{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:4R2L7HA2ZXCXL4Y53HDOPFYNSQ","short_pith_number":"pith:4R2L7HA2","schema_version":"1.0","canonical_sha256":"e474bf9c1acdc575f31dd9c6e7970d940e910c85efdde2e4fba6d52e07d10aa1","source":{"kind":"arxiv","id":"1711.08855","version":4},"attestation_state":"computed","paper":{"title":"Theory for the rheology of dense non-Brownian suspensions: divergence of viscosities and $\\mu$-$J$ rheology","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.soft","authors_text":"Hisao Hayakawa, Koshiro Suzuki","submitted_at":"2017-11-24T01:40:14Z","abstract_excerpt":"A systematic microscopic theory for the rheology of dense non-Brownian suspensions characterized by the volume fraction $\\varphi$ is developed. The theory successfully derives the critical behavior in the vicinity of the jamming point (volume fraction $\\varphi_{J}$), for both the pressure $P$ and the shear stress $\\sigma_{xy}$, i.e. $P \\sim \\sigma_{xy} \\sim \\dot\\gamma \\eta_0 \\delta\\varphi^{-2}$, where $\\dot\\gamma$ is the shear rate, $\\eta_0$ is the shear viscosity of the solvent, and $\\delta\\varphi = \\varphi_J - \\varphi > 0$ is the distance from the jamming point. It also successfully describe"},"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":"1711.08855","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2017-11-24T01:40:14Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"4fa0f3e8bd666fb1536d2f43029b7e7a75e5627eecf743ffa1b86e73c85fc76d","abstract_canon_sha256":"30b7d9d8a0ebb50d37acb3387a3d39b265c60b1890a5b5cd3142d2cabcdbe959"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:53:51.905711Z","signature_b64":"1uv6g2RQdBlh8KH2awlbwdgHyWiq0d3U+eVRTlOubC1W7LlDAQuDorQOMX+2QQzRfaSQ0XMc0DHGRT9TtCjsDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e474bf9c1acdc575f31dd9c6e7970d940e910c85efdde2e4fba6d52e07d10aa1","last_reissued_at":"2026-05-17T23:53:51.905011Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:53:51.905011Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Theory for the rheology of dense non-Brownian suspensions: divergence of viscosities and $\\mu$-$J$ rheology","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.soft","authors_text":"Hisao Hayakawa, Koshiro Suzuki","submitted_at":"2017-11-24T01:40:14Z","abstract_excerpt":"A systematic microscopic theory for the rheology of dense non-Brownian suspensions characterized by the volume fraction $\\varphi$ is developed. The theory successfully derives the critical behavior in the vicinity of the jamming point (volume fraction $\\varphi_{J}$), for both the pressure $P$ and the shear stress $\\sigma_{xy}$, i.e. $P \\sim \\sigma_{xy} \\sim \\dot\\gamma \\eta_0 \\delta\\varphi^{-2}$, where $\\dot\\gamma$ is the shear rate, $\\eta_0$ is the shear viscosity of the solvent, and $\\delta\\varphi = \\varphi_J - \\varphi > 0$ is the distance from the jamming point. It also successfully describe"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.08855","kind":"arxiv","version":4},"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":"1711.08855","created_at":"2026-05-17T23:53:51.905123+00:00"},{"alias_kind":"arxiv_version","alias_value":"1711.08855v4","created_at":"2026-05-17T23:53:51.905123+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.08855","created_at":"2026-05-17T23:53:51.905123+00:00"},{"alias_kind":"pith_short_12","alias_value":"4R2L7HA2ZXCX","created_at":"2026-05-18T12:31:00.734936+00:00"},{"alias_kind":"pith_short_16","alias_value":"4R2L7HA2ZXCXL4Y5","created_at":"2026-05-18T12:31:00.734936+00:00"},{"alias_kind":"pith_short_8","alias_value":"4R2L7HA2","created_at":"2026-05-18T12:31:00.734936+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/4R2L7HA2ZXCXL4Y53HDOPFYNSQ","json":"https://pith.science/pith/4R2L7HA2ZXCXL4Y53HDOPFYNSQ.json","graph_json":"https://pith.science/api/pith-number/4R2L7HA2ZXCXL4Y53HDOPFYNSQ/graph.json","events_json":"https://pith.science/api/pith-number/4R2L7HA2ZXCXL4Y53HDOPFYNSQ/events.json","paper":"https://pith.science/paper/4R2L7HA2"},"agent_actions":{"view_html":"https://pith.science/pith/4R2L7HA2ZXCXL4Y53HDOPFYNSQ","download_json":"https://pith.science/pith/4R2L7HA2ZXCXL4Y53HDOPFYNSQ.json","view_paper":"https://pith.science/paper/4R2L7HA2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1711.08855&json=true","fetch_graph":"https://pith.science/api/pith-number/4R2L7HA2ZXCXL4Y53HDOPFYNSQ/graph.json","fetch_events":"https://pith.science/api/pith-number/4R2L7HA2ZXCXL4Y53HDOPFYNSQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4R2L7HA2ZXCXL4Y53HDOPFYNSQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4R2L7HA2ZXCXL4Y53HDOPFYNSQ/action/storage_attestation","attest_author":"https://pith.science/pith/4R2L7HA2ZXCXL4Y53HDOPFYNSQ/action/author_attestation","sign_citation":"https://pith.science/pith/4R2L7HA2ZXCXL4Y53HDOPFYNSQ/action/citation_signature","submit_replication":"https://pith.science/pith/4R2L7HA2ZXCXL4Y53HDOPFYNSQ/action/replication_record"}},"created_at":"2026-05-17T23:53:51.905123+00:00","updated_at":"2026-05-17T23:53:51.905123+00:00"}