{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:GNCOLD7KDWYEMH6B43M6YS3GPW","short_pith_number":"pith:GNCOLD7K","schema_version":"1.0","canonical_sha256":"3344e58fea1db0461fc1e6d9ec4b667da50218d5eea65bc833a314238f9fc8b4","source":{"kind":"arxiv","id":"hep-lat/0103029","version":2},"attestation_state":"computed","paper":{"title":"Flavor Symmetry and the Static Potential with Hypercubic Blocking","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Hasenfratz, F. Knechtli (U. of Colorado)","submitted_at":"2001-03-26T18:37:16Z","abstract_excerpt":"We introduce a new smearing transformation, the hypercubic (HYP) fat link. The hypercubic fat link mixes gauge links within hypercubes attached to the original link only. Using quenched lattices at beta = 5.7 and 6.0 we show that HYP fat links improve flavor symmetry by an order of magnitude relative to the thin link staggered action. The static potential measured on HYP smeared lattices agrees with the thin link potential at distances r/a >= 2 and has greatly reduced statistical errors. These quenched results will be used in forthcoming dynamical simulations of HYP staggered fermions."},"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":"hep-lat/0103029","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2001-03-26T18:37:16Z","cross_cats_sorted":[],"title_canon_sha256":"4a77594c42582a19da1cb79aa4730d8d689a7f362dd739887299472fd2799579","abstract_canon_sha256":"b7f70bd4dc2c3af96458610a0b7aec42c1208df66c074083b112827a18def099"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:27:07.889830Z","signature_b64":"ZqpWzBAiB9NuoNUAazc2ZYQYyoylInbbpixSZWbYMrj1kDEag0PyoOYZmQ5NQFlsMVWTVNEkVp5dhn5tNGJbBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3344e58fea1db0461fc1e6d9ec4b667da50218d5eea65bc833a314238f9fc8b4","last_reissued_at":"2026-07-04T16:27:07.889467Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:27:07.889467Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Flavor Symmetry and the Static Potential with Hypercubic Blocking","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Hasenfratz, F. Knechtli (U. of Colorado)","submitted_at":"2001-03-26T18:37:16Z","abstract_excerpt":"We introduce a new smearing transformation, the hypercubic (HYP) fat link. The hypercubic fat link mixes gauge links within hypercubes attached to the original link only. Using quenched lattices at beta = 5.7 and 6.0 we show that HYP fat links improve flavor symmetry by an order of magnitude relative to the thin link staggered action. The static potential measured on HYP smeared lattices agrees with the thin link potential at distances r/a >= 2 and has greatly reduced statistical errors. These quenched results will be used in forthcoming dynamical simulations of HYP staggered fermions."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0103029","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-lat/0103029/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"hep-lat/0103029","created_at":"2026-07-04T16:27:07.889529+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0103029v2","created_at":"2026-07-04T16:27:07.889529+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0103029","created_at":"2026-07-04T16:27:07.889529+00:00"},{"alias_kind":"pith_short_12","alias_value":"GNCOLD7KDWYE","created_at":"2026-07-04T16:27:07.889529+00:00"},{"alias_kind":"pith_short_16","alias_value":"GNCOLD7KDWYEMH6B","created_at":"2026-07-04T16:27:07.889529+00:00"},{"alias_kind":"pith_short_8","alias_value":"GNCOLD7K","created_at":"2026-07-04T16:27:07.889529+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":4,"sample":[{"citing_arxiv_id":"2607.07143","citing_title":"Hints for string breaking in QCD","ref_index":56,"is_internal_anchor":true},{"citing_arxiv_id":"2605.20034","citing_title":"Charmonium properties at high temperatures from lattice QCD","ref_index":47,"is_internal_anchor":true},{"citing_arxiv_id":"2602.02436","citing_title":"Wilson loops with neural networks","ref_index":41,"is_internal_anchor":true},{"citing_arxiv_id":"2604.12419","citing_title":"Hybrid Renormalization for Baryon Distribution Amplitudes from Lattice QCD in LaMET","ref_index":22,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GNCOLD7KDWYEMH6B43M6YS3GPW","json":"https://pith.science/pith/GNCOLD7KDWYEMH6B43M6YS3GPW.json","graph_json":"https://pith.science/api/pith-number/GNCOLD7KDWYEMH6B43M6YS3GPW/graph.json","events_json":"https://pith.science/api/pith-number/GNCOLD7KDWYEMH6B43M6YS3GPW/events.json","paper":"https://pith.science/paper/GNCOLD7K"},"agent_actions":{"view_html":"https://pith.science/pith/GNCOLD7KDWYEMH6B43M6YS3GPW","download_json":"https://pith.science/pith/GNCOLD7KDWYEMH6B43M6YS3GPW.json","view_paper":"https://pith.science/paper/GNCOLD7K","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/0103029&json=true","fetch_graph":"https://pith.science/api/pith-number/GNCOLD7KDWYEMH6B43M6YS3GPW/graph.json","fetch_events":"https://pith.science/api/pith-number/GNCOLD7KDWYEMH6B43M6YS3GPW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GNCOLD7KDWYEMH6B43M6YS3GPW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GNCOLD7KDWYEMH6B43M6YS3GPW/action/storage_attestation","attest_author":"https://pith.science/pith/GNCOLD7KDWYEMH6B43M6YS3GPW/action/author_attestation","sign_citation":"https://pith.science/pith/GNCOLD7KDWYEMH6B43M6YS3GPW/action/citation_signature","submit_replication":"https://pith.science/pith/GNCOLD7KDWYEMH6B43M6YS3GPW/action/replication_record"}},"created_at":"2026-07-04T16:27:07.889529+00:00","updated_at":"2026-07-04T16:27:07.889529+00:00"}