{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:BPAKGMZMCWJN2RYRWUGYU3G2CC","short_pith_number":"pith:BPAKGMZM","schema_version":"1.0","canonical_sha256":"0bc0a3332c1592dd4711b50d8a6cda10a59a6f13da97ad369c621b098314680c","source":{"kind":"arxiv","id":"1211.7169","version":1},"attestation_state":"computed","paper":{"title":"Quark mass, scale and volume dependence of topological charge density correlator in Lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Abhishek Chowdhury, A. Harindranath, Asit K. De, Jyotirmoy Maiti, Santanu Mondal","submitted_at":"2012-11-30T07:19:27Z","abstract_excerpt":"We study the two-point Topological Charge Density Correlator (TCDC) in lattice QCD with two degenerate flavours of naive Wilson fermions and unimproved Wilson gauge action at two values of lattice spacings and different volumes, for a range of quark masses. Configurations are generated with DDHMC algorithm and smoothed with HYP smearing. In order to shed light on the mechanisms leading to the observed suppression of topological susceptibility with respect to the decreasing quark mass and decreasing volume, in this work, we carry out a detailed study of the two-point TCDC. We have shown that, ("},"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":"1211.7169","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-11-30T07:19:27Z","cross_cats_sorted":[],"title_canon_sha256":"b8b2157e2d32aab3fa09a7aef9e5ad5f7b33409e46fac0d9673f7f13eaf5d843","abstract_canon_sha256":"84d96c9ad876aaf068d6aa80f2b5ab24eebaf38ba8a96f6115cfea90358cd145"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:39:31.472114Z","signature_b64":"pn5IX3MvuwxXHsx27jTReCjdyIy1j0RAmIIomnRXVLPW+97hiefrbDw7WXif9BNtKiiV1HP2EaTJ5mS9nin/AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0bc0a3332c1592dd4711b50d8a6cda10a59a6f13da97ad369c621b098314680c","last_reissued_at":"2026-05-18T03:39:31.471280Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:39:31.471280Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quark mass, scale and volume dependence of topological charge density correlator in Lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Abhishek Chowdhury, A. Harindranath, Asit K. De, Jyotirmoy Maiti, Santanu Mondal","submitted_at":"2012-11-30T07:19:27Z","abstract_excerpt":"We study the two-point Topological Charge Density Correlator (TCDC) in lattice QCD with two degenerate flavours of naive Wilson fermions and unimproved Wilson gauge action at two values of lattice spacings and different volumes, for a range of quark masses. Configurations are generated with DDHMC algorithm and smoothed with HYP smearing. In order to shed light on the mechanisms leading to the observed suppression of topological susceptibility with respect to the decreasing quark mass and decreasing volume, in this work, we carry out a detailed study of the two-point TCDC. We have shown that, ("},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.7169","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":"1211.7169","created_at":"2026-05-18T03:39:31.471429+00:00"},{"alias_kind":"arxiv_version","alias_value":"1211.7169v1","created_at":"2026-05-18T03:39:31.471429+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.7169","created_at":"2026-05-18T03:39:31.471429+00:00"},{"alias_kind":"pith_short_12","alias_value":"BPAKGMZMCWJN","created_at":"2026-05-18T12:27:01.376967+00:00"},{"alias_kind":"pith_short_16","alias_value":"BPAKGMZMCWJN2RYR","created_at":"2026-05-18T12:27:01.376967+00:00"},{"alias_kind":"pith_short_8","alias_value":"BPAKGMZM","created_at":"2026-05-18T12:27:01.376967+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/BPAKGMZMCWJN2RYRWUGYU3G2CC","json":"https://pith.science/pith/BPAKGMZMCWJN2RYRWUGYU3G2CC.json","graph_json":"https://pith.science/api/pith-number/BPAKGMZMCWJN2RYRWUGYU3G2CC/graph.json","events_json":"https://pith.science/api/pith-number/BPAKGMZMCWJN2RYRWUGYU3G2CC/events.json","paper":"https://pith.science/paper/BPAKGMZM"},"agent_actions":{"view_html":"https://pith.science/pith/BPAKGMZMCWJN2RYRWUGYU3G2CC","download_json":"https://pith.science/pith/BPAKGMZMCWJN2RYRWUGYU3G2CC.json","view_paper":"https://pith.science/paper/BPAKGMZM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1211.7169&json=true","fetch_graph":"https://pith.science/api/pith-number/BPAKGMZMCWJN2RYRWUGYU3G2CC/graph.json","fetch_events":"https://pith.science/api/pith-number/BPAKGMZMCWJN2RYRWUGYU3G2CC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BPAKGMZMCWJN2RYRWUGYU3G2CC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BPAKGMZMCWJN2RYRWUGYU3G2CC/action/storage_attestation","attest_author":"https://pith.science/pith/BPAKGMZMCWJN2RYRWUGYU3G2CC/action/author_attestation","sign_citation":"https://pith.science/pith/BPAKGMZMCWJN2RYRWUGYU3G2CC/action/citation_signature","submit_replication":"https://pith.science/pith/BPAKGMZMCWJN2RYRWUGYU3G2CC/action/replication_record"}},"created_at":"2026-05-18T03:39:31.471429+00:00","updated_at":"2026-05-18T03:39:31.471429+00:00"}