{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:CPUAAA3BQJCALV3334IZXMND55","short_pith_number":"pith:CPUAAA3B","canonical_record":{"source":{"id":"1409.6459","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-09-23T09:42:30Z","cross_cats_sorted":[],"title_canon_sha256":"95ed7899f9b5c43e2297edf395320060384faad3cd5e6c69c6a260ecec3f1052","abstract_canon_sha256":"e22ab944037155b7bbaf5430ca23ddfbb2af4f732bab7afeb62c38a8e893d1fe"},"schema_version":"1.0"},"canonical_sha256":"13e8000361824405d77bdf119bb1a3ef52aa2f0afc61f8eefec69fa89791dbaa","source":{"kind":"arxiv","id":"1409.6459","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.6459","created_at":"2026-05-18T02:18:51Z"},{"alias_kind":"arxiv_version","alias_value":"1409.6459v2","created_at":"2026-05-18T02:18:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.6459","created_at":"2026-05-18T02:18:51Z"},{"alias_kind":"pith_short_12","alias_value":"CPUAAA3BQJCA","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_16","alias_value":"CPUAAA3BQJCALV33","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_8","alias_value":"CPUAAA3B","created_at":"2026-05-18T12:28:22Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:CPUAAA3BQJCALV3334IZXMND55","target":"record","payload":{"canonical_record":{"source":{"id":"1409.6459","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-09-23T09:42:30Z","cross_cats_sorted":[],"title_canon_sha256":"95ed7899f9b5c43e2297edf395320060384faad3cd5e6c69c6a260ecec3f1052","abstract_canon_sha256":"e22ab944037155b7bbaf5430ca23ddfbb2af4f732bab7afeb62c38a8e893d1fe"},"schema_version":"1.0"},"canonical_sha256":"13e8000361824405d77bdf119bb1a3ef52aa2f0afc61f8eefec69fa89791dbaa","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:18:51.613562Z","signature_b64":"+geD6hRYYMtUmt6w3/GZlh00NnrYM9FmtvGButypGimPUnu9xwNGYpqwfCL+h4Loj/fZNFXPS7a/RbNySmkADw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"13e8000361824405d77bdf119bb1a3ef52aa2f0afc61f8eefec69fa89791dbaa","last_reissued_at":"2026-05-18T02:18:51.612979Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:18:51.612979Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1409.6459","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:18:51Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nvEetnas/OWyqTwBVA+tQMJsix+MdKD/ukZsjEvyDEuFy3U6DBx/TtUb5v6vwG6TFD13drBC70NR+a64/8fqBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T14:50:01.678841Z"},"content_sha256":"51f479c65afbc9280e7d4b9a252ec72fdcf43f50aba57ea0647f0a4ebc6ab81d","schema_version":"1.0","event_id":"sha256:51f479c65afbc9280e7d4b9a252ec72fdcf43f50aba57ea0647f0a4ebc6ab81d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:CPUAAA3BQJCALV3334IZXMND55","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Correlation and localization properties of topological charge density and the pseudoscalar glueball mass in SU(3) lattice Yang-Mills theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Abhishek Chowdhury, A. Harindranath, Jyotirmoy Maiti","submitted_at":"2014-09-23T09:42:30Z","abstract_excerpt":"Towards the goal of extracting the continuum properties, we have studied the Topological Charge Density Correlator (TCDC) and the Inverse Participation Ratio (IPR) for the topological charge density ($q(x)$) in SU(3) Lattice Yang-Mills theory for relatively small lattice spacings including some smaller than those explored before. With the help of recently proposed open boundary condition, it is possible to compute observables at a smaller lattice spacing since {\\em trapping problem} is absent. On the other hand, the reference energy scale provided by Wilson flow allows us to study their scalin"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.6459","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":""},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:18:51Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4HEKvcpQjK45ZK574SyPeVZcpuy9l0un6dRfsM1qiDpIWzwMwOrnEQpR33f2nXX4rtN1HaBBEtzW3bmPZErMBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T14:50:01.679573Z"},"content_sha256":"6cbe6f1269e14a3861193a8343905726be0ee6a32b13373e0ac61209ae20883d","schema_version":"1.0","event_id":"sha256:6cbe6f1269e14a3861193a8343905726be0ee6a32b13373e0ac61209ae20883d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/CPUAAA3BQJCALV3334IZXMND55/bundle.json","state_url":"https://pith.science/pith/CPUAAA3BQJCALV3334IZXMND55/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/CPUAAA3BQJCALV3334IZXMND55/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-29T14:50:01Z","links":{"resolver":"https://pith.science/pith/CPUAAA3BQJCALV3334IZXMND55","bundle":"https://pith.science/pith/CPUAAA3BQJCALV3334IZXMND55/bundle.json","state":"https://pith.science/pith/CPUAAA3BQJCALV3334IZXMND55/state.json","well_known_bundle":"https://pith.science/.well-known/pith/CPUAAA3BQJCALV3334IZXMND55/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:CPUAAA3BQJCALV3334IZXMND55","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"e22ab944037155b7bbaf5430ca23ddfbb2af4f732bab7afeb62c38a8e893d1fe","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-09-23T09:42:30Z","title_canon_sha256":"95ed7899f9b5c43e2297edf395320060384faad3cd5e6c69c6a260ecec3f1052"},"schema_version":"1.0","source":{"id":"1409.6459","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.6459","created_at":"2026-05-18T02:18:51Z"},{"alias_kind":"arxiv_version","alias_value":"1409.6459v2","created_at":"2026-05-18T02:18:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.6459","created_at":"2026-05-18T02:18:51Z"},{"alias_kind":"pith_short_12","alias_value":"CPUAAA3BQJCA","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_16","alias_value":"CPUAAA3BQJCALV33","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_8","alias_value":"CPUAAA3B","created_at":"2026-05-18T12:28:22Z"}],"graph_snapshots":[{"event_id":"sha256:6cbe6f1269e14a3861193a8343905726be0ee6a32b13373e0ac61209ae20883d","target":"graph","created_at":"2026-05-18T02:18:51Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"Towards the goal of extracting the continuum properties, we have studied the Topological Charge Density Correlator (TCDC) and the Inverse Participation Ratio (IPR) for the topological charge density ($q(x)$) in SU(3) Lattice Yang-Mills theory for relatively small lattice spacings including some smaller than those explored before. With the help of recently proposed open boundary condition, it is possible to compute observables at a smaller lattice spacing since {\\em trapping problem} is absent. On the other hand, the reference energy scale provided by Wilson flow allows us to study their scalin","authors_text":"Abhishek Chowdhury, A. Harindranath, Jyotirmoy Maiti","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-09-23T09:42:30Z","title":"Correlation and localization properties of topological charge density and the pseudoscalar glueball mass in SU(3) lattice Yang-Mills theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.6459","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:51f479c65afbc9280e7d4b9a252ec72fdcf43f50aba57ea0647f0a4ebc6ab81d","target":"record","created_at":"2026-05-18T02:18:51Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"e22ab944037155b7bbaf5430ca23ddfbb2af4f732bab7afeb62c38a8e893d1fe","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-09-23T09:42:30Z","title_canon_sha256":"95ed7899f9b5c43e2297edf395320060384faad3cd5e6c69c6a260ecec3f1052"},"schema_version":"1.0","source":{"id":"1409.6459","kind":"arxiv","version":2}},"canonical_sha256":"13e8000361824405d77bdf119bb1a3ef52aa2f0afc61f8eefec69fa89791dbaa","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"13e8000361824405d77bdf119bb1a3ef52aa2f0afc61f8eefec69fa89791dbaa","first_computed_at":"2026-05-18T02:18:51.612979Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:18:51.612979Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"+geD6hRYYMtUmt6w3/GZlh00NnrYM9FmtvGButypGimPUnu9xwNGYpqwfCL+h4Loj/fZNFXPS7a/RbNySmkADw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:18:51.613562Z","signed_message":"canonical_sha256_bytes"},"source_id":"1409.6459","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:51f479c65afbc9280e7d4b9a252ec72fdcf43f50aba57ea0647f0a4ebc6ab81d","sha256:6cbe6f1269e14a3861193a8343905726be0ee6a32b13373e0ac61209ae20883d"],"state_sha256":"fefcb9eb36b367562dba1121fce69f2ed8d71f741f3d5da1ec053e7e5e5396fb"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"19kjQFo1LMXlNeO4od2G6SaAeixm5daFf26QhSNdsRJNhbJjXclPisgmOj9SFa5jgEn12Prfpw/vf2g3MDSZBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-29T14:50:01.683124Z","bundle_sha256":"bd072711254265748154b904b900c68788ff5faf6a043e3a5c0a28a8dca2f75c"}}