{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:LPXGOAAPHAQ77VH2T3HRVKFFX7","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":"938e3f8bb264f891729e45ec6bb8809608c8cd435eb8d285aa129b6695de8287","cross_cats_sorted":["math.IT","physics.data-an"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cs.IT","submitted_at":"2025-01-15T15:30:31Z","title_canon_sha256":"040cc19531e5d302878fc21936c1dc06a65cca0bc6bcfe55df8865f219d928d0"},"schema_version":"1.0","source":{"id":"2501.08865","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2501.08865","created_at":"2026-07-05T10:01:27Z"},{"alias_kind":"arxiv_version","alias_value":"2501.08865v1","created_at":"2026-07-05T10:01:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2501.08865","created_at":"2026-07-05T10:01:27Z"},{"alias_kind":"pith_short_12","alias_value":"LPXGOAAPHAQ7","created_at":"2026-07-05T10:01:27Z"},{"alias_kind":"pith_short_16","alias_value":"LPXGOAAPHAQ77VH2","created_at":"2026-07-05T10:01:27Z"},{"alias_kind":"pith_short_8","alias_value":"LPXGOAAP","created_at":"2026-07-05T10:01:27Z"}],"graph_snapshots":[{"event_id":"sha256:009fc0a72fc04ee51b061f2955402725f7ba62a2028d14d2a88ad8ebd690de69","target":"graph","created_at":"2026-07-05T10:01:27Z","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/2501.08865/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We show how (resource) bounded rationality can be understood as the interplay of two fundamental moral principles: deontology and utilitarianism. In particular, we interpret deontology as a regularisation function in an optimal control problem, coupled with a free parameter, the inverse temperature, to shield the individual from expected utility. We discuss the information geometry of bounded rationality and aspects of its relation to rate distortion theory. A central role is played by Markov kernels and regular conditional probability, which are also studied geometrically. A gradient equation","authors_text":"Roland M. Friedrich","cross_cats":["math.IT","physics.data-an"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cs.IT","submitted_at":"2025-01-15T15:30:31Z","title":"The geometry of moral decision making"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2501.08865","kind":"arxiv","version":1},"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:a0244b7b420b7f77d117779b34db4110dcd4c02d2dee454d616695a4c8491d56","target":"record","created_at":"2026-07-05T10:01:27Z","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":"938e3f8bb264f891729e45ec6bb8809608c8cd435eb8d285aa129b6695de8287","cross_cats_sorted":["math.IT","physics.data-an"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cs.IT","submitted_at":"2025-01-15T15:30:31Z","title_canon_sha256":"040cc19531e5d302878fc21936c1dc06a65cca0bc6bcfe55df8865f219d928d0"},"schema_version":"1.0","source":{"id":"2501.08865","kind":"arxiv","version":1}},"canonical_sha256":"5bee67000f3821ffd4fa9ecf1aa8a5bfde62770347917bc6406a128918c30016","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5bee67000f3821ffd4fa9ecf1aa8a5bfde62770347917bc6406a128918c30016","first_computed_at":"2026-07-05T10:01:27.342869Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:01:27.342869Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"GbnG6YHsPTJUej1fkwjj/TgAZAKidDFeKir2dHl26+rGBtDhkTL9RvsmUiLkrJk+wXgHHkYXkL+6cVy6calWAg==","signature_status":"signed_v1","signed_at":"2026-07-05T10:01:27.343354Z","signed_message":"canonical_sha256_bytes"},"source_id":"2501.08865","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a0244b7b420b7f77d117779b34db4110dcd4c02d2dee454d616695a4c8491d56","sha256:009fc0a72fc04ee51b061f2955402725f7ba62a2028d14d2a88ad8ebd690de69"],"state_sha256":"18a5ab86009321234a9709f1a7e3f664e23fb1c52d882809798e50db72da75b5"}