{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:WZ24J7CPU3QOIEDNCPKOXDVBS5","short_pith_number":"pith:WZ24J7CP","canonical_record":{"source":{"id":"1708.04549","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-08-14T12:39:00Z","cross_cats_sorted":[],"title_canon_sha256":"34d4a1f86de7a25fa88cd5d285fbeb5c6fdb16ba2ca93ef8a0f2e2f96834cea5","abstract_canon_sha256":"c5ea469df6f105340626bd42d070ab814b7b78c918f45ba67fae6d604ba4acaa"},"schema_version":"1.0"},"canonical_sha256":"b675c4fc4fa6e0e4106d13d4eb8ea19772c0ad5d6df284fef5ceec72eaf7546d","source":{"kind":"arxiv","id":"1708.04549","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.04549","created_at":"2026-05-17T23:47:21Z"},{"alias_kind":"arxiv_version","alias_value":"1708.04549v1","created_at":"2026-05-17T23:47:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.04549","created_at":"2026-05-17T23:47:21Z"},{"alias_kind":"pith_short_12","alias_value":"WZ24J7CPU3QO","created_at":"2026-05-18T12:31:53Z"},{"alias_kind":"pith_short_16","alias_value":"WZ24J7CPU3QOIEDN","created_at":"2026-05-18T12:31:53Z"},{"alias_kind":"pith_short_8","alias_value":"WZ24J7CP","created_at":"2026-05-18T12:31:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:WZ24J7CPU3QOIEDNCPKOXDVBS5","target":"record","payload":{"canonical_record":{"source":{"id":"1708.04549","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-08-14T12:39:00Z","cross_cats_sorted":[],"title_canon_sha256":"34d4a1f86de7a25fa88cd5d285fbeb5c6fdb16ba2ca93ef8a0f2e2f96834cea5","abstract_canon_sha256":"c5ea469df6f105340626bd42d070ab814b7b78c918f45ba67fae6d604ba4acaa"},"schema_version":"1.0"},"canonical_sha256":"b675c4fc4fa6e0e4106d13d4eb8ea19772c0ad5d6df284fef5ceec72eaf7546d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:47:21.246543Z","signature_b64":"ajTtDy7B4QFBcQtBCQcOIauWOTsxHT4NlnfWX/uYlp1esfzhmRLcDE2SSzkLLV9EL8ScKGeGyIUP+1Sg/ZkeDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b675c4fc4fa6e0e4106d13d4eb8ea19772c0ad5d6df284fef5ceec72eaf7546d","last_reissued_at":"2026-05-17T23:47:21.246036Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:47:21.246036Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1708.04549","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":"2026-05-17T23:47:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RSFximn03avwVJugdDueOPIFOlgy4sKtA8vuzonLGKioVwQymc3s0/g1DYXnw+gmS20Oy3e2Qos6txT9CFFDDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T17:02:58.401858Z"},"content_sha256":"f3eac178b54e72d6f58c9f79444bfe321bb4f51020b3242b9df9b552359a8725","schema_version":"1.0","event_id":"sha256:f3eac178b54e72d6f58c9f79444bfe321bb4f51020b3242b9df9b552359a8725"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:WZ24J7CPU3QOIEDNCPKOXDVBS5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Thermodynamics of strongly interacting matter in a hybrid model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Abhijit Bhattacharyya, Kinkar Saha, Rajarshi Ray, Sanjay K. Ghosh, Sibaji Raha, Soumitra Maity, Subhasis Samanta, Sudipa Upadhaya","submitted_at":"2017-08-14T12:39:00Z","abstract_excerpt":"The equation of state and fluctuations of conserved charges in a strongly interacting medium under equilibrium conditions form the baseline upon which various possible scenarios in relativistic heavy-ion collision experiments are built. Many of these quantities have been obtained in the lattice QCD framework with reliable continuum extrapolations. Recently the Polyakov$-$Nambu$-$Jona-Lasinio model has been reparametrized to some extent to reproduce quantitatively the lattice QCD equation of state at vanishing chemical potentials. The agreement was precise except at low temperatures, possibly d"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.04549","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":"2026-05-17T23:47:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"00Gskts5YUcZH6e53O2rRek1n0ZIJW34FpwPDdDDrI9MxedT1kUuFLFC5VCefc+FTk7fc45u2iywUkZFmpn8Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T17:02:58.402574Z"},"content_sha256":"0825b4c73eeb3e08412dda692b2ee02b80efe9c1b761f432e74d7058ab97fe20","schema_version":"1.0","event_id":"sha256:0825b4c73eeb3e08412dda692b2ee02b80efe9c1b761f432e74d7058ab97fe20"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/WZ24J7CPU3QOIEDNCPKOXDVBS5/bundle.json","state_url":"https://pith.science/pith/WZ24J7CPU3QOIEDNCPKOXDVBS5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/WZ24J7CPU3QOIEDNCPKOXDVBS5/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":"2026-05-25T17:02:58Z","links":{"resolver":"https://pith.science/pith/WZ24J7CPU3QOIEDNCPKOXDVBS5","bundle":"https://pith.science/pith/WZ24J7CPU3QOIEDNCPKOXDVBS5/bundle.json","state":"https://pith.science/pith/WZ24J7CPU3QOIEDNCPKOXDVBS5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/WZ24J7CPU3QOIEDNCPKOXDVBS5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:WZ24J7CPU3QOIEDNCPKOXDVBS5","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":"c5ea469df6f105340626bd42d070ab814b7b78c918f45ba67fae6d604ba4acaa","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-08-14T12:39:00Z","title_canon_sha256":"34d4a1f86de7a25fa88cd5d285fbeb5c6fdb16ba2ca93ef8a0f2e2f96834cea5"},"schema_version":"1.0","source":{"id":"1708.04549","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.04549","created_at":"2026-05-17T23:47:21Z"},{"alias_kind":"arxiv_version","alias_value":"1708.04549v1","created_at":"2026-05-17T23:47:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.04549","created_at":"2026-05-17T23:47:21Z"},{"alias_kind":"pith_short_12","alias_value":"WZ24J7CPU3QO","created_at":"2026-05-18T12:31:53Z"},{"alias_kind":"pith_short_16","alias_value":"WZ24J7CPU3QOIEDN","created_at":"2026-05-18T12:31:53Z"},{"alias_kind":"pith_short_8","alias_value":"WZ24J7CP","created_at":"2026-05-18T12:31:53Z"}],"graph_snapshots":[{"event_id":"sha256:0825b4c73eeb3e08412dda692b2ee02b80efe9c1b761f432e74d7058ab97fe20","target":"graph","created_at":"2026-05-17T23:47:21Z","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":"The equation of state and fluctuations of conserved charges in a strongly interacting medium under equilibrium conditions form the baseline upon which various possible scenarios in relativistic heavy-ion collision experiments are built. Many of these quantities have been obtained in the lattice QCD framework with reliable continuum extrapolations. Recently the Polyakov$-$Nambu$-$Jona-Lasinio model has been reparametrized to some extent to reproduce quantitatively the lattice QCD equation of state at vanishing chemical potentials. The agreement was precise except at low temperatures, possibly d","authors_text":"Abhijit Bhattacharyya, Kinkar Saha, Rajarshi Ray, Sanjay K. Ghosh, Sibaji Raha, Soumitra Maity, Subhasis Samanta, Sudipa Upadhaya","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-08-14T12:39:00Z","title":"Thermodynamics of strongly interacting matter in a hybrid model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.04549","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:f3eac178b54e72d6f58c9f79444bfe321bb4f51020b3242b9df9b552359a8725","target":"record","created_at":"2026-05-17T23:47:21Z","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":"c5ea469df6f105340626bd42d070ab814b7b78c918f45ba67fae6d604ba4acaa","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-08-14T12:39:00Z","title_canon_sha256":"34d4a1f86de7a25fa88cd5d285fbeb5c6fdb16ba2ca93ef8a0f2e2f96834cea5"},"schema_version":"1.0","source":{"id":"1708.04549","kind":"arxiv","version":1}},"canonical_sha256":"b675c4fc4fa6e0e4106d13d4eb8ea19772c0ad5d6df284fef5ceec72eaf7546d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b675c4fc4fa6e0e4106d13d4eb8ea19772c0ad5d6df284fef5ceec72eaf7546d","first_computed_at":"2026-05-17T23:47:21.246036Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:47:21.246036Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ajTtDy7B4QFBcQtBCQcOIauWOTsxHT4NlnfWX/uYlp1esfzhmRLcDE2SSzkLLV9EL8ScKGeGyIUP+1Sg/ZkeDQ==","signature_status":"signed_v1","signed_at":"2026-05-17T23:47:21.246543Z","signed_message":"canonical_sha256_bytes"},"source_id":"1708.04549","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f3eac178b54e72d6f58c9f79444bfe321bb4f51020b3242b9df9b552359a8725","sha256:0825b4c73eeb3e08412dda692b2ee02b80efe9c1b761f432e74d7058ab97fe20"],"state_sha256":"dbe65bc667129c9e4ceb50ba0b737ea64deade1e420b71951ffedcb1c0ddb14a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kjf9V+z5yt1wfFCXsM6sTqJ5yvyy+5/V/vEPRRlEPA6xJeMk546OfLm+F3rkwT5CDUjWxL+X2TcKr62q4M47Aw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T17:02:58.406374Z","bundle_sha256":"6f9c95ddc5f54af4c7afc776c54f92252b8041c79222342eba55f2fc4313617a"}}