z"}],"graph_snapshots":[{"event_id":"sha256:2276fdb6888df47866fc606fd5529d34ab2ee6edc17fbc6aa86a2e6e44207d2a","target":"graph","created_at":"2026-05-18T01:55:23Z","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":"The magnetic moments of the low-lying spin-parity $J^P=$ $1/2^-$, $3/2^-$ $\\Lambda$ resonances, like, for example, $\\Lambda(1405)$ $1/2^-$, $\\Lambda(1520)$ $3/2^-$, as well as their transition magnetic moments, are calculated using the chiral quark model. The results found are compared with those obtained from the nonrelativistic quark model and those of unitary chiral theories, where some of these states are generated through the dynamics of two hadron coupled channels and their unitarization.","authors_text":"A. Mart\\'inez Torres, Harleen Dahiya, K. P. Khemchandani, Neetika Sharma","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-08-02T13:29:58Z","title":"Magnetic moments of the low-lying $J^P=\\,1/2^-$, $3/2^-$ $\\Lambda$ resonances within the framework of the chiral quark model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1208.0477","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":"sha256:6dc2016d0d849480cb493dea1f9f5340db746f2e64f2f9077cff263bc0e87d0b","target":"record","created_at":"2026-05-18T01:55:23Z","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":"95a96dcfb894c749f986a16bb980fcb6d316e6090b0e1bb99ad77e29c5c92e7c","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-08-02T13:29:58Z","title_canon_sha256":"dad3aa92ade406dc8c394e481d52be337345bc4fccaa0d13e305df605219367e"},"schema_version":"1.0","source":{"id":"1208.0477","kind":"arxiv","version":1}},"canonical_sha256":"f42986e3788dbe07352db7ee83a9161ffbb56ac7ba42fff5c40f9a7f7a6b67a2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f42986e3788dbe07352db7ee83a9161ffbb56ac7ba42fff5c40f9a7f7a6b67a2","first_computed_at":"2026-05-18T01:55:23.839376Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:55:23.839376Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"/qb3+k4HO8myR0TpqIPMiDTKirkoHh26cPZO8lWpajWyRWjUIDKWXkWRHLeKvRpS/i8cs5t3y2bP1kj8ge/xBA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:55:23.839897Z","signed_message":"canonical_sha256_bytes"},"source_id":"1208.0477","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6dc2016d0d849480cb493dea1f9f5340db746f2e64f2f9077cff263bc0e87d0b","sha256:2276fdb6888df47866fc606fd5529d34ab2ee6edc17fbc6aa86a2e6e44207d2a"],"state_sha256":"ec7de564320da1d140e0f3bdc634693fb820b86589594da2ca061e45a3374e4d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8O8pyF+RWfLafEFh13IKZsifbcUcSaLYTpHHCg2tPQk2EioTwqrHwrAEXxQNxGvTVE/XIvfuf/Bm9sWtVKgpBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-05T01:49:10.226618Z","bundle_sha256":"71aeec0bd96ea6cbe86f9cfa88db0c0d0941f35b6c33ecee6fd28c089732ceec"}}