{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:BQ7ZUNXSL7CSACEEV3RCDXFX2V","short_pith_number":"pith:BQ7ZUNXS","schema_version":"1.0","canonical_sha256":"0c3f9a36f25fc5200884aee221dcb7d5444eeeb1548d581c7c13aefd2a4fba33","source":{"kind":"arxiv","id":"1109.6343","version":1},"attestation_state":"computed","paper":{"title":"Holographic zero sound at finite temperature","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","hep-ph"],"primary_cat":"hep-th","authors_text":"Andrei O. Starinets, Richard A. Davison","submitted_at":"2011-09-28T20:21:47Z","abstract_excerpt":"We use gauge-gravity duality to study the temperature dependence of the zero sound mode and the fundamental matter diffusion mode in the strongly coupled {\\cal N}=4 SU(N_c) supersymmetric Yang-Mills theory with N_f {\\cal N}=2 hypermultiplets in the N_c>>1, N_c>>N_f limit, which is holographically realized via the D3/D7 brane system. In the high density limit \\mu>>T, three regimes can be identified in the behavior of these modes, analogous to the collisionless quantum, collisionless thermal and hydrodynamic regimes of a Landau Fermi-liquid. The transitions between the three regimes are characte"},"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":"1109.6343","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-09-28T20:21:47Z","cross_cats_sorted":["cond-mat.str-el","hep-ph"],"title_canon_sha256":"b358cab4442193abd0b2b38ef67567cd8f2d84ba654da0503289c184a4948025","abstract_canon_sha256":"be414c21df7869e716cc98d9ca9b565110b0e46958fb1ac29accc874e0e33d2a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:04:18.804077Z","signature_b64":"1Wa6zmRHST0cHquIre543KlGHtT1T/IaedBjCLWHJwHxTnJlIfwC0mRgjFzF21P9e0PlDQLHrsFJWy5Xjd4cBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0c3f9a36f25fc5200884aee221dcb7d5444eeeb1548d581c7c13aefd2a4fba33","last_reissued_at":"2026-05-18T04:04:18.803360Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:04:18.803360Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Holographic zero sound at finite temperature","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","hep-ph"],"primary_cat":"hep-th","authors_text":"Andrei O. Starinets, Richard A. Davison","submitted_at":"2011-09-28T20:21:47Z","abstract_excerpt":"We use gauge-gravity duality to study the temperature dependence of the zero sound mode and the fundamental matter diffusion mode in the strongly coupled {\\cal N}=4 SU(N_c) supersymmetric Yang-Mills theory with N_f {\\cal N}=2 hypermultiplets in the N_c>>1, N_c>>N_f limit, which is holographically realized via the D3/D7 brane system. In the high density limit \\mu>>T, three regimes can be identified in the behavior of these modes, analogous to the collisionless quantum, collisionless thermal and hydrodynamic regimes of a Landau Fermi-liquid. The transitions between the three regimes are characte"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1109.6343","kind":"arxiv","version":1},"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":"1109.6343","created_at":"2026-05-18T04:04:18.803455+00:00"},{"alias_kind":"arxiv_version","alias_value":"1109.6343v1","created_at":"2026-05-18T04:04:18.803455+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1109.6343","created_at":"2026-05-18T04:04:18.803455+00:00"},{"alias_kind":"pith_short_12","alias_value":"BQ7ZUNXSL7CS","created_at":"2026-05-18T12:26:24.575870+00:00"},{"alias_kind":"pith_short_16","alias_value":"BQ7ZUNXSL7CSACEE","created_at":"2026-05-18T12:26:24.575870+00:00"},{"alias_kind":"pith_short_8","alias_value":"BQ7ZUNXS","created_at":"2026-05-18T12:26:24.575870+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.09461","citing_title":"Holographic D-brane constructions with dynamical gauge fields","ref_index":64,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BQ7ZUNXSL7CSACEEV3RCDXFX2V","json":"https://pith.science/pith/BQ7ZUNXSL7CSACEEV3RCDXFX2V.json","graph_json":"https://pith.science/api/pith-number/BQ7ZUNXSL7CSACEEV3RCDXFX2V/graph.json","events_json":"https://pith.science/api/pith-number/BQ7ZUNXSL7CSACEEV3RCDXFX2V/events.json","paper":"https://pith.science/paper/BQ7ZUNXS"},"agent_actions":{"view_html":"https://pith.science/pith/BQ7ZUNXSL7CSACEEV3RCDXFX2V","download_json":"https://pith.science/pith/BQ7ZUNXSL7CSACEEV3RCDXFX2V.json","view_paper":"https://pith.science/paper/BQ7ZUNXS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1109.6343&json=true","fetch_graph":"https://pith.science/api/pith-number/BQ7ZUNXSL7CSACEEV3RCDXFX2V/graph.json","fetch_events":"https://pith.science/api/pith-number/BQ7ZUNXSL7CSACEEV3RCDXFX2V/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BQ7ZUNXSL7CSACEEV3RCDXFX2V/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BQ7ZUNXSL7CSACEEV3RCDXFX2V/action/storage_attestation","attest_author":"https://pith.science/pith/BQ7ZUNXSL7CSACEEV3RCDXFX2V/action/author_attestation","sign_citation":"https://pith.science/pith/BQ7ZUNXSL7CSACEEV3RCDXFX2V/action/citation_signature","submit_replication":"https://pith.science/pith/BQ7ZUNXSL7CSACEEV3RCDXFX2V/action/replication_record"}},"created_at":"2026-05-18T04:04:18.803455+00:00","updated_at":"2026-05-18T04:04:18.803455+00:00"}