{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:FPLFLFWEOTCJNYN7Y6HFKC4Z2B","short_pith_number":"pith:FPLFLFWE","canonical_record":{"source":{"id":"1403.4576","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-03-18T19:03:12Z","cross_cats_sorted":[],"title_canon_sha256":"0dc19578605f7484400a7d30d123f92e27e237c5f108de5f29139d5141ba1a5d","abstract_canon_sha256":"fed49e4fda6232c5759c10ccff4c16941a4f4773ca3826b9aff3b345366cb382"},"schema_version":"1.0"},"canonical_sha256":"2bd65596c474c496e1bfc78e550b99d04d405a41bc4c02167ef7f680e7a56775","source":{"kind":"arxiv","id":"1403.4576","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1403.4576","created_at":"2026-05-18T02:45:49Z"},{"alias_kind":"arxiv_version","alias_value":"1403.4576v2","created_at":"2026-05-18T02:45:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.4576","created_at":"2026-05-18T02:45:49Z"},{"alias_kind":"pith_short_12","alias_value":"FPLFLFWEOTCJ","created_at":"2026-05-18T12:28:28Z"},{"alias_kind":"pith_short_16","alias_value":"FPLFLFWEOTCJNYN7","created_at":"2026-05-18T12:28:28Z"},{"alias_kind":"pith_short_8","alias_value":"FPLFLFWE","created_at":"2026-05-18T12:28:28Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:FPLFLFWEOTCJNYN7Y6HFKC4Z2B","target":"record","payload":{"canonical_record":{"source":{"id":"1403.4576","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-03-18T19:03:12Z","cross_cats_sorted":[],"title_canon_sha256":"0dc19578605f7484400a7d30d123f92e27e237c5f108de5f29139d5141ba1a5d","abstract_canon_sha256":"fed49e4fda6232c5759c10ccff4c16941a4f4773ca3826b9aff3b345366cb382"},"schema_version":"1.0"},"canonical_sha256":"2bd65596c474c496e1bfc78e550b99d04d405a41bc4c02167ef7f680e7a56775","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:45:49.484035Z","signature_b64":"pL0vO0+AaSin4pZJQotEJPCoQVcIALFeM8N3H4l3JCquDuPh7kotJJwajmT7KfIrIg77qhRTuFudprx68kPMBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2bd65596c474c496e1bfc78e550b99d04d405a41bc4c02167ef7f680e7a56775","last_reissued_at":"2026-05-18T02:45:49.483573Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:45:49.483573Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1403.4576","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":"2026-05-18T02:45:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mtV+CEcPMFRSyYZYTaiXXP+GwoRuXoagEccg45vnsx/bJo8ruFlxT7L6p6SikBc3VjrD77cV+IHkwaa566lNDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T02:06:40.326723Z"},"content_sha256":"4837e72a2efb6641f26ed529a4c473a518c0f95c5e0f447b0dd7ff8ea12e0fd6","schema_version":"1.0","event_id":"sha256:4837e72a2efb6641f26ed529a4c473a518c0f95c5e0f447b0dd7ff8ea12e0fd6"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:FPLFLFWEOTCJNYN7Y6HFKC4Z2B","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Freeze-out parameters from electric charge and baryon number fluctuations: is there consistency?","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"C. Ratti, K. K. Szabo, S. Borsanyi, S. D. Katz, S. Krieg, Z. Fodor","submitted_at":"2014-03-18T19:03:12Z","abstract_excerpt":"Recent results for moments of multiplicity distributions of net-protons and net-electric charge from the STAR collaboration are compared to lattice QCD results for higher order fluctuations of baryon number and electric charge by the Wuppertal-Budapest collaboration, with the purpose of extracting the freeze-out temperature and chemical potential. All lattice simulations are performed for a system of 2+1 dynamical quark flavors, at the physical mass for light and strange quarks; all results are continuum extrapolated. We show that it is possible to extract an upper value for the freeze-out tem"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.4576","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":"2026-05-18T02:45:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jCGP9ZlW4x71oBcnFftRtgri+4OGiDIXckq6WMgC9D0KX7bGHjzK25KUMVrKRjOo6jwvXp/fZaVLCmzMUILwCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T02:06:40.327504Z"},"content_sha256":"0b402387dc4d97441479acd6ea2a5af7e342b4646e0d2dd99c9a519e98596836","schema_version":"1.0","event_id":"sha256:0b402387dc4d97441479acd6ea2a5af7e342b4646e0d2dd99c9a519e98596836"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FPLFLFWEOTCJNYN7Y6HFKC4Z2B/bundle.json","state_url":"https://pith.science/pith/FPLFLFWEOTCJNYN7Y6HFKC4Z2B/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FPLFLFWEOTCJNYN7Y6HFKC4Z2B/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":"2026-06-01T02:06:40Z","links":{"resolver":"https://pith.science/pith/FPLFLFWEOTCJNYN7Y6HFKC4Z2B","bundle":"https://pith.science/pith/FPLFLFWEOTCJNYN7Y6HFKC4Z2B/bundle.json","state":"https://pith.science/pith/FPLFLFWEOTCJNYN7Y6HFKC4Z2B/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FPLFLFWEOTCJNYN7Y6HFKC4Z2B/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:FPLFLFWEOTCJNYN7Y6HFKC4Z2B","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":"fed49e4fda6232c5759c10ccff4c16941a4f4773ca3826b9aff3b345366cb382","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-03-18T19:03:12Z","title_canon_sha256":"0dc19578605f7484400a7d30d123f92e27e237c5f108de5f29139d5141ba1a5d"},"schema_version":"1.0","source":{"id":"1403.4576","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1403.4576","created_at":"2026-05-18T02:45:49Z"},{"alias_kind":"arxiv_version","alias_value":"1403.4576v2","created_at":"2026-05-18T02:45:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.4576","created_at":"2026-05-18T02:45:49Z"},{"alias_kind":"pith_short_12","alias_value":"FPLFLFWEOTCJ","created_at":"2026-05-18T12:28:28Z"},{"alias_kind":"pith_short_16","alias_value":"FPLFLFWEOTCJNYN7","created_at":"2026-05-18T12:28:28Z"},{"alias_kind":"pith_short_8","alias_value":"FPLFLFWE","created_at":"2026-05-18T12:28:28Z"}],"graph_snapshots":[{"event_id":"sha256:0b402387dc4d97441479acd6ea2a5af7e342b4646e0d2dd99c9a519e98596836","target":"graph","created_at":"2026-05-18T02:45:49Z","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":"Recent results for moments of multiplicity distributions of net-protons and net-electric charge from the STAR collaboration are compared to lattice QCD results for higher order fluctuations of baryon number and electric charge by the Wuppertal-Budapest collaboration, with the purpose of extracting the freeze-out temperature and chemical potential. All lattice simulations are performed for a system of 2+1 dynamical quark flavors, at the physical mass for light and strange quarks; all results are continuum extrapolated. We show that it is possible to extract an upper value for the freeze-out tem","authors_text":"C. Ratti, K. K. Szabo, S. Borsanyi, S. D. Katz, S. Krieg, Z. Fodor","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-03-18T19:03:12Z","title":"Freeze-out parameters from electric charge and baryon number fluctuations: is there consistency?"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.4576","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":"sha256:4837e72a2efb6641f26ed529a4c473a518c0f95c5e0f447b0dd7ff8ea12e0fd6","target":"record","created_at":"2026-05-18T02:45:49Z","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":"fed49e4fda6232c5759c10ccff4c16941a4f4773ca3826b9aff3b345366cb382","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-03-18T19:03:12Z","title_canon_sha256":"0dc19578605f7484400a7d30d123f92e27e237c5f108de5f29139d5141ba1a5d"},"schema_version":"1.0","source":{"id":"1403.4576","kind":"arxiv","version":2}},"canonical_sha256":"2bd65596c474c496e1bfc78e550b99d04d405a41bc4c02167ef7f680e7a56775","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2bd65596c474c496e1bfc78e550b99d04d405a41bc4c02167ef7f680e7a56775","first_computed_at":"2026-05-18T02:45:49.483573Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:45:49.483573Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"pL0vO0+AaSin4pZJQotEJPCoQVcIALFeM8N3H4l3JCquDuPh7kotJJwajmT7KfIrIg77qhRTuFudprx68kPMBw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:45:49.484035Z","signed_message":"canonical_sha256_bytes"},"source_id":"1403.4576","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4837e72a2efb6641f26ed529a4c473a518c0f95c5e0f447b0dd7ff8ea12e0fd6","sha256:0b402387dc4d97441479acd6ea2a5af7e342b4646e0d2dd99c9a519e98596836"],"state_sha256":"4b8646035a702d2bdfc3523b0cffcc9afe867dd49ba78606ffcf67bc40f8c29d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0zOKUQlOBH0LVh2cglwf/SmASjo2XqXm8+Ka7SPdXFFzCRoLzEFI5a5AfOgtp28rFOEqDNTlch9pMSq4acVuBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T02:06:40.331300Z","bundle_sha256":"c43a73f0c24bb6a46193c07a0e8f56d963a7fd9b5226419500313ff069c01448"}}