{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:EATDES6PQ7USL7M3TCCU3OA5OV","short_pith_number":"pith:EATDES6P","schema_version":"1.0","canonical_sha256":"2026324bcf87e925fd9b98854db81d754352ac3b1911f314fcfb3ad84f8f34c0","source":{"kind":"arxiv","id":"1604.05092","version":3},"attestation_state":"computed","paper":{"title":"Hyperscaling violation and the shear diffusion constant","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Debangshu Mukherjee, Kedar S. Kolekar, K. Narayan","submitted_at":"2016-04-18T11:18:22Z","abstract_excerpt":"We consider holographic theories in bulk $(d+1)$-dimensions with Lifshitz and hyperscaling violating exponents $z,\\theta$ at finite temperature. By studying shear gravitational modes in the near-horizon region given certain self-consistent approximations, we obtain the corresponding shear diffusion constant on an appropriately defined stretched horizon, adapting the analysis of Kovtun, Son and Starinets. For generic exponents with $d-z-\\theta>-1$, we find that the diffusion constant has power law scaling with the temperature, motivating us to guess a universal relation for the viscosity bound."},"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":"1604.05092","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-04-18T11:18:22Z","cross_cats_sorted":[],"title_canon_sha256":"2f06018176b71132cc8b9ec933f87cad7d3d345cc42099ed78ba9d30d41e9b1c","abstract_canon_sha256":"2ecb4f1e16f2fd71cc75f9f1ac01cb777ca458e1807100016593b7d1150c1810"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:10:05.677839Z","signature_b64":"Wy5AFVpoKp2WeNCZfmk2nFnBXlAxJm1quTkLrupVvxv/LGpcRb94icQr85nZ3/6OdU66ID4KBfhqni6EK8F/DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2026324bcf87e925fd9b98854db81d754352ac3b1911f314fcfb3ad84f8f34c0","last_reissued_at":"2026-05-18T01:10:05.677212Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:10:05.677212Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hyperscaling violation and the shear diffusion constant","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Debangshu Mukherjee, Kedar S. Kolekar, K. Narayan","submitted_at":"2016-04-18T11:18:22Z","abstract_excerpt":"We consider holographic theories in bulk $(d+1)$-dimensions with Lifshitz and hyperscaling violating exponents $z,\\theta$ at finite temperature. By studying shear gravitational modes in the near-horizon region given certain self-consistent approximations, we obtain the corresponding shear diffusion constant on an appropriately defined stretched horizon, adapting the analysis of Kovtun, Son and Starinets. For generic exponents with $d-z-\\theta>-1$, we find that the diffusion constant has power law scaling with the temperature, motivating us to guess a universal relation for the viscosity bound."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.05092","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":"1604.05092","created_at":"2026-05-18T01:10:05.677334+00:00"},{"alias_kind":"arxiv_version","alias_value":"1604.05092v3","created_at":"2026-05-18T01:10:05.677334+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.05092","created_at":"2026-05-18T01:10:05.677334+00:00"},{"alias_kind":"pith_short_12","alias_value":"EATDES6PQ7US","created_at":"2026-05-18T12:30:12.583610+00:00"},{"alias_kind":"pith_short_16","alias_value":"EATDES6PQ7USL7M3","created_at":"2026-05-18T12:30:12.583610+00:00"},{"alias_kind":"pith_short_8","alias_value":"EATDES6P","created_at":"2026-05-18T12:30:12.583610+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/EATDES6PQ7USL7M3TCCU3OA5OV","json":"https://pith.science/pith/EATDES6PQ7USL7M3TCCU3OA5OV.json","graph_json":"https://pith.science/api/pith-number/EATDES6PQ7USL7M3TCCU3OA5OV/graph.json","events_json":"https://pith.science/api/pith-number/EATDES6PQ7USL7M3TCCU3OA5OV/events.json","paper":"https://pith.science/paper/EATDES6P"},"agent_actions":{"view_html":"https://pith.science/pith/EATDES6PQ7USL7M3TCCU3OA5OV","download_json":"https://pith.science/pith/EATDES6PQ7USL7M3TCCU3OA5OV.json","view_paper":"https://pith.science/paper/EATDES6P","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1604.05092&json=true","fetch_graph":"https://pith.science/api/pith-number/EATDES6PQ7USL7M3TCCU3OA5OV/graph.json","fetch_events":"https://pith.science/api/pith-number/EATDES6PQ7USL7M3TCCU3OA5OV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EATDES6PQ7USL7M3TCCU3OA5OV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EATDES6PQ7USL7M3TCCU3OA5OV/action/storage_attestation","attest_author":"https://pith.science/pith/EATDES6PQ7USL7M3TCCU3OA5OV/action/author_attestation","sign_citation":"https://pith.science/pith/EATDES6PQ7USL7M3TCCU3OA5OV/action/citation_signature","submit_replication":"https://pith.science/pith/EATDES6PQ7USL7M3TCCU3OA5OV/action/replication_record"}},"created_at":"2026-05-18T01:10:05.677334+00:00","updated_at":"2026-05-18T01:10:05.677334+00:00"}