{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:NBY3H3PHSCYEZTGPB5575U2K2N","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":"ddf140cb7807fa8495c4c679167b7a260884cd09ca492b5faac1f7323a7a7d0a","cross_cats_sorted":["hep-lat","hep-ph","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2024-06-25T15:22:49Z","title_canon_sha256":"c8a88687012350aa124e5b0425eb91cba6fafc64c0d182b101ed8a40abe51158"},"schema_version":"1.0","source":{"id":"2406.17638","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2406.17638","created_at":"2026-07-05T09:16:50Z"},{"alias_kind":"arxiv_version","alias_value":"2406.17638v2","created_at":"2026-07-05T09:16:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2406.17638","created_at":"2026-07-05T09:16:50Z"},{"alias_kind":"pith_short_12","alias_value":"NBY3H3PHSCYE","created_at":"2026-07-05T09:16:50Z"},{"alias_kind":"pith_short_16","alias_value":"NBY3H3PHSCYEZTGP","created_at":"2026-07-05T09:16:50Z"},{"alias_kind":"pith_short_8","alias_value":"NBY3H3PH","created_at":"2026-07-05T09:16:50Z"}],"graph_snapshots":[{"event_id":"sha256:fc79e71d23de97ae7969981b537f563378b6dbaf5b254c70c1405e9e933fd9e8","target":"graph","created_at":"2026-07-05T09:16:50Z","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/2406.17638/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Understanding the strong interactions within baryonic systems beyond the up and down quark sector is pivotal for a comprehensive description of nuclear forces. This study explores the interactions involving hyperons, particularly the $\\Lambda$ particle, within the framework of nuclear lattice effective field theory (NLEFT). By incorporating $\\Lambda$ hyperons into the NLEFT framework, we extend our investigation into the $S = -1$ sector, allowing us to probe the third dimension of the nuclear chart. We calculate the $\\Lambda$ separation energies ($B_{\\Lambda}$) of hypernuclei up to the medium-","authors_text":"Fabian Hildenbrand, Serdar Elhatisari, Ulf-G. Mei{\\ss}ner, Zhengxue Ren","cross_cats":["hep-lat","hep-ph","physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2024-06-25T15:22:49Z","title":"Towards Hypernuclei from Nuclear Lattice Effective Field Theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2406.17638","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:a45b38c168fab9e9e86fb11a6957d1e8d569dddfbad1fcf4decf40fe8a6d9fe5","target":"record","created_at":"2026-07-05T09:16:50Z","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":"ddf140cb7807fa8495c4c679167b7a260884cd09ca492b5faac1f7323a7a7d0a","cross_cats_sorted":["hep-lat","hep-ph","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2024-06-25T15:22:49Z","title_canon_sha256":"c8a88687012350aa124e5b0425eb91cba6fafc64c0d182b101ed8a40abe51158"},"schema_version":"1.0","source":{"id":"2406.17638","kind":"arxiv","version":2}},"canonical_sha256":"6871b3ede790b04ccccf0f7bfed34ad34a2ab366efcf4b0adace7c0374d5539b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6871b3ede790b04ccccf0f7bfed34ad34a2ab366efcf4b0adace7c0374d5539b","first_computed_at":"2026-07-05T09:16:50.487180Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T09:16:50.487180Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"h7uXwhtVitUhJBPKy+di+ofOWXuyYnx2cn9Z9EW1/riLpGMsAIA5/1ta3cUfPygi1ZTKQEbhqbNgbgLCK7qhBw==","signature_status":"signed_v1","signed_at":"2026-07-05T09:16:50.487789Z","signed_message":"canonical_sha256_bytes"},"source_id":"2406.17638","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a45b38c168fab9e9e86fb11a6957d1e8d569dddfbad1fcf4decf40fe8a6d9fe5","sha256:fc79e71d23de97ae7969981b537f563378b6dbaf5b254c70c1405e9e933fd9e8"],"state_sha256":"d10a962697fc15d80b5ac5d3cb1e6517f769f909314eb3b892dfb1ff20b39621"}