{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:W2PKFWFBOKJ7XZQSB3WIZ7T6RF","short_pith_number":"pith:W2PKFWFB","canonical_record":{"source":{"id":"1807.02497","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2018-07-06T17:31:36Z","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.mtrl-sci","cond-mat.stat-mech"],"title_canon_sha256":"ec9e151262b3f3a3a05da544b72504897cd583eaeb998ca0383d247c5b1c7b19","abstract_canon_sha256":"a458fdfb26c575c977fda7f4d0ef2c45668a9f303ccf5d053c922bc84d6c0539"},"schema_version":"1.0"},"canonical_sha256":"b69ea2d8a17293fbe6120eec8cfe7e897fc53e5a3670cfa7ec464a0646ff1d77","source":{"kind":"arxiv","id":"1807.02497","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1807.02497","created_at":"2026-05-18T00:04:33Z"},{"alias_kind":"arxiv_version","alias_value":"1807.02497v2","created_at":"2026-05-18T00:04:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.02497","created_at":"2026-05-18T00:04:33Z"},{"alias_kind":"pith_short_12","alias_value":"W2PKFWFBOKJ7","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_16","alias_value":"W2PKFWFBOKJ7XZQS","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_8","alias_value":"W2PKFWFB","created_at":"2026-05-18T12:32:59Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:W2PKFWFBOKJ7XZQSB3WIZ7T6RF","target":"record","payload":{"canonical_record":{"source":{"id":"1807.02497","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2018-07-06T17:31:36Z","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.mtrl-sci","cond-mat.stat-mech"],"title_canon_sha256":"ec9e151262b3f3a3a05da544b72504897cd583eaeb998ca0383d247c5b1c7b19","abstract_canon_sha256":"a458fdfb26c575c977fda7f4d0ef2c45668a9f303ccf5d053c922bc84d6c0539"},"schema_version":"1.0"},"canonical_sha256":"b69ea2d8a17293fbe6120eec8cfe7e897fc53e5a3670cfa7ec464a0646ff1d77","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:04:33.966206Z","signature_b64":"1XBaOPZZFQgXAFPE/FJTVTle+pZ0nijsQnjubK8wZM7uWisWPQlzIxt10gf7Myxu5yB55E99WhkFSo4wNKlsBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b69ea2d8a17293fbe6120eec8cfe7e897fc53e5a3670cfa7ec464a0646ff1d77","last_reissued_at":"2026-05-18T00:04:33.965668Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:04:33.965668Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1807.02497","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:04:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nDK5IxZS3JualVp6Q/LS0hF87mnjvt9wlQqbhCHbyB2x1gxqm0LY/is+Msvpk6mJfrAc5MJasMxJVvR9vLZJCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T09:28:37.057839Z"},"content_sha256":"fd8a39e0b1890634ee58e650038188c9a19bb03f709976819ead4e277b7310c2","schema_version":"1.0","event_id":"sha256:fd8a39e0b1890634ee58e650038188c9a19bb03f709976819ead4e277b7310c2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:W2PKFWFBOKJ7XZQSB3WIZ7T6RF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Creep dynamics of athermal amorphous materials: a mesoscopic approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn","cond-mat.mtrl-sci","cond-mat.stat-mech"],"primary_cat":"cond-mat.soft","authors_text":"Chen Liu, Ezequiel E. Ferrero, Jean-Louis Barrat, Kirsten Martens","submitted_at":"2018-07-06T17:31:36Z","abstract_excerpt":"Yield stress fluids display complex dynamics, in particular when driven into the transient regime between the solid and the flowing state. Inspired by creep experiments on dense amorphous materials, we implement mesocale elasto-plastic descriptions to analyze such transient dynamics in athermal systems. Both our mean-field and space-dependent approaches consistently reproduce the typical experimental strain rate responses to different applied steps in stress. Moreover, they allow us to understand basic processes involved in the strain rate slowing down (creep) and the strain rate acceleration "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.02497","kind":"arxiv","version":2},"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":"2026-05-18T00:04:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RHM+WVkKDrjLd6dNcMbCV5FIVitAJFmTP+DwBfmHPt7sgrldDd09W0tirCzs0cZ8FWgorov4tces2nZCmWDkAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T09:28:37.058277Z"},"content_sha256":"3ad08141890d08956a4c9e80c109c7307480c8d5a6bda10a8839fd41a5260a29","schema_version":"1.0","event_id":"sha256:3ad08141890d08956a4c9e80c109c7307480c8d5a6bda10a8839fd41a5260a29"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/W2PKFWFBOKJ7XZQSB3WIZ7T6RF/bundle.json","state_url":"https://pith.science/pith/W2PKFWFBOKJ7XZQSB3WIZ7T6RF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/W2PKFWFBOKJ7XZQSB3WIZ7T6RF/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":"2026-05-27T09:28:37Z","links":{"resolver":"https://pith.science/pith/W2PKFWFBOKJ7XZQSB3WIZ7T6RF","bundle":"https://pith.science/pith/W2PKFWFBOKJ7XZQSB3WIZ7T6RF/bundle.json","state":"https://pith.science/pith/W2PKFWFBOKJ7XZQSB3WIZ7T6RF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/W2PKFWFBOKJ7XZQSB3WIZ7T6RF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:W2PKFWFBOKJ7XZQSB3WIZ7T6RF","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":"a458fdfb26c575c977fda7f4d0ef2c45668a9f303ccf5d053c922bc84d6c0539","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.mtrl-sci","cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2018-07-06T17:31:36Z","title_canon_sha256":"ec9e151262b3f3a3a05da544b72504897cd583eaeb998ca0383d247c5b1c7b19"},"schema_version":"1.0","source":{"id":"1807.02497","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1807.02497","created_at":"2026-05-18T00:04:33Z"},{"alias_kind":"arxiv_version","alias_value":"1807.02497v2","created_at":"2026-05-18T00:04:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.02497","created_at":"2026-05-18T00:04:33Z"},{"alias_kind":"pith_short_12","alias_value":"W2PKFWFBOKJ7","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_16","alias_value":"W2PKFWFBOKJ7XZQS","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_8","alias_value":"W2PKFWFB","created_at":"2026-05-18T12:32:59Z"}],"graph_snapshots":[{"event_id":"sha256:3ad08141890d08956a4c9e80c109c7307480c8d5a6bda10a8839fd41a5260a29","target":"graph","created_at":"2026-05-18T00:04:33Z","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":"Yield stress fluids display complex dynamics, in particular when driven into the transient regime between the solid and the flowing state. Inspired by creep experiments on dense amorphous materials, we implement mesocale elasto-plastic descriptions to analyze such transient dynamics in athermal systems. Both our mean-field and space-dependent approaches consistently reproduce the typical experimental strain rate responses to different applied steps in stress. Moreover, they allow us to understand basic processes involved in the strain rate slowing down (creep) and the strain rate acceleration ","authors_text":"Chen Liu, Ezequiel E. Ferrero, Jean-Louis Barrat, Kirsten Martens","cross_cats":["cond-mat.dis-nn","cond-mat.mtrl-sci","cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2018-07-06T17:31:36Z","title":"Creep dynamics of athermal amorphous materials: a mesoscopic approach"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.02497","kind":"arxiv","version":2},"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:fd8a39e0b1890634ee58e650038188c9a19bb03f709976819ead4e277b7310c2","target":"record","created_at":"2026-05-18T00:04:33Z","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":"a458fdfb26c575c977fda7f4d0ef2c45668a9f303ccf5d053c922bc84d6c0539","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.mtrl-sci","cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2018-07-06T17:31:36Z","title_canon_sha256":"ec9e151262b3f3a3a05da544b72504897cd583eaeb998ca0383d247c5b1c7b19"},"schema_version":"1.0","source":{"id":"1807.02497","kind":"arxiv","version":2}},"canonical_sha256":"b69ea2d8a17293fbe6120eec8cfe7e897fc53e5a3670cfa7ec464a0646ff1d77","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b69ea2d8a17293fbe6120eec8cfe7e897fc53e5a3670cfa7ec464a0646ff1d77","first_computed_at":"2026-05-18T00:04:33.965668Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:04:33.965668Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"1XBaOPZZFQgXAFPE/FJTVTle+pZ0nijsQnjubK8wZM7uWisWPQlzIxt10gf7Myxu5yB55E99WhkFSo4wNKlsBA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:04:33.966206Z","signed_message":"canonical_sha256_bytes"},"source_id":"1807.02497","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fd8a39e0b1890634ee58e650038188c9a19bb03f709976819ead4e277b7310c2","sha256:3ad08141890d08956a4c9e80c109c7307480c8d5a6bda10a8839fd41a5260a29"],"state_sha256":"3a89b2bbc8087281c63865f1aff21b1e18dc1b95f9c64a100648f9697e70e100"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lnURLyvg4bBJwtQTPSXpzK8XxkCpoGPSNh55JOwbk6Ty5FZ5GcALPMPS3HvRnEVL/GnOujxqtu/xX460WSErBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T09:28:37.061797Z","bundle_sha256":"ad2e5388f3e98ef2678914717a54ecdeeeda714ffda71b154f20c95f6280db33"}}