{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:FPSWWTQ2X6CRHHZUIOHAZY4AIR","short_pith_number":"pith:FPSWWTQ2","canonical_record":{"source":{"id":"1409.5975","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-09-21T11:57:46Z","cross_cats_sorted":[],"title_canon_sha256":"1810f7d4b6d7e1ef3eaa6c5688f0f50bf7014939d63630a1506400b122412301","abstract_canon_sha256":"a066a8255b640170824a13acb40eb9c1696d4f504c3287e70614b7c721b9037b"},"schema_version":"1.0"},"canonical_sha256":"2be56b4e1abf85139f34438e0ce3804466e2bacabb2f97e97858bf10688002fd","source":{"kind":"arxiv","id":"1409.5975","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.5975","created_at":"2026-05-18T02:31:46Z"},{"alias_kind":"arxiv_version","alias_value":"1409.5975v1","created_at":"2026-05-18T02:31:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.5975","created_at":"2026-05-18T02:31:46Z"},{"alias_kind":"pith_short_12","alias_value":"FPSWWTQ2X6CR","created_at":"2026-05-18T12:28:28Z"},{"alias_kind":"pith_short_16","alias_value":"FPSWWTQ2X6CRHHZU","created_at":"2026-05-18T12:28:28Z"},{"alias_kind":"pith_short_8","alias_value":"FPSWWTQ2","created_at":"2026-05-18T12:28:28Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:FPSWWTQ2X6CRHHZUIOHAZY4AIR","target":"record","payload":{"canonical_record":{"source":{"id":"1409.5975","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-09-21T11:57:46Z","cross_cats_sorted":[],"title_canon_sha256":"1810f7d4b6d7e1ef3eaa6c5688f0f50bf7014939d63630a1506400b122412301","abstract_canon_sha256":"a066a8255b640170824a13acb40eb9c1696d4f504c3287e70614b7c721b9037b"},"schema_version":"1.0"},"canonical_sha256":"2be56b4e1abf85139f34438e0ce3804466e2bacabb2f97e97858bf10688002fd","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:31:46.586550Z","signature_b64":"ouBK4aEy5HoO9Xx7QBO8Kt/cTcJdjK2c1ZmgeyCHwrRs9wnCMNaxLg7yj5bq8968nOn2pG9xWMh2QG6CavkfBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2be56b4e1abf85139f34438e0ce3804466e2bacabb2f97e97858bf10688002fd","last_reissued_at":"2026-05-18T02:31:46.586033Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:31:46.586033Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1409.5975","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:31:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+h6g0ufr/eKhmgfn/C3OHv9e3iVN+0bCmzQsuRqvzVI9Dvz/gIl/2jTXiLvqE+GhROuzfcAgDS88Oh4Pi0oEDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T21:48:24.404678Z"},"content_sha256":"a1b993a934ba324a783f9561421b9a06631166d35b39f2d56e6e7cfcb609893b","schema_version":"1.0","event_id":"sha256:a1b993a934ba324a783f9561421b9a06631166d35b39f2d56e6e7cfcb609893b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:FPSWWTQ2X6CRHHZUIOHAZY4AIR","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Statistical Power Law due to Reservoir Fluctuations and the Universal Thermostat Independence Principle","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Gergely Gabor Barnafoldi, Karoly Urmossy, Peter Van, Tamas Sandor Biro","submitted_at":"2014-09-21T11:57:46Z","abstract_excerpt":"Certain fluctuations in particle number at fixed total energy lead exactly to a cut-power law distribution in the one-particle energy, via the induced fluctuations in the phase-space volume ratio. The temperature parameter is expressed automatically by an equipartition relation, while the q-parameter is related to the scaled variance and to the expectation value of the particle number. For the binomial distribution q is smaller, for the negative binomial q is larger than one. These results also represent an approximation for general particle number distributions in the reservoir up to second o"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.5975","kind":"arxiv","version":1},"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":"2026-05-18T02:31:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/zCYWST3aDPMYKVuaQsuEIjqg7BC6WPYkIL4w0mfdxheDATb3KJPm5kSizj9QKuIhfn5ip2SLIz3Ueb60sU7CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T21:48:24.405356Z"},"content_sha256":"5ac8a7d96ef236c362bcc0a9b0f7ea6e1a724e3527d1845e6b8e1beb7b1d3de3","schema_version":"1.0","event_id":"sha256:5ac8a7d96ef236c362bcc0a9b0f7ea6e1a724e3527d1845e6b8e1beb7b1d3de3"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FPSWWTQ2X6CRHHZUIOHAZY4AIR/bundle.json","state_url":"https://pith.science/pith/FPSWWTQ2X6CRHHZUIOHAZY4AIR/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FPSWWTQ2X6CRHHZUIOHAZY4AIR/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":"2026-05-25T21:48:24Z","links":{"resolver":"https://pith.science/pith/FPSWWTQ2X6CRHHZUIOHAZY4AIR","bundle":"https://pith.science/pith/FPSWWTQ2X6CRHHZUIOHAZY4AIR/bundle.json","state":"https://pith.science/pith/FPSWWTQ2X6CRHHZUIOHAZY4AIR/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FPSWWTQ2X6CRHHZUIOHAZY4AIR/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:FPSWWTQ2X6CRHHZUIOHAZY4AIR","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":"a066a8255b640170824a13acb40eb9c1696d4f504c3287e70614b7c721b9037b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-09-21T11:57:46Z","title_canon_sha256":"1810f7d4b6d7e1ef3eaa6c5688f0f50bf7014939d63630a1506400b122412301"},"schema_version":"1.0","source":{"id":"1409.5975","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.5975","created_at":"2026-05-18T02:31:46Z"},{"alias_kind":"arxiv_version","alias_value":"1409.5975v1","created_at":"2026-05-18T02:31:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.5975","created_at":"2026-05-18T02:31:46Z"},{"alias_kind":"pith_short_12","alias_value":"FPSWWTQ2X6CR","created_at":"2026-05-18T12:28:28Z"},{"alias_kind":"pith_short_16","alias_value":"FPSWWTQ2X6CRHHZU","created_at":"2026-05-18T12:28:28Z"},{"alias_kind":"pith_short_8","alias_value":"FPSWWTQ2","created_at":"2026-05-18T12:28:28Z"}],"graph_snapshots":[{"event_id":"sha256:5ac8a7d96ef236c362bcc0a9b0f7ea6e1a724e3527d1845e6b8e1beb7b1d3de3","target":"graph","created_at":"2026-05-18T02:31:46Z","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"},"paper":{"abstract_excerpt":"Certain fluctuations in particle number at fixed total energy lead exactly to a cut-power law distribution in the one-particle energy, via the induced fluctuations in the phase-space volume ratio. The temperature parameter is expressed automatically by an equipartition relation, while the q-parameter is related to the scaled variance and to the expectation value of the particle number. For the binomial distribution q is smaller, for the negative binomial q is larger than one. These results also represent an approximation for general particle number distributions in the reservoir up to second o","authors_text":"Gergely Gabor Barnafoldi, Karoly Urmossy, Peter Van, Tamas Sandor Biro","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-09-21T11:57:46Z","title":"Statistical Power Law due to Reservoir Fluctuations and the Universal Thermostat Independence Principle"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.5975","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:a1b993a934ba324a783f9561421b9a06631166d35b39f2d56e6e7cfcb609893b","target":"record","created_at":"2026-05-18T02:31:46Z","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":"a066a8255b640170824a13acb40eb9c1696d4f504c3287e70614b7c721b9037b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-09-21T11:57:46Z","title_canon_sha256":"1810f7d4b6d7e1ef3eaa6c5688f0f50bf7014939d63630a1506400b122412301"},"schema_version":"1.0","source":{"id":"1409.5975","kind":"arxiv","version":1}},"canonical_sha256":"2be56b4e1abf85139f34438e0ce3804466e2bacabb2f97e97858bf10688002fd","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2be56b4e1abf85139f34438e0ce3804466e2bacabb2f97e97858bf10688002fd","first_computed_at":"2026-05-18T02:31:46.586033Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:31:46.586033Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ouBK4aEy5HoO9Xx7QBO8Kt/cTcJdjK2c1ZmgeyCHwrRs9wnCMNaxLg7yj5bq8968nOn2pG9xWMh2QG6CavkfBA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:31:46.586550Z","signed_message":"canonical_sha256_bytes"},"source_id":"1409.5975","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a1b993a934ba324a783f9561421b9a06631166d35b39f2d56e6e7cfcb609893b","sha256:5ac8a7d96ef236c362bcc0a9b0f7ea6e1a724e3527d1845e6b8e1beb7b1d3de3"],"state_sha256":"080dff2ce1f11c7bef2b4cb660192219b456f190d832d446eba61385a1aff8f7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dTabDzt26aQSPa49pBLkxI66O9F4b3vL5X25WNlSF9St0t+yxiVpa2F56eo07YdWimi8i5a3tBmacDA3DRkfCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T21:48:24.409105Z","bundle_sha256":"7c6c6f706b47687a4fa30f7ecc47a89a1cb1e3795b2484e074d2e30c384d728b"}}