{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:7OTONIO2DSN3QGXEVIVFZ2MJPR","short_pith_number":"pith:7OTONIO2","schema_version":"1.0","canonical_sha256":"fba6e6a1da1c9bb81ae4aa2a5ce9897c44c9a77ddf7c7346256ec34c6f99ed55","source":{"kind":"arxiv","id":"1709.01932","version":2},"attestation_state":"computed","paper":{"title":"Toward Holographic Reconstruction of Bulk Geometry from Lattice Simulations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-th","authors_text":"Enrico Rinaldi, Evan Berkowitz, Jonathan Maltz, Masanori Hanada, Pavlos Vranas","submitted_at":"2017-09-06T18:00:03Z","abstract_excerpt":"A black hole described in $SU(N)$ gauge theory consists of $N$ D-branes. By separating one of the D-branes from others and studying the interaction between them, the black hole geometry can be probed. In order to obtain quantitative results, we employ the lattice Monte Carlo simulation. As a proof of the concept, we perform an explicit calculation in the matrix model dual to the black zero-brane in type IIA string theory. We demonstrate this method actually works in the high temperature region, where the stringy correction is large. We argue possible dual gravity interpretations."},"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":"1709.01932","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-09-06T18:00:03Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"50a940d380901e95e287b79506216cf21243cf506049b25ffe21d84a1924fa82","abstract_canon_sha256":"96cff51fb53f028ff9768c67ff67910f8b77819faac17fde4bf2e3ef940c62a9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:23:58.905161Z","signature_b64":"RPDCWIGXFeHTT29VX864ru4LDbzNQOugUVH9HM/cal8m66hKz1e9OUtGZXA1YXbYg8Mu49KzqEy2FFZ/+pKkCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fba6e6a1da1c9bb81ae4aa2a5ce9897c44c9a77ddf7c7346256ec34c6f99ed55","last_reissued_at":"2026-05-18T00:23:58.904579Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:23:58.904579Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Toward Holographic Reconstruction of Bulk Geometry from Lattice Simulations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-th","authors_text":"Enrico Rinaldi, Evan Berkowitz, Jonathan Maltz, Masanori Hanada, Pavlos Vranas","submitted_at":"2017-09-06T18:00:03Z","abstract_excerpt":"A black hole described in $SU(N)$ gauge theory consists of $N$ D-branes. By separating one of the D-branes from others and studying the interaction between them, the black hole geometry can be probed. In order to obtain quantitative results, we employ the lattice Monte Carlo simulation. As a proof of the concept, we perform an explicit calculation in the matrix model dual to the black zero-brane in type IIA string theory. We demonstrate this method actually works in the high temperature region, where the stringy correction is large. We argue possible dual gravity interpretations."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.01932","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":"1709.01932","created_at":"2026-05-18T00:23:58.904663+00:00"},{"alias_kind":"arxiv_version","alias_value":"1709.01932v2","created_at":"2026-05-18T00:23:58.904663+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.01932","created_at":"2026-05-18T00:23:58.904663+00:00"},{"alias_kind":"pith_short_12","alias_value":"7OTONIO2DSN3","created_at":"2026-05-18T12:31:05.417338+00:00"},{"alias_kind":"pith_short_16","alias_value":"7OTONIO2DSN3QGXE","created_at":"2026-05-18T12:31:05.417338+00:00"},{"alias_kind":"pith_short_8","alias_value":"7OTONIO2","created_at":"2026-05-18T12:31:05.417338+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.13407","citing_title":"Finite-temperature phase diagram of the BMN matrix model on the lattice","ref_index":24,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7OTONIO2DSN3QGXEVIVFZ2MJPR","json":"https://pith.science/pith/7OTONIO2DSN3QGXEVIVFZ2MJPR.json","graph_json":"https://pith.science/api/pith-number/7OTONIO2DSN3QGXEVIVFZ2MJPR/graph.json","events_json":"https://pith.science/api/pith-number/7OTONIO2DSN3QGXEVIVFZ2MJPR/events.json","paper":"https://pith.science/paper/7OTONIO2"},"agent_actions":{"view_html":"https://pith.science/pith/7OTONIO2DSN3QGXEVIVFZ2MJPR","download_json":"https://pith.science/pith/7OTONIO2DSN3QGXEVIVFZ2MJPR.json","view_paper":"https://pith.science/paper/7OTONIO2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1709.01932&json=true","fetch_graph":"https://pith.science/api/pith-number/7OTONIO2DSN3QGXEVIVFZ2MJPR/graph.json","fetch_events":"https://pith.science/api/pith-number/7OTONIO2DSN3QGXEVIVFZ2MJPR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7OTONIO2DSN3QGXEVIVFZ2MJPR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7OTONIO2DSN3QGXEVIVFZ2MJPR/action/storage_attestation","attest_author":"https://pith.science/pith/7OTONIO2DSN3QGXEVIVFZ2MJPR/action/author_attestation","sign_citation":"https://pith.science/pith/7OTONIO2DSN3QGXEVIVFZ2MJPR/action/citation_signature","submit_replication":"https://pith.science/pith/7OTONIO2DSN3QGXEVIVFZ2MJPR/action/replication_record"}},"created_at":"2026-05-18T00:23:58.904663+00:00","updated_at":"2026-05-18T00:23:58.904663+00:00"}