{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:CAQOKTF6LLM2SVFJX6WEA5FNF7","short_pith_number":"pith:CAQOKTF6","canonical_record":{"source":{"id":"1402.5982","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-02-24T21:14:32Z","cross_cats_sorted":["nucl-ex","nucl-th"],"title_canon_sha256":"6094aeb6ba8cc564c1b6c1b38e8098f1ad7ac507f7faf54bbb540900ea59a7c6","abstract_canon_sha256":"ad744df0bdff72918ac1570d5aba19cbe22207e6fb28c13892d9a7696f43fbe8"},"schema_version":"1.0"},"canonical_sha256":"1020e54cbe5ad9a954a9bfac4074ad2fdd95e391a05071513bef43303474f4d5","source":{"kind":"arxiv","id":"1402.5982","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1402.5982","created_at":"2026-05-18T00:16:34Z"},{"alias_kind":"arxiv_version","alias_value":"1402.5982v2","created_at":"2026-05-18T00:16:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.5982","created_at":"2026-05-18T00:16:34Z"},{"alias_kind":"pith_short_12","alias_value":"CAQOKTF6LLM2","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_16","alias_value":"CAQOKTF6LLM2SVFJ","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_8","alias_value":"CAQOKTF6","created_at":"2026-05-18T12:28:22Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:CAQOKTF6LLM2SVFJX6WEA5FNF7","target":"record","payload":{"canonical_record":{"source":{"id":"1402.5982","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-02-24T21:14:32Z","cross_cats_sorted":["nucl-ex","nucl-th"],"title_canon_sha256":"6094aeb6ba8cc564c1b6c1b38e8098f1ad7ac507f7faf54bbb540900ea59a7c6","abstract_canon_sha256":"ad744df0bdff72918ac1570d5aba19cbe22207e6fb28c13892d9a7696f43fbe8"},"schema_version":"1.0"},"canonical_sha256":"1020e54cbe5ad9a954a9bfac4074ad2fdd95e391a05071513bef43303474f4d5","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:16:34.330548Z","signature_b64":"8MYm5IG5lYifdQKzEp5WE0e7EM2fZhLe3FAGQXYqO/y/oc/a/47vR2VwuGwvK2JvDfYXsQUQFNL4eD5WjbF4DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1020e54cbe5ad9a954a9bfac4074ad2fdd95e391a05071513bef43303474f4d5","last_reissued_at":"2026-05-18T00:16:34.330060Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:16:34.330060Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1402.5982","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:16:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"a5U0+JFPePXkOUcntuMvIbV4FT44PH71ffge5jeBBbcI+/bgCv03KOrHJZ9ISVd9JyOhsCAnxdOu07hjiuDICw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T01:07:28.525977Z"},"content_sha256":"f5a7b37532e2bf3cf1f8b07272325fab2dc251f121835798f243fed2351640df","schema_version":"1.0","event_id":"sha256:f5a7b37532e2bf3cf1f8b07272325fab2dc251f121835798f243fed2351640df"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:CAQOKTF6LLM2SVFJX6WEA5FNF7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Criticality of the net-baryon number probability distribution at finite density","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Bengt Friman, Kenji Morita, Krzysztof Redlich","submitted_at":"2014-02-24T21:14:32Z","abstract_excerpt":"We compute the probability distribution $P(N)$ of the net-baryon number at finite temperature and quark-chemical potential, $\\mu$, at a physical value of the pion mass in the quark-meson model within the functional renormalization group scheme. For $\\mu/T<1$, the model exhibits the chiral crossover transition which belongs to the universality class of the $O(4)$ spin system in three dimensions. We explore the influence of the chiral crossover transition on the properties of the net baryon number probability distribution, $P(N)$. By considering ratios of $P(N)$ to the Skellam function, with the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.5982","kind":"arxiv","version":2},"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":"2026-05-18T00:16:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qyruucnky5l10vXTcQruJbIcoSZD6sS+cJZJamPpeZfv8EnhwDS+2NN+rudFBN/+qBnUeHll7kguyBRXHCG3BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T01:07:28.526584Z"},"content_sha256":"4b740e10feaecabc33fd2c941644dc0706bd2ac53ba6f014c4f50b78c905f8f3","schema_version":"1.0","event_id":"sha256:4b740e10feaecabc33fd2c941644dc0706bd2ac53ba6f014c4f50b78c905f8f3"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/CAQOKTF6LLM2SVFJX6WEA5FNF7/bundle.json","state_url":"https://pith.science/pith/CAQOKTF6LLM2SVFJX6WEA5FNF7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/CAQOKTF6LLM2SVFJX6WEA5FNF7/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":"2026-05-20T01:07:28Z","links":{"resolver":"https://pith.science/pith/CAQOKTF6LLM2SVFJX6WEA5FNF7","bundle":"https://pith.science/pith/CAQOKTF6LLM2SVFJX6WEA5FNF7/bundle.json","state":"https://pith.science/pith/CAQOKTF6LLM2SVFJX6WEA5FNF7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/CAQOKTF6LLM2SVFJX6WEA5FNF7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:CAQOKTF6LLM2SVFJX6WEA5FNF7","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":"ad744df0bdff72918ac1570d5aba19cbe22207e6fb28c13892d9a7696f43fbe8","cross_cats_sorted":["nucl-ex","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-02-24T21:14:32Z","title_canon_sha256":"6094aeb6ba8cc564c1b6c1b38e8098f1ad7ac507f7faf54bbb540900ea59a7c6"},"schema_version":"1.0","source":{"id":"1402.5982","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1402.5982","created_at":"2026-05-18T00:16:34Z"},{"alias_kind":"arxiv_version","alias_value":"1402.5982v2","created_at":"2026-05-18T00:16:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.5982","created_at":"2026-05-18T00:16:34Z"},{"alias_kind":"pith_short_12","alias_value":"CAQOKTF6LLM2","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_16","alias_value":"CAQOKTF6LLM2SVFJ","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_8","alias_value":"CAQOKTF6","created_at":"2026-05-18T12:28:22Z"}],"graph_snapshots":[{"event_id":"sha256:4b740e10feaecabc33fd2c941644dc0706bd2ac53ba6f014c4f50b78c905f8f3","target":"graph","created_at":"2026-05-18T00:16:34Z","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":"We compute the probability distribution $P(N)$ of the net-baryon number at finite temperature and quark-chemical potential, $\\mu$, at a physical value of the pion mass in the quark-meson model within the functional renormalization group scheme. For $\\mu/T<1$, the model exhibits the chiral crossover transition which belongs to the universality class of the $O(4)$ spin system in three dimensions. We explore the influence of the chiral crossover transition on the properties of the net baryon number probability distribution, $P(N)$. By considering ratios of $P(N)$ to the Skellam function, with the","authors_text":"Bengt Friman, Kenji Morita, Krzysztof Redlich","cross_cats":["nucl-ex","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-02-24T21:14:32Z","title":"Criticality of the net-baryon number probability distribution at finite density"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.5982","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:f5a7b37532e2bf3cf1f8b07272325fab2dc251f121835798f243fed2351640df","target":"record","created_at":"2026-05-18T00:16:34Z","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":"ad744df0bdff72918ac1570d5aba19cbe22207e6fb28c13892d9a7696f43fbe8","cross_cats_sorted":["nucl-ex","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-02-24T21:14:32Z","title_canon_sha256":"6094aeb6ba8cc564c1b6c1b38e8098f1ad7ac507f7faf54bbb540900ea59a7c6"},"schema_version":"1.0","source":{"id":"1402.5982","kind":"arxiv","version":2}},"canonical_sha256":"1020e54cbe5ad9a954a9bfac4074ad2fdd95e391a05071513bef43303474f4d5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1020e54cbe5ad9a954a9bfac4074ad2fdd95e391a05071513bef43303474f4d5","first_computed_at":"2026-05-18T00:16:34.330060Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:16:34.330060Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"8MYm5IG5lYifdQKzEp5WE0e7EM2fZhLe3FAGQXYqO/y/oc/a/47vR2VwuGwvK2JvDfYXsQUQFNL4eD5WjbF4DA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:16:34.330548Z","signed_message":"canonical_sha256_bytes"},"source_id":"1402.5982","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f5a7b37532e2bf3cf1f8b07272325fab2dc251f121835798f243fed2351640df","sha256:4b740e10feaecabc33fd2c941644dc0706bd2ac53ba6f014c4f50b78c905f8f3"],"state_sha256":"54d1979f2f6ed2a4425a92e82056ab938fcf36be0afddb666501d50272974d0f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sEfWj9qFJLn3Z47rfsmBAlGgf2ZCMnwIM8ED+OM5t9jYUXITlIM4uOXHf7QFCVMQIqaagwQd4RHpInq6XaEwBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-20T01:07:28.530403Z","bundle_sha256":"d892b754f58ea1c389513de3f80736406f7efdafbfed1026872b98f731399ea4"}}