{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:Q2NKW7YFYU4CFRNWYFXIWAPDM7","short_pith_number":"pith:Q2NKW7YF","canonical_record":{"source":{"id":"1711.07559","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-20T21:46:58Z","cross_cats_sorted":[],"title_canon_sha256":"f5a3f0554927d9af8360a8b8d5acf70e1038469541d6dabd3193ef445e20de1b","abstract_canon_sha256":"3cb54a1f02ebe46b7aef0537a19964c07d7821afb692f254b9b629e8b68f3f14"},"schema_version":"1.0"},"canonical_sha256":"869aab7f05c53822c5b6c16e8b01e367ca49985e17d226e0b453d92205db9074","source":{"kind":"arxiv","id":"1711.07559","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.07559","created_at":"2026-05-18T00:07:28Z"},{"alias_kind":"arxiv_version","alias_value":"1711.07559v3","created_at":"2026-05-18T00:07:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.07559","created_at":"2026-05-18T00:07:28Z"},{"alias_kind":"pith_short_12","alias_value":"Q2NKW7YFYU4C","created_at":"2026-05-18T12:31:37Z"},{"alias_kind":"pith_short_16","alias_value":"Q2NKW7YFYU4CFRNW","created_at":"2026-05-18T12:31:37Z"},{"alias_kind":"pith_short_8","alias_value":"Q2NKW7YF","created_at":"2026-05-18T12:31:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:Q2NKW7YFYU4CFRNWYFXIWAPDM7","target":"record","payload":{"canonical_record":{"source":{"id":"1711.07559","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-20T21:46:58Z","cross_cats_sorted":[],"title_canon_sha256":"f5a3f0554927d9af8360a8b8d5acf70e1038469541d6dabd3193ef445e20de1b","abstract_canon_sha256":"3cb54a1f02ebe46b7aef0537a19964c07d7821afb692f254b9b629e8b68f3f14"},"schema_version":"1.0"},"canonical_sha256":"869aab7f05c53822c5b6c16e8b01e367ca49985e17d226e0b453d92205db9074","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:07:28.146919Z","signature_b64":"TqR9r663W3rlp1aA/vYbdpyoAA+LBuc+52ob850SiGBR3tpRxvtlQ6WG3LZwXoeAWxcqgUrvabiVEBr1G4qNDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"869aab7f05c53822c5b6c16e8b01e367ca49985e17d226e0b453d92205db9074","last_reissued_at":"2026-05-18T00:07:28.146258Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:07:28.146258Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1711.07559","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:07:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Z6pGrhvi8snjea3E1UY6+QJKQro5F0zQ+2AI0MCvBi4T0zzIjr+UQk6y0DRQlf5ZixpRwb6RpbszUwxo0OF+AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T16:46:35.588671Z"},"content_sha256":"e7e389979bbe355387322818e4e493a81ea92993ba10d0f507faff95cbb6d8b4","schema_version":"1.0","event_id":"sha256:e7e389979bbe355387322818e4e493a81ea92993ba10d0f507faff95cbb6d8b4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:Q2NKW7YFYU4CFRNWYFXIWAPDM7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Finite size effects in strongly interacting matter at zero chemical potential from Polyakov loop Nambu-Jona-Lasinio model in the light of lattice data","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. G. Grunfeld, G. Lugones","submitted_at":"2017-11-20T21:46:58Z","abstract_excerpt":"We study finite volume effects within the Polyakov loop Nambu-Jona-Lasinio model for two light and one heavy quarks at vanishing baryon chemical potential and finite temperatures. We include three different Polyakov loop potentials and ensure that the predictions of our effective model in bulk are compatible with lattice QCD results. Finite size effects are taken into account by means of the Multiple Reflection Expansion formalism. We analyze several thermodynamic quantities including the interaction measure, the speed of sound, the surface tension, and the curvature energy and find that they "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.07559","kind":"arxiv","version":3},"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":"2026-05-18T00:07:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3niUSakbnJtZdTo8jbRLTwmi9QCp5hoy+wYAW1F+MjL5BzhSgespP9EUmEaTyw1uIhVFh7jV0CG5IYQ8PuXqDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T16:46:35.589017Z"},"content_sha256":"5adf9155d6adf44b6fe69b4ed57d217be6b6ab30c4ce004061685bae6eca0ec7","schema_version":"1.0","event_id":"sha256:5adf9155d6adf44b6fe69b4ed57d217be6b6ab30c4ce004061685bae6eca0ec7"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/Q2NKW7YFYU4CFRNWYFXIWAPDM7/bundle.json","state_url":"https://pith.science/pith/Q2NKW7YFYU4CFRNWYFXIWAPDM7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/Q2NKW7YFYU4CFRNWYFXIWAPDM7/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":"2026-05-21T16:46:35Z","links":{"resolver":"https://pith.science/pith/Q2NKW7YFYU4CFRNWYFXIWAPDM7","bundle":"https://pith.science/pith/Q2NKW7YFYU4CFRNWYFXIWAPDM7/bundle.json","state":"https://pith.science/pith/Q2NKW7YFYU4CFRNWYFXIWAPDM7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/Q2NKW7YFYU4CFRNWYFXIWAPDM7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:Q2NKW7YFYU4CFRNWYFXIWAPDM7","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":"3cb54a1f02ebe46b7aef0537a19964c07d7821afb692f254b9b629e8b68f3f14","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-20T21:46:58Z","title_canon_sha256":"f5a3f0554927d9af8360a8b8d5acf70e1038469541d6dabd3193ef445e20de1b"},"schema_version":"1.0","source":{"id":"1711.07559","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.07559","created_at":"2026-05-18T00:07:28Z"},{"alias_kind":"arxiv_version","alias_value":"1711.07559v3","created_at":"2026-05-18T00:07:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.07559","created_at":"2026-05-18T00:07:28Z"},{"alias_kind":"pith_short_12","alias_value":"Q2NKW7YFYU4C","created_at":"2026-05-18T12:31:37Z"},{"alias_kind":"pith_short_16","alias_value":"Q2NKW7YFYU4CFRNW","created_at":"2026-05-18T12:31:37Z"},{"alias_kind":"pith_short_8","alias_value":"Q2NKW7YF","created_at":"2026-05-18T12:31:37Z"}],"graph_snapshots":[{"event_id":"sha256:5adf9155d6adf44b6fe69b4ed57d217be6b6ab30c4ce004061685bae6eca0ec7","target":"graph","created_at":"2026-05-18T00:07:28Z","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 study finite volume effects within the Polyakov loop Nambu-Jona-Lasinio model for two light and one heavy quarks at vanishing baryon chemical potential and finite temperatures. We include three different Polyakov loop potentials and ensure that the predictions of our effective model in bulk are compatible with lattice QCD results. Finite size effects are taken into account by means of the Multiple Reflection Expansion formalism. We analyze several thermodynamic quantities including the interaction measure, the speed of sound, the surface tension, and the curvature energy and find that they ","authors_text":"A. G. Grunfeld, G. Lugones","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-20T21:46:58Z","title":"Finite size effects in strongly interacting matter at zero chemical potential from Polyakov loop Nambu-Jona-Lasinio model in the light of lattice data"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.07559","kind":"arxiv","version":3},"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:e7e389979bbe355387322818e4e493a81ea92993ba10d0f507faff95cbb6d8b4","target":"record","created_at":"2026-05-18T00:07:28Z","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":"3cb54a1f02ebe46b7aef0537a19964c07d7821afb692f254b9b629e8b68f3f14","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-20T21:46:58Z","title_canon_sha256":"f5a3f0554927d9af8360a8b8d5acf70e1038469541d6dabd3193ef445e20de1b"},"schema_version":"1.0","source":{"id":"1711.07559","kind":"arxiv","version":3}},"canonical_sha256":"869aab7f05c53822c5b6c16e8b01e367ca49985e17d226e0b453d92205db9074","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"869aab7f05c53822c5b6c16e8b01e367ca49985e17d226e0b453d92205db9074","first_computed_at":"2026-05-18T00:07:28.146258Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:07:28.146258Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"TqR9r663W3rlp1aA/vYbdpyoAA+LBuc+52ob850SiGBR3tpRxvtlQ6WG3LZwXoeAWxcqgUrvabiVEBr1G4qNDw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:07:28.146919Z","signed_message":"canonical_sha256_bytes"},"source_id":"1711.07559","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e7e389979bbe355387322818e4e493a81ea92993ba10d0f507faff95cbb6d8b4","sha256:5adf9155d6adf44b6fe69b4ed57d217be6b6ab30c4ce004061685bae6eca0ec7"],"state_sha256":"fefac93da39bb9d2fd9a7746e41cdc3bfe6772cdbacd33e2b81b40764fcb295b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VAa8i1IsDS2CRe2puW9CS6BwOcv9cu8N2P6ZiGccxWjsQRqu18j/imkl5BvXId0T8Y9CicE0nPNQeqIj9X/xBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-21T16:46:35.590999Z","bundle_sha256":"6d1142d7d602d2359acd61d3da8e9b77d2c075a0021b509fdbdd7bc60fac3054"}}