{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:67PAVYY7CE7JACICZMJW4CWPQK","short_pith_number":"pith:67PAVYY7","schema_version":"1.0","canonical_sha256":"f7de0ae31f113e900902cb136e0acf828bce05464c64db257951fa88d32b8666","source":{"kind":"arxiv","id":"1311.5208","version":1},"attestation_state":"computed","paper":{"title":"Further studies of QCD with sextet quarks","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"D. K. Sinclair, J. B. Kogut","submitted_at":"2013-11-20T20:32:44Z","abstract_excerpt":"We continue our simulations of QCD with 2 flavours of colour-sextet quarks as a model for walking technicolor. QCD with 3 flavours of colour-sextet quarks is also studied for comparison with the 2-flavour theory. We simulate these theories at finite temperatures T, using lattices with a finite extent $N_t a=1/T$ in the (Euclidean) time direction. The lattice coupling at the chiral-symmetry-restoration transition is measured as a function of $N_t$. If this is indeed a finite-temperature transition, the evolution of this coupling with $N_t$ as $N_t \\rightarrow \\infty$ and hence the lattice spaci"},"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":"1311.5208","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-11-20T20:32:44Z","cross_cats_sorted":[],"title_canon_sha256":"8729525b5f0eba51754aee11b2d5af2ccd12d255352bc3df90325a69635c2870","abstract_canon_sha256":"0f717e096d4ee41f3e25867836d50b85e2c7f50ab7ac14eb08a5b9017ecbd422"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:06:34.911385Z","signature_b64":"utFhrBB+o52wHrjA61q9xQD9rlNayGc1nlwC5of2PuSpCBQuj9UWf+R9UseQJWfSly68YDhyIYb63LbeAPypCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f7de0ae31f113e900902cb136e0acf828bce05464c64db257951fa88d32b8666","last_reissued_at":"2026-05-18T03:06:34.910750Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:06:34.910750Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Further studies of QCD with sextet quarks","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"D. K. Sinclair, J. B. Kogut","submitted_at":"2013-11-20T20:32:44Z","abstract_excerpt":"We continue our simulations of QCD with 2 flavours of colour-sextet quarks as a model for walking technicolor. QCD with 3 flavours of colour-sextet quarks is also studied for comparison with the 2-flavour theory. We simulate these theories at finite temperatures T, using lattices with a finite extent $N_t a=1/T$ in the (Euclidean) time direction. The lattice coupling at the chiral-symmetry-restoration transition is measured as a function of $N_t$. If this is indeed a finite-temperature transition, the evolution of this coupling with $N_t$ as $N_t \\rightarrow \\infty$ and hence the lattice spaci"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.5208","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":"1311.5208","created_at":"2026-05-18T03:06:34.910834+00:00"},{"alias_kind":"arxiv_version","alias_value":"1311.5208v1","created_at":"2026-05-18T03:06:34.910834+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.5208","created_at":"2026-05-18T03:06:34.910834+00:00"},{"alias_kind":"pith_short_12","alias_value":"67PAVYY7CE7J","created_at":"2026-05-18T12:27:36.564083+00:00"},{"alias_kind":"pith_short_16","alias_value":"67PAVYY7CE7JACIC","created_at":"2026-05-18T12:27:36.564083+00:00"},{"alias_kind":"pith_short_8","alias_value":"67PAVYY7","created_at":"2026-05-18T12:27:36.564083+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/67PAVYY7CE7JACICZMJW4CWPQK","json":"https://pith.science/pith/67PAVYY7CE7JACICZMJW4CWPQK.json","graph_json":"https://pith.science/api/pith-number/67PAVYY7CE7JACICZMJW4CWPQK/graph.json","events_json":"https://pith.science/api/pith-number/67PAVYY7CE7JACICZMJW4CWPQK/events.json","paper":"https://pith.science/paper/67PAVYY7"},"agent_actions":{"view_html":"https://pith.science/pith/67PAVYY7CE7JACICZMJW4CWPQK","download_json":"https://pith.science/pith/67PAVYY7CE7JACICZMJW4CWPQK.json","view_paper":"https://pith.science/paper/67PAVYY7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1311.5208&json=true","fetch_graph":"https://pith.science/api/pith-number/67PAVYY7CE7JACICZMJW4CWPQK/graph.json","fetch_events":"https://pith.science/api/pith-number/67PAVYY7CE7JACICZMJW4CWPQK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/67PAVYY7CE7JACICZMJW4CWPQK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/67PAVYY7CE7JACICZMJW4CWPQK/action/storage_attestation","attest_author":"https://pith.science/pith/67PAVYY7CE7JACICZMJW4CWPQK/action/author_attestation","sign_citation":"https://pith.science/pith/67PAVYY7CE7JACICZMJW4CWPQK/action/citation_signature","submit_replication":"https://pith.science/pith/67PAVYY7CE7JACICZMJW4CWPQK/action/replication_record"}},"created_at":"2026-05-18T03:06:34.910834+00:00","updated_at":"2026-05-18T03:06:34.910834+00:00"}