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We show that in the limit of zero frequency this cross section coincides with the area of the horizon. From this result we find \\eta=\\pi/8 N^2T^3. We conjecture that for finite 't Hooft coupling (g_YM)^2N the shear viscosity is \\eta=f((g_YM)^2N) N^2T^3, where f(x) is a monotonic function that decreases"},"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":"hep-th/0104066","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2001-04-06T21:41:44Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"6bfc35fb29463f5e931444c01a9814b3c1d861631b57c36767bd7e076d18c849","abstract_canon_sha256":"1a1abb1e2bfdf08099c5a4fa3c12dc35fde9eb7bff17bce1fbeb28d7f2e2692e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:22:06.600724Z","signature_b64":"snD+5gQXM/aG1B/ONQSmJuz9lfCaGHZBxhbLUz2p1K+xY+G8IJnQUv1tjoJwWr8cuHGnk1+AQR/RH9POsfYgDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"74f54e3e65a96062be5864685fabed4228124a189179dc42bd0c27d2ee61b8c3","last_reissued_at":"2026-07-04T17:22:06.600269Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:22:06.600269Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Shear viscosity of strongly coupled N=4 supersymmetric Yang-Mills plasma","license":"","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-th","authors_text":"A.O. 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