{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:YLMLPHPEKL3PIXK67BKV5TJMY4","short_pith_number":"pith:YLMLPHPE","schema_version":"1.0","canonical_sha256":"c2d8b79de452f6f45d5ef8555ecd2cc73cefd121e12696b8e9681c2617ed1976","source":{"kind":"arxiv","id":"1605.02804","version":2},"attestation_state":"computed","paper":{"title":"Holographic confinement in inhomogenous backgrounds","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Donald Marolf, Jason Wien","submitted_at":"2016-05-09T22:58:50Z","abstract_excerpt":"As noted by Witten, compactifying a $d$-dimensional holographic CFT on an $S^1$ gives a class of $(d-1)$-dimensional confining theories with gravity duals. The prototypical bulk solution dual to the ground state is a double Wick rotation of the AdS$_{d+1}$ Schwarzschild black hole known as the AdS soliton. We generalize such examples by allowing slow variations in the size of the $S^1$, and thus in the confinement scale. Coefficients governing the second order response of the system are computed for $3 \\le d \\le 8$ using a derivative expansion closely related to the fluid-gravity correspondenc"},"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":"1605.02804","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-05-09T22:58:50Z","cross_cats_sorted":[],"title_canon_sha256":"0c197fc976f8cb9bde2505fba862c47754734dd75018d12d1d174e0edc7fd241","abstract_canon_sha256":"895f3e70ac7799f908842cf3d75ef5d863f698e533286e45a0826d4a3805ffb7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:08:17.203575Z","signature_b64":"xrMcFndBCMRw5Ra0DPA8l2+vYe6cwwc8FTL4bJg34fcvpcHIZbrCo1NaT8GJoU+wlhgkVSklrm/B2jzbHydAAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c2d8b79de452f6f45d5ef8555ecd2cc73cefd121e12696b8e9681c2617ed1976","last_reissued_at":"2026-05-18T01:08:17.202858Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:08:17.202858Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Holographic confinement in inhomogenous backgrounds","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Donald Marolf, Jason Wien","submitted_at":"2016-05-09T22:58:50Z","abstract_excerpt":"As noted by Witten, compactifying a $d$-dimensional holographic CFT on an $S^1$ gives a class of $(d-1)$-dimensional confining theories with gravity duals. The prototypical bulk solution dual to the ground state is a double Wick rotation of the AdS$_{d+1}$ Schwarzschild black hole known as the AdS soliton. We generalize such examples by allowing slow variations in the size of the $S^1$, and thus in the confinement scale. Coefficients governing the second order response of the system are computed for $3 \\le d \\le 8$ using a derivative expansion closely related to the fluid-gravity correspondenc"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.02804","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":"1605.02804","created_at":"2026-05-18T01:08:17.202970+00:00"},{"alias_kind":"arxiv_version","alias_value":"1605.02804v2","created_at":"2026-05-18T01:08:17.202970+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.02804","created_at":"2026-05-18T01:08:17.202970+00:00"},{"alias_kind":"pith_short_12","alias_value":"YLMLPHPEKL3P","created_at":"2026-05-18T12:30:53.716459+00:00"},{"alias_kind":"pith_short_16","alias_value":"YLMLPHPEKL3PIXK6","created_at":"2026-05-18T12:30:53.716459+00:00"},{"alias_kind":"pith_short_8","alias_value":"YLMLPHPE","created_at":"2026-05-18T12:30:53.716459+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/YLMLPHPEKL3PIXK67BKV5TJMY4","json":"https://pith.science/pith/YLMLPHPEKL3PIXK67BKV5TJMY4.json","graph_json":"https://pith.science/api/pith-number/YLMLPHPEKL3PIXK67BKV5TJMY4/graph.json","events_json":"https://pith.science/api/pith-number/YLMLPHPEKL3PIXK67BKV5TJMY4/events.json","paper":"https://pith.science/paper/YLMLPHPE"},"agent_actions":{"view_html":"https://pith.science/pith/YLMLPHPEKL3PIXK67BKV5TJMY4","download_json":"https://pith.science/pith/YLMLPHPEKL3PIXK67BKV5TJMY4.json","view_paper":"https://pith.science/paper/YLMLPHPE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1605.02804&json=true","fetch_graph":"https://pith.science/api/pith-number/YLMLPHPEKL3PIXK67BKV5TJMY4/graph.json","fetch_events":"https://pith.science/api/pith-number/YLMLPHPEKL3PIXK67BKV5TJMY4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YLMLPHPEKL3PIXK67BKV5TJMY4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YLMLPHPEKL3PIXK67BKV5TJMY4/action/storage_attestation","attest_author":"https://pith.science/pith/YLMLPHPEKL3PIXK67BKV5TJMY4/action/author_attestation","sign_citation":"https://pith.science/pith/YLMLPHPEKL3PIXK67BKV5TJMY4/action/citation_signature","submit_replication":"https://pith.science/pith/YLMLPHPEKL3PIXK67BKV5TJMY4/action/replication_record"}},"created_at":"2026-05-18T01:08:17.202970+00:00","updated_at":"2026-05-18T01:08:17.202970+00:00"}