{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:LJ7NLFQ3IG24M5Z5YRDXY7US7Z","short_pith_number":"pith:LJ7NLFQ3","canonical_record":{"source":{"id":"1410.1091","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-10-04T20:27:15Z","cross_cats_sorted":[],"title_canon_sha256":"3f8207c8140db9719bbd0affdd878ffebac780f53426ca7d983f16e2304f3b27","abstract_canon_sha256":"ab1f0e99a50caff4c8f8bf194be0ec706d01ccda2d92053fc486446ac05f274e"},"schema_version":"1.0"},"canonical_sha256":"5a7ed5961b41b5c6773dc4477c7e92fe74bdba93f461580ce2dae68a03f4479d","source":{"kind":"arxiv","id":"1410.1091","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1410.1091","created_at":"2026-05-18T02:04:10Z"},{"alias_kind":"arxiv_version","alias_value":"1410.1091v1","created_at":"2026-05-18T02:04:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.1091","created_at":"2026-05-18T02:04:10Z"},{"alias_kind":"pith_short_12","alias_value":"LJ7NLFQ3IG24","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"LJ7NLFQ3IG24M5Z5","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"LJ7NLFQ3","created_at":"2026-05-18T12:28:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:LJ7NLFQ3IG24M5Z5YRDXY7US7Z","target":"record","payload":{"canonical_record":{"source":{"id":"1410.1091","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-10-04T20:27:15Z","cross_cats_sorted":[],"title_canon_sha256":"3f8207c8140db9719bbd0affdd878ffebac780f53426ca7d983f16e2304f3b27","abstract_canon_sha256":"ab1f0e99a50caff4c8f8bf194be0ec706d01ccda2d92053fc486446ac05f274e"},"schema_version":"1.0"},"canonical_sha256":"5a7ed5961b41b5c6773dc4477c7e92fe74bdba93f461580ce2dae68a03f4479d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:04:10.444095Z","signature_b64":"Q3W5l5VbgdKlbRTeuISJNekhvYIyBbyL9QgnpA7g1BlbXfmEwuHr0k1yJvUSbYGvlXeF3mwhkRxwlcnTTpHNAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5a7ed5961b41b5c6773dc4477c7e92fe74bdba93f461580ce2dae68a03f4479d","last_reissued_at":"2026-05-18T02:04:10.443521Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:04:10.443521Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1410.1091","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:04:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6FwN3w5KZWLC3P6aLr1OyanqNOBGvY3SptmprGIsZJOiGuKlGIr+0mSHpnFn5bn7Sm9UMnyXBnouX4cCcBg2Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T02:00:08.458578Z"},"content_sha256":"43974cc4e312f6a030a5704adff134eb3898f348d6f3ddaf1c91de881d07360a","schema_version":"1.0","event_id":"sha256:43974cc4e312f6a030a5704adff134eb3898f348d6f3ddaf1c91de881d07360a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:LJ7NLFQ3IG24M5Z5YRDXY7US7Z","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"On the gluon operator effective potential in holographic Yang-Mills theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Elias Kiritsis, Francesco Nitti, Wenliang Li","submitted_at":"2014-10-04T20:27:15Z","abstract_excerpt":"The holographic formalism is applied to the calculation of the effective potential for the scalar glueball operator. Three different versions of this operator are defined, and for each we compute the associated effective potential and discuss its properties and scheme ambiguities. Contact is made to earlier attempts to guess this effective potential from the conformal anomaly. We apply our results to the Improved Holographic QCD model calculating the glueball condensate."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.1091","kind":"arxiv","version":1},"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":"2026-05-18T02:04:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"E3TaTlbhHhR98YEsPqZYtSiO4jsleODeN9WSbh5itNiOAoay66hKBcYDXFyW3ISLmjvSd920rv0KddatBlQRBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T02:00:08.459255Z"},"content_sha256":"dbc7bf63f708e24229ec68343b5f300fcdc0a3a3a6cc5d99d8cb7b8572fdf7f7","schema_version":"1.0","event_id":"sha256:dbc7bf63f708e24229ec68343b5f300fcdc0a3a3a6cc5d99d8cb7b8572fdf7f7"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LJ7NLFQ3IG24M5Z5YRDXY7US7Z/bundle.json","state_url":"https://pith.science/pith/LJ7NLFQ3IG24M5Z5YRDXY7US7Z/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LJ7NLFQ3IG24M5Z5YRDXY7US7Z/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":"2026-05-26T02:00:08Z","links":{"resolver":"https://pith.science/pith/LJ7NLFQ3IG24M5Z5YRDXY7US7Z","bundle":"https://pith.science/pith/LJ7NLFQ3IG24M5Z5YRDXY7US7Z/bundle.json","state":"https://pith.science/pith/LJ7NLFQ3IG24M5Z5YRDXY7US7Z/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LJ7NLFQ3IG24M5Z5YRDXY7US7Z/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:LJ7NLFQ3IG24M5Z5YRDXY7US7Z","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":"ab1f0e99a50caff4c8f8bf194be0ec706d01ccda2d92053fc486446ac05f274e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-10-04T20:27:15Z","title_canon_sha256":"3f8207c8140db9719bbd0affdd878ffebac780f53426ca7d983f16e2304f3b27"},"schema_version":"1.0","source":{"id":"1410.1091","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1410.1091","created_at":"2026-05-18T02:04:10Z"},{"alias_kind":"arxiv_version","alias_value":"1410.1091v1","created_at":"2026-05-18T02:04:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.1091","created_at":"2026-05-18T02:04:10Z"},{"alias_kind":"pith_short_12","alias_value":"LJ7NLFQ3IG24","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"LJ7NLFQ3IG24M5Z5","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"LJ7NLFQ3","created_at":"2026-05-18T12:28:38Z"}],"graph_snapshots":[{"event_id":"sha256:dbc7bf63f708e24229ec68343b5f300fcdc0a3a3a6cc5d99d8cb7b8572fdf7f7","target":"graph","created_at":"2026-05-18T02:04:10Z","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":"The holographic formalism is applied to the calculation of the effective potential for the scalar glueball operator. Three different versions of this operator are defined, and for each we compute the associated effective potential and discuss its properties and scheme ambiguities. Contact is made to earlier attempts to guess this effective potential from the conformal anomaly. We apply our results to the Improved Holographic QCD model calculating the glueball condensate.","authors_text":"Elias Kiritsis, Francesco Nitti, Wenliang Li","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-10-04T20:27:15Z","title":"On the gluon operator effective potential in holographic Yang-Mills theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.1091","kind":"arxiv","version":1},"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":"sha256:43974cc4e312f6a030a5704adff134eb3898f348d6f3ddaf1c91de881d07360a","target":"record","created_at":"2026-05-18T02:04:10Z","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":"ab1f0e99a50caff4c8f8bf194be0ec706d01ccda2d92053fc486446ac05f274e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-10-04T20:27:15Z","title_canon_sha256":"3f8207c8140db9719bbd0affdd878ffebac780f53426ca7d983f16e2304f3b27"},"schema_version":"1.0","source":{"id":"1410.1091","kind":"arxiv","version":1}},"canonical_sha256":"5a7ed5961b41b5c6773dc4477c7e92fe74bdba93f461580ce2dae68a03f4479d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5a7ed5961b41b5c6773dc4477c7e92fe74bdba93f461580ce2dae68a03f4479d","first_computed_at":"2026-05-18T02:04:10.443521Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:04:10.443521Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Q3W5l5VbgdKlbRTeuISJNekhvYIyBbyL9QgnpA7g1BlbXfmEwuHr0k1yJvUSbYGvlXeF3mwhkRxwlcnTTpHNAg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:04:10.444095Z","signed_message":"canonical_sha256_bytes"},"source_id":"1410.1091","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:43974cc4e312f6a030a5704adff134eb3898f348d6f3ddaf1c91de881d07360a","sha256:dbc7bf63f708e24229ec68343b5f300fcdc0a3a3a6cc5d99d8cb7b8572fdf7f7"],"state_sha256":"c8c06c5c69633f287b77a78800005bb6cd1f8100924cd80e6f622d8424467fdb"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rjFrRDXCrPwOdCnNSPk19ieWWGKWeaGhICM1VR5m2Izosp2IOihF8KdW3KEdqZtc7HdAiZtzg+VAD9SfYtUqCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T02:00:08.464199Z","bundle_sha256":"da45582a60a21e7f3cfde7b16325a800d158a19cc01d9529cc57372306e8f54e"}}