{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:SWQJ37MT3LDVFDQXS7OC6XIO5Q","short_pith_number":"pith:SWQJ37MT","schema_version":"1.0","canonical_sha256":"95a09dfd93dac7528e1797dc2f5d0eec1a2cb5d5c9f96591741cee6fd956f387","source":{"kind":"arxiv","id":"1303.2684","version":1},"attestation_state":"computed","paper":{"title":"Ultrasoft fermion mode and off-diagonal Boltzmann equation in quark-gluon plasma at high temperature","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Daisuke Satow","submitted_at":"2013-03-11T20:52:12Z","abstract_excerpt":"We derive the generalized Boltzmann equation (GBE) near equilibrium from the Kadanoff-Baym equation for quark excitation with ultrasoft momentum (~g^2T, g: coupling constant, T: temperature) in quantum chromodynamics (QCD) at extremely high T, and show that the equation is equivalent to the self-consistent equation derived in the resummed perturbation scheme used to analyze the quark propagator. We obtain the expressions of the dispersion relation, the damping rate, and the strength of a quark excitation with ultrasoft momentum by solving the GBE. We also show that the GBE enables us to obtain"},"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":"1303.2684","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-03-11T20:52:12Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"a614aa2f8e448fc3a2b3f65d43bae86e9d6edc2313b66755deb008692056f9f3","abstract_canon_sha256":"94b64f0a980396c1b537b816ab7c8ba72af260831121a7d1943b266b9a0bfff5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:25:26.966167Z","signature_b64":"GwODsBlZyDjUjIyq8KoPHu/DY/zWzyr635A8imjVwca4brr3rTmrL+ZzAimPYgBp/OqpvIxY3rafPlvxo/JiBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"95a09dfd93dac7528e1797dc2f5d0eec1a2cb5d5c9f96591741cee6fd956f387","last_reissued_at":"2026-05-18T03:25:26.965435Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:25:26.965435Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Ultrasoft fermion mode and off-diagonal Boltzmann equation in quark-gluon plasma at high temperature","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Daisuke Satow","submitted_at":"2013-03-11T20:52:12Z","abstract_excerpt":"We derive the generalized Boltzmann equation (GBE) near equilibrium from the Kadanoff-Baym equation for quark excitation with ultrasoft momentum (~g^2T, g: coupling constant, T: temperature) in quantum chromodynamics (QCD) at extremely high T, and show that the equation is equivalent to the self-consistent equation derived in the resummed perturbation scheme used to analyze the quark propagator. We obtain the expressions of the dispersion relation, the damping rate, and the strength of a quark excitation with ultrasoft momentum by solving the GBE. We also show that the GBE enables us to obtain"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.2684","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1303.2684","created_at":"2026-05-18T03:25:26.965533+00:00"},{"alias_kind":"arxiv_version","alias_value":"1303.2684v1","created_at":"2026-05-18T03:25:26.965533+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.2684","created_at":"2026-05-18T03:25:26.965533+00:00"},{"alias_kind":"pith_short_12","alias_value":"SWQJ37MT3LDV","created_at":"2026-05-18T12:27:59.945178+00:00"},{"alias_kind":"pith_short_16","alias_value":"SWQJ37MT3LDVFDQX","created_at":"2026-05-18T12:27:59.945178+00:00"},{"alias_kind":"pith_short_8","alias_value":"SWQJ37MT","created_at":"2026-05-18T12:27:59.945178+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/SWQJ37MT3LDVFDQXS7OC6XIO5Q","json":"https://pith.science/pith/SWQJ37MT3LDVFDQXS7OC6XIO5Q.json","graph_json":"https://pith.science/api/pith-number/SWQJ37MT3LDVFDQXS7OC6XIO5Q/graph.json","events_json":"https://pith.science/api/pith-number/SWQJ37MT3LDVFDQXS7OC6XIO5Q/events.json","paper":"https://pith.science/paper/SWQJ37MT"},"agent_actions":{"view_html":"https://pith.science/pith/SWQJ37MT3LDVFDQXS7OC6XIO5Q","download_json":"https://pith.science/pith/SWQJ37MT3LDVFDQXS7OC6XIO5Q.json","view_paper":"https://pith.science/paper/SWQJ37MT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1303.2684&json=true","fetch_graph":"https://pith.science/api/pith-number/SWQJ37MT3LDVFDQXS7OC6XIO5Q/graph.json","fetch_events":"https://pith.science/api/pith-number/SWQJ37MT3LDVFDQXS7OC6XIO5Q/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SWQJ37MT3LDVFDQXS7OC6XIO5Q/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SWQJ37MT3LDVFDQXS7OC6XIO5Q/action/storage_attestation","attest_author":"https://pith.science/pith/SWQJ37MT3LDVFDQXS7OC6XIO5Q/action/author_attestation","sign_citation":"https://pith.science/pith/SWQJ37MT3LDVFDQXS7OC6XIO5Q/action/citation_signature","submit_replication":"https://pith.science/pith/SWQJ37MT3LDVFDQXS7OC6XIO5Q/action/replication_record"}},"created_at":"2026-05-18T03:25:26.965533+00:00","updated_at":"2026-05-18T03:25:26.965533+00:00"}