{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:K437I4Z2HFQWYN4YSYKPATEMX7","short_pith_number":"pith:K437I4Z2","schema_version":"1.0","canonical_sha256":"5737f4733a39616c37989614f04c8cbfcae98ce2539f214d72f768252ff78438","source":{"kind":"arxiv","id":"1011.2822","version":1},"attestation_state":"computed","paper":{"title":"Spectral properties of quarks above Tc -- thermal mass, dispersion relation, and self-energy --","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Masakiyo Kitazawa","submitted_at":"2010-11-12T04:28:45Z","abstract_excerpt":"Spectral properties of quarks above the critical temperature for deconfinement are analyzed in quenched lattice QCD on lattices of size 128^3x16. We study quark spectral function in energy and momentum space, focusing on the values of the thermal mass and the dispersion relations of normal and plasmino modes at nonzero momentum, as well as their spatial volume dependence. Our numerical result suggests that the dispersion relation of the plasmino mode has a minimum at nonzero momentum even near the critical temperature. The quark self-energy is also analyzed by using the analyticy of the invers"},"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":"1011.2822","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2010-11-12T04:28:45Z","cross_cats_sorted":[],"title_canon_sha256":"8b96d4fe35f526db6f33c0a5748832d73c91ccdfb36d5960b88b4e150297e521","abstract_canon_sha256":"ba86812689421d1e03844f2357925f3773d362b1821b841bd80b939c98a89c89"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:36:08.117961Z","signature_b64":"j47hmYZNQ0T4mKDvcqz5A45VSmm6YY0sl13V9uSCNn+qfgXsNrYac3fvAKCV3t3PAISDhh12zyVuJCeLL22eBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5737f4733a39616c37989614f04c8cbfcae98ce2539f214d72f768252ff78438","last_reissued_at":"2026-05-18T04:36:08.117458Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:36:08.117458Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Spectral properties of quarks above Tc -- thermal mass, dispersion relation, and self-energy --","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Masakiyo Kitazawa","submitted_at":"2010-11-12T04:28:45Z","abstract_excerpt":"Spectral properties of quarks above the critical temperature for deconfinement are analyzed in quenched lattice QCD on lattices of size 128^3x16. We study quark spectral function in energy and momentum space, focusing on the values of the thermal mass and the dispersion relations of normal and plasmino modes at nonzero momentum, as well as their spatial volume dependence. Our numerical result suggests that the dispersion relation of the plasmino mode has a minimum at nonzero momentum even near the critical temperature. The quark self-energy is also analyzed by using the analyticy of the invers"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1011.2822","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":"1011.2822","created_at":"2026-05-18T04:36:08.117542+00:00"},{"alias_kind":"arxiv_version","alias_value":"1011.2822v1","created_at":"2026-05-18T04:36:08.117542+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1011.2822","created_at":"2026-05-18T04:36:08.117542+00:00"},{"alias_kind":"pith_short_12","alias_value":"K437I4Z2HFQW","created_at":"2026-05-18T12:26:09.077623+00:00"},{"alias_kind":"pith_short_16","alias_value":"K437I4Z2HFQWYN4Y","created_at":"2026-05-18T12:26:09.077623+00:00"},{"alias_kind":"pith_short_8","alias_value":"K437I4Z2","created_at":"2026-05-18T12:26:09.077623+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/K437I4Z2HFQWYN4YSYKPATEMX7","json":"https://pith.science/pith/K437I4Z2HFQWYN4YSYKPATEMX7.json","graph_json":"https://pith.science/api/pith-number/K437I4Z2HFQWYN4YSYKPATEMX7/graph.json","events_json":"https://pith.science/api/pith-number/K437I4Z2HFQWYN4YSYKPATEMX7/events.json","paper":"https://pith.science/paper/K437I4Z2"},"agent_actions":{"view_html":"https://pith.science/pith/K437I4Z2HFQWYN4YSYKPATEMX7","download_json":"https://pith.science/pith/K437I4Z2HFQWYN4YSYKPATEMX7.json","view_paper":"https://pith.science/paper/K437I4Z2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1011.2822&json=true","fetch_graph":"https://pith.science/api/pith-number/K437I4Z2HFQWYN4YSYKPATEMX7/graph.json","fetch_events":"https://pith.science/api/pith-number/K437I4Z2HFQWYN4YSYKPATEMX7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/K437I4Z2HFQWYN4YSYKPATEMX7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/K437I4Z2HFQWYN4YSYKPATEMX7/action/storage_attestation","attest_author":"https://pith.science/pith/K437I4Z2HFQWYN4YSYKPATEMX7/action/author_attestation","sign_citation":"https://pith.science/pith/K437I4Z2HFQWYN4YSYKPATEMX7/action/citation_signature","submit_replication":"https://pith.science/pith/K437I4Z2HFQWYN4YSYKPATEMX7/action/replication_record"}},"created_at":"2026-05-18T04:36:08.117542+00:00","updated_at":"2026-05-18T04:36:08.117542+00:00"}