{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:UWTCGE6QMNRDNN37I4JCOT55WH","short_pith_number":"pith:UWTCGE6Q","canonical_record":{"source":{"id":"1710.06218","kind":"arxiv","version":16},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-10-17T11:31:59Z","cross_cats_sorted":["nucl-ex","quant-ph"],"title_canon_sha256":"1e72e36d6264c4996458902c932c6fb92af71e6c2e68a5416112ec0f69efca7b","abstract_canon_sha256":"5f7c1f621651de65bdb0b3254e4882b66d337dff99117370d9bb5897ed3e79e7"},"schema_version":"1.0"},"canonical_sha256":"a5a62313d0636236b77f4712274fbdb1eb8ad7f0d3c880b25c7cb23cc706bff3","source":{"kind":"arxiv","id":"1710.06218","version":16},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.06218","created_at":"2026-05-18T00:11:11Z"},{"alias_kind":"arxiv_version","alias_value":"1710.06218v16","created_at":"2026-05-18T00:11:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.06218","created_at":"2026-05-18T00:11:11Z"},{"alias_kind":"pith_short_12","alias_value":"UWTCGE6QMNRD","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_16","alias_value":"UWTCGE6QMNRDNN37","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_8","alias_value":"UWTCGE6Q","created_at":"2026-05-18T12:31:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:UWTCGE6QMNRDNN37I4JCOT55WH","target":"record","payload":{"canonical_record":{"source":{"id":"1710.06218","kind":"arxiv","version":16},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-10-17T11:31:59Z","cross_cats_sorted":["nucl-ex","quant-ph"],"title_canon_sha256":"1e72e36d6264c4996458902c932c6fb92af71e6c2e68a5416112ec0f69efca7b","abstract_canon_sha256":"5f7c1f621651de65bdb0b3254e4882b66d337dff99117370d9bb5897ed3e79e7"},"schema_version":"1.0"},"canonical_sha256":"a5a62313d0636236b77f4712274fbdb1eb8ad7f0d3c880b25c7cb23cc706bff3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:11:11.471961Z","signature_b64":"YU8HQfvIgWYIq5aCiP7iGBNkk0buAVAwHMmcpCzDF4XCb6bJHxcBceQYR/tTcnVpfNtBBrUvTzYO+7MJDAZgAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a5a62313d0636236b77f4712274fbdb1eb8ad7f0d3c880b25c7cb23cc706bff3","last_reissued_at":"2026-05-18T00:11:11.471083Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:11:11.471083Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1710.06218","source_version":16,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:11:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"J9UrNJNVm4xd2reFEbaA/YReff4PGCk+FvM8N4FLKlcvHsTMgbdrBcwBUIuUm72zwBIzQiXySV2Qr/NkNxK8Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T08:11:19.210433Z"},"content_sha256":"b230370cc1353b698b6045750f3e8645e7a694a2360c583f766efa1ba5510274","schema_version":"1.0","event_id":"sha256:b230370cc1353b698b6045750f3e8645e7a694a2360c583f766efa1ba5510274"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:UWTCGE6QMNRDNN37I4JCOT55WH","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Study of the Q.Q Interaction- Single Particle Behavior to Elliott's Rotations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex","quant-ph"],"primary_cat":"nucl-th","authors_text":"Arun Kingan, Larry Zamick, Xiaofei Yu","submitted_at":"2017-10-17T11:31:59Z","abstract_excerpt":"We perform shell model calculations using a quadrupole-quadrupole interaction (Q.Q).We show results in single j shell spaces and the full S-D shell . We show that one gets useful results with Q.Q in both spaces.. We emphasize the importance of the choice of single particle energies in order to obtain the results of Elliott using a Q.Q interaction without the momentum terms. We show a J(J+1) spectrum for a ground state band but with B(E2)'s different from the rotational model. We also show excited J(J-1), J((J-1) and J(J+3) spectra.We find spectra starting with J=0 which have both even J and od"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.06218","kind":"arxiv","version":16},"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":"2026-05-18T00:11:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XneB544kyGP3Di9mfDKqbrtxW3zgpflsx9MNjF9kCVJUKdngWYZIFpX/eGBqqdcbDOwP8x5wAIPjlhcrnLZqBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T08:11:19.211138Z"},"content_sha256":"f208c1b51c28a04679c772616bcd1981e7735fce4defbe0fe12dcf32b291735e","schema_version":"1.0","event_id":"sha256:f208c1b51c28a04679c772616bcd1981e7735fce4defbe0fe12dcf32b291735e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UWTCGE6QMNRDNN37I4JCOT55WH/bundle.json","state_url":"https://pith.science/pith/UWTCGE6QMNRDNN37I4JCOT55WH/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UWTCGE6QMNRDNN37I4JCOT55WH/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":"2026-05-30T08:11:19Z","links":{"resolver":"https://pith.science/pith/UWTCGE6QMNRDNN37I4JCOT55WH","bundle":"https://pith.science/pith/UWTCGE6QMNRDNN37I4JCOT55WH/bundle.json","state":"https://pith.science/pith/UWTCGE6QMNRDNN37I4JCOT55WH/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UWTCGE6QMNRDNN37I4JCOT55WH/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:UWTCGE6QMNRDNN37I4JCOT55WH","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":"5f7c1f621651de65bdb0b3254e4882b66d337dff99117370d9bb5897ed3e79e7","cross_cats_sorted":["nucl-ex","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-10-17T11:31:59Z","title_canon_sha256":"1e72e36d6264c4996458902c932c6fb92af71e6c2e68a5416112ec0f69efca7b"},"schema_version":"1.0","source":{"id":"1710.06218","kind":"arxiv","version":16}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.06218","created_at":"2026-05-18T00:11:11Z"},{"alias_kind":"arxiv_version","alias_value":"1710.06218v16","created_at":"2026-05-18T00:11:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.06218","created_at":"2026-05-18T00:11:11Z"},{"alias_kind":"pith_short_12","alias_value":"UWTCGE6QMNRD","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_16","alias_value":"UWTCGE6QMNRDNN37","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_8","alias_value":"UWTCGE6Q","created_at":"2026-05-18T12:31:49Z"}],"graph_snapshots":[{"event_id":"sha256:f208c1b51c28a04679c772616bcd1981e7735fce4defbe0fe12dcf32b291735e","target":"graph","created_at":"2026-05-18T00:11:11Z","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 perform shell model calculations using a quadrupole-quadrupole interaction (Q.Q).We show results in single j shell spaces and the full S-D shell . We show that one gets useful results with Q.Q in both spaces.. We emphasize the importance of the choice of single particle energies in order to obtain the results of Elliott using a Q.Q interaction without the momentum terms. We show a J(J+1) spectrum for a ground state band but with B(E2)'s different from the rotational model. We also show excited J(J-1), J((J-1) and J(J+3) spectra.We find spectra starting with J=0 which have both even J and od","authors_text":"Arun Kingan, Larry Zamick, Xiaofei Yu","cross_cats":["nucl-ex","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-10-17T11:31:59Z","title":"Study of the Q.Q Interaction- Single Particle Behavior to Elliott's Rotations"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.06218","kind":"arxiv","version":16},"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:b230370cc1353b698b6045750f3e8645e7a694a2360c583f766efa1ba5510274","target":"record","created_at":"2026-05-18T00:11:11Z","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":"5f7c1f621651de65bdb0b3254e4882b66d337dff99117370d9bb5897ed3e79e7","cross_cats_sorted":["nucl-ex","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-10-17T11:31:59Z","title_canon_sha256":"1e72e36d6264c4996458902c932c6fb92af71e6c2e68a5416112ec0f69efca7b"},"schema_version":"1.0","source":{"id":"1710.06218","kind":"arxiv","version":16}},"canonical_sha256":"a5a62313d0636236b77f4712274fbdb1eb8ad7f0d3c880b25c7cb23cc706bff3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a5a62313d0636236b77f4712274fbdb1eb8ad7f0d3c880b25c7cb23cc706bff3","first_computed_at":"2026-05-18T00:11:11.471083Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:11:11.471083Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"YU8HQfvIgWYIq5aCiP7iGBNkk0buAVAwHMmcpCzDF4XCb6bJHxcBceQYR/tTcnVpfNtBBrUvTzYO+7MJDAZgAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:11:11.471961Z","signed_message":"canonical_sha256_bytes"},"source_id":"1710.06218","source_kind":"arxiv","source_version":16}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b230370cc1353b698b6045750f3e8645e7a694a2360c583f766efa1ba5510274","sha256:f208c1b51c28a04679c772616bcd1981e7735fce4defbe0fe12dcf32b291735e"],"state_sha256":"ae8e8a4645ab492fbaccd185708159c8ecab5b653e5e4e0206cfbfa092aec287"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3mViWw+YRuMKR0XQvjYuG5AyNXRCh+vmVbWWkvr8wHNMZa49L8ilqUZWhWYM+iuVJ0+DX2kGacStR+xWZAlxCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T08:11:19.214859Z","bundle_sha256":"a52d1bc43f7601e06a9f6ca9d2a2b828020a00eb8443cc8bd9bf00a133b7927b"}}