{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:7PENMKIQH7DASA6QVKANKZ7N5G","short_pith_number":"pith:7PENMKIQ","schema_version":"1.0","canonical_sha256":"fbc8d629103fc60903d0aa80d567ede99666f1509a6963adc872e7229ef9ee7c","source":{"kind":"arxiv","id":"0705.3870","version":2},"attestation_state":"computed","paper":{"title":"Metallic AdS/CFT","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Andreas Karch, Andy O'Bannon","submitted_at":"2007-05-26T03:23:15Z","abstract_excerpt":"We use the AdS/CFT correspondence to compute the conductivity of massive N=2 hypermultiplet fields at finite baryon number density in an N=4 SU(N_c) super-Yang-Mills theory plasma in the large N_c, large 't Hooft coupling limit. The finite baryon density provides charge carriers analogous to electrons in a metal. An external electric field then induces a finite current which we determine directly. Our result for the conductivity is good for all values of the mass, external field and density, modulo statements about the yet-incomplete phase diagram. In the appropriate limits it agrees with know"},"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":"0705.3870","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2007-05-26T03:23:15Z","cross_cats_sorted":[],"title_canon_sha256":"dc6a9f23ec1260a8f64984d6553e03b34ed09555e5e07c08207f0ba7cd2c3772","abstract_canon_sha256":"eda5d96f4974d07a3926ad942403dc1e7f25f04c2428902c5454065cb9601079"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:41:14.409681Z","signature_b64":"WF1dR0dc77U5Q2sXKGDgHoC9/7fKbjuyjt4OJxCRmXc8Pwr5PcQEZGczG0r9FPKnyqN8axAIUXPaxvZbfD51Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fbc8d629103fc60903d0aa80d567ede99666f1509a6963adc872e7229ef9ee7c","last_reissued_at":"2026-07-04T15:41:14.409276Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:41:14.409276Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Metallic AdS/CFT","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Andreas Karch, Andy O'Bannon","submitted_at":"2007-05-26T03:23:15Z","abstract_excerpt":"We use the AdS/CFT correspondence to compute the conductivity of massive N=2 hypermultiplet fields at finite baryon number density in an N=4 SU(N_c) super-Yang-Mills theory plasma in the large N_c, large 't Hooft coupling limit. The finite baryon density provides charge carriers analogous to electrons in a metal. An external electric field then induces a finite current which we determine directly. Our result for the conductivity is good for all values of the mass, external field and density, modulo statements about the yet-incomplete phase diagram. In the appropriate limits it agrees with know"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0705.3870","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/0705.3870/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"0705.3870","created_at":"2026-07-04T15:41:14.409348+00:00"},{"alias_kind":"arxiv_version","alias_value":"0705.3870v2","created_at":"2026-07-04T15:41:14.409348+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0705.3870","created_at":"2026-07-04T15:41:14.409348+00:00"},{"alias_kind":"pith_short_12","alias_value":"7PENMKIQH7DA","created_at":"2026-07-04T15:41:14.409348+00:00"},{"alias_kind":"pith_short_16","alias_value":"7PENMKIQH7DASA6Q","created_at":"2026-07-04T15:41:14.409348+00:00"},{"alias_kind":"pith_short_8","alias_value":"7PENMKIQ","created_at":"2026-07-04T15:41:14.409348+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":6,"internal_anchor_count":4,"sample":[{"citing_arxiv_id":"2605.04586","citing_title":"Bound states and deconfinement from Romans supergravity with magnetic flux","ref_index":56,"is_internal_anchor":true},{"citing_arxiv_id":"2512.19694","citing_title":"Linear response beyond hydrodynamic poles","ref_index":44,"is_internal_anchor":true},{"citing_arxiv_id":"2605.16931","citing_title":"Nonlinear response of the chiral magnetic effect in the D3/D7 holographic model","ref_index":7,"is_internal_anchor":true},{"citing_arxiv_id":"2506.09461","citing_title":"Holographic D-brane constructions with dynamical gauge fields","ref_index":20,"is_internal_anchor":true},{"citing_arxiv_id":"2605.04586","citing_title":"Bound states and deconfinement from Romans supergravity with magnetic flux","ref_index":56,"is_internal_anchor":false},{"citing_arxiv_id":"2604.04424","citing_title":"D-instanton Effects on the Holographic Weyl Semimetals","ref_index":55,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7PENMKIQH7DASA6QVKANKZ7N5G","json":"https://pith.science/pith/7PENMKIQH7DASA6QVKANKZ7N5G.json","graph_json":"https://pith.science/api/pith-number/7PENMKIQH7DASA6QVKANKZ7N5G/graph.json","events_json":"https://pith.science/api/pith-number/7PENMKIQH7DASA6QVKANKZ7N5G/events.json","paper":"https://pith.science/paper/7PENMKIQ"},"agent_actions":{"view_html":"https://pith.science/pith/7PENMKIQH7DASA6QVKANKZ7N5G","download_json":"https://pith.science/pith/7PENMKIQH7DASA6QVKANKZ7N5G.json","view_paper":"https://pith.science/paper/7PENMKIQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0705.3870&json=true","fetch_graph":"https://pith.science/api/pith-number/7PENMKIQH7DASA6QVKANKZ7N5G/graph.json","fetch_events":"https://pith.science/api/pith-number/7PENMKIQH7DASA6QVKANKZ7N5G/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7PENMKIQH7DASA6QVKANKZ7N5G/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7PENMKIQH7DASA6QVKANKZ7N5G/action/storage_attestation","attest_author":"https://pith.science/pith/7PENMKIQH7DASA6QVKANKZ7N5G/action/author_attestation","sign_citation":"https://pith.science/pith/7PENMKIQH7DASA6QVKANKZ7N5G/action/citation_signature","submit_replication":"https://pith.science/pith/7PENMKIQH7DASA6QVKANKZ7N5G/action/replication_record"}},"created_at":"2026-07-04T15:41:14.409348+00:00","updated_at":"2026-07-04T15:41:14.409348+00:00"}