{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:3QJIQORUSWA5HRJZVBPVAP5RCK","short_pith_number":"pith:3QJIQORU","schema_version":"1.0","canonical_sha256":"dc12883a349581d3c539a85f503fb1129b55ca1a72f89ef3be849b3af6b6e75b","source":{"kind":"arxiv","id":"1110.6825","version":3},"attestation_state":"computed","paper":{"title":"Violation of the Holographic Viscosity Bound in a Strongly Coupled Anisotropic Plasma","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-th","authors_text":"Anton Rebhan, Dominik Steineder","submitted_at":"2011-10-31T15:16:57Z","abstract_excerpt":"We study the conductivity and shear viscosity tensors of a strongly coupled N=4 super-Yang-Mills plasma which is kept anisotropic by a theta parameter that depends linearly on one of the spatial dimensions. Its holographic dual is given by an anisotropic axion-dilaton-gravity background and has recently been proposed by Mateos and Trancanelli as a model for the pre-equilibrium stage of quark-gluon plasma in heavy-ion collisions. By applying the membrane paradigm which we also check by numerical evaluation of Kubo formula and lowest lying quasinormal modes, we find that the shear viscosity pure"},"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":"1110.6825","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-10-31T15:16:57Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"64bd97b9850bfd0c93fc6ea267ea6256a566fc61de153c89e78de725ed9d97f8","abstract_canon_sha256":"9ab309c5c9b00c55c0954e28b2f84b8dd234999fb1ba826e11336f203a66507b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:23:01.596439Z","signature_b64":"HvEuP9a/jGjmRziXiucZ1jl7d1Tat5NfvghAOjwjRyhrprVG/cvI7nD0fk8OOe4iibyp4G/ph7UE5/0m+OZuCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dc12883a349581d3c539a85f503fb1129b55ca1a72f89ef3be849b3af6b6e75b","last_reissued_at":"2026-05-18T03:23:01.595961Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:23:01.595961Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Violation of the Holographic Viscosity Bound in a Strongly Coupled Anisotropic Plasma","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-th","authors_text":"Anton Rebhan, Dominik Steineder","submitted_at":"2011-10-31T15:16:57Z","abstract_excerpt":"We study the conductivity and shear viscosity tensors of a strongly coupled N=4 super-Yang-Mills plasma which is kept anisotropic by a theta parameter that depends linearly on one of the spatial dimensions. Its holographic dual is given by an anisotropic axion-dilaton-gravity background and has recently been proposed by Mateos and Trancanelli as a model for the pre-equilibrium stage of quark-gluon plasma in heavy-ion collisions. By applying the membrane paradigm which we also check by numerical evaluation of Kubo formula and lowest lying quasinormal modes, we find that the shear viscosity pure"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1110.6825","kind":"arxiv","version":3},"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":"1110.6825","created_at":"2026-05-18T03:23:01.596032+00:00"},{"alias_kind":"arxiv_version","alias_value":"1110.6825v3","created_at":"2026-05-18T03:23:01.596032+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1110.6825","created_at":"2026-05-18T03:23:01.596032+00:00"},{"alias_kind":"pith_short_12","alias_value":"3QJIQORUSWA5","created_at":"2026-05-18T12:26:18.847500+00:00"},{"alias_kind":"pith_short_16","alias_value":"3QJIQORUSWA5HRJZ","created_at":"2026-05-18T12:26:18.847500+00:00"},{"alias_kind":"pith_short_8","alias_value":"3QJIQORU","created_at":"2026-05-18T12:26:18.847500+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.24046","citing_title":"Low-energy hadronic physics in holographic $\\mathrm{QCD_{3}}$ with anisotropy","ref_index":20,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3QJIQORUSWA5HRJZVBPVAP5RCK","json":"https://pith.science/pith/3QJIQORUSWA5HRJZVBPVAP5RCK.json","graph_json":"https://pith.science/api/pith-number/3QJIQORUSWA5HRJZVBPVAP5RCK/graph.json","events_json":"https://pith.science/api/pith-number/3QJIQORUSWA5HRJZVBPVAP5RCK/events.json","paper":"https://pith.science/paper/3QJIQORU"},"agent_actions":{"view_html":"https://pith.science/pith/3QJIQORUSWA5HRJZVBPVAP5RCK","download_json":"https://pith.science/pith/3QJIQORUSWA5HRJZVBPVAP5RCK.json","view_paper":"https://pith.science/paper/3QJIQORU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1110.6825&json=true","fetch_graph":"https://pith.science/api/pith-number/3QJIQORUSWA5HRJZVBPVAP5RCK/graph.json","fetch_events":"https://pith.science/api/pith-number/3QJIQORUSWA5HRJZVBPVAP5RCK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3QJIQORUSWA5HRJZVBPVAP5RCK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3QJIQORUSWA5HRJZVBPVAP5RCK/action/storage_attestation","attest_author":"https://pith.science/pith/3QJIQORUSWA5HRJZVBPVAP5RCK/action/author_attestation","sign_citation":"https://pith.science/pith/3QJIQORUSWA5HRJZVBPVAP5RCK/action/citation_signature","submit_replication":"https://pith.science/pith/3QJIQORUSWA5HRJZVBPVAP5RCK/action/replication_record"}},"created_at":"2026-05-18T03:23:01.596032+00:00","updated_at":"2026-05-18T03:23:01.596032+00:00"}