{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:YHFMWAWNZVPKJB2MCRJOKJNZ4Q","short_pith_number":"pith:YHFMWAWN","canonical_record":{"source":{"id":"1808.05227","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-08-15T18:00:03Z","cross_cats_sorted":[],"title_canon_sha256":"4bea7682168ff745abaa6948ce11117c830a1db90f1ed9aa404e2102d0af24b5","abstract_canon_sha256":"8c35bdc106a4e55ab79ff05fd6ae2a195e0a50ca52099770aacf8e822129c8b1"},"schema_version":"1.0"},"canonical_sha256":"c1cacb02cdcd5ea4874c1452e525b9e4038effff6868d2c0590cff78aeb2f529","source":{"kind":"arxiv","id":"1808.05227","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1808.05227","created_at":"2026-07-05T00:57:21Z"},{"alias_kind":"arxiv_version","alias_value":"1808.05227v3","created_at":"2026-07-05T00:57:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1808.05227","created_at":"2026-07-05T00:57:21Z"},{"alias_kind":"pith_short_12","alias_value":"YHFMWAWNZVPK","created_at":"2026-07-05T00:57:21Z"},{"alias_kind":"pith_short_16","alias_value":"YHFMWAWNZVPKJB2M","created_at":"2026-07-05T00:57:21Z"},{"alias_kind":"pith_short_8","alias_value":"YHFMWAWN","created_at":"2026-07-05T00:57:21Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:YHFMWAWNZVPKJB2MCRJOKJNZ4Q","target":"record","payload":{"canonical_record":{"source":{"id":"1808.05227","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-08-15T18:00:03Z","cross_cats_sorted":[],"title_canon_sha256":"4bea7682168ff745abaa6948ce11117c830a1db90f1ed9aa404e2102d0af24b5","abstract_canon_sha256":"8c35bdc106a4e55ab79ff05fd6ae2a195e0a50ca52099770aacf8e822129c8b1"},"schema_version":"1.0"},"canonical_sha256":"c1cacb02cdcd5ea4874c1452e525b9e4038effff6868d2c0590cff78aeb2f529","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:57:21.674137Z","signature_b64":"Z6zx6q1THZF/2yVinDft1LryRq0YgyuNvwe/No7Hk2Y8acPXgRcligVaBnikOMtABGJ0LxxpxON4M2fcrVcRBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c1cacb02cdcd5ea4874c1452e525b9e4038effff6868d2c0590cff78aeb2f529","last_reissued_at":"2026-07-05T00:57:21.673717Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:57:21.673717Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1808.05227","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T00:57:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sQazoDvTucDac2OZocPCoShNSynDcyOFChFxsQdLsGitqw40OCw79TKR5okpQgYybQXNTWSs7JTqYTaAb6h0DA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-10T08:45:24.257963Z"},"content_sha256":"a202104e281d3580540facaf2e38766b9172a8cd5126d54eb9380183836af555","schema_version":"1.0","event_id":"sha256:a202104e281d3580540facaf2e38766b9172a8cd5126d54eb9380183836af555"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:YHFMWAWNZVPKJB2MCRJOKJNZ4Q","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Nonperturbative properties of Yang-Mills theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Markus Q. Huber","submitted_at":"2018-08-15T18:00:03Z","abstract_excerpt":"Yang-Mills theories are an important building block of the standard model and in particular of quantum chromodynamics. Its correlation functions describe the behavior of its elementary particles, the gauge bosons. In quantum chromodynamics, the correlation functions of the gluons are basic ingredients for calculations of hadrons from bound state equations or properties of its phase diagram with functional methods. Correlation functions of gluons are defined only in a gauge fixed setting. The focus of many studies is the Landau gauge which has some features that alleviate calculations. I discus"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1808.05227","kind":"arxiv","version":3},"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/1808.05227/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":"2026-07-05T00:57:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dmwLkBEWjoRdSm0kDRMt3kyrKVVu3D2BufZsZXN99nZ6JvQGe9RVgJ7H+o0tD0rII9hgPndBccDkUa2cPmgjCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-10T08:45:24.258766Z"},"content_sha256":"f3d75941020eda35018f7c7ae020cd29689ce6d6ec69907cdabcd989a9239e7b","schema_version":"1.0","event_id":"sha256:f3d75941020eda35018f7c7ae020cd29689ce6d6ec69907cdabcd989a9239e7b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YHFMWAWNZVPKJB2MCRJOKJNZ4Q/bundle.json","state_url":"https://pith.science/pith/YHFMWAWNZVPKJB2MCRJOKJNZ4Q/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YHFMWAWNZVPKJB2MCRJOKJNZ4Q/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":"2026-08-10T08:45:24Z","links":{"resolver":"https://pith.science/pith/YHFMWAWNZVPKJB2MCRJOKJNZ4Q","bundle":"https://pith.science/pith/YHFMWAWNZVPKJB2MCRJOKJNZ4Q/bundle.json","state":"https://pith.science/pith/YHFMWAWNZVPKJB2MCRJOKJNZ4Q/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YHFMWAWNZVPKJB2MCRJOKJNZ4Q/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:YHFMWAWNZVPKJB2MCRJOKJNZ4Q","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":"8c35bdc106a4e55ab79ff05fd6ae2a195e0a50ca52099770aacf8e822129c8b1","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-08-15T18:00:03Z","title_canon_sha256":"4bea7682168ff745abaa6948ce11117c830a1db90f1ed9aa404e2102d0af24b5"},"schema_version":"1.0","source":{"id":"1808.05227","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1808.05227","created_at":"2026-07-05T00:57:21Z"},{"alias_kind":"arxiv_version","alias_value":"1808.05227v3","created_at":"2026-07-05T00:57:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1808.05227","created_at":"2026-07-05T00:57:21Z"},{"alias_kind":"pith_short_12","alias_value":"YHFMWAWNZVPK","created_at":"2026-07-05T00:57:21Z"},{"alias_kind":"pith_short_16","alias_value":"YHFMWAWNZVPKJB2M","created_at":"2026-07-05T00:57:21Z"},{"alias_kind":"pith_short_8","alias_value":"YHFMWAWN","created_at":"2026-07-05T00:57:21Z"}],"graph_snapshots":[{"event_id":"sha256:f3d75941020eda35018f7c7ae020cd29689ce6d6ec69907cdabcd989a9239e7b","target":"graph","created_at":"2026-07-05T00:57:21Z","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/1808.05227/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Yang-Mills theories are an important building block of the standard model and in particular of quantum chromodynamics. Its correlation functions describe the behavior of its elementary particles, the gauge bosons. In quantum chromodynamics, the correlation functions of the gluons are basic ingredients for calculations of hadrons from bound state equations or properties of its phase diagram with functional methods. Correlation functions of gluons are defined only in a gauge fixed setting. The focus of many studies is the Landau gauge which has some features that alleviate calculations. I discus","authors_text":"Markus Q. Huber","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-08-15T18:00:03Z","title":"Nonperturbative properties of Yang-Mills theories"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1808.05227","kind":"arxiv","version":3},"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:a202104e281d3580540facaf2e38766b9172a8cd5126d54eb9380183836af555","target":"record","created_at":"2026-07-05T00:57:21Z","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":"8c35bdc106a4e55ab79ff05fd6ae2a195e0a50ca52099770aacf8e822129c8b1","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-08-15T18:00:03Z","title_canon_sha256":"4bea7682168ff745abaa6948ce11117c830a1db90f1ed9aa404e2102d0af24b5"},"schema_version":"1.0","source":{"id":"1808.05227","kind":"arxiv","version":3}},"canonical_sha256":"c1cacb02cdcd5ea4874c1452e525b9e4038effff6868d2c0590cff78aeb2f529","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c1cacb02cdcd5ea4874c1452e525b9e4038effff6868d2c0590cff78aeb2f529","first_computed_at":"2026-07-05T00:57:21.673717Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T00:57:21.673717Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Z6zx6q1THZF/2yVinDft1LryRq0YgyuNvwe/No7Hk2Y8acPXgRcligVaBnikOMtABGJ0LxxpxON4M2fcrVcRBw==","signature_status":"signed_v1","signed_at":"2026-07-05T00:57:21.674137Z","signed_message":"canonical_sha256_bytes"},"source_id":"1808.05227","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a202104e281d3580540facaf2e38766b9172a8cd5126d54eb9380183836af555","sha256:f3d75941020eda35018f7c7ae020cd29689ce6d6ec69907cdabcd989a9239e7b"],"state_sha256":"64e213ef7a653a5a86eae63cb963b7fd3bdbbc21604f07ff16ee44aca9d6effe"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hqVnCiiNmsvjIS/4K3a4jjgCujnUGjLexQoidF3CMtrdgfIG3qMqP+DaI8VhbdWtobAgl7Dwe3LcKkLkoiPCDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-10T08:45:24.264503Z","bundle_sha256":"91ff1c87d49ec0d566f29f31e628df7a89388da41adef48e82589b1f6b87df28"}}