{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:4VUAMC34WLV6WQP6R7ULXR4QA5","short_pith_number":"pith:4VUAMC34","canonical_record":{"source":{"id":"1105.0837","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2011-05-04T14:28:40Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"dc2c8f0dd673bfeb37754f0bcd927afd4cbdf7fbc454d4c453a4617b80f43f4f","abstract_canon_sha256":"00bd80e0744dd7c6c58aeb10d888adabf75e336954acceb246bce5f4dce23554"},"schema_version":"1.0"},"canonical_sha256":"e568060b7cb2ebeb41fe8fe8bbc790075b43e32f147b35a497a248f83e4c7e82","source":{"kind":"arxiv","id":"1105.0837","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1105.0837","created_at":"2026-05-18T03:00:27Z"},{"alias_kind":"arxiv_version","alias_value":"1105.0837v2","created_at":"2026-05-18T03:00:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.0837","created_at":"2026-05-18T03:00:27Z"},{"alias_kind":"pith_short_12","alias_value":"4VUAMC34WLV6","created_at":"2026-05-18T12:26:20Z"},{"alias_kind":"pith_short_16","alias_value":"4VUAMC34WLV6WQP6","created_at":"2026-05-18T12:26:20Z"},{"alias_kind":"pith_short_8","alias_value":"4VUAMC34","created_at":"2026-05-18T12:26:20Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:4VUAMC34WLV6WQP6R7ULXR4QA5","target":"record","payload":{"canonical_record":{"source":{"id":"1105.0837","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2011-05-04T14:28:40Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"dc2c8f0dd673bfeb37754f0bcd927afd4cbdf7fbc454d4c453a4617b80f43f4f","abstract_canon_sha256":"00bd80e0744dd7c6c58aeb10d888adabf75e336954acceb246bce5f4dce23554"},"schema_version":"1.0"},"canonical_sha256":"e568060b7cb2ebeb41fe8fe8bbc790075b43e32f147b35a497a248f83e4c7e82","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:00:27.289039Z","signature_b64":"p6uV065PSHmwNxtazH7SlE3KQL8KfXcAOv+vZQu32eeeLxEeF0L8TfoDMrJ16ZsMXr8+UzmChZJb8d+U5KupBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e568060b7cb2ebeb41fe8fe8bbc790075b43e32f147b35a497a248f83e4c7e82","last_reissued_at":"2026-05-18T03:00:27.288373Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:00:27.288373Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1105.0837","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":"2026-05-18T03:00:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3WMnyeSLRHUlXKv9dF0L2twNw5taD/BkbMbjGMdgC06DK3kcRixRLD+4/z5ovdB1+jvoH+6c+NtMdulmeOxEDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T15:57:38.473297Z"},"content_sha256":"4aaa8d06ff94dbe82e5ce4d5b9caee0357c0aa2afbb933d479493c8a67f89342","schema_version":"1.0","event_id":"sha256:4aaa8d06ff94dbe82e5ce4d5b9caee0357c0aa2afbb933d479493c8a67f89342"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:4VUAMC34WLV6WQP6R7ULXR4QA5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"General Treatment of Vortical, Toroidal, and Compression Modes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"J. Kvasil, P.-G. Reinhard, P. Vesely, V.O. Nesterenko, W. Kleinig","submitted_at":"2011-05-04T14:28:40Z","abstract_excerpt":"The multipole vortical, toroidal, and compression modes are analyzed. Following the vorticity concept of Ravenhall and Wambach, the vortical operator is derived and related in a simple way to the toroidal and compression operators. The strength functions and velocity fields of the modes are analyzed in $^{208}$Pb within the random-phase-approximation using the Skyrme force SLy6. Both convection and magnetization nuclear currents are taken into account. It is shown that the isoscalar (isovector) vortical and toroidal modes are dominated by the convection (magnetization) nuclear current while th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.0837","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":"2026-05-18T03:00:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1xmqEyTrVNOUeIEnQFwuofDglFNfUcbaDA8sRnDfCi+c95NZ2gJF8VfJp2z2vpvLuI/7i+ojDuqK5SjOBXrfBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T15:57:38.473653Z"},"content_sha256":"ca9ee20744401a94a6401cecd200fe85b5df09257b2010c730d79118918f713d","schema_version":"1.0","event_id":"sha256:ca9ee20744401a94a6401cecd200fe85b5df09257b2010c730d79118918f713d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4VUAMC34WLV6WQP6R7ULXR4QA5/bundle.json","state_url":"https://pith.science/pith/4VUAMC34WLV6WQP6R7ULXR4QA5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4VUAMC34WLV6WQP6R7ULXR4QA5/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":"2026-06-01T15:57:38Z","links":{"resolver":"https://pith.science/pith/4VUAMC34WLV6WQP6R7ULXR4QA5","bundle":"https://pith.science/pith/4VUAMC34WLV6WQP6R7ULXR4QA5/bundle.json","state":"https://pith.science/pith/4VUAMC34WLV6WQP6R7ULXR4QA5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4VUAMC34WLV6WQP6R7ULXR4QA5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:4VUAMC34WLV6WQP6R7ULXR4QA5","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":"00bd80e0744dd7c6c58aeb10d888adabf75e336954acceb246bce5f4dce23554","cross_cats_sorted":["nucl-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2011-05-04T14:28:40Z","title_canon_sha256":"dc2c8f0dd673bfeb37754f0bcd927afd4cbdf7fbc454d4c453a4617b80f43f4f"},"schema_version":"1.0","source":{"id":"1105.0837","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1105.0837","created_at":"2026-05-18T03:00:27Z"},{"alias_kind":"arxiv_version","alias_value":"1105.0837v2","created_at":"2026-05-18T03:00:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.0837","created_at":"2026-05-18T03:00:27Z"},{"alias_kind":"pith_short_12","alias_value":"4VUAMC34WLV6","created_at":"2026-05-18T12:26:20Z"},{"alias_kind":"pith_short_16","alias_value":"4VUAMC34WLV6WQP6","created_at":"2026-05-18T12:26:20Z"},{"alias_kind":"pith_short_8","alias_value":"4VUAMC34","created_at":"2026-05-18T12:26:20Z"}],"graph_snapshots":[{"event_id":"sha256:ca9ee20744401a94a6401cecd200fe85b5df09257b2010c730d79118918f713d","target":"graph","created_at":"2026-05-18T03:00:27Z","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 multipole vortical, toroidal, and compression modes are analyzed. Following the vorticity concept of Ravenhall and Wambach, the vortical operator is derived and related in a simple way to the toroidal and compression operators. The strength functions and velocity fields of the modes are analyzed in $^{208}$Pb within the random-phase-approximation using the Skyrme force SLy6. Both convection and magnetization nuclear currents are taken into account. It is shown that the isoscalar (isovector) vortical and toroidal modes are dominated by the convection (magnetization) nuclear current while th","authors_text":"J. Kvasil, P.-G. Reinhard, P. Vesely, V.O. Nesterenko, W. Kleinig","cross_cats":["nucl-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2011-05-04T14:28:40Z","title":"General Treatment of Vortical, Toroidal, and Compression Modes"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.0837","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":"sha256:4aaa8d06ff94dbe82e5ce4d5b9caee0357c0aa2afbb933d479493c8a67f89342","target":"record","created_at":"2026-05-18T03:00:27Z","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":"00bd80e0744dd7c6c58aeb10d888adabf75e336954acceb246bce5f4dce23554","cross_cats_sorted":["nucl-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2011-05-04T14:28:40Z","title_canon_sha256":"dc2c8f0dd673bfeb37754f0bcd927afd4cbdf7fbc454d4c453a4617b80f43f4f"},"schema_version":"1.0","source":{"id":"1105.0837","kind":"arxiv","version":2}},"canonical_sha256":"e568060b7cb2ebeb41fe8fe8bbc790075b43e32f147b35a497a248f83e4c7e82","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e568060b7cb2ebeb41fe8fe8bbc790075b43e32f147b35a497a248f83e4c7e82","first_computed_at":"2026-05-18T03:00:27.288373Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:00:27.288373Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"p6uV065PSHmwNxtazH7SlE3KQL8KfXcAOv+vZQu32eeeLxEeF0L8TfoDMrJ16ZsMXr8+UzmChZJb8d+U5KupBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:00:27.289039Z","signed_message":"canonical_sha256_bytes"},"source_id":"1105.0837","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4aaa8d06ff94dbe82e5ce4d5b9caee0357c0aa2afbb933d479493c8a67f89342","sha256:ca9ee20744401a94a6401cecd200fe85b5df09257b2010c730d79118918f713d"],"state_sha256":"b9230b41705426803dbbc14e82ef46350c725ef5d91ec12685bafa9893f4b0ab"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fqsWDoZ/JR6B/yS3uWhdYo5lSYFYBsuEIJ+DoMX6YrvtOTbeq9j3COsOGf562C3RO+vm6BNxaHcg1H5iek2zCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T15:57:38.475587Z","bundle_sha256":"50d91b592f9120a645ac7b948ed982a9dac5f5cd676e01002958c0a2db94632e"}}