{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2008:FFKAIRWX2J553P2TAIVGY6L6KO","short_pith_number":"pith:FFKAIRWX","canonical_record":{"source":{"id":"0811.0184","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2008-11-03T02:33:56Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"6e02a54e94c47f1d406e83a3b2f123268109b291eb2fb6b9b8cf1f4893797b20","abstract_canon_sha256":"80bd8cd867a60c478c9312ed686c19de3bee4629135a359c73b7c8a58233c382"},"schema_version":"1.0"},"canonical_sha256":"29540446d7d27bddbf53022a6c797e5381aa8b1932bfa9fce7cc1e65e523b169","source":{"kind":"arxiv","id":"0811.0184","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0811.0184","created_at":"2026-07-04T15:37:31Z"},{"alias_kind":"arxiv_version","alias_value":"0811.0184v2","created_at":"2026-07-04T15:37:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0811.0184","created_at":"2026-07-04T15:37:31Z"},{"alias_kind":"pith_short_12","alias_value":"FFKAIRWX2J55","created_at":"2026-07-04T15:37:31Z"},{"alias_kind":"pith_short_16","alias_value":"FFKAIRWX2J553P2T","created_at":"2026-07-04T15:37:31Z"},{"alias_kind":"pith_short_8","alias_value":"FFKAIRWX","created_at":"2026-07-04T15:37:31Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2008:FFKAIRWX2J553P2TAIVGY6L6KO","target":"record","payload":{"canonical_record":{"source":{"id":"0811.0184","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2008-11-03T02:33:56Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"6e02a54e94c47f1d406e83a3b2f123268109b291eb2fb6b9b8cf1f4893797b20","abstract_canon_sha256":"80bd8cd867a60c478c9312ed686c19de3bee4629135a359c73b7c8a58233c382"},"schema_version":"1.0"},"canonical_sha256":"29540446d7d27bddbf53022a6c797e5381aa8b1932bfa9fce7cc1e65e523b169","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:37:31.752558Z","signature_b64":"+t0+wfRgfRpHK/zRHQ8NMCM0i807mGlSG3qbSKuTRMFKoRMwuSHfTCLwumqTJdrtt6B5zo0rR0pI5fIBnx8NAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"29540446d7d27bddbf53022a6c797e5381aa8b1932bfa9fce7cc1e65e523b169","last_reissued_at":"2026-07-04T15:37:31.752154Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:37:31.752154Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0811.0184","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":"2026-07-04T15:37:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Fkb3UFsm+oTr8n3oFDb5mUWq5d8wCFojHG6YPJ/xmgsygl4T/VI0ckqo5L+P3GRS2PJQ+EJsu7DoOt3pfshJDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-15T05:09:56.386373Z"},"content_sha256":"0cd876949e61c19e1a487e763e3130532d65468f694d92536935d111be79213c","schema_version":"1.0","event_id":"sha256:0cd876949e61c19e1a487e763e3130532d65468f694d92536935d111be79213c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2008:FFKAIRWX2J553P2TAIVGY6L6KO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Baryonic Response of Dense Holographic QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Ismail Zahed, Keun-Young Kim","submitted_at":"2008-11-03T02:33:56Z","abstract_excerpt":"The response function of a homogeneous and dense hadronic system to a time-dependent (baryon) vector potential is discussed for holographic dense QCD (D4/D8 embedding) both in the confined and deconfined phases. Confined holographic QCD is an uncompressible and static baryonic insulator at large N_c and large \\lambda, with a gapped vector spectrum and a massless pion. Deconfined holographic QCD is a diffusive conductor with restored chiral symmetry and a gapped transverse baryonic current. Similarly, dense D3/D7 is diffusive for any non-zero temperature at large N_c and large \\lambda. At zero "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0811.0184","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/0811.0184/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":"2026-07-04T15:37:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"p+pP++QLzFFNZvl05/QSUjvbWTHMi4JL5BGzbW+1ffZsT/MwpoW45bTo+Dgq37fokzyYyl5vfHkKCkbxFYcjBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-15T05:09:56.386881Z"},"content_sha256":"bf87e4a9b5a4b8596bac1ff207a032cf0836596ed9b99ea3d71fbec665a3adec","schema_version":"1.0","event_id":"sha256:bf87e4a9b5a4b8596bac1ff207a032cf0836596ed9b99ea3d71fbec665a3adec"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FFKAIRWX2J553P2TAIVGY6L6KO/bundle.json","state_url":"https://pith.science/pith/FFKAIRWX2J553P2TAIVGY6L6KO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FFKAIRWX2J553P2TAIVGY6L6KO/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":"2026-08-15T05:09:56Z","links":{"resolver":"https://pith.science/pith/FFKAIRWX2J553P2TAIVGY6L6KO","bundle":"https://pith.science/pith/FFKAIRWX2J553P2TAIVGY6L6KO/bundle.json","state":"https://pith.science/pith/FFKAIRWX2J553P2TAIVGY6L6KO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FFKAIRWX2J553P2TAIVGY6L6KO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2008:FFKAIRWX2J553P2TAIVGY6L6KO","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":"80bd8cd867a60c478c9312ed686c19de3bee4629135a359c73b7c8a58233c382","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2008-11-03T02:33:56Z","title_canon_sha256":"6e02a54e94c47f1d406e83a3b2f123268109b291eb2fb6b9b8cf1f4893797b20"},"schema_version":"1.0","source":{"id":"0811.0184","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0811.0184","created_at":"2026-07-04T15:37:31Z"},{"alias_kind":"arxiv_version","alias_value":"0811.0184v2","created_at":"2026-07-04T15:37:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0811.0184","created_at":"2026-07-04T15:37:31Z"},{"alias_kind":"pith_short_12","alias_value":"FFKAIRWX2J55","created_at":"2026-07-04T15:37:31Z"},{"alias_kind":"pith_short_16","alias_value":"FFKAIRWX2J553P2T","created_at":"2026-07-04T15:37:31Z"},{"alias_kind":"pith_short_8","alias_value":"FFKAIRWX","created_at":"2026-07-04T15:37:31Z"}],"graph_snapshots":[{"event_id":"sha256:bf87e4a9b5a4b8596bac1ff207a032cf0836596ed9b99ea3d71fbec665a3adec","target":"graph","created_at":"2026-07-04T15:37:31Z","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/0811.0184/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The response function of a homogeneous and dense hadronic system to a time-dependent (baryon) vector potential is discussed for holographic dense QCD (D4/D8 embedding) both in the confined and deconfined phases. Confined holographic QCD is an uncompressible and static baryonic insulator at large N_c and large \\lambda, with a gapped vector spectrum and a massless pion. Deconfined holographic QCD is a diffusive conductor with restored chiral symmetry and a gapped transverse baryonic current. Similarly, dense D3/D7 is diffusive for any non-zero temperature at large N_c and large \\lambda. At zero ","authors_text":"Ismail Zahed, Keun-Young Kim","cross_cats":["hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2008-11-03T02:33:56Z","title":"Baryonic Response of Dense Holographic QCD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0811.0184","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":"sha256:0cd876949e61c19e1a487e763e3130532d65468f694d92536935d111be79213c","target":"record","created_at":"2026-07-04T15:37:31Z","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":"80bd8cd867a60c478c9312ed686c19de3bee4629135a359c73b7c8a58233c382","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2008-11-03T02:33:56Z","title_canon_sha256":"6e02a54e94c47f1d406e83a3b2f123268109b291eb2fb6b9b8cf1f4893797b20"},"schema_version":"1.0","source":{"id":"0811.0184","kind":"arxiv","version":2}},"canonical_sha256":"29540446d7d27bddbf53022a6c797e5381aa8b1932bfa9fce7cc1e65e523b169","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"29540446d7d27bddbf53022a6c797e5381aa8b1932bfa9fce7cc1e65e523b169","first_computed_at":"2026-07-04T15:37:31.752154Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:37:31.752154Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"+t0+wfRgfRpHK/zRHQ8NMCM0i807mGlSG3qbSKuTRMFKoRMwuSHfTCLwumqTJdrtt6B5zo0rR0pI5fIBnx8NAg==","signature_status":"signed_v1","signed_at":"2026-07-04T15:37:31.752558Z","signed_message":"canonical_sha256_bytes"},"source_id":"0811.0184","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0cd876949e61c19e1a487e763e3130532d65468f694d92536935d111be79213c","sha256:bf87e4a9b5a4b8596bac1ff207a032cf0836596ed9b99ea3d71fbec665a3adec"],"state_sha256":"85d307308a5e0c5d270666ed98f25b3c1dc8dcc40f6933ad30856f786c7af3f7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"m25m7YnzYT75Izo3MNvgoA5Vo4KtytoolzJQ1tT9da+nC/92wy6RwFybcsD/QJKNTnIg7NvnXhGKP5yMV7hACw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-15T05:09:56.391067Z","bundle_sha256":"757e9652024b61e20938dd3a5c88b09fc8673b73e06749baddf0cab5f605a5e4"}}