{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:DW7K2HJSBRICKRAP6CGUBTFGEN","short_pith_number":"pith:DW7K2HJS","schema_version":"1.0","canonical_sha256":"1dbead1d320c5025440ff08d40cca6235321bcab6a60f743c46f2155885f967c","source":{"kind":"arxiv","id":"2309.14626","version":1},"attestation_state":"computed","paper":{"title":"On Hyperelastic Crease","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.app-ph","authors_text":"Kyung-Suk Kim, Mrityunjay Kothari, Siyuan Song","submitted_at":"2023-09-26T02:31:20Z","abstract_excerpt":"We present analyses of crease-formation and stability criteria for incompressible hyperelastic solids. A generic singular perturbation over a laterally compressed half-space creates a far-field eigenmode of three energy-release angular sectors separated by two energy-elevating sectors of incremental deformation. The far-field eigenmode braces the energy-release field of the surface flaw against the transition to a self-similar crease field, and the braced-incremental-deformation (bid) field has a unique shape factor that determines the creasing stability. The shape factor, which is identified "},"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":"2309.14626","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2023-09-26T02:31:20Z","cross_cats_sorted":[],"title_canon_sha256":"2cd1c299d03d46209feb9b163b1d8822d6ad023f5247285d856c543e2638f2dd","abstract_canon_sha256":"cc8bc6d10edd06ca182991316bfc32e97458ea8002e0ed001245056e0d20be6c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:54:27.815485Z","signature_b64":"9pCfgAmRH22rxZ0RbVQkXS/vWY5rpwpdI0/5u+KAK/Rfz6NAXW54PQxXGG6IIkfrTOOO387aQMnHeiU1qdUDAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1dbead1d320c5025440ff08d40cca6235321bcab6a60f743c46f2155885f967c","last_reissued_at":"2026-07-05T06:54:27.815070Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:54:27.815070Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On Hyperelastic Crease","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.app-ph","authors_text":"Kyung-Suk Kim, Mrityunjay Kothari, Siyuan Song","submitted_at":"2023-09-26T02:31:20Z","abstract_excerpt":"We present analyses of crease-formation and stability criteria for incompressible hyperelastic solids. A generic singular perturbation over a laterally compressed half-space creates a far-field eigenmode of three energy-release angular sectors separated by two energy-elevating sectors of incremental deformation. The far-field eigenmode braces the energy-release field of the surface flaw against the transition to a self-similar crease field, and the braced-incremental-deformation (bid) field has a unique shape factor that determines the creasing stability. The shape factor, which is identified "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2309.14626","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2309.14626/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2309.14626","created_at":"2026-07-05T06:54:27.815132+00:00"},{"alias_kind":"arxiv_version","alias_value":"2309.14626v1","created_at":"2026-07-05T06:54:27.815132+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2309.14626","created_at":"2026-07-05T06:54:27.815132+00:00"},{"alias_kind":"pith_short_12","alias_value":"DW7K2HJSBRIC","created_at":"2026-07-05T06:54:27.815132+00:00"},{"alias_kind":"pith_short_16","alias_value":"DW7K2HJSBRICKRAP","created_at":"2026-07-05T06:54:27.815132+00:00"},{"alias_kind":"pith_short_8","alias_value":"DW7K2HJS","created_at":"2026-07-05T06:54:27.815132+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/DW7K2HJSBRICKRAP6CGUBTFGEN","json":"https://pith.science/pith/DW7K2HJSBRICKRAP6CGUBTFGEN.json","graph_json":"https://pith.science/api/pith-number/DW7K2HJSBRICKRAP6CGUBTFGEN/graph.json","events_json":"https://pith.science/api/pith-number/DW7K2HJSBRICKRAP6CGUBTFGEN/events.json","paper":"https://pith.science/paper/DW7K2HJS"},"agent_actions":{"view_html":"https://pith.science/pith/DW7K2HJSBRICKRAP6CGUBTFGEN","download_json":"https://pith.science/pith/DW7K2HJSBRICKRAP6CGUBTFGEN.json","view_paper":"https://pith.science/paper/DW7K2HJS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2309.14626&json=true","fetch_graph":"https://pith.science/api/pith-number/DW7K2HJSBRICKRAP6CGUBTFGEN/graph.json","fetch_events":"https://pith.science/api/pith-number/DW7K2HJSBRICKRAP6CGUBTFGEN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DW7K2HJSBRICKRAP6CGUBTFGEN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DW7K2HJSBRICKRAP6CGUBTFGEN/action/storage_attestation","attest_author":"https://pith.science/pith/DW7K2HJSBRICKRAP6CGUBTFGEN/action/author_attestation","sign_citation":"https://pith.science/pith/DW7K2HJSBRICKRAP6CGUBTFGEN/action/citation_signature","submit_replication":"https://pith.science/pith/DW7K2HJSBRICKRAP6CGUBTFGEN/action/replication_record"}},"created_at":"2026-07-05T06:54:27.815132+00:00","updated_at":"2026-07-05T06:54:27.815132+00:00"}