{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:7NLUJP3YNMRVWLIAF2AFHN3DSX","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":"7393ac0371745c141940c47cb004271f5339d49c653599e49c2b65639bf21a0d","cross_cats_sorted":["astro-ph.HE","hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2024-04-09T14:02:34Z","title_canon_sha256":"75dd88f697e9e1f281f38b8f7beb74328fe31091ec596873b3d8c65d5fdd2455"},"schema_version":"1.0","source":{"id":"2404.06323","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2404.06323","created_at":"2026-07-05T10:41:46Z"},{"alias_kind":"arxiv_version","alias_value":"2404.06323v3","created_at":"2026-07-05T10:41:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2404.06323","created_at":"2026-07-05T10:41:46Z"},{"alias_kind":"pith_short_12","alias_value":"7NLUJP3YNMRV","created_at":"2026-07-05T10:41:46Z"},{"alias_kind":"pith_short_16","alias_value":"7NLUJP3YNMRVWLIA","created_at":"2026-07-05T10:41:46Z"},{"alias_kind":"pith_short_8","alias_value":"7NLUJP3Y","created_at":"2026-07-05T10:41:46Z"}],"graph_snapshots":[{"event_id":"sha256:9d0a835fba71c3eed5b1568fb11492b30c259fee3c8dc4044505d415e4f4f109","target":"graph","created_at":"2026-07-05T10:41:46Z","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/2404.06323/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Constraining the equation of state (EOS) of strongly interacting, dense matter is the focus of intense experimental, observational, and theoretical effort. Chiral effective field theory ($\\chi$EFT) can describe the EOS between the typical densities of nuclei and those in the outer cores of neutron stars while perturbative QCD (pQCD) can be applied to properties of deconfined quark matter, both with quantified theoretical uncertainties. However, describing the full range of densities in between with a single EOS that has well-quantified uncertainties is a challenging problem. Bayesian multi-mod","authors_text":"A. C. Semposki, C. Drischler, D. R. Phillips, J. A. Melendez, R. J. Furnstahl","cross_cats":["astro-ph.HE","hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2024-04-09T14:02:34Z","title":"From chiral EFT to perturbative QCD: a Bayesian model mixing approach to symmetric nuclear matter"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2404.06323","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":"sha256:362d0f947397791d7ac8a08db323bf2ae3d4a48940c8bb9061721473c6dfbb75","target":"record","created_at":"2026-07-05T10:41:46Z","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":"7393ac0371745c141940c47cb004271f5339d49c653599e49c2b65639bf21a0d","cross_cats_sorted":["astro-ph.HE","hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2024-04-09T14:02:34Z","title_canon_sha256":"75dd88f697e9e1f281f38b8f7beb74328fe31091ec596873b3d8c65d5fdd2455"},"schema_version":"1.0","source":{"id":"2404.06323","kind":"arxiv","version":3}},"canonical_sha256":"fb5744bf786b235b2d002e8053b76395f123e822ebf68e72896b10e52d1671b1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"fb5744bf786b235b2d002e8053b76395f123e822ebf68e72896b10e52d1671b1","first_computed_at":"2026-07-05T10:41:46.113966Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:41:46.113966Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"rneljnfhiqpOKknzkkK8YKtrKRq13UBNUCwh97EwbZkJGEF092hgdpR3m0Xd5nnAobX1Aa2v9Soe65mz9SWsDQ==","signature_status":"signed_v1","signed_at":"2026-07-05T10:41:46.114452Z","signed_message":"canonical_sha256_bytes"},"source_id":"2404.06323","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:362d0f947397791d7ac8a08db323bf2ae3d4a48940c8bb9061721473c6dfbb75","sha256:9d0a835fba71c3eed5b1568fb11492b30c259fee3c8dc4044505d415e4f4f109"],"state_sha256":"197e0687ce9a378d253896f7a479738a1b9d14f8fee12464b3bab1565b9e0b58"}