{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:J4VYZJHUO6IMI2ER52BW5W7XTD","short_pith_number":"pith:J4VYZJHU","canonical_record":{"source":{"id":"1505.05752","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-05-21T14:39:28Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"7c312041a5df880a4c5f358ea4591993e345937c73711abad938e5fbdd72524e","abstract_canon_sha256":"d6fdb7a58239f1b20f5030a3c8c4bb2cb8eebf6f8f6ef43b586ee6c4cb1b2e73"},"schema_version":"1.0"},"canonical_sha256":"4f2b8ca4f47790c46891ee836edbf798d4c3ffdd72cfcc552c81940ba6550e17","source":{"kind":"arxiv","id":"1505.05752","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1505.05752","created_at":"2026-05-18T01:27:38Z"},{"alias_kind":"arxiv_version","alias_value":"1505.05752v2","created_at":"2026-05-18T01:27:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1505.05752","created_at":"2026-05-18T01:27:38Z"},{"alias_kind":"pith_short_12","alias_value":"J4VYZJHUO6IM","created_at":"2026-05-18T12:29:27Z"},{"alias_kind":"pith_short_16","alias_value":"J4VYZJHUO6IMI2ER","created_at":"2026-05-18T12:29:27Z"},{"alias_kind":"pith_short_8","alias_value":"J4VYZJHU","created_at":"2026-05-18T12:29:27Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:J4VYZJHUO6IMI2ER52BW5W7XTD","target":"record","payload":{"canonical_record":{"source":{"id":"1505.05752","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-05-21T14:39:28Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"7c312041a5df880a4c5f358ea4591993e345937c73711abad938e5fbdd72524e","abstract_canon_sha256":"d6fdb7a58239f1b20f5030a3c8c4bb2cb8eebf6f8f6ef43b586ee6c4cb1b2e73"},"schema_version":"1.0"},"canonical_sha256":"4f2b8ca4f47790c46891ee836edbf798d4c3ffdd72cfcc552c81940ba6550e17","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:27:38.343716Z","signature_b64":"VaEcfKFOtmxWjTDO+4NsVcbpbBNMQE54TRx8u2yBMc8bbX1+Sypy9Xx4Q5dcewCbaIplW+/R0owQy1E24rONAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4f2b8ca4f47790c46891ee836edbf798d4c3ffdd72cfcc552c81940ba6550e17","last_reissued_at":"2026-05-18T01:27:38.343112Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:27:38.343112Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1505.05752","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":"2026-05-18T01:27:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XbB8abgz6ICOKufW7nvnZuBbYyTjuLHDpnNQZU6mnlT0z2G+HNnEDiLRLQlqqVstVe7MfDdVJh6IVOsZBoR1Bw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T09:19:44.588939Z"},"content_sha256":"8281db8d7d0eaa2825b0d1e5728a5619378ceef62bba1bca8cfa3ef654be1133","schema_version":"1.0","event_id":"sha256:8281db8d7d0eaa2825b0d1e5728a5619378ceef62bba1bca8cfa3ef654be1133"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:J4VYZJHUO6IMI2ER52BW5W7XTD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Polyakov loop fluctuations in Dirac eigenmode expansion","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"Chihiro Sasaki, Hideo Suganuma, Krzysztof Redlich, Takahiro M. Doi","submitted_at":"2015-05-21T14:39:28Z","abstract_excerpt":"We investigate correlations of the Polyakov loop fluctuations with eigenmodes of the lattice Dirac operator. Their analytic relations are derived on the temporally odd-number size lattice with the normal non-twisted periodic boundary condition for the link-variables. We find that the low-lying Dirac modes yield negligible contributions to the Polyakov loop fluctuations. This property is confirmed to be valid in confined and deconfined phase by numerical simulations in SU(3) quenched QCD. These results indicate that there is no direct, one-to-one correspondence between confinement and chiral sy"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.05752","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":"2026-05-18T01:27:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"E8Z9wGGklZZ8jUZCTcLUn5d8+3A5AdoFFRf0hg0m+4GnFdP+A4hUPt8HHWnvO1EXyCV/9w67h3Q2WheSkgYwDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T09:19:44.589290Z"},"content_sha256":"e1b627a3652ff734984cbaf108f7bea5d419c2eaef7406d524cb8eb3c5403d0a","schema_version":"1.0","event_id":"sha256:e1b627a3652ff734984cbaf108f7bea5d419c2eaef7406d524cb8eb3c5403d0a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/J4VYZJHUO6IMI2ER52BW5W7XTD/bundle.json","state_url":"https://pith.science/pith/J4VYZJHUO6IMI2ER52BW5W7XTD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/J4VYZJHUO6IMI2ER52BW5W7XTD/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":"2026-06-03T09:19:44Z","links":{"resolver":"https://pith.science/pith/J4VYZJHUO6IMI2ER52BW5W7XTD","bundle":"https://pith.science/pith/J4VYZJHUO6IMI2ER52BW5W7XTD/bundle.json","state":"https://pith.science/pith/J4VYZJHUO6IMI2ER52BW5W7XTD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/J4VYZJHUO6IMI2ER52BW5W7XTD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:J4VYZJHUO6IMI2ER52BW5W7XTD","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":"d6fdb7a58239f1b20f5030a3c8c4bb2cb8eebf6f8f6ef43b586ee6c4cb1b2e73","cross_cats_sorted":["hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-05-21T14:39:28Z","title_canon_sha256":"7c312041a5df880a4c5f358ea4591993e345937c73711abad938e5fbdd72524e"},"schema_version":"1.0","source":{"id":"1505.05752","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1505.05752","created_at":"2026-05-18T01:27:38Z"},{"alias_kind":"arxiv_version","alias_value":"1505.05752v2","created_at":"2026-05-18T01:27:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1505.05752","created_at":"2026-05-18T01:27:38Z"},{"alias_kind":"pith_short_12","alias_value":"J4VYZJHUO6IM","created_at":"2026-05-18T12:29:27Z"},{"alias_kind":"pith_short_16","alias_value":"J4VYZJHUO6IMI2ER","created_at":"2026-05-18T12:29:27Z"},{"alias_kind":"pith_short_8","alias_value":"J4VYZJHU","created_at":"2026-05-18T12:29:27Z"}],"graph_snapshots":[{"event_id":"sha256:e1b627a3652ff734984cbaf108f7bea5d419c2eaef7406d524cb8eb3c5403d0a","target":"graph","created_at":"2026-05-18T01:27:38Z","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":"We investigate correlations of the Polyakov loop fluctuations with eigenmodes of the lattice Dirac operator. Their analytic relations are derived on the temporally odd-number size lattice with the normal non-twisted periodic boundary condition for the link-variables. We find that the low-lying Dirac modes yield negligible contributions to the Polyakov loop fluctuations. This property is confirmed to be valid in confined and deconfined phase by numerical simulations in SU(3) quenched QCD. These results indicate that there is no direct, one-to-one correspondence between confinement and chiral sy","authors_text":"Chihiro Sasaki, Hideo Suganuma, Krzysztof Redlich, Takahiro M. Doi","cross_cats":["hep-ph","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-05-21T14:39:28Z","title":"Polyakov loop fluctuations in Dirac eigenmode expansion"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.05752","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":"sha256:8281db8d7d0eaa2825b0d1e5728a5619378ceef62bba1bca8cfa3ef654be1133","target":"record","created_at":"2026-05-18T01:27:38Z","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":"d6fdb7a58239f1b20f5030a3c8c4bb2cb8eebf6f8f6ef43b586ee6c4cb1b2e73","cross_cats_sorted":["hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-05-21T14:39:28Z","title_canon_sha256":"7c312041a5df880a4c5f358ea4591993e345937c73711abad938e5fbdd72524e"},"schema_version":"1.0","source":{"id":"1505.05752","kind":"arxiv","version":2}},"canonical_sha256":"4f2b8ca4f47790c46891ee836edbf798d4c3ffdd72cfcc552c81940ba6550e17","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4f2b8ca4f47790c46891ee836edbf798d4c3ffdd72cfcc552c81940ba6550e17","first_computed_at":"2026-05-18T01:27:38.343112Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:27:38.343112Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"VaEcfKFOtmxWjTDO+4NsVcbpbBNMQE54TRx8u2yBMc8bbX1+Sypy9Xx4Q5dcewCbaIplW+/R0owQy1E24rONAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:27:38.343716Z","signed_message":"canonical_sha256_bytes"},"source_id":"1505.05752","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8281db8d7d0eaa2825b0d1e5728a5619378ceef62bba1bca8cfa3ef654be1133","sha256:e1b627a3652ff734984cbaf108f7bea5d419c2eaef7406d524cb8eb3c5403d0a"],"state_sha256":"6c04cdb62f33f1a837107aadfc0bf42781e45487a1edc7d49f14b7c177876e8f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DHUFCNR0ADbBhcWDc6PJr4GjTai6u3ll9MD/R81wm0Youkn+X+p9kRQq7kxdM9Qjq+MSzpdNy8SSKra5jM/vDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T09:19:44.591362Z","bundle_sha256":"8477966b3396c9eb7a427c700b1938f7a5618329263b02062af229b400304619"}}