{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:ISMTBW4HMRVBYG7BRCL5APHB6G","short_pith_number":"pith:ISMTBW4H","schema_version":"1.0","canonical_sha256":"449930db87646a1c1be18897d03ce1f19c706cc346270de6f794d027e95555f8","source":{"kind":"arxiv","id":"1209.0374","version":2},"attestation_state":"computed","paper":{"title":"Lattice QCD Simulations in External Background Fields","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Massimo D'Elia","submitted_at":"2012-09-03T14:59:30Z","abstract_excerpt":"We discuss recent results and future prospects regarding the investigation, by lattice simulations, of the non-perturbative properties of QCD and of its phase diagram in presence of magnetic or chromomagnetic background fields. After a brief introduction to the formulation of lattice QCD in presence of external fields, we focus on studies regarding the effects of external fields on chiral symmetry breaking, on its restoration at finite temperature and on deconfinement. We conclude with a few comments regarding the effects of electromagnetic background fields on gluodynamics."},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1209.0374","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-09-03T14:59:30Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"3efeecf9b6a316678270e2ca3957708e31e825b0421924c37d7e0fb2505b20aa","abstract_canon_sha256":"1d0435198c9aaf38f2b66bc78f72358d4bd99268dde6d1ecebad791656c63936"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:54:48.007711Z","signature_b64":"XSQH3hxxQ00wyXscLuJ5wcP7vEcvcDbP2QaLqcn0fR9NXYH6nN91D7Htnz1853zEJDjQ3av9vwyvM87hwsi8AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"449930db87646a1c1be18897d03ce1f19c706cc346270de6f794d027e95555f8","last_reissued_at":"2026-05-18T01:54:48.007060Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:54:48.007060Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Lattice QCD Simulations in External Background Fields","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Massimo D'Elia","submitted_at":"2012-09-03T14:59:30Z","abstract_excerpt":"We discuss recent results and future prospects regarding the investigation, by lattice simulations, of the non-perturbative properties of QCD and of its phase diagram in presence of magnetic or chromomagnetic background fields. After a brief introduction to the formulation of lattice QCD in presence of external fields, we focus on studies regarding the effects of external fields on chiral symmetry breaking, on its restoration at finite temperature and on deconfinement. We conclude with a few comments regarding the effects of electromagnetic background fields on gluodynamics."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1209.0374","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1209.0374","created_at":"2026-05-18T01:54:48.007176+00:00"},{"alias_kind":"arxiv_version","alias_value":"1209.0374v2","created_at":"2026-05-18T01:54:48.007176+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1209.0374","created_at":"2026-05-18T01:54:48.007176+00:00"},{"alias_kind":"pith_short_12","alias_value":"ISMTBW4HMRVB","created_at":"2026-05-18T12:27:09.501522+00:00"},{"alias_kind":"pith_short_16","alias_value":"ISMTBW4HMRVBYG7B","created_at":"2026-05-18T12:27:09.501522+00:00"},{"alias_kind":"pith_short_8","alias_value":"ISMTBW4H","created_at":"2026-05-18T12:27:09.501522+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2511.19255","citing_title":"Magnetic susceptibility of a hot hadronic medium and quark degrees of freedom near the QCD cross-over point","ref_index":9,"is_internal_anchor":true},{"citing_arxiv_id":"2601.22422","citing_title":"Spectral function for pions in magnetic field","ref_index":12,"is_internal_anchor":true},{"citing_arxiv_id":"2604.06248","citing_title":"Relativistic Barnett effect and Curie law in a rigidly rotating free Fermi gas","ref_index":20,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ISMTBW4HMRVBYG7BRCL5APHB6G","json":"https://pith.science/pith/ISMTBW4HMRVBYG7BRCL5APHB6G.json","graph_json":"https://pith.science/api/pith-number/ISMTBW4HMRVBYG7BRCL5APHB6G/graph.json","events_json":"https://pith.science/api/pith-number/ISMTBW4HMRVBYG7BRCL5APHB6G/events.json","paper":"https://pith.science/paper/ISMTBW4H"},"agent_actions":{"view_html":"https://pith.science/pith/ISMTBW4HMRVBYG7BRCL5APHB6G","download_json":"https://pith.science/pith/ISMTBW4HMRVBYG7BRCL5APHB6G.json","view_paper":"https://pith.science/paper/ISMTBW4H","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1209.0374&json=true","fetch_graph":"https://pith.science/api/pith-number/ISMTBW4HMRVBYG7BRCL5APHB6G/graph.json","fetch_events":"https://pith.science/api/pith-number/ISMTBW4HMRVBYG7BRCL5APHB6G/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ISMTBW4HMRVBYG7BRCL5APHB6G/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ISMTBW4HMRVBYG7BRCL5APHB6G/action/storage_attestation","attest_author":"https://pith.science/pith/ISMTBW4HMRVBYG7BRCL5APHB6G/action/author_attestation","sign_citation":"https://pith.science/pith/ISMTBW4HMRVBYG7BRCL5APHB6G/action/citation_signature","submit_replication":"https://pith.science/pith/ISMTBW4HMRVBYG7BRCL5APHB6G/action/replication_record"}},"created_at":"2026-05-18T01:54:48.007176+00:00","updated_at":"2026-05-18T01:54:48.007176+00:00"}