{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:2DPZTSJUTI5F6BQ5HFZPT4Z6GX","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":"2c2d8f827bcffcc05964e2916ad92e6b812ff7ea1300c90d385c20b29d0d7859","cross_cats_sorted":["cond-mat.stat-mech","physics.plasm-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2022-04-29T17:37:13Z","title_canon_sha256":"0a37a76e8b65571e5c0674c551654ea93285595a8d0311e51af2de136d9b4489"},"schema_version":"1.0","source":{"id":"2204.14260","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2204.14260","created_at":"2026-07-05T05:22:29Z"},{"alias_kind":"arxiv_version","alias_value":"2204.14260v2","created_at":"2026-07-05T05:22:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2204.14260","created_at":"2026-07-05T05:22:29Z"},{"alias_kind":"pith_short_12","alias_value":"2DPZTSJUTI5F","created_at":"2026-07-05T05:22:29Z"},{"alias_kind":"pith_short_16","alias_value":"2DPZTSJUTI5F6BQ5","created_at":"2026-07-05T05:22:29Z"},{"alias_kind":"pith_short_8","alias_value":"2DPZTSJU","created_at":"2026-07-05T05:22:29Z"}],"graph_snapshots":[{"event_id":"sha256:57607b149f656931a122cd5c6cf11621f62c2385c42c06e2eaa5e879c582da8c","target":"graph","created_at":"2026-07-05T05:22:29Z","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/2204.14260/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The rigorous description of correlated quantum many-body systems constitutes one of the most challenging tasks in contemporary physics and related disciplines. In this context, a particularly useful tool is the concept of effective pair potentials that take into account the effects of the complex many-body medium consistently. In this work, we present extensive, highly accurate \\emph{ab initio} path integral Monte Carlo (PIMC) results for the effective interaction and the effective force between two electrons in the presence of the uniform electron gas (UEG). This gives us a direct insight int","authors_text":"Attila Cangi, Jan Vorberger, Panagiotis Tolias, Tobias Dornheim, Zhandos Moldabekov","cross_cats":["cond-mat.stat-mech","physics.plasm-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2022-04-29T17:37:13Z","title":"Effective electronic forces and potentials from ab initio path integral Monte Carlo simulations"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2204.14260","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":"sha256:0bd2b73c804cfebe0f1d1621a83a32a32ecdcbfeb27188bd383006ac19a96527","target":"record","created_at":"2026-07-05T05:22:29Z","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":"2c2d8f827bcffcc05964e2916ad92e6b812ff7ea1300c90d385c20b29d0d7859","cross_cats_sorted":["cond-mat.stat-mech","physics.plasm-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2022-04-29T17:37:13Z","title_canon_sha256":"0a37a76e8b65571e5c0674c551654ea93285595a8d0311e51af2de136d9b4489"},"schema_version":"1.0","source":{"id":"2204.14260","kind":"arxiv","version":2}},"canonical_sha256":"d0df99c9349a3a5f061d3972f9f33e35c1978b051c04f8f00b30c76138704424","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d0df99c9349a3a5f061d3972f9f33e35c1978b051c04f8f00b30c76138704424","first_computed_at":"2026-07-05T05:22:29.281019Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:22:29.281019Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"2w6Nk0SnAEI6p7dUHG/vinLqtNje1IDdkezbzHISE5wbIBdsoQuwr1Fm7UtMR3/8DGBVLq7NNdISNFwPwiS+Cw==","signature_status":"signed_v1","signed_at":"2026-07-05T05:22:29.281472Z","signed_message":"canonical_sha256_bytes"},"source_id":"2204.14260","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0bd2b73c804cfebe0f1d1621a83a32a32ecdcbfeb27188bd383006ac19a96527","sha256:57607b149f656931a122cd5c6cf11621f62c2385c42c06e2eaa5e879c582da8c"],"state_sha256":"7a1018e076ded00afbdb926804a43fb9d230f29110c842e58d8439ba8f0ec2fc"}