{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:MQS3KXAGNOYUVMPRCJAXQUPHWI","short_pith_number":"pith:MQS3KXAG","canonical_record":{"source":{"id":"1401.1192","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-01-06T20:37:49Z","cross_cats_sorted":[],"title_canon_sha256":"a056b7e82f2466cab47a12d4a123f24fe0fb1afe17418247cdbdcb12386271f5","abstract_canon_sha256":"75acdf75555de48e763b038ae70a699f77d1a171f6d4340b07a5281229fb279e"},"schema_version":"1.0"},"canonical_sha256":"6425b55c066bb14ab1f112417851e7b215675d33a259bd067e91d93ef76a5359","source":{"kind":"arxiv","id":"1401.1192","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1401.1192","created_at":"2026-05-18T02:44:00Z"},{"alias_kind":"arxiv_version","alias_value":"1401.1192v2","created_at":"2026-05-18T02:44:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.1192","created_at":"2026-05-18T02:44:00Z"},{"alias_kind":"pith_short_12","alias_value":"MQS3KXAGNOYU","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"MQS3KXAGNOYUVMPR","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"MQS3KXAG","created_at":"2026-05-18T12:28:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:MQS3KXAGNOYUVMPRCJAXQUPHWI","target":"record","payload":{"canonical_record":{"source":{"id":"1401.1192","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-01-06T20:37:49Z","cross_cats_sorted":[],"title_canon_sha256":"a056b7e82f2466cab47a12d4a123f24fe0fb1afe17418247cdbdcb12386271f5","abstract_canon_sha256":"75acdf75555de48e763b038ae70a699f77d1a171f6d4340b07a5281229fb279e"},"schema_version":"1.0"},"canonical_sha256":"6425b55c066bb14ab1f112417851e7b215675d33a259bd067e91d93ef76a5359","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:44:00.517577Z","signature_b64":"R6HiP4hZr2FOrAfdkRuzzP5+q76FCQK2seH2YOuwY7dmRPx6aK3f9JzlZ0WQwtMoZlEvnL20Ok94DVx+Ep8/CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6425b55c066bb14ab1f112417851e7b215675d33a259bd067e91d93ef76a5359","last_reissued_at":"2026-05-18T02:44:00.517037Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:44:00.517037Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1401.1192","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":"2026-05-18T02:44:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4mUuB2L68BTNPOUgp/7wAYJQe0UQ9eimOUM73XFuSJ0FLugGeMKfduXbskfcN8tKayJaKdRMKwr8vIX1P3SvAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T14:31:45.209464Z"},"content_sha256":"69770a54f2d44d62b42274328b6e98c69735732a1cf2fbcd5c922d07c0501b76","schema_version":"1.0","event_id":"sha256:69770a54f2d44d62b42274328b6e98c69735732a1cf2fbcd5c922d07c0501b76"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:MQS3KXAGNOYUVMPRCJAXQUPHWI","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Gluon Propagator in Fractional Analytic Perturbation Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Cesar Ayala, Gorazd Cveti\\v{c}, Pedro Allendes","submitted_at":"2014-01-06T20:37:49Z","abstract_excerpt":"We consider the gluon propagator in the Landau gauge at low spacelike momenta and with the dressing function $Z(Q^2)$ at the two-loop order. We incorporate the nonperturbative effects by making the (noninteger) powers of the QCD coupling in the dressing function $Z(Q^2)$ analytic (holomorphic) via the Fractional Analytic Perturbation Theory (FAPT) model, and simultaneously introducing the gluon dynamical mass in the propagator as motivated by the previous analyses of the Dyson-Schwinger equations. The obtained propagator has behavior compatible with the unquenched lattice data ($N_f=2+1$) at l"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.1192","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":"2026-05-18T02:44:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/pIK1VguMEp/XYsYWwBTgSr+BLQnkL+jf42IaCH8Lg5CaPc1tbp94cmySpF+GoETCuxKhyOQ2zERG5qgCnqDCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T14:31:45.210124Z"},"content_sha256":"d3cb8e2ae83bcfabb32fd2376b948e8cb768034b92baf31c994c867a71c6e365","schema_version":"1.0","event_id":"sha256:d3cb8e2ae83bcfabb32fd2376b948e8cb768034b92baf31c994c867a71c6e365"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MQS3KXAGNOYUVMPRCJAXQUPHWI/bundle.json","state_url":"https://pith.science/pith/MQS3KXAGNOYUVMPRCJAXQUPHWI/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MQS3KXAGNOYUVMPRCJAXQUPHWI/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":"2026-06-02T14:31:45Z","links":{"resolver":"https://pith.science/pith/MQS3KXAGNOYUVMPRCJAXQUPHWI","bundle":"https://pith.science/pith/MQS3KXAGNOYUVMPRCJAXQUPHWI/bundle.json","state":"https://pith.science/pith/MQS3KXAGNOYUVMPRCJAXQUPHWI/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MQS3KXAGNOYUVMPRCJAXQUPHWI/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:MQS3KXAGNOYUVMPRCJAXQUPHWI","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":"75acdf75555de48e763b038ae70a699f77d1a171f6d4340b07a5281229fb279e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-01-06T20:37:49Z","title_canon_sha256":"a056b7e82f2466cab47a12d4a123f24fe0fb1afe17418247cdbdcb12386271f5"},"schema_version":"1.0","source":{"id":"1401.1192","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1401.1192","created_at":"2026-05-18T02:44:00Z"},{"alias_kind":"arxiv_version","alias_value":"1401.1192v2","created_at":"2026-05-18T02:44:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.1192","created_at":"2026-05-18T02:44:00Z"},{"alias_kind":"pith_short_12","alias_value":"MQS3KXAGNOYU","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"MQS3KXAGNOYUVMPR","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"MQS3KXAG","created_at":"2026-05-18T12:28:38Z"}],"graph_snapshots":[{"event_id":"sha256:d3cb8e2ae83bcfabb32fd2376b948e8cb768034b92baf31c994c867a71c6e365","target":"graph","created_at":"2026-05-18T02:44:00Z","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 consider the gluon propagator in the Landau gauge at low spacelike momenta and with the dressing function $Z(Q^2)$ at the two-loop order. We incorporate the nonperturbative effects by making the (noninteger) powers of the QCD coupling in the dressing function $Z(Q^2)$ analytic (holomorphic) via the Fractional Analytic Perturbation Theory (FAPT) model, and simultaneously introducing the gluon dynamical mass in the propagator as motivated by the previous analyses of the Dyson-Schwinger equations. The obtained propagator has behavior compatible with the unquenched lattice data ($N_f=2+1$) at l","authors_text":"Cesar Ayala, Gorazd Cveti\\v{c}, Pedro Allendes","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-01-06T20:37:49Z","title":"Gluon Propagator in Fractional Analytic Perturbation Theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.1192","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":"sha256:69770a54f2d44d62b42274328b6e98c69735732a1cf2fbcd5c922d07c0501b76","target":"record","created_at":"2026-05-18T02:44:00Z","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":"75acdf75555de48e763b038ae70a699f77d1a171f6d4340b07a5281229fb279e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-01-06T20:37:49Z","title_canon_sha256":"a056b7e82f2466cab47a12d4a123f24fe0fb1afe17418247cdbdcb12386271f5"},"schema_version":"1.0","source":{"id":"1401.1192","kind":"arxiv","version":2}},"canonical_sha256":"6425b55c066bb14ab1f112417851e7b215675d33a259bd067e91d93ef76a5359","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6425b55c066bb14ab1f112417851e7b215675d33a259bd067e91d93ef76a5359","first_computed_at":"2026-05-18T02:44:00.517037Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:44:00.517037Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"R6HiP4hZr2FOrAfdkRuzzP5+q76FCQK2seH2YOuwY7dmRPx6aK3f9JzlZ0WQwtMoZlEvnL20Ok94DVx+Ep8/CQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:44:00.517577Z","signed_message":"canonical_sha256_bytes"},"source_id":"1401.1192","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:69770a54f2d44d62b42274328b6e98c69735732a1cf2fbcd5c922d07c0501b76","sha256:d3cb8e2ae83bcfabb32fd2376b948e8cb768034b92baf31c994c867a71c6e365"],"state_sha256":"23e935fe460adf32b325d1e1a8bb2850372620c1db5029df06a447d960195f1c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"p57hg2LVolQvBAVD4+KwxEjMZkB2hEv8Ibeu+ggg+SYVtm/yKvMmnWU4gQV6oY/QE9rSInfPIdCoq1CPXum6Dg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T14:31:45.213188Z","bundle_sha256":"090dae58db49859cff1f36fc6fe18acda871c37826caabd9d429492078736aa6"}}