{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:OUHXJ5RBTVQBMEOC2LIVEWBSEP","short_pith_number":"pith:OUHXJ5RB","schema_version":"1.0","canonical_sha256":"750f74f6219d601611c2d2d152583223d0410e49cf47109e4590bad6428dd5c4","source":{"kind":"arxiv","id":"1811.01614","version":1},"attestation_state":"computed","paper":{"title":"Temporal Correlators in the Continuous Time Formulation of Strong Coupling Lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-lat","authors_text":"Marc Klegrewe, Wolfgang Unger","submitted_at":"2018-11-05T11:09:46Z","abstract_excerpt":"We present results for lattice QCD in the limit of infinite gauge coupling on a discrete spatial but continuous Euclidean time lattice. A worm type Monte Carlo algorithm is applied in order to sample two-point functions which gives access to the measurement of mesonic temporal correlators. The continuous time limit, based on sending $N_\\tau\\rightarrow \\infty$ and the bare anistotropy to infinity while fixing the temperature in a non-perturbative setup, has various advantages: the algorithm is sign problem free, fast, and accumulates high statistics for correlation functions. Even though the me"},"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":"1811.01614","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-11-05T11:09:46Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"588d0e85b079577249931b171917b3fd5452ec3fbde2adb5d76aff1de27d0837","abstract_canon_sha256":"cbd11df1e27589d703297ee8c195f8dd9ce3725a60fcc292885e2167b09a5103"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:01:33.803001Z","signature_b64":"z3ep0F3z/iHTrhL0Tv045wVyKXsmiO+54GdizZ5rXsI6yH3GirNeAvZZSVSFIwGD5JL/jLaK8THYK3GzP+kMAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"750f74f6219d601611c2d2d152583223d0410e49cf47109e4590bad6428dd5c4","last_reissued_at":"2026-05-18T00:01:33.802464Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:01:33.802464Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Temporal Correlators in the Continuous Time Formulation of Strong Coupling Lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-lat","authors_text":"Marc Klegrewe, Wolfgang Unger","submitted_at":"2018-11-05T11:09:46Z","abstract_excerpt":"We present results for lattice QCD in the limit of infinite gauge coupling on a discrete spatial but continuous Euclidean time lattice. A worm type Monte Carlo algorithm is applied in order to sample two-point functions which gives access to the measurement of mesonic temporal correlators. The continuous time limit, based on sending $N_\\tau\\rightarrow \\infty$ and the bare anistotropy to infinity while fixing the temperature in a non-perturbative setup, has various advantages: the algorithm is sign problem free, fast, and accumulates high statistics for correlation functions. Even though the me"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.01614","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":"1811.01614","created_at":"2026-05-18T00:01:33.802557+00:00"},{"alias_kind":"arxiv_version","alias_value":"1811.01614v1","created_at":"2026-05-18T00:01:33.802557+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.01614","created_at":"2026-05-18T00:01:33.802557+00:00"},{"alias_kind":"pith_short_12","alias_value":"OUHXJ5RBTVQB","created_at":"2026-05-18T12:32:43.782077+00:00"},{"alias_kind":"pith_short_16","alias_value":"OUHXJ5RBTVQBMEOC","created_at":"2026-05-18T12:32:43.782077+00:00"},{"alias_kind":"pith_short_8","alias_value":"OUHXJ5RB","created_at":"2026-05-18T12:32:43.782077+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/OUHXJ5RBTVQBMEOC2LIVEWBSEP","json":"https://pith.science/pith/OUHXJ5RBTVQBMEOC2LIVEWBSEP.json","graph_json":"https://pith.science/api/pith-number/OUHXJ5RBTVQBMEOC2LIVEWBSEP/graph.json","events_json":"https://pith.science/api/pith-number/OUHXJ5RBTVQBMEOC2LIVEWBSEP/events.json","paper":"https://pith.science/paper/OUHXJ5RB"},"agent_actions":{"view_html":"https://pith.science/pith/OUHXJ5RBTVQBMEOC2LIVEWBSEP","download_json":"https://pith.science/pith/OUHXJ5RBTVQBMEOC2LIVEWBSEP.json","view_paper":"https://pith.science/paper/OUHXJ5RB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1811.01614&json=true","fetch_graph":"https://pith.science/api/pith-number/OUHXJ5RBTVQBMEOC2LIVEWBSEP/graph.json","fetch_events":"https://pith.science/api/pith-number/OUHXJ5RBTVQBMEOC2LIVEWBSEP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OUHXJ5RBTVQBMEOC2LIVEWBSEP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OUHXJ5RBTVQBMEOC2LIVEWBSEP/action/storage_attestation","attest_author":"https://pith.science/pith/OUHXJ5RBTVQBMEOC2LIVEWBSEP/action/author_attestation","sign_citation":"https://pith.science/pith/OUHXJ5RBTVQBMEOC2LIVEWBSEP/action/citation_signature","submit_replication":"https://pith.science/pith/OUHXJ5RBTVQBMEOC2LIVEWBSEP/action/replication_record"}},"created_at":"2026-05-18T00:01:33.802557+00:00","updated_at":"2026-05-18T00:01:33.802557+00:00"}