{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:QV6LAUHVBOZRCTRJZSEUJFZQOZ","short_pith_number":"pith:QV6LAUHV","canonical_record":{"source":{"id":"1312.5513","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"nucl-th","submitted_at":"2013-12-19T12:35:59Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"bbf6de8dae95c1d73f1bcf49c5b5f26fa6b5430492af54c8a535271598004d06","abstract_canon_sha256":"f3d23344fca438f33135dc378e06279aea18a57827ad66e463fd5902b380ae68"},"schema_version":"1.0"},"canonical_sha256":"857cb050f50bb3114e29cc89449730765e9b09769b8d99dfb8f57896ccdc3330","source":{"kind":"arxiv","id":"1312.5513","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1312.5513","created_at":"2026-05-18T02:39:16Z"},{"alias_kind":"arxiv_version","alias_value":"1312.5513v3","created_at":"2026-05-18T02:39:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.5513","created_at":"2026-05-18T02:39:16Z"},{"alias_kind":"pith_short_12","alias_value":"QV6LAUHVBOZR","created_at":"2026-05-18T12:27:57Z"},{"alias_kind":"pith_short_16","alias_value":"QV6LAUHVBOZRCTRJ","created_at":"2026-05-18T12:27:57Z"},{"alias_kind":"pith_short_8","alias_value":"QV6LAUHV","created_at":"2026-05-18T12:27:57Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:QV6LAUHVBOZRCTRJZSEUJFZQOZ","target":"record","payload":{"canonical_record":{"source":{"id":"1312.5513","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"nucl-th","submitted_at":"2013-12-19T12:35:59Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"bbf6de8dae95c1d73f1bcf49c5b5f26fa6b5430492af54c8a535271598004d06","abstract_canon_sha256":"f3d23344fca438f33135dc378e06279aea18a57827ad66e463fd5902b380ae68"},"schema_version":"1.0"},"canonical_sha256":"857cb050f50bb3114e29cc89449730765e9b09769b8d99dfb8f57896ccdc3330","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:39:16.601136Z","signature_b64":"YSt3Bgd7Cdy5rwgAiBYRsumPRI+FwGiSUax7dQmIo/87QyWzrsKd1VT09H8pN3DhUQ6m5i8pqxVCZ2dKnQlHCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"857cb050f50bb3114e29cc89449730765e9b09769b8d99dfb8f57896ccdc3330","last_reissued_at":"2026-05-18T02:39:16.600712Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:39:16.600712Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1312.5513","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:39:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zhgp0t4N2mppnc7tjFVI3x8Q7DcJnMSWsfa4ciqf9CoOrPHkbPvDv4DkqDoO5EqS1K2H+R05NJh3O2mJHlONBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T07:16:42.630380Z"},"content_sha256":"4cef8dea1c88eca285bf0efbc40f9d024c64e326e1274f66bfd1c36543a9a295","schema_version":"1.0","event_id":"sha256:4cef8dea1c88eca285bf0efbc40f9d024c64e326e1274f66bfd1c36543a9a295"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:QV6LAUHVBOZRCTRJZSEUJFZQOZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Robust upper limit on the neutron single-particle energy of the $i_{13/2}$ orbit","license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"H. Jiang, Y. Lei","submitted_at":"2013-12-19T12:35:59Z","abstract_excerpt":"The boundary of the neutron $i_{13/2}$ single-particle energy is investigated with exact shell-model calculations, where random two-body interactions are adopted to overcome the bias from effective interactions. Excitation energies of $3^-_1$ state in $^{134}$Te and $^{136}$Xe, as well as those of $13/2^+_1$ states in $^{135}$Te and $^{137}$Xe, are taken as touchstones of our samplings. A robust upper limit of $\\varepsilon_{i13/2}<3.1$ MeV emerges in our calculations, given the mixing of $i_{13/2}$ single-neutron configuration and $f_{7/2}\\otimes 3^-$ configuration in $13/2^+_1$ states of $N=8"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.5513","kind":"arxiv","version":3},"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":"2026-05-18T02:39:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6r2NrLrrBuDzKDc5P6I0e1aeehQ3MqXJ+YFOKgBBnzYEQ/KdMioqYExQn8T/kfb3G6KEAICA5eSfZ5EydC60Cg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T07:16:42.630740Z"},"content_sha256":"bbccfb9e0d40cc241acfcb366e4fbb52747446821e086e63ddd986989923ccef","schema_version":"1.0","event_id":"sha256:bbccfb9e0d40cc241acfcb366e4fbb52747446821e086e63ddd986989923ccef"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/QV6LAUHVBOZRCTRJZSEUJFZQOZ/bundle.json","state_url":"https://pith.science/pith/QV6LAUHVBOZRCTRJZSEUJFZQOZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/QV6LAUHVBOZRCTRJZSEUJFZQOZ/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":"2026-06-03T07:16:42Z","links":{"resolver":"https://pith.science/pith/QV6LAUHVBOZRCTRJZSEUJFZQOZ","bundle":"https://pith.science/pith/QV6LAUHVBOZRCTRJZSEUJFZQOZ/bundle.json","state":"https://pith.science/pith/QV6LAUHVBOZRCTRJZSEUJFZQOZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/QV6LAUHVBOZRCTRJZSEUJFZQOZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:QV6LAUHVBOZRCTRJZSEUJFZQOZ","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":"f3d23344fca438f33135dc378e06279aea18a57827ad66e463fd5902b380ae68","cross_cats_sorted":["nucl-ex"],"license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"nucl-th","submitted_at":"2013-12-19T12:35:59Z","title_canon_sha256":"bbf6de8dae95c1d73f1bcf49c5b5f26fa6b5430492af54c8a535271598004d06"},"schema_version":"1.0","source":{"id":"1312.5513","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1312.5513","created_at":"2026-05-18T02:39:16Z"},{"alias_kind":"arxiv_version","alias_value":"1312.5513v3","created_at":"2026-05-18T02:39:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.5513","created_at":"2026-05-18T02:39:16Z"},{"alias_kind":"pith_short_12","alias_value":"QV6LAUHVBOZR","created_at":"2026-05-18T12:27:57Z"},{"alias_kind":"pith_short_16","alias_value":"QV6LAUHVBOZRCTRJ","created_at":"2026-05-18T12:27:57Z"},{"alias_kind":"pith_short_8","alias_value":"QV6LAUHV","created_at":"2026-05-18T12:27:57Z"}],"graph_snapshots":[{"event_id":"sha256:bbccfb9e0d40cc241acfcb366e4fbb52747446821e086e63ddd986989923ccef","target":"graph","created_at":"2026-05-18T02:39:16Z","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 boundary of the neutron $i_{13/2}$ single-particle energy is investigated with exact shell-model calculations, where random two-body interactions are adopted to overcome the bias from effective interactions. Excitation energies of $3^-_1$ state in $^{134}$Te and $^{136}$Xe, as well as those of $13/2^+_1$ states in $^{135}$Te and $^{137}$Xe, are taken as touchstones of our samplings. A robust upper limit of $\\varepsilon_{i13/2}<3.1$ MeV emerges in our calculations, given the mixing of $i_{13/2}$ single-neutron configuration and $f_{7/2}\\otimes 3^-$ configuration in $13/2^+_1$ states of $N=8","authors_text":"H. Jiang, Y. Lei","cross_cats":["nucl-ex"],"headline":"","license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"nucl-th","submitted_at":"2013-12-19T12:35:59Z","title":"Robust upper limit on the neutron single-particle energy of the $i_{13/2}$ orbit"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.5513","kind":"arxiv","version":3},"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":"sha256:4cef8dea1c88eca285bf0efbc40f9d024c64e326e1274f66bfd1c36543a9a295","target":"record","created_at":"2026-05-18T02:39:16Z","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":"f3d23344fca438f33135dc378e06279aea18a57827ad66e463fd5902b380ae68","cross_cats_sorted":["nucl-ex"],"license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"nucl-th","submitted_at":"2013-12-19T12:35:59Z","title_canon_sha256":"bbf6de8dae95c1d73f1bcf49c5b5f26fa6b5430492af54c8a535271598004d06"},"schema_version":"1.0","source":{"id":"1312.5513","kind":"arxiv","version":3}},"canonical_sha256":"857cb050f50bb3114e29cc89449730765e9b09769b8d99dfb8f57896ccdc3330","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"857cb050f50bb3114e29cc89449730765e9b09769b8d99dfb8f57896ccdc3330","first_computed_at":"2026-05-18T02:39:16.600712Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:39:16.600712Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"YSt3Bgd7Cdy5rwgAiBYRsumPRI+FwGiSUax7dQmIo/87QyWzrsKd1VT09H8pN3DhUQ6m5i8pqxVCZ2dKnQlHCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:39:16.601136Z","signed_message":"canonical_sha256_bytes"},"source_id":"1312.5513","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4cef8dea1c88eca285bf0efbc40f9d024c64e326e1274f66bfd1c36543a9a295","sha256:bbccfb9e0d40cc241acfcb366e4fbb52747446821e086e63ddd986989923ccef"],"state_sha256":"e0654f81d14bdf13029d86ba6c4b60ff4cef20839e96f8dc268ad511459b401a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gPMulg2aVEBzgScy20swwUO2jXKuUa/2H1lP+xttGX9WagseiNlcTCCgkmURSB4YdS5XHYvPZMMU67zHi1WnDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T07:16:42.632733Z","bundle_sha256":"bd0e326f4d8f755aafbcd4d225c95c56c7223de8ddacf0af3275728d166da27c"}}