{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:NKB64HSFNSK57BXTBLRAACAKSG","short_pith_number":"pith:NKB64HSF","canonical_record":{"source":{"id":"1404.5329","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-04-21T20:50:40Z","cross_cats_sorted":[],"title_canon_sha256":"6a1add52c72250f18c32c1ccb854b0a06e07a2c3e112d44d687c70c082d6ad86","abstract_canon_sha256":"ce3268a0b38aded20f9bd26b6942968261e5071a836643412ce3b635a9c2da95"},"schema_version":"1.0"},"canonical_sha256":"6a83ee1e456c95df86f30ae200080a919ed8b39aaf89b00d0af67825d0db1b73","source":{"kind":"arxiv","id":"1404.5329","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1404.5329","created_at":"2026-05-18T01:43:26Z"},{"alias_kind":"arxiv_version","alias_value":"1404.5329v3","created_at":"2026-05-18T01:43:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.5329","created_at":"2026-05-18T01:43:26Z"},{"alias_kind":"pith_short_12","alias_value":"NKB64HSFNSK5","created_at":"2026-05-18T12:28:41Z"},{"alias_kind":"pith_short_16","alias_value":"NKB64HSFNSK57BXT","created_at":"2026-05-18T12:28:41Z"},{"alias_kind":"pith_short_8","alias_value":"NKB64HSF","created_at":"2026-05-18T12:28:41Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:NKB64HSFNSK57BXTBLRAACAKSG","target":"record","payload":{"canonical_record":{"source":{"id":"1404.5329","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-04-21T20:50:40Z","cross_cats_sorted":[],"title_canon_sha256":"6a1add52c72250f18c32c1ccb854b0a06e07a2c3e112d44d687c70c082d6ad86","abstract_canon_sha256":"ce3268a0b38aded20f9bd26b6942968261e5071a836643412ce3b635a9c2da95"},"schema_version":"1.0"},"canonical_sha256":"6a83ee1e456c95df86f30ae200080a919ed8b39aaf89b00d0af67825d0db1b73","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:43:26.648514Z","signature_b64":"bCXdu3RVg38UMYzRvuKoWaIkfH7n7KjAA+KGlOw/RI+9l3GbrSITcs09JyglkbLV7+Akbqbv0ZjYBApc1HYLAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6a83ee1e456c95df86f30ae200080a919ed8b39aaf89b00d0af67825d0db1b73","last_reissued_at":"2026-05-18T01:43:26.647866Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:43:26.647866Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1404.5329","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:43:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DYPVHMu0D/+XUiM6cJAybRFWu6pDCB3VVE7AK8S7V4dGfqNrjWKzFLxIncdFbyzoa0Emre+yR7kMwLPG8wT9BQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T14:30:52.778481Z"},"content_sha256":"476d3b708368aa8debb34436b83a5674d16f7a2b494c4fca338f5afd6f965f91","schema_version":"1.0","event_id":"sha256:476d3b708368aa8debb34436b83a5674d16f7a2b494c4fca338f5afd6f965f91"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:NKB64HSFNSK57BXTBLRAACAKSG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Stationary distribution functions for Tokamak-plasmas in the weak-collisional transport regime by MaxEnt principle","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Alberto Sonnino, Giorgio Sonnino, Gy\\\"orgy Steinbrecher, Pasquale Nardone, Philippe Peeters","submitted_at":"2014-04-21T20:50:40Z","abstract_excerpt":"In previous works, we derived stationary density distribution functions (DDF) where the local equilibrium is determined by imposing the maximum entropy (MaxEnt) principle, under the scale invariance restrictions, and the minimum entropy production theorem. In this paper we demonstrate that it is possible to reobtain these DDF solely from the MaxEnt principle subject to suitable scale invariant restrictions in all the variables. For the sake of concreteness, we analyze the example of ohmic, fully ionized, tokamak-plasmas, in the weak-collisional transport regime. In this case we show that it is"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.5329","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:43:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"aNts36MWPfbEkqnoCYoRrdid989To4kozRwI0JcY6QZ/8SVQm9QrmDWXGefyoeW8FOh1ABHh56psRyovraDSAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T14:30:52.778831Z"},"content_sha256":"40d99e69f9edf77f84823e6906c6b3d8676c6e9ed8aa51bcffe58bee553951d7","schema_version":"1.0","event_id":"sha256:40d99e69f9edf77f84823e6906c6b3d8676c6e9ed8aa51bcffe58bee553951d7"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/NKB64HSFNSK57BXTBLRAACAKSG/bundle.json","state_url":"https://pith.science/pith/NKB64HSFNSK57BXTBLRAACAKSG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/NKB64HSFNSK57BXTBLRAACAKSG/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-03T14:30:52Z","links":{"resolver":"https://pith.science/pith/NKB64HSFNSK57BXTBLRAACAKSG","bundle":"https://pith.science/pith/NKB64HSFNSK57BXTBLRAACAKSG/bundle.json","state":"https://pith.science/pith/NKB64HSFNSK57BXTBLRAACAKSG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/NKB64HSFNSK57BXTBLRAACAKSG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:NKB64HSFNSK57BXTBLRAACAKSG","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":"ce3268a0b38aded20f9bd26b6942968261e5071a836643412ce3b635a9c2da95","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-04-21T20:50:40Z","title_canon_sha256":"6a1add52c72250f18c32c1ccb854b0a06e07a2c3e112d44d687c70c082d6ad86"},"schema_version":"1.0","source":{"id":"1404.5329","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1404.5329","created_at":"2026-05-18T01:43:26Z"},{"alias_kind":"arxiv_version","alias_value":"1404.5329v3","created_at":"2026-05-18T01:43:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.5329","created_at":"2026-05-18T01:43:26Z"},{"alias_kind":"pith_short_12","alias_value":"NKB64HSFNSK5","created_at":"2026-05-18T12:28:41Z"},{"alias_kind":"pith_short_16","alias_value":"NKB64HSFNSK57BXT","created_at":"2026-05-18T12:28:41Z"},{"alias_kind":"pith_short_8","alias_value":"NKB64HSF","created_at":"2026-05-18T12:28:41Z"}],"graph_snapshots":[{"event_id":"sha256:40d99e69f9edf77f84823e6906c6b3d8676c6e9ed8aa51bcffe58bee553951d7","target":"graph","created_at":"2026-05-18T01:43:26Z","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"},"paper":{"abstract_excerpt":"In previous works, we derived stationary density distribution functions (DDF) where the local equilibrium is determined by imposing the maximum entropy (MaxEnt) principle, under the scale invariance restrictions, and the minimum entropy production theorem. In this paper we demonstrate that it is possible to reobtain these DDF solely from the MaxEnt principle subject to suitable scale invariant restrictions in all the variables. For the sake of concreteness, we analyze the example of ohmic, fully ionized, tokamak-plasmas, in the weak-collisional transport regime. In this case we show that it is","authors_text":"Alberto Sonnino, Giorgio Sonnino, Gy\\\"orgy Steinbrecher, Pasquale Nardone, Philippe Peeters","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-04-21T20:50:40Z","title":"Stationary distribution functions for Tokamak-plasmas in the weak-collisional transport regime by MaxEnt principle"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.5329","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":"sha256:476d3b708368aa8debb34436b83a5674d16f7a2b494c4fca338f5afd6f965f91","target":"record","created_at":"2026-05-18T01:43:26Z","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":"ce3268a0b38aded20f9bd26b6942968261e5071a836643412ce3b635a9c2da95","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-04-21T20:50:40Z","title_canon_sha256":"6a1add52c72250f18c32c1ccb854b0a06e07a2c3e112d44d687c70c082d6ad86"},"schema_version":"1.0","source":{"id":"1404.5329","kind":"arxiv","version":3}},"canonical_sha256":"6a83ee1e456c95df86f30ae200080a919ed8b39aaf89b00d0af67825d0db1b73","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6a83ee1e456c95df86f30ae200080a919ed8b39aaf89b00d0af67825d0db1b73","first_computed_at":"2026-05-18T01:43:26.647866Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:43:26.647866Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"bCXdu3RVg38UMYzRvuKoWaIkfH7n7KjAA+KGlOw/RI+9l3GbrSITcs09JyglkbLV7+Akbqbv0ZjYBApc1HYLAw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:43:26.648514Z","signed_message":"canonical_sha256_bytes"},"source_id":"1404.5329","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:476d3b708368aa8debb34436b83a5674d16f7a2b494c4fca338f5afd6f965f91","sha256:40d99e69f9edf77f84823e6906c6b3d8676c6e9ed8aa51bcffe58bee553951d7"],"state_sha256":"c88c391b8d10147eb2685fccbc1e79302c8b0237616097044e915e95847dd07d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PITLCxgLOsXeOhLYwQGORbjMC0JXIh4OdzO0Y0PZN2EoLZZMY5yu7zPftkma13Vc6uBeLiYk/4eCefrA62akAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T14:30:52.780694Z","bundle_sha256":"7937805ecc78789c29a518593f4f5518db3695c0e8cf290428e9e76d1d3f6efd"}}