{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:KLLTBKJONHUKTEKNHUWW2NSS6Y","short_pith_number":"pith:KLLTBKJO","canonical_record":{"source":{"id":"1408.5457","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-08-23T05:07:36Z","cross_cats_sorted":["hep-th","nucl-th"],"title_canon_sha256":"9f58e819cc01e1e9497bd48393b082e74959dc27b364b8928f76683378378bf2","abstract_canon_sha256":"2a2fbb252f89d1ef0663eaca30d2621971ea233396b9be75983fa00107330363"},"schema_version":"1.0"},"canonical_sha256":"52d730a92e69e8a9914d3d2d6d3652f6376f21e70cd384ca90629f116c127d25","source":{"kind":"arxiv","id":"1408.5457","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1408.5457","created_at":"2026-05-18T01:22:43Z"},{"alias_kind":"arxiv_version","alias_value":"1408.5457v1","created_at":"2026-05-18T01:22:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1408.5457","created_at":"2026-05-18T01:22:43Z"},{"alias_kind":"pith_short_12","alias_value":"KLLTBKJONHUK","created_at":"2026-05-18T12:28:35Z"},{"alias_kind":"pith_short_16","alias_value":"KLLTBKJONHUKTEKN","created_at":"2026-05-18T12:28:35Z"},{"alias_kind":"pith_short_8","alias_value":"KLLTBKJO","created_at":"2026-05-18T12:28:35Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:KLLTBKJONHUKTEKNHUWW2NSS6Y","target":"record","payload":{"canonical_record":{"source":{"id":"1408.5457","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-08-23T05:07:36Z","cross_cats_sorted":["hep-th","nucl-th"],"title_canon_sha256":"9f58e819cc01e1e9497bd48393b082e74959dc27b364b8928f76683378378bf2","abstract_canon_sha256":"2a2fbb252f89d1ef0663eaca30d2621971ea233396b9be75983fa00107330363"},"schema_version":"1.0"},"canonical_sha256":"52d730a92e69e8a9914d3d2d6d3652f6376f21e70cd384ca90629f116c127d25","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:22:43.413788Z","signature_b64":"aWY4hvytBlZg9UovGt4yELnf6Vfln7MZCWvRYghDLwr7UJkfFJWiJOm0Gt9lgfhfYrdgF7a6RATenSClfwh7Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"52d730a92e69e8a9914d3d2d6d3652f6376f21e70cd384ca90629f116c127d25","last_reissued_at":"2026-05-18T01:22:43.413349Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:22:43.413349Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1408.5457","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":"2026-05-18T01:22:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wIA4C8tz8fHci3JxFJkxQf4VO4YjLgkt6VInOyDphMPXDp4x0VMwJuwzlnJTkF+iBgd4O8L+QRTQViygdUMEDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T11:42:03.056264Z"},"content_sha256":"c1a0b5d0435e25f200ea9c5022da93f27aa11221bf96a9f9472cf6cdcdaebbec","schema_version":"1.0","event_id":"sha256:c1a0b5d0435e25f200ea9c5022da93f27aa11221bf96a9f9472cf6cdcdaebbec"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:KLLTBKJONHUKTEKNHUWW2NSS6Y","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Anomalous magnetic moment of hot quarks, inverse magnetic catalysis and reentrance of chiral symmetry broken phase","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"N. Sadooghi, Sh. Fayazbakhsh","submitted_at":"2014-08-23T05:07:36Z","abstract_excerpt":"The effect of anomalous magnetic moment of quarks on thermodynamic properties of the chiral condensate is studied, using of a two-flavor Nambu--Jona-Lasinio model at finite temperature $T$, chemical potential $\\mu$, and in the presence of a uniform magnetic field $eB$. To this purpose, the Schwinger linear-in-$B$ ansatz for the quark anomalous magnetic moment in term of the nonperturbative Bohr magneton is considered. In a two-dimensional flavor space, it leads to the correction $\\hat{T}_{Sch}=\\hat{\\kappa}\\hat{Q} eB$ in the energy dispersion relation of quarks. Here, $\\hat{Q}$ is the quark cha"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1408.5457","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":"2026-05-18T01:22:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2nNkQ02P7f8xSNHLO+tysfl0P7l0Gn49XAYpJFxLAsYsxtdsIaTQ4zEH4OKJciwzLWGD2jRA89wbMeuWBECqBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T11:42:03.057047Z"},"content_sha256":"63a9a29dc5b4dcd9b1b6c52d2edeb842134d743eae51e61b5df41b5ff0e5b2af","schema_version":"1.0","event_id":"sha256:63a9a29dc5b4dcd9b1b6c52d2edeb842134d743eae51e61b5df41b5ff0e5b2af"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KLLTBKJONHUKTEKNHUWW2NSS6Y/bundle.json","state_url":"https://pith.science/pith/KLLTBKJONHUKTEKNHUWW2NSS6Y/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KLLTBKJONHUKTEKNHUWW2NSS6Y/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":"2026-05-27T11:42:03Z","links":{"resolver":"https://pith.science/pith/KLLTBKJONHUKTEKNHUWW2NSS6Y","bundle":"https://pith.science/pith/KLLTBKJONHUKTEKNHUWW2NSS6Y/bundle.json","state":"https://pith.science/pith/KLLTBKJONHUKTEKNHUWW2NSS6Y/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KLLTBKJONHUKTEKNHUWW2NSS6Y/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:KLLTBKJONHUKTEKNHUWW2NSS6Y","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":"2a2fbb252f89d1ef0663eaca30d2621971ea233396b9be75983fa00107330363","cross_cats_sorted":["hep-th","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-08-23T05:07:36Z","title_canon_sha256":"9f58e819cc01e1e9497bd48393b082e74959dc27b364b8928f76683378378bf2"},"schema_version":"1.0","source":{"id":"1408.5457","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1408.5457","created_at":"2026-05-18T01:22:43Z"},{"alias_kind":"arxiv_version","alias_value":"1408.5457v1","created_at":"2026-05-18T01:22:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1408.5457","created_at":"2026-05-18T01:22:43Z"},{"alias_kind":"pith_short_12","alias_value":"KLLTBKJONHUK","created_at":"2026-05-18T12:28:35Z"},{"alias_kind":"pith_short_16","alias_value":"KLLTBKJONHUKTEKN","created_at":"2026-05-18T12:28:35Z"},{"alias_kind":"pith_short_8","alias_value":"KLLTBKJO","created_at":"2026-05-18T12:28:35Z"}],"graph_snapshots":[{"event_id":"sha256:63a9a29dc5b4dcd9b1b6c52d2edeb842134d743eae51e61b5df41b5ff0e5b2af","target":"graph","created_at":"2026-05-18T01:22:43Z","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 effect of anomalous magnetic moment of quarks on thermodynamic properties of the chiral condensate is studied, using of a two-flavor Nambu--Jona-Lasinio model at finite temperature $T$, chemical potential $\\mu$, and in the presence of a uniform magnetic field $eB$. To this purpose, the Schwinger linear-in-$B$ ansatz for the quark anomalous magnetic moment in term of the nonperturbative Bohr magneton is considered. In a two-dimensional flavor space, it leads to the correction $\\hat{T}_{Sch}=\\hat{\\kappa}\\hat{Q} eB$ in the energy dispersion relation of quarks. Here, $\\hat{Q}$ is the quark cha","authors_text":"N. Sadooghi, Sh. Fayazbakhsh","cross_cats":["hep-th","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-08-23T05:07:36Z","title":"Anomalous magnetic moment of hot quarks, inverse magnetic catalysis and reentrance of chiral symmetry broken phase"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1408.5457","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:c1a0b5d0435e25f200ea9c5022da93f27aa11221bf96a9f9472cf6cdcdaebbec","target":"record","created_at":"2026-05-18T01:22:43Z","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":"2a2fbb252f89d1ef0663eaca30d2621971ea233396b9be75983fa00107330363","cross_cats_sorted":["hep-th","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-08-23T05:07:36Z","title_canon_sha256":"9f58e819cc01e1e9497bd48393b082e74959dc27b364b8928f76683378378bf2"},"schema_version":"1.0","source":{"id":"1408.5457","kind":"arxiv","version":1}},"canonical_sha256":"52d730a92e69e8a9914d3d2d6d3652f6376f21e70cd384ca90629f116c127d25","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"52d730a92e69e8a9914d3d2d6d3652f6376f21e70cd384ca90629f116c127d25","first_computed_at":"2026-05-18T01:22:43.413349Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:22:43.413349Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"aWY4hvytBlZg9UovGt4yELnf6Vfln7MZCWvRYghDLwr7UJkfFJWiJOm0Gt9lgfhfYrdgF7a6RATenSClfwh7Aw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:22:43.413788Z","signed_message":"canonical_sha256_bytes"},"source_id":"1408.5457","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c1a0b5d0435e25f200ea9c5022da93f27aa11221bf96a9f9472cf6cdcdaebbec","sha256:63a9a29dc5b4dcd9b1b6c52d2edeb842134d743eae51e61b5df41b5ff0e5b2af"],"state_sha256":"569fd865103a4b8c4951fcc68e2ca90c01b9e474be69a9496eb46a6f3d1c6939"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tgn5fXicjDkusWbYfaFuY4aFtNKvPo7RZzIusu9Enaj1kuayuilMtOds4RMAa6hr3ppunOGQmiSX95g457quCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T11:42:03.060685Z","bundle_sha256":"5ffff0bff949a7952b55a9b44377cf227b575eadabcf680d823bdb6c621ab633"}}