{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:6PC4RQA4T7DBQWEAGXVDT7VMLX","short_pith_number":"pith:6PC4RQA4","canonical_record":{"source":{"id":"2210.15789","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2022-10-27T22:19:08Z","cross_cats_sorted":[],"title_canon_sha256":"a80a53579b21430154ecb77e918e0dcbc2bef00d6f406f0f15a4899852805797","abstract_canon_sha256":"29db13c59f798c9543ff7878f44805f841ee1e4943cf6caff9cacc7559a29094"},"schema_version":"1.0"},"canonical_sha256":"f3c5c8c01c9fc618588035ea39feac5dfe40b3c5ce2688f8e320788df896240d","source":{"kind":"arxiv","id":"2210.15789","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2210.15789","created_at":"2026-07-05T06:15:43Z"},{"alias_kind":"arxiv_version","alias_value":"2210.15789v2","created_at":"2026-07-05T06:15:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2210.15789","created_at":"2026-07-05T06:15:43Z"},{"alias_kind":"pith_short_12","alias_value":"6PC4RQA4T7DB","created_at":"2026-07-05T06:15:43Z"},{"alias_kind":"pith_short_16","alias_value":"6PC4RQA4T7DBQWEA","created_at":"2026-07-05T06:15:43Z"},{"alias_kind":"pith_short_8","alias_value":"6PC4RQA4","created_at":"2026-07-05T06:15:43Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:6PC4RQA4T7DBQWEAGXVDT7VMLX","target":"record","payload":{"canonical_record":{"source":{"id":"2210.15789","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2022-10-27T22:19:08Z","cross_cats_sorted":[],"title_canon_sha256":"a80a53579b21430154ecb77e918e0dcbc2bef00d6f406f0f15a4899852805797","abstract_canon_sha256":"29db13c59f798c9543ff7878f44805f841ee1e4943cf6caff9cacc7559a29094"},"schema_version":"1.0"},"canonical_sha256":"f3c5c8c01c9fc618588035ea39feac5dfe40b3c5ce2688f8e320788df896240d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:15:43.560031Z","signature_b64":"yl4EBWgAUAg+scCPgSRGJhWE3Po0UdKMjj8/y3DarKbaO2OYKQ5ApXmbSsx6xdC60cGlw+dX5Yri18i8ERnLBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f3c5c8c01c9fc618588035ea39feac5dfe40b3c5ce2688f8e320788df896240d","last_reissued_at":"2026-07-05T06:15:43.559522Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:15:43.559522Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2210.15789","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":"2026-07-05T06:15:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"joOyCrDK6omB1wdhp0RqLtkDjEqXJkpTuFVUC5R7ABycaDl9iMkRiUJQsLYbBLevJBSGPREZznzp1yooJqxcBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-09T18:30:26.052345Z"},"content_sha256":"197c3f0ed88dfdb4d90d30e074c893e7ed1361509abbbcacbcfcd901a1e19fa1","schema_version":"1.0","event_id":"sha256:197c3f0ed88dfdb4d90d30e074c893e7ed1361509abbbcacbcfcd901a1e19fa1"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:6PC4RQA4T7DBQWEAGXVDT7VMLX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Large-time correlation functions in bosonic lattice field theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Cagin Yunus, William Detmold","submitted_at":"2022-10-27T22:19:08Z","abstract_excerpt":"Large-time correlation functions have a pivotal role in extracting particle masses from Euclidean lattice field theory calculations, however little is known about the statistical properties of these quantities. In this work, the asymptotic form of the distributions of the correlation functions at vanishing momentum is determined for bosonic interacting lattice field theories with a unique gapped vacuum. It is demonstrated that the deviations from the asymptotic form at large Euclidean times can be utilized to determine the spectrum of the theory."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2210.15789","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2210.15789/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-05T06:15:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"t3LTm3JVrtBDlQilezu/83UJCdfZHH+2rg2+pigWjimkWS1nCZeQOeqI0lc3Azublwwm+JTfgrlBHXLIQbi3Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-09T18:30:26.053053Z"},"content_sha256":"083d1e0ddc7a306f07ec2fee6964b43e3320c002ca4faf3f7d695df989dfba3a","schema_version":"1.0","event_id":"sha256:083d1e0ddc7a306f07ec2fee6964b43e3320c002ca4faf3f7d695df989dfba3a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6PC4RQA4T7DBQWEAGXVDT7VMLX/bundle.json","state_url":"https://pith.science/pith/6PC4RQA4T7DBQWEAGXVDT7VMLX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6PC4RQA4T7DBQWEAGXVDT7VMLX/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":"2026-08-09T18:30:26Z","links":{"resolver":"https://pith.science/pith/6PC4RQA4T7DBQWEAGXVDT7VMLX","bundle":"https://pith.science/pith/6PC4RQA4T7DBQWEAGXVDT7VMLX/bundle.json","state":"https://pith.science/pith/6PC4RQA4T7DBQWEAGXVDT7VMLX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6PC4RQA4T7DBQWEAGXVDT7VMLX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:6PC4RQA4T7DBQWEAGXVDT7VMLX","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":"29db13c59f798c9543ff7878f44805f841ee1e4943cf6caff9cacc7559a29094","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2022-10-27T22:19:08Z","title_canon_sha256":"a80a53579b21430154ecb77e918e0dcbc2bef00d6f406f0f15a4899852805797"},"schema_version":"1.0","source":{"id":"2210.15789","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2210.15789","created_at":"2026-07-05T06:15:43Z"},{"alias_kind":"arxiv_version","alias_value":"2210.15789v2","created_at":"2026-07-05T06:15:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2210.15789","created_at":"2026-07-05T06:15:43Z"},{"alias_kind":"pith_short_12","alias_value":"6PC4RQA4T7DB","created_at":"2026-07-05T06:15:43Z"},{"alias_kind":"pith_short_16","alias_value":"6PC4RQA4T7DBQWEA","created_at":"2026-07-05T06:15:43Z"},{"alias_kind":"pith_short_8","alias_value":"6PC4RQA4","created_at":"2026-07-05T06:15:43Z"}],"graph_snapshots":[{"event_id":"sha256:083d1e0ddc7a306f07ec2fee6964b43e3320c002ca4faf3f7d695df989dfba3a","target":"graph","created_at":"2026-07-05T06:15:43Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2210.15789/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Large-time correlation functions have a pivotal role in extracting particle masses from Euclidean lattice field theory calculations, however little is known about the statistical properties of these quantities. In this work, the asymptotic form of the distributions of the correlation functions at vanishing momentum is determined for bosonic interacting lattice field theories with a unique gapped vacuum. It is demonstrated that the deviations from the asymptotic form at large Euclidean times can be utilized to determine the spectrum of the theory.","authors_text":"Cagin Yunus, William Detmold","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2022-10-27T22:19:08Z","title":"Large-time correlation functions in bosonic lattice field theories"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2210.15789","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":"sha256:197c3f0ed88dfdb4d90d30e074c893e7ed1361509abbbcacbcfcd901a1e19fa1","target":"record","created_at":"2026-07-05T06:15:43Z","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":"29db13c59f798c9543ff7878f44805f841ee1e4943cf6caff9cacc7559a29094","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2022-10-27T22:19:08Z","title_canon_sha256":"a80a53579b21430154ecb77e918e0dcbc2bef00d6f406f0f15a4899852805797"},"schema_version":"1.0","source":{"id":"2210.15789","kind":"arxiv","version":2}},"canonical_sha256":"f3c5c8c01c9fc618588035ea39feac5dfe40b3c5ce2688f8e320788df896240d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f3c5c8c01c9fc618588035ea39feac5dfe40b3c5ce2688f8e320788df896240d","first_computed_at":"2026-07-05T06:15:43.559522Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:15:43.559522Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"yl4EBWgAUAg+scCPgSRGJhWE3Po0UdKMjj8/y3DarKbaO2OYKQ5ApXmbSsx6xdC60cGlw+dX5Yri18i8ERnLBg==","signature_status":"signed_v1","signed_at":"2026-07-05T06:15:43.560031Z","signed_message":"canonical_sha256_bytes"},"source_id":"2210.15789","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:197c3f0ed88dfdb4d90d30e074c893e7ed1361509abbbcacbcfcd901a1e19fa1","sha256:083d1e0ddc7a306f07ec2fee6964b43e3320c002ca4faf3f7d695df989dfba3a"],"state_sha256":"9b8404b1c6e765d98610472812a617c4e11ed522e95637169820b344b6430c4f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Gnvxz//Xww5bxt9kszdLqr2dpt2yVB8yVrEjqaFpjluBfEmt/I7BmB3k3gEyogTgN6sZzel4YopWTrNPkyBMDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-09T18:30:26.057673Z","bundle_sha256":"5ce4d72b127d0a91604d18e696ad4a22024be6b81c494eed18e946c9d39c63a2"}}