{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:O5SHIYNPKTN4BXJRQTPCAPEOBX","short_pith_number":"pith:O5SHIYNP","canonical_record":{"source":{"id":"1511.02039","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-11-06T11:41:38Z","cross_cats_sorted":[],"title_canon_sha256":"ef692c3acda290ead48f6e9d6b03e66f3e84082be50a525ea4ac7cf8c28d188e","abstract_canon_sha256":"202356233a7d0a9d67751d67f273dff29176a71228af2310303d27a449f59ee2"},"schema_version":"1.0"},"canonical_sha256":"77647461af54dbc0dd3184de203c8e0dde21726a70c040dfe8c4c44014969057","source":{"kind":"arxiv","id":"1511.02039","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1511.02039","created_at":"2026-05-18T01:26:57Z"},{"alias_kind":"arxiv_version","alias_value":"1511.02039v2","created_at":"2026-05-18T01:26:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.02039","created_at":"2026-05-18T01:26:57Z"},{"alias_kind":"pith_short_12","alias_value":"O5SHIYNPKTN4","created_at":"2026-05-18T12:29:34Z"},{"alias_kind":"pith_short_16","alias_value":"O5SHIYNPKTN4BXJR","created_at":"2026-05-18T12:29:34Z"},{"alias_kind":"pith_short_8","alias_value":"O5SHIYNP","created_at":"2026-05-18T12:29:34Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:O5SHIYNPKTN4BXJRQTPCAPEOBX","target":"record","payload":{"canonical_record":{"source":{"id":"1511.02039","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-11-06T11:41:38Z","cross_cats_sorted":[],"title_canon_sha256":"ef692c3acda290ead48f6e9d6b03e66f3e84082be50a525ea4ac7cf8c28d188e","abstract_canon_sha256":"202356233a7d0a9d67751d67f273dff29176a71228af2310303d27a449f59ee2"},"schema_version":"1.0"},"canonical_sha256":"77647461af54dbc0dd3184de203c8e0dde21726a70c040dfe8c4c44014969057","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:26:57.054679Z","signature_b64":"PLEVIf3lnjiU6NSdDM9yfN3nDq7vUlJhmm3c2XuTlboo9PwS/g5QADbuchKgcwBJnjQiUzOjYgJwxbhAaKg/BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"77647461af54dbc0dd3184de203c8e0dde21726a70c040dfe8c4c44014969057","last_reissued_at":"2026-05-18T01:26:57.054110Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:26:57.054110Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1511.02039","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":"2026-05-18T01:26:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0P1onGLIfQ5razY7gtKpJSkYNs5ZxmgjlZFu5tQGJ7v7ZnEHZ60IWBOI0gzkqgpOHx56crboTD9MHtxybEL/Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T11:31:04.796547Z"},"content_sha256":"5040f1c5be90071f940fbc65b194cc6bdb0aa99f4cf85389e86a188012bf45de","schema_version":"1.0","event_id":"sha256:5040f1c5be90071f940fbc65b194cc6bdb0aa99f4cf85389e86a188012bf45de"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:O5SHIYNPKTN4BXJRQTPCAPEOBX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dirac spectrum representation of Polyakov loop fluctuations in lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Chihiro Sasaki, Hideo Suganuma, Krzysztof Redlich, Takahiro M. Doi","submitted_at":"2015-11-06T11:41:38Z","abstract_excerpt":"Dirac spectrum representations of the Polyakov loop fluctuations are derived on the temporally odd-number lattice, where the temporal length is odd with the periodic boundary condition. We investigate the Polyakov loop fluctuations based on these analytical relations. It is semianalytically and numerically found that the low-lying Dirac eigenmodes have little contribution to the Polyakov loop fluctuations, which are sensitive probe for the quark deconfinement. Our results suggest no direct one-to-one corresponding between quark confinement and chiral symmetry breaking in QCD."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.02039","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":"2026-05-18T01:26:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tIFoy9UjLw9kSp0KSHjKNUCMm9S0eMjVuY9n5wKd9neGFWtM5cGlSAT9bmTq2rllDfzFNYR1FCU+QumzVcJWBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T11:31:04.796895Z"},"content_sha256":"91b80a74846b1170d9dadc88ba3072db350bc454da685d9ec8d89df8020525e9","schema_version":"1.0","event_id":"sha256:91b80a74846b1170d9dadc88ba3072db350bc454da685d9ec8d89df8020525e9"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/O5SHIYNPKTN4BXJRQTPCAPEOBX/bundle.json","state_url":"https://pith.science/pith/O5SHIYNPKTN4BXJRQTPCAPEOBX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/O5SHIYNPKTN4BXJRQTPCAPEOBX/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":"2026-05-28T11:31:04Z","links":{"resolver":"https://pith.science/pith/O5SHIYNPKTN4BXJRQTPCAPEOBX","bundle":"https://pith.science/pith/O5SHIYNPKTN4BXJRQTPCAPEOBX/bundle.json","state":"https://pith.science/pith/O5SHIYNPKTN4BXJRQTPCAPEOBX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/O5SHIYNPKTN4BXJRQTPCAPEOBX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:O5SHIYNPKTN4BXJRQTPCAPEOBX","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":"202356233a7d0a9d67751d67f273dff29176a71228af2310303d27a449f59ee2","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-11-06T11:41:38Z","title_canon_sha256":"ef692c3acda290ead48f6e9d6b03e66f3e84082be50a525ea4ac7cf8c28d188e"},"schema_version":"1.0","source":{"id":"1511.02039","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1511.02039","created_at":"2026-05-18T01:26:57Z"},{"alias_kind":"arxiv_version","alias_value":"1511.02039v2","created_at":"2026-05-18T01:26:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.02039","created_at":"2026-05-18T01:26:57Z"},{"alias_kind":"pith_short_12","alias_value":"O5SHIYNPKTN4","created_at":"2026-05-18T12:29:34Z"},{"alias_kind":"pith_short_16","alias_value":"O5SHIYNPKTN4BXJR","created_at":"2026-05-18T12:29:34Z"},{"alias_kind":"pith_short_8","alias_value":"O5SHIYNP","created_at":"2026-05-18T12:29:34Z"}],"graph_snapshots":[{"event_id":"sha256:91b80a74846b1170d9dadc88ba3072db350bc454da685d9ec8d89df8020525e9","target":"graph","created_at":"2026-05-18T01:26:57Z","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":"Dirac spectrum representations of the Polyakov loop fluctuations are derived on the temporally odd-number lattice, where the temporal length is odd with the periodic boundary condition. We investigate the Polyakov loop fluctuations based on these analytical relations. It is semianalytically and numerically found that the low-lying Dirac eigenmodes have little contribution to the Polyakov loop fluctuations, which are sensitive probe for the quark deconfinement. Our results suggest no direct one-to-one corresponding between quark confinement and chiral symmetry breaking in QCD.","authors_text":"Chihiro Sasaki, Hideo Suganuma, Krzysztof Redlich, Takahiro M. Doi","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-11-06T11:41:38Z","title":"Dirac spectrum representation of Polyakov loop fluctuations in lattice QCD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.02039","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":"sha256:5040f1c5be90071f940fbc65b194cc6bdb0aa99f4cf85389e86a188012bf45de","target":"record","created_at":"2026-05-18T01:26:57Z","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":"202356233a7d0a9d67751d67f273dff29176a71228af2310303d27a449f59ee2","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-11-06T11:41:38Z","title_canon_sha256":"ef692c3acda290ead48f6e9d6b03e66f3e84082be50a525ea4ac7cf8c28d188e"},"schema_version":"1.0","source":{"id":"1511.02039","kind":"arxiv","version":2}},"canonical_sha256":"77647461af54dbc0dd3184de203c8e0dde21726a70c040dfe8c4c44014969057","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"77647461af54dbc0dd3184de203c8e0dde21726a70c040dfe8c4c44014969057","first_computed_at":"2026-05-18T01:26:57.054110Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:26:57.054110Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"PLEVIf3lnjiU6NSdDM9yfN3nDq7vUlJhmm3c2XuTlboo9PwS/g5QADbuchKgcwBJnjQiUzOjYgJwxbhAaKg/BA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:26:57.054679Z","signed_message":"canonical_sha256_bytes"},"source_id":"1511.02039","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5040f1c5be90071f940fbc65b194cc6bdb0aa99f4cf85389e86a188012bf45de","sha256:91b80a74846b1170d9dadc88ba3072db350bc454da685d9ec8d89df8020525e9"],"state_sha256":"e98e71491ad9dbc7084528c322cda8223b9f10c7d25a5613db85b18dcaa5e598"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OE7zOFTRsqlcRuiJ+B+ZgQdzTDeqvvK387Fd53sgaz/6dT5ThmbiOFFjTS1nSK812B04tMW/2T6GGpCMIAm+Cw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T11:31:04.798883Z","bundle_sha256":"8371a4fc5c8e094d06fb9f0299a2bbd08fd06185cd31b660f1eed639df4adef3"}}