{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2005:T3BUHRDU6G2CKNRGRIQO4SSVSL","short_pith_number":"pith:T3BUHRDU","canonical_record":{"source":{"id":"physics/0510119","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"physics.atm-clus","submitted_at":"2005-10-13T12:21:11Z","cross_cats_sorted":[],"title_canon_sha256":"86a5f667da7f48be0bf4ad6f7e7401aadd1913b4330f4241e1c0884fccb32f44","abstract_canon_sha256":"8c9fac3f9ffe4803930165dbebcfa7a3fcc83034f29c45be861461407f514f49"},"schema_version":"1.0"},"canonical_sha256":"9ec343c474f1b42536268a20ee4a5592d966490eb8aa8f8597775a0ab065f975","source":{"kind":"arxiv","id":"physics/0510119","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"physics/0510119","created_at":"2026-05-18T01:08:46Z"},{"alias_kind":"arxiv_version","alias_value":"physics/0510119v1","created_at":"2026-05-18T01:08:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.physics/0510119","created_at":"2026-05-18T01:08:46Z"},{"alias_kind":"pith_short_12","alias_value":"T3BUHRDU6G2C","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_16","alias_value":"T3BUHRDU6G2CKNRG","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_8","alias_value":"T3BUHRDU","created_at":"2026-05-18T12:25:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2005:T3BUHRDU6G2CKNRGRIQO4SSVSL","target":"record","payload":{"canonical_record":{"source":{"id":"physics/0510119","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"physics.atm-clus","submitted_at":"2005-10-13T12:21:11Z","cross_cats_sorted":[],"title_canon_sha256":"86a5f667da7f48be0bf4ad6f7e7401aadd1913b4330f4241e1c0884fccb32f44","abstract_canon_sha256":"8c9fac3f9ffe4803930165dbebcfa7a3fcc83034f29c45be861461407f514f49"},"schema_version":"1.0"},"canonical_sha256":"9ec343c474f1b42536268a20ee4a5592d966490eb8aa8f8597775a0ab065f975","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:08:46.768437Z","signature_b64":"jllqbmj6q9Kp9/u4ysUFccQSN5NHdZj6rXXX8RnfhFCABTcBOzZ3L2yS+xJPgoVgkkQKQ5TqwHsXnFdZgMQWAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9ec343c474f1b42536268a20ee4a5592d966490eb8aa8f8597775a0ab065f975","last_reissued_at":"2026-05-18T01:08:46.767743Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:08:46.767743Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"physics/0510119","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":"2026-05-18T01:08:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"k1T1+venhFvNwR03PTTEjbEKkNxd5wjwkYfloBxS8D/XM0TsmWS8IHJWiU2pC/9fb87pbQuZ7NIPB2w8lQLaAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T03:13:16.920483Z"},"content_sha256":"dcef7fb5cb4ea9cbc9072c8cbfa7e25fc0d7178700614abd8f76e02831f3826c","schema_version":"1.0","event_id":"sha256:dcef7fb5cb4ea9cbc9072c8cbfa7e25fc0d7178700614abd8f76e02831f3826c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2005:T3BUHRDU6G2CKNRGRIQO4SSVSL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Growth kinetics of a nanoprotuberance under the action of an oscillating nanotip","license":"","headline":"","cross_cats":[],"primary_cat":"physics.atm-clus","authors_text":"Denis Michel (CPMOH), Jean-Pierre Aim\\'e (CPMOH), Laurent Nony (L2MP), Rodolphe Boisgard (CPMOH)","submitted_at":"2005-10-13T12:21:11Z","abstract_excerpt":"The atomic force microscope is a versatile tool that allows many routes to be used for investigating the mechanical properties of soft materials on the nanometer scale. In the present work, experiments were performed on polystyrene polymer films of various molecular weight by approaching a vibrating nanotip towards the surface. The variation of the oscillating amplitude of the cantilever is interpreted as the result of the growth process of a nanoprotuberance. The growth rate is found to be dependent of the magnitude of the oscillating amplitude and of the molecular weight. A model is develope"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"physics/0510119","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":"2026-05-18T01:08:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pLZ4iXxnh2q5f+WKrdMoUN/uoK4osx83QnJ4pGiGMJyoS+DfbI1u7KwdQLkww9tHZZAiLRkg6O2OSymOF+ILBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T03:13:16.920827Z"},"content_sha256":"3cc063f889b3a3b8f423ee3564eaf04447fd86e36bce3487692807e42fc955ed","schema_version":"1.0","event_id":"sha256:3cc063f889b3a3b8f423ee3564eaf04447fd86e36bce3487692807e42fc955ed"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/T3BUHRDU6G2CKNRGRIQO4SSVSL/bundle.json","state_url":"https://pith.science/pith/T3BUHRDU6G2CKNRGRIQO4SSVSL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/T3BUHRDU6G2CKNRGRIQO4SSVSL/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":"2026-06-24T03:13:16Z","links":{"resolver":"https://pith.science/pith/T3BUHRDU6G2CKNRGRIQO4SSVSL","bundle":"https://pith.science/pith/T3BUHRDU6G2CKNRGRIQO4SSVSL/bundle.json","state":"https://pith.science/pith/T3BUHRDU6G2CKNRGRIQO4SSVSL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/T3BUHRDU6G2CKNRGRIQO4SSVSL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2005:T3BUHRDU6G2CKNRGRIQO4SSVSL","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":"8c9fac3f9ffe4803930165dbebcfa7a3fcc83034f29c45be861461407f514f49","cross_cats_sorted":[],"license":"","primary_cat":"physics.atm-clus","submitted_at":"2005-10-13T12:21:11Z","title_canon_sha256":"86a5f667da7f48be0bf4ad6f7e7401aadd1913b4330f4241e1c0884fccb32f44"},"schema_version":"1.0","source":{"id":"physics/0510119","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"physics/0510119","created_at":"2026-05-18T01:08:46Z"},{"alias_kind":"arxiv_version","alias_value":"physics/0510119v1","created_at":"2026-05-18T01:08:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.physics/0510119","created_at":"2026-05-18T01:08:46Z"},{"alias_kind":"pith_short_12","alias_value":"T3BUHRDU6G2C","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_16","alias_value":"T3BUHRDU6G2CKNRG","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_8","alias_value":"T3BUHRDU","created_at":"2026-05-18T12:25:53Z"}],"graph_snapshots":[{"event_id":"sha256:3cc063f889b3a3b8f423ee3564eaf04447fd86e36bce3487692807e42fc955ed","target":"graph","created_at":"2026-05-18T01:08:46Z","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":"The atomic force microscope is a versatile tool that allows many routes to be used for investigating the mechanical properties of soft materials on the nanometer scale. In the present work, experiments were performed on polystyrene polymer films of various molecular weight by approaching a vibrating nanotip towards the surface. The variation of the oscillating amplitude of the cantilever is interpreted as the result of the growth process of a nanoprotuberance. The growth rate is found to be dependent of the magnitude of the oscillating amplitude and of the molecular weight. A model is develope","authors_text":"Denis Michel (CPMOH), Jean-Pierre Aim\\'e (CPMOH), Laurent Nony (L2MP), Rodolphe Boisgard (CPMOH)","cross_cats":[],"headline":"","license":"","primary_cat":"physics.atm-clus","submitted_at":"2005-10-13T12:21:11Z","title":"Growth kinetics of a nanoprotuberance under the action of an oscillating nanotip"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"physics/0510119","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:dcef7fb5cb4ea9cbc9072c8cbfa7e25fc0d7178700614abd8f76e02831f3826c","target":"record","created_at":"2026-05-18T01:08:46Z","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":"8c9fac3f9ffe4803930165dbebcfa7a3fcc83034f29c45be861461407f514f49","cross_cats_sorted":[],"license":"","primary_cat":"physics.atm-clus","submitted_at":"2005-10-13T12:21:11Z","title_canon_sha256":"86a5f667da7f48be0bf4ad6f7e7401aadd1913b4330f4241e1c0884fccb32f44"},"schema_version":"1.0","source":{"id":"physics/0510119","kind":"arxiv","version":1}},"canonical_sha256":"9ec343c474f1b42536268a20ee4a5592d966490eb8aa8f8597775a0ab065f975","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9ec343c474f1b42536268a20ee4a5592d966490eb8aa8f8597775a0ab065f975","first_computed_at":"2026-05-18T01:08:46.767743Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:08:46.767743Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"jllqbmj6q9Kp9/u4ysUFccQSN5NHdZj6rXXX8RnfhFCABTcBOzZ3L2yS+xJPgoVgkkQKQ5TqwHsXnFdZgMQWAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:08:46.768437Z","signed_message":"canonical_sha256_bytes"},"source_id":"physics/0510119","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:dcef7fb5cb4ea9cbc9072c8cbfa7e25fc0d7178700614abd8f76e02831f3826c","sha256:3cc063f889b3a3b8f423ee3564eaf04447fd86e36bce3487692807e42fc955ed"],"state_sha256":"d5f94b2d8aadf74b7aab0e7a54554dc40316704891990faca8c19820d476818d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cWu2EMUslsCzFbEEwk8l0Ke2V3ICvLO1V4OEfu/OgmC3P6Lxurf4f2DrNqmmW+SdoTrOTUYKEw6y8Pe1fuDhAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-24T03:13:16.922766Z","bundle_sha256":"451fcbddff9c67dce39f6f77778fc109211f53c8b2257a90f64cfb7e9744e5d7"}}