{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:SRIQEXCERJNRINEWFXVREYQ6SD","short_pith_number":"pith:SRIQEXCE","canonical_record":{"source":{"id":"1405.5446","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.AP","submitted_at":"2014-05-21T14:57:19Z","cross_cats_sorted":[],"title_canon_sha256":"596587fc503ff28a8a51394ba68d2aa7500d6f1218f22f9b14fc35e3ccf1a84e","abstract_canon_sha256":"9b9566f3ced5987a85beb7096f1ed25bd57d8f2435df8ec3678b1072017c1daa"},"schema_version":"1.0"},"canonical_sha256":"9451025c448a5b1434962deb12621e90fa0c633da33f85dc5338e6bc16be5ad0","source":{"kind":"arxiv","id":"1405.5446","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1405.5446","created_at":"2026-05-18T02:51:24Z"},{"alias_kind":"arxiv_version","alias_value":"1405.5446v1","created_at":"2026-05-18T02:51:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1405.5446","created_at":"2026-05-18T02:51:24Z"},{"alias_kind":"pith_short_12","alias_value":"SRIQEXCERJNR","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_16","alias_value":"SRIQEXCERJNRINEW","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_8","alias_value":"SRIQEXCE","created_at":"2026-05-18T12:28:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:SRIQEXCERJNRINEWFXVREYQ6SD","target":"record","payload":{"canonical_record":{"source":{"id":"1405.5446","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.AP","submitted_at":"2014-05-21T14:57:19Z","cross_cats_sorted":[],"title_canon_sha256":"596587fc503ff28a8a51394ba68d2aa7500d6f1218f22f9b14fc35e3ccf1a84e","abstract_canon_sha256":"9b9566f3ced5987a85beb7096f1ed25bd57d8f2435df8ec3678b1072017c1daa"},"schema_version":"1.0"},"canonical_sha256":"9451025c448a5b1434962deb12621e90fa0c633da33f85dc5338e6bc16be5ad0","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:51:24.178273Z","signature_b64":"SwjivDJZz3B6NSWaTTsui3pK1lGCgwQkg73pvSY/qKmh2ixbupXf5KmmwNa5Ah7CryMqvYdhEDiLknzxBYB7BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9451025c448a5b1434962deb12621e90fa0c633da33f85dc5338e6bc16be5ad0","last_reissued_at":"2026-05-18T02:51:24.177705Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:51:24.177705Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1405.5446","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:51:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Jmm6M8BGih3TzV0UGRBJL3ZVB8rgsgwVQEiEi7DtsPr8X8f5T8ZkPnoBE30sJyzz4a5HPXUcJkchvnR96AFkBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T08:13:52.981211Z"},"content_sha256":"938fabe64f9ff7f02a37ace34a839f7a63682b8be8b5a7efafe7fdd14bc24b3e","schema_version":"1.0","event_id":"sha256:938fabe64f9ff7f02a37ace34a839f7a63682b8be8b5a7efafe7fdd14bc24b3e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:SRIQEXCERJNRINEWFXVREYQ6SD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Asymptotic analysis of a Neumann problem in a domain with cusp. Application to the collision problem of rigid bodies in a perfect fluid","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"math.AP","authors_text":"Alexandre Munnier (INRIA Nancy - Grand Est / IECN / LMAM), IECL), Karim Ramdani (INRIA Nancy - Grand Est / IECN / LMAM","submitted_at":"2014-05-21T14:57:19Z","abstract_excerpt":"We study a two dimensional collision problem for a rigid solid immersed in a cavity filled with a perfect fluid. We are led to investigate the asymptotic behavior of the Dirichlet energy associated to the solution of a Laplace Neumann problem as the distance $\\varepsilon>0$ between the solid and the cavity's bottom tends to zero. Denoting by $\\alpha>0$ the tangency exponent at the contact point, we prove that the solid always reaches the cavity in finite time, but with a non zero velocity for $\\alpha <2$ (real shock case), and with null velocity for $\\alpha \\geqslant 2$ (smooth landing case). "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1405.5446","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":""},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:51:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"K/x33NvQYtOTf8DjJI2p2iHic6ngzaK7LYM96dryEFkFgzm4oWI0aO6B8MTe0GccfQf7HMaA+TjKyst1/i5pCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T08:13:52.981703Z"},"content_sha256":"468c8ffb3d913122c2aa79bd036dee01b0783d11e0d59306c3ba1c1f07f19f11","schema_version":"1.0","event_id":"sha256:468c8ffb3d913122c2aa79bd036dee01b0783d11e0d59306c3ba1c1f07f19f11"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/SRIQEXCERJNRINEWFXVREYQ6SD/bundle.json","state_url":"https://pith.science/pith/SRIQEXCERJNRINEWFXVREYQ6SD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/SRIQEXCERJNRINEWFXVREYQ6SD/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-21T08:13:52Z","links":{"resolver":"https://pith.science/pith/SRIQEXCERJNRINEWFXVREYQ6SD","bundle":"https://pith.science/pith/SRIQEXCERJNRINEWFXVREYQ6SD/bundle.json","state":"https://pith.science/pith/SRIQEXCERJNRINEWFXVREYQ6SD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/SRIQEXCERJNRINEWFXVREYQ6SD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:SRIQEXCERJNRINEWFXVREYQ6SD","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"9b9566f3ced5987a85beb7096f1ed25bd57d8f2435df8ec3678b1072017c1daa","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.AP","submitted_at":"2014-05-21T14:57:19Z","title_canon_sha256":"596587fc503ff28a8a51394ba68d2aa7500d6f1218f22f9b14fc35e3ccf1a84e"},"schema_version":"1.0","source":{"id":"1405.5446","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1405.5446","created_at":"2026-05-18T02:51:24Z"},{"alias_kind":"arxiv_version","alias_value":"1405.5446v1","created_at":"2026-05-18T02:51:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1405.5446","created_at":"2026-05-18T02:51:24Z"},{"alias_kind":"pith_short_12","alias_value":"SRIQEXCERJNR","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_16","alias_value":"SRIQEXCERJNRINEW","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_8","alias_value":"SRIQEXCE","created_at":"2026-05-18T12:28:49Z"}],"graph_snapshots":[{"event_id":"sha256:468c8ffb3d913122c2aa79bd036dee01b0783d11e0d59306c3ba1c1f07f19f11","target":"graph","created_at":"2026-05-18T02:51:24Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We study a two dimensional collision problem for a rigid solid immersed in a cavity filled with a perfect fluid. We are led to investigate the asymptotic behavior of the Dirichlet energy associated to the solution of a Laplace Neumann problem as the distance $\\varepsilon>0$ between the solid and the cavity's bottom tends to zero. Denoting by $\\alpha>0$ the tangency exponent at the contact point, we prove that the solid always reaches the cavity in finite time, but with a non zero velocity for $\\alpha <2$ (real shock case), and with null velocity for $\\alpha \\geqslant 2$ (smooth landing case). ","authors_text":"Alexandre Munnier (INRIA Nancy - Grand Est / IECN / LMAM), IECL), Karim Ramdani (INRIA Nancy - Grand Est / IECN / LMAM","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.AP","submitted_at":"2014-05-21T14:57:19Z","title":"Asymptotic analysis of a Neumann problem in a domain with cusp. Application to the collision problem of rigid bodies in a perfect fluid"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1405.5446","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:938fabe64f9ff7f02a37ace34a839f7a63682b8be8b5a7efafe7fdd14bc24b3e","target":"record","created_at":"2026-05-18T02:51:24Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"9b9566f3ced5987a85beb7096f1ed25bd57d8f2435df8ec3678b1072017c1daa","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.AP","submitted_at":"2014-05-21T14:57:19Z","title_canon_sha256":"596587fc503ff28a8a51394ba68d2aa7500d6f1218f22f9b14fc35e3ccf1a84e"},"schema_version":"1.0","source":{"id":"1405.5446","kind":"arxiv","version":1}},"canonical_sha256":"9451025c448a5b1434962deb12621e90fa0c633da33f85dc5338e6bc16be5ad0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9451025c448a5b1434962deb12621e90fa0c633da33f85dc5338e6bc16be5ad0","first_computed_at":"2026-05-18T02:51:24.177705Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:51:24.177705Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"SwjivDJZz3B6NSWaTTsui3pK1lGCgwQkg73pvSY/qKmh2ixbupXf5KmmwNa5Ah7CryMqvYdhEDiLknzxBYB7BQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:51:24.178273Z","signed_message":"canonical_sha256_bytes"},"source_id":"1405.5446","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:938fabe64f9ff7f02a37ace34a839f7a63682b8be8b5a7efafe7fdd14bc24b3e","sha256:468c8ffb3d913122c2aa79bd036dee01b0783d11e0d59306c3ba1c1f07f19f11"],"state_sha256":"3277352d1258c9e260c98fd068f1f85c38530574a33365eee435ddea14e2662a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7GDea9yF0SQhSDFq4p5mg1ECOOOMhkifSr3D286h9c66CJQ0rK+Vp3ikDDrzYLqnYeakTKOtO2tpVxGaLgZJAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-21T08:13:52.984699Z","bundle_sha256":"77f763f200bb1e84d9e2d2e2d518e92edfa2688ed42f56baab5b5734b7f98a62"}}