{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:T32NDEZHSIGDCP6CPYALCW3ACO","short_pith_number":"pith:T32NDEZH","schema_version":"1.0","canonical_sha256":"9ef4d19327920c313fc27e00b15b6013818574b763e3390f4e78e5475e3c3db9","source":{"kind":"arxiv","id":"1510.07911","version":2},"attestation_state":"computed","paper":{"title":"Wormholes, Emergent Gauge Fields, and the Weak Gravity Conjecture","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Daniel Harlow","submitted_at":"2015-10-27T14:09:49Z","abstract_excerpt":"This paper revisits the question of reconstructing bulk gauge fields as boundary operators in AdS/CFT. In the presence of the wormhole dual to the thermofield double state of two CFTs, the existence of bulk gauge fields is in some tension with the microscopic tensor factorization of the Hilbert space. I explain how this tension can be resolved by splitting the gauge field into charged constituents, and I argue that this leads to a new argument for the \"principle of completeness\", which states that the charge lattice of a gauge theory coupled to gravity must be fully populated. I also claim tha"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1510.07911","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-10-27T14:09:49Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"681db23c24ffd9ed67f52f6cf223729c09efc786c5af6e9a18b32dc3888eb2c8","abstract_canon_sha256":"ce0a1ba9fe29c65b98ca30479997021fe78b5375eba7ab1b4952a327ab92cffe"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:20:42.190997Z","signature_b64":"iXj0MvxDgEbAsGTCTYfQE2DMMgKEqlEhSRh9CFpDOwmesjjtG3LXoCIHLuDcUVwrhMOv95nFj2Nje7JKNJbiBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9ef4d19327920c313fc27e00b15b6013818574b763e3390f4e78e5475e3c3db9","last_reissued_at":"2026-05-18T01:20:42.190531Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:20:42.190531Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Wormholes, Emergent Gauge Fields, and the Weak Gravity Conjecture","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Daniel Harlow","submitted_at":"2015-10-27T14:09:49Z","abstract_excerpt":"This paper revisits the question of reconstructing bulk gauge fields as boundary operators in AdS/CFT. In the presence of the wormhole dual to the thermofield double state of two CFTs, the existence of bulk gauge fields is in some tension with the microscopic tensor factorization of the Hilbert space. I explain how this tension can be resolved by splitting the gauge field into charged constituents, and I argue that this leads to a new argument for the \"principle of completeness\", which states that the charge lattice of a gauge theory coupled to gravity must be fully populated. I also claim tha"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1510.07911","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1510.07911","created_at":"2026-05-18T01:20:42.190599+00:00"},{"alias_kind":"arxiv_version","alias_value":"1510.07911v2","created_at":"2026-05-18T01:20:42.190599+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1510.07911","created_at":"2026-05-18T01:20:42.190599+00:00"},{"alias_kind":"pith_short_12","alias_value":"T32NDEZHSIGD","created_at":"2026-05-18T12:29:42.218222+00:00"},{"alias_kind":"pith_short_16","alias_value":"T32NDEZHSIGDCP6C","created_at":"2026-05-18T12:29:42.218222+00:00"},{"alias_kind":"pith_short_8","alias_value":"T32NDEZH","created_at":"2026-05-18T12:29:42.218222+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2511.09613","citing_title":"Bounds on Discrete Gauge Symmetries in Supergravity","ref_index":5,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/T32NDEZHSIGDCP6CPYALCW3ACO","json":"https://pith.science/pith/T32NDEZHSIGDCP6CPYALCW3ACO.json","graph_json":"https://pith.science/api/pith-number/T32NDEZHSIGDCP6CPYALCW3ACO/graph.json","events_json":"https://pith.science/api/pith-number/T32NDEZHSIGDCP6CPYALCW3ACO/events.json","paper":"https://pith.science/paper/T32NDEZH"},"agent_actions":{"view_html":"https://pith.science/pith/T32NDEZHSIGDCP6CPYALCW3ACO","download_json":"https://pith.science/pith/T32NDEZHSIGDCP6CPYALCW3ACO.json","view_paper":"https://pith.science/paper/T32NDEZH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1510.07911&json=true","fetch_graph":"https://pith.science/api/pith-number/T32NDEZHSIGDCP6CPYALCW3ACO/graph.json","fetch_events":"https://pith.science/api/pith-number/T32NDEZHSIGDCP6CPYALCW3ACO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/T32NDEZHSIGDCP6CPYALCW3ACO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/T32NDEZHSIGDCP6CPYALCW3ACO/action/storage_attestation","attest_author":"https://pith.science/pith/T32NDEZHSIGDCP6CPYALCW3ACO/action/author_attestation","sign_citation":"https://pith.science/pith/T32NDEZHSIGDCP6CPYALCW3ACO/action/citation_signature","submit_replication":"https://pith.science/pith/T32NDEZHSIGDCP6CPYALCW3ACO/action/replication_record"}},"created_at":"2026-05-18T01:20:42.190599+00:00","updated_at":"2026-05-18T01:20:42.190599+00:00"}