{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:HEIET2Z377AZVOTFRCUWLZ2WNF","short_pith_number":"pith:HEIET2Z3","canonical_record":{"source":{"id":"1312.0119","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-11-30T16:03:13Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"894050b20b37b09c9d7dd17c136a9c346602fed3a4a39896f2a704f8770439ca","abstract_canon_sha256":"fa889021182731bff7886774d1d71a10aea36641497cfdfb508b8a0f558aeb5d"},"schema_version":"1.0"},"canonical_sha256":"391049eb3bffc19aba6588a965e75669585f57e7e4690f90e0fd7ed9bcdfa0b2","source":{"kind":"arxiv","id":"1312.0119","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1312.0119","created_at":"2026-05-18T03:05:46Z"},{"alias_kind":"arxiv_version","alias_value":"1312.0119v1","created_at":"2026-05-18T03:05:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.0119","created_at":"2026-05-18T03:05:46Z"},{"alias_kind":"pith_short_12","alias_value":"HEIET2Z377AZ","created_at":"2026-05-18T12:27:46Z"},{"alias_kind":"pith_short_16","alias_value":"HEIET2Z377AZVOTF","created_at":"2026-05-18T12:27:46Z"},{"alias_kind":"pith_short_8","alias_value":"HEIET2Z3","created_at":"2026-05-18T12:27:46Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:HEIET2Z377AZVOTFRCUWLZ2WNF","target":"record","payload":{"canonical_record":{"source":{"id":"1312.0119","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-11-30T16:03:13Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"894050b20b37b09c9d7dd17c136a9c346602fed3a4a39896f2a704f8770439ca","abstract_canon_sha256":"fa889021182731bff7886774d1d71a10aea36641497cfdfb508b8a0f558aeb5d"},"schema_version":"1.0"},"canonical_sha256":"391049eb3bffc19aba6588a965e75669585f57e7e4690f90e0fd7ed9bcdfa0b2","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:05:46.728756Z","signature_b64":"NKhOyBuxUW0fqVScI+wJjDrfgYoRYdO1JAMIwJ16SBurlwWokUOtgl93OI1djZD7Zc+kLreMDOxW1TU73n4TAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"391049eb3bffc19aba6588a965e75669585f57e7e4690f90e0fd7ed9bcdfa0b2","last_reissued_at":"2026-05-18T03:05:46.728019Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:05:46.728019Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1312.0119","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":"2026-05-18T03:05:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wFNYGVhV1YcTMFHZylFzUAEXTr3aQaqVrqqyZdjUWYNE3kNr9JPY+KImRQLcamHnEAu/NCX5v06E4+qij7q3CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T18:09:19.820149Z"},"content_sha256":"337e5c36533b4e45377c97990f7bf00b5df43855c04e92b228d1f2bfd3afb7cd","schema_version":"1.0","event_id":"sha256:337e5c36533b4e45377c97990f7bf00b5df43855c04e92b228d1f2bfd3afb7cd"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:HEIET2Z377AZVOTFRCUWLZ2WNF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Chiral phase transition of $N_f$=2+1 QCD with the HISQ action","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-lat","authors_text":"A. Bazavov, F. Karsch, H.-T. Ding, P. Petreczky, Swagato Mukherjee, Y. Maezawa","submitted_at":"2013-11-30T16:03:13Z","abstract_excerpt":"We present studies of universal properties of the chiral phase transition in $N_f$=2+1 QCD based on the simulations using Highly Improved Staggered fermions on lattices with temporal extent $N_\\tau$=6. We analyze the quark mass and volume dependence of the chiral condensates and chiral susceptibilities in QCD with two degenerate light quarks and a strange quark. The strange quark mass is chosen to be fixed to its physical value ($m^{phy}_s$) and five values of light quark masses ($m_l$) that are varied in the interval 1/20$\\gtrsim m_l/m^{phy}_s \\gtrsim$1/80. Here various quark masses correspon"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.0119","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":"2026-05-18T03:05:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dv6eAPhmfbEj07UGtyqP7G1QIT/pB/XKc8vHYxp41+7qsIfsDa3hXmBpxIxVOMqXVcixD+b/yK/Qkgh/vQsYDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T18:09:19.820604Z"},"content_sha256":"085220f96f9301f254bad73d37d48321d9744a578688bc093a2710092a8f2460","schema_version":"1.0","event_id":"sha256:085220f96f9301f254bad73d37d48321d9744a578688bc093a2710092a8f2460"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HEIET2Z377AZVOTFRCUWLZ2WNF/bundle.json","state_url":"https://pith.science/pith/HEIET2Z377AZVOTFRCUWLZ2WNF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HEIET2Z377AZVOTFRCUWLZ2WNF/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":"2026-08-06T18:09:19Z","links":{"resolver":"https://pith.science/pith/HEIET2Z377AZVOTFRCUWLZ2WNF","bundle":"https://pith.science/pith/HEIET2Z377AZVOTFRCUWLZ2WNF/bundle.json","state":"https://pith.science/pith/HEIET2Z377AZVOTFRCUWLZ2WNF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HEIET2Z377AZVOTFRCUWLZ2WNF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:HEIET2Z377AZVOTFRCUWLZ2WNF","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":"fa889021182731bff7886774d1d71a10aea36641497cfdfb508b8a0f558aeb5d","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-11-30T16:03:13Z","title_canon_sha256":"894050b20b37b09c9d7dd17c136a9c346602fed3a4a39896f2a704f8770439ca"},"schema_version":"1.0","source":{"id":"1312.0119","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1312.0119","created_at":"2026-05-18T03:05:46Z"},{"alias_kind":"arxiv_version","alias_value":"1312.0119v1","created_at":"2026-05-18T03:05:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.0119","created_at":"2026-05-18T03:05:46Z"},{"alias_kind":"pith_short_12","alias_value":"HEIET2Z377AZ","created_at":"2026-05-18T12:27:46Z"},{"alias_kind":"pith_short_16","alias_value":"HEIET2Z377AZVOTF","created_at":"2026-05-18T12:27:46Z"},{"alias_kind":"pith_short_8","alias_value":"HEIET2Z3","created_at":"2026-05-18T12:27:46Z"}],"graph_snapshots":[{"event_id":"sha256:085220f96f9301f254bad73d37d48321d9744a578688bc093a2710092a8f2460","target":"graph","created_at":"2026-05-18T03:05:46Z","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 present studies of universal properties of the chiral phase transition in $N_f$=2+1 QCD based on the simulations using Highly Improved Staggered fermions on lattices with temporal extent $N_\\tau$=6. We analyze the quark mass and volume dependence of the chiral condensates and chiral susceptibilities in QCD with two degenerate light quarks and a strange quark. The strange quark mass is chosen to be fixed to its physical value ($m^{phy}_s$) and five values of light quark masses ($m_l$) that are varied in the interval 1/20$\\gtrsim m_l/m^{phy}_s \\gtrsim$1/80. Here various quark masses correspon","authors_text":"A. Bazavov, F. Karsch, H.-T. Ding, P. Petreczky, Swagato Mukherjee, Y. Maezawa","cross_cats":["nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-11-30T16:03:13Z","title":"Chiral phase transition of $N_f$=2+1 QCD with the HISQ action"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.0119","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":"sha256:337e5c36533b4e45377c97990f7bf00b5df43855c04e92b228d1f2bfd3afb7cd","target":"record","created_at":"2026-05-18T03:05:46Z","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":"fa889021182731bff7886774d1d71a10aea36641497cfdfb508b8a0f558aeb5d","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-11-30T16:03:13Z","title_canon_sha256":"894050b20b37b09c9d7dd17c136a9c346602fed3a4a39896f2a704f8770439ca"},"schema_version":"1.0","source":{"id":"1312.0119","kind":"arxiv","version":1}},"canonical_sha256":"391049eb3bffc19aba6588a965e75669585f57e7e4690f90e0fd7ed9bcdfa0b2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"391049eb3bffc19aba6588a965e75669585f57e7e4690f90e0fd7ed9bcdfa0b2","first_computed_at":"2026-05-18T03:05:46.728019Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:05:46.728019Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"NKhOyBuxUW0fqVScI+wJjDrfgYoRYdO1JAMIwJ16SBurlwWokUOtgl93OI1djZD7Zc+kLreMDOxW1TU73n4TAA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:05:46.728756Z","signed_message":"canonical_sha256_bytes"},"source_id":"1312.0119","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:337e5c36533b4e45377c97990f7bf00b5df43855c04e92b228d1f2bfd3afb7cd","sha256:085220f96f9301f254bad73d37d48321d9744a578688bc093a2710092a8f2460"],"state_sha256":"649279d1fb3922e4d9f32163160e0a14815a3a09cd1b7e9d1d82d6ee13df4a10"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qMLZ+kMmpG6na+Mq5BvyXpTf7E8jNhcOxTh250KSGHeM8+CCh+gAJ8Q5m+QeVap6wkYPYDlCR961r/pMDty6BQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-06T18:09:19.825771Z","bundle_sha256":"2746dd81ba316766dc32718fe8170fef1d2c02d695073649aba8ff554f8a0e55"}}