{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:A7WZNIJBVZ3CDNVR6G6IMQBPGO","short_pith_number":"pith:A7WZNIJB","canonical_record":{"source":{"id":"1611.10144","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-11-30T13:42:44Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"61cd90f75231164778f247acbddd5b2d88530c4aa70397b8c9cc901c98a16034","abstract_canon_sha256":"e6efc3174cc158f5ce92cc3c8da676d3ec07d46344ebb9330c49bcc419ed3477"},"schema_version":"1.0"},"canonical_sha256":"07ed96a121ae7621b6b1f1bc86402f339191aacc90bc6d1f20a4b974b5778d32","source":{"kind":"arxiv","id":"1611.10144","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1611.10144","created_at":"2026-05-18T00:36:32Z"},{"alias_kind":"arxiv_version","alias_value":"1611.10144v2","created_at":"2026-05-18T00:36:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.10144","created_at":"2026-05-18T00:36:32Z"},{"alias_kind":"pith_short_12","alias_value":"A7WZNIJBVZ3C","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_16","alias_value":"A7WZNIJBVZ3CDNVR","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_8","alias_value":"A7WZNIJB","created_at":"2026-05-18T12:30:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:A7WZNIJBVZ3CDNVR6G6IMQBPGO","target":"record","payload":{"canonical_record":{"source":{"id":"1611.10144","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-11-30T13:42:44Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"61cd90f75231164778f247acbddd5b2d88530c4aa70397b8c9cc901c98a16034","abstract_canon_sha256":"e6efc3174cc158f5ce92cc3c8da676d3ec07d46344ebb9330c49bcc419ed3477"},"schema_version":"1.0"},"canonical_sha256":"07ed96a121ae7621b6b1f1bc86402f339191aacc90bc6d1f20a4b974b5778d32","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:36:32.923142Z","signature_b64":"QZh2vAcwd9e/QtKeVBerqQsBDC+xqosZEjREe+f+6Kw4rtHAMF/2jd86g+poUMLNtEKysoTzT2EFuj6OrszVAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"07ed96a121ae7621b6b1f1bc86402f339191aacc90bc6d1f20a4b974b5778d32","last_reissued_at":"2026-05-18T00:36:32.922524Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:36:32.922524Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1611.10144","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":"2026-05-18T00:36:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nWz0qIZADVmY9uMXRRQeDbsUSTAZV+8pSLWHDC/TvlbfjvAMuztM5u42oo6h5vdtiP0eDUVAt0iGb7Jj9p2CAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T00:38:10.236206Z"},"content_sha256":"908c1351cd871add2d515cd3d8063a1838bcd50f12bc990a925715c40b5a06cc","schema_version":"1.0","event_id":"sha256:908c1351cd871add2d515cd3d8063a1838bcd50f12bc990a925715c40b5a06cc"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:A7WZNIJBVZ3CDNVR6G6IMQBPGO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Higher-order baryon number susceptibilities: interplay between the chiral and the nuclear liquid-gas transitions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"A. Mukherjee, J. Steinheimer, S. Schramm","submitted_at":"2016-11-30T13:42:44Z","abstract_excerpt":"We use an improved version of the SU(3) flavour parity-doublet quark-hadron model to investigate the higher order baryon number susceptibilities near the chiral and the nuclear liquid-gas transitions. The parity-doublet model has been improved by adding higher-order interaction terms of the scalar fields in the effective mean field Lagrangian, resulting in a much-improved description of nuclear ground-state properties, in particular the nuclear compressibility. The resulting phase diagram of the model agrees qualitatively with expectations from lattice QCD, i.e., it shows a crossover at zero n"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.10144","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":"2026-05-18T00:36:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rqv6uZZ3pJO8dECbYyvTmR9jSh6LtENEuES8R6rvAWIKlPhw1trtkMqbV97ooVTxa8uQhVQiG+bUKYsCsJ03AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T00:38:10.236888Z"},"content_sha256":"a2c8b17a996d078bf2bb14f9d0e5aec9c447cbd8726b8871afabc38566357d41","schema_version":"1.0","event_id":"sha256:a2c8b17a996d078bf2bb14f9d0e5aec9c447cbd8726b8871afabc38566357d41"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/A7WZNIJBVZ3CDNVR6G6IMQBPGO/bundle.json","state_url":"https://pith.science/pith/A7WZNIJBVZ3CDNVR6G6IMQBPGO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/A7WZNIJBVZ3CDNVR6G6IMQBPGO/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":"2026-05-26T00:38:10Z","links":{"resolver":"https://pith.science/pith/A7WZNIJBVZ3CDNVR6G6IMQBPGO","bundle":"https://pith.science/pith/A7WZNIJBVZ3CDNVR6G6IMQBPGO/bundle.json","state":"https://pith.science/pith/A7WZNIJBVZ3CDNVR6G6IMQBPGO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/A7WZNIJBVZ3CDNVR6G6IMQBPGO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:A7WZNIJBVZ3CDNVR6G6IMQBPGO","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":"e6efc3174cc158f5ce92cc3c8da676d3ec07d46344ebb9330c49bcc419ed3477","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-11-30T13:42:44Z","title_canon_sha256":"61cd90f75231164778f247acbddd5b2d88530c4aa70397b8c9cc901c98a16034"},"schema_version":"1.0","source":{"id":"1611.10144","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1611.10144","created_at":"2026-05-18T00:36:32Z"},{"alias_kind":"arxiv_version","alias_value":"1611.10144v2","created_at":"2026-05-18T00:36:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.10144","created_at":"2026-05-18T00:36:32Z"},{"alias_kind":"pith_short_12","alias_value":"A7WZNIJBVZ3C","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_16","alias_value":"A7WZNIJBVZ3CDNVR","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_8","alias_value":"A7WZNIJB","created_at":"2026-05-18T12:30:04Z"}],"graph_snapshots":[{"event_id":"sha256:a2c8b17a996d078bf2bb14f9d0e5aec9c447cbd8726b8871afabc38566357d41","target":"graph","created_at":"2026-05-18T00:36:32Z","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 use an improved version of the SU(3) flavour parity-doublet quark-hadron model to investigate the higher order baryon number susceptibilities near the chiral and the nuclear liquid-gas transitions. The parity-doublet model has been improved by adding higher-order interaction terms of the scalar fields in the effective mean field Lagrangian, resulting in a much-improved description of nuclear ground-state properties, in particular the nuclear compressibility. The resulting phase diagram of the model agrees qualitatively with expectations from lattice QCD, i.e., it shows a crossover at zero n","authors_text":"A. Mukherjee, J. Steinheimer, S. Schramm","cross_cats":["hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-11-30T13:42:44Z","title":"Higher-order baryon number susceptibilities: interplay between the chiral and the nuclear liquid-gas transitions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.10144","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":"sha256:908c1351cd871add2d515cd3d8063a1838bcd50f12bc990a925715c40b5a06cc","target":"record","created_at":"2026-05-18T00:36:32Z","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":"e6efc3174cc158f5ce92cc3c8da676d3ec07d46344ebb9330c49bcc419ed3477","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-11-30T13:42:44Z","title_canon_sha256":"61cd90f75231164778f247acbddd5b2d88530c4aa70397b8c9cc901c98a16034"},"schema_version":"1.0","source":{"id":"1611.10144","kind":"arxiv","version":2}},"canonical_sha256":"07ed96a121ae7621b6b1f1bc86402f339191aacc90bc6d1f20a4b974b5778d32","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"07ed96a121ae7621b6b1f1bc86402f339191aacc90bc6d1f20a4b974b5778d32","first_computed_at":"2026-05-18T00:36:32.922524Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:36:32.922524Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"QZh2vAcwd9e/QtKeVBerqQsBDC+xqosZEjREe+f+6Kw4rtHAMF/2jd86g+poUMLNtEKysoTzT2EFuj6OrszVAw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:36:32.923142Z","signed_message":"canonical_sha256_bytes"},"source_id":"1611.10144","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:908c1351cd871add2d515cd3d8063a1838bcd50f12bc990a925715c40b5a06cc","sha256:a2c8b17a996d078bf2bb14f9d0e5aec9c447cbd8726b8871afabc38566357d41"],"state_sha256":"882cb6d0d62d507fa4e1bd8b6ac4f72340ac4c71da0383d2a5b2911be2033e04"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QdRck3cZ6pcL7p4jTCaWwvQ2MpHNRdtRiFqrIN6rZUvy/y4OPMhOMXdapgOKTGRc1mv1C2vApckcfbPfwdOWCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T00:38:10.240081Z","bundle_sha256":"bc96dc538245a8177f966ae1e01fb9410865122db26eb0822cfdfbc7c2941630"}}