{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2020:BG5RTD32C266GJQR5VJRIQAXGK","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":"ac01fcedc1c50263bdf83d08085b0df33efb1e0520d74a54e4c61ad162ccd75d","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2020-12-07T06:03:45Z","title_canon_sha256":"63772368e9438e06bed7276accf1d2c66efaf0ac5ffe8984e78a80a1bbc711d9"},"schema_version":"1.0","source":{"id":"2012.03465","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2012.03465","created_at":"2026-07-05T02:17:43Z"},{"alias_kind":"arxiv_version","alias_value":"2012.03465v2","created_at":"2026-07-05T02:17:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2012.03465","created_at":"2026-07-05T02:17:43Z"},{"alias_kind":"pith_short_12","alias_value":"BG5RTD32C266","created_at":"2026-07-05T02:17:43Z"},{"alias_kind":"pith_short_16","alias_value":"BG5RTD32C266GJQR","created_at":"2026-07-05T02:17:43Z"},{"alias_kind":"pith_short_8","alias_value":"BG5RTD32","created_at":"2026-07-05T02:17:43Z"}],"graph_snapshots":[{"event_id":"sha256:10a8c8fd7035f085dbdbb4258bed03fc177783afe66ff64b604607011f46e1d5","target":"graph","created_at":"2026-07-05T02:17:43Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2012.03465/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The nuclear level density of $^{115}$Sn has been measured in an excitation energy range of $\\sim $2 - 9 MeV using the experimental neutron evaporation spectra from the $^{115}$In($p,n$)$^{115}$Sn reaction. The experimental level densities were compared with the microscopic Hartree-Fock BCS (HFBCS), Hartree-Fock-Bogoliubov plus combinatorial (HFB+C), and an exact pairing plus independent particle model (EP+IPM) calculations. It is observed that the EP+IPM provides the most accurate description of the experimental data. The thermal properties (entropy and temperature) of $^{115}$Sn have been inv","authors_text":"A. Sen, C. Bhattacharya, Deepak Pandit, D. Mondal, D. Paul, G. Mukherjee, K. Atreya, K. Banerjee, N. Quang Hung, Pratap Roy, R. Pandey, S. Kundu, S. Manna, S. Mukhopadhyay, S. Pal, T. K. Ghosh, T. K. Rana","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2020-12-07T06:03:45Z","title":"Nuclear level density and thermal properties of $^{115}$Sn from neutron evaporation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2012.03465","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:c63c6e783b0d1f035289701d513393c0b6bfbcc8c5406ad08f96c93ce6b205b0","target":"record","created_at":"2026-07-05T02:17:43Z","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":"ac01fcedc1c50263bdf83d08085b0df33efb1e0520d74a54e4c61ad162ccd75d","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2020-12-07T06:03:45Z","title_canon_sha256":"63772368e9438e06bed7276accf1d2c66efaf0ac5ffe8984e78a80a1bbc711d9"},"schema_version":"1.0","source":{"id":"2012.03465","kind":"arxiv","version":2}},"canonical_sha256":"09bb198f7a16bde32611ed5314401732a6ff6dcfdeac28993e3105d3c9c02b39","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"09bb198f7a16bde32611ed5314401732a6ff6dcfdeac28993e3105d3c9c02b39","first_computed_at":"2026-07-05T02:17:43.815879Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T02:17:43.815879Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"cZ/DPYKwyc91jzF4usapjCQXBpoOj6dyK6ZvTlndy0Y4c1j5DuHx/4rYK6wuzob4SExVV8P++9ETzd+WO7rkAA==","signature_status":"signed_v1","signed_at":"2026-07-05T02:17:43.816276Z","signed_message":"canonical_sha256_bytes"},"source_id":"2012.03465","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c63c6e783b0d1f035289701d513393c0b6bfbcc8c5406ad08f96c93ce6b205b0","sha256:10a8c8fd7035f085dbdbb4258bed03fc177783afe66ff64b604607011f46e1d5"],"state_sha256":"88d711a557b4518cee2b2c59aeb3ab0375c553e1b0ceb5701cf178bb6918fd61"}