{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:GN7Z4OQWVV3BK6JT4FEVPNUYBV","short_pith_number":"pith:GN7Z4OQW","canonical_record":{"source":{"id":"1106.3160","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2011-06-16T07:03:15Z","cross_cats_sorted":["physics.comp-ph"],"title_canon_sha256":"a9bac5f65b90504b7ef6dac8f478d8e8f10e7798272494252d5a30e560e1f8d3","abstract_canon_sha256":"9631e443962672e91b96fcf90f954a1be6cd7005ad0647ef477e2cf9100f2a98"},"schema_version":"1.0"},"canonical_sha256":"337f9e3a16ad76157933e14957b6980d609689f86c06461c43e806ce6cd20703","source":{"kind":"arxiv","id":"1106.3160","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1106.3160","created_at":"2026-05-18T03:44:02Z"},{"alias_kind":"arxiv_version","alias_value":"1106.3160v2","created_at":"2026-05-18T03:44:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.3160","created_at":"2026-05-18T03:44:02Z"},{"alias_kind":"pith_short_12","alias_value":"GN7Z4OQWVV3B","created_at":"2026-05-18T12:26:30Z"},{"alias_kind":"pith_short_16","alias_value":"GN7Z4OQWVV3BK6JT","created_at":"2026-05-18T12:26:30Z"},{"alias_kind":"pith_short_8","alias_value":"GN7Z4OQW","created_at":"2026-05-18T12:26:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:GN7Z4OQWVV3BK6JT4FEVPNUYBV","target":"record","payload":{"canonical_record":{"source":{"id":"1106.3160","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2011-06-16T07:03:15Z","cross_cats_sorted":["physics.comp-ph"],"title_canon_sha256":"a9bac5f65b90504b7ef6dac8f478d8e8f10e7798272494252d5a30e560e1f8d3","abstract_canon_sha256":"9631e443962672e91b96fcf90f954a1be6cd7005ad0647ef477e2cf9100f2a98"},"schema_version":"1.0"},"canonical_sha256":"337f9e3a16ad76157933e14957b6980d609689f86c06461c43e806ce6cd20703","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:44:02.851834Z","signature_b64":"Ej2MvhL19QTy+kHi2DxZSiVby+L/clOt+dod2LP7PqdZYWaX5IQp/E/Kt821+cub2nBUgA9Z4onCWGVIXu90Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"337f9e3a16ad76157933e14957b6980d609689f86c06461c43e806ce6cd20703","last_reissued_at":"2026-05-18T03:44:02.851007Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:44:02.851007Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1106.3160","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":"2026-05-18T03:44:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HCfz6oEvH4cq5Z9W/pXJYfnZYUJvF12lUZMq15dgX1TptPttjzj/6firbb5oWJJZJTnSkDk2GIWC6/A85buzDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T07:10:23.896357Z"},"content_sha256":"67fe26448b907c87b01eabbc3e8740c9c5986b14df9648ea84982910f58cd08e","schema_version":"1.0","event_id":"sha256:67fe26448b907c87b01eabbc3e8740c9c5986b14df9648ea84982910f58cd08e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:GN7Z4OQWVV3BK6JT4FEVPNUYBV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Silicon dry oxidation kinetics at low temperature in the nanometric range: Modeling and experiment","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.comp-ph"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Christophe Krzeminski (IEMN), Emmanuel Dubois (IEMN), Evelyne Lampin (IEMN), Guilhem Larrieu (IEMN), Julien Penaud (IEMN)","submitted_at":"2011-06-16T07:03:15Z","abstract_excerpt":"Kinetics of silicon dry oxidation are investigated theoretically and experimentally at low temperature in the nanometer range where the limits of the Deal and Grove model becomes critical. Based on a fine control of the oxidation process conditions, experiments allow the investigation of the growth kinetics of nanometric oxide layer. The theoretical model is formulated using a reaction rate approach. In this framework, the oxide thickness is estimated with the evolution of the various species during the reaction. Standard oxidation models and the reaction rate approach are confronted with thes"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.3160","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":"2026-05-18T03:44:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"l0AGvRaIyBbQVbzTtHGFn1n+/0SwL8N9N/C7zkhGWc3jttiWNVslQxF7mRHNbUzr8s8J56JkVoIWZ06iqEEHDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T07:10:23.896716Z"},"content_sha256":"b85a90ab7090ccba33f451d97ea906ec33b4c81f0a65b4b9220a31c35247c478","schema_version":"1.0","event_id":"sha256:b85a90ab7090ccba33f451d97ea906ec33b4c81f0a65b4b9220a31c35247c478"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GN7Z4OQWVV3BK6JT4FEVPNUYBV/bundle.json","state_url":"https://pith.science/pith/GN7Z4OQWVV3BK6JT4FEVPNUYBV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GN7Z4OQWVV3BK6JT4FEVPNUYBV/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":"2026-06-24T07:10:23Z","links":{"resolver":"https://pith.science/pith/GN7Z4OQWVV3BK6JT4FEVPNUYBV","bundle":"https://pith.science/pith/GN7Z4OQWVV3BK6JT4FEVPNUYBV/bundle.json","state":"https://pith.science/pith/GN7Z4OQWVV3BK6JT4FEVPNUYBV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GN7Z4OQWVV3BK6JT4FEVPNUYBV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:GN7Z4OQWVV3BK6JT4FEVPNUYBV","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":"9631e443962672e91b96fcf90f954a1be6cd7005ad0647ef477e2cf9100f2a98","cross_cats_sorted":["physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2011-06-16T07:03:15Z","title_canon_sha256":"a9bac5f65b90504b7ef6dac8f478d8e8f10e7798272494252d5a30e560e1f8d3"},"schema_version":"1.0","source":{"id":"1106.3160","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1106.3160","created_at":"2026-05-18T03:44:02Z"},{"alias_kind":"arxiv_version","alias_value":"1106.3160v2","created_at":"2026-05-18T03:44:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.3160","created_at":"2026-05-18T03:44:02Z"},{"alias_kind":"pith_short_12","alias_value":"GN7Z4OQWVV3B","created_at":"2026-05-18T12:26:30Z"},{"alias_kind":"pith_short_16","alias_value":"GN7Z4OQWVV3BK6JT","created_at":"2026-05-18T12:26:30Z"},{"alias_kind":"pith_short_8","alias_value":"GN7Z4OQW","created_at":"2026-05-18T12:26:30Z"}],"graph_snapshots":[{"event_id":"sha256:b85a90ab7090ccba33f451d97ea906ec33b4c81f0a65b4b9220a31c35247c478","target":"graph","created_at":"2026-05-18T03:44:02Z","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":"Kinetics of silicon dry oxidation are investigated theoretically and experimentally at low temperature in the nanometer range where the limits of the Deal and Grove model becomes critical. Based on a fine control of the oxidation process conditions, experiments allow the investigation of the growth kinetics of nanometric oxide layer. The theoretical model is formulated using a reaction rate approach. In this framework, the oxide thickness is estimated with the evolution of the various species during the reaction. Standard oxidation models and the reaction rate approach are confronted with thes","authors_text":"Christophe Krzeminski (IEMN), Emmanuel Dubois (IEMN), Evelyne Lampin (IEMN), Guilhem Larrieu (IEMN), Julien Penaud (IEMN)","cross_cats":["physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2011-06-16T07:03:15Z","title":"Silicon dry oxidation kinetics at low temperature in the nanometric range: Modeling and experiment"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.3160","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":"sha256:67fe26448b907c87b01eabbc3e8740c9c5986b14df9648ea84982910f58cd08e","target":"record","created_at":"2026-05-18T03:44:02Z","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":"9631e443962672e91b96fcf90f954a1be6cd7005ad0647ef477e2cf9100f2a98","cross_cats_sorted":["physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2011-06-16T07:03:15Z","title_canon_sha256":"a9bac5f65b90504b7ef6dac8f478d8e8f10e7798272494252d5a30e560e1f8d3"},"schema_version":"1.0","source":{"id":"1106.3160","kind":"arxiv","version":2}},"canonical_sha256":"337f9e3a16ad76157933e14957b6980d609689f86c06461c43e806ce6cd20703","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"337f9e3a16ad76157933e14957b6980d609689f86c06461c43e806ce6cd20703","first_computed_at":"2026-05-18T03:44:02.851007Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:44:02.851007Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Ej2MvhL19QTy+kHi2DxZSiVby+L/clOt+dod2LP7PqdZYWaX5IQp/E/Kt821+cub2nBUgA9Z4onCWGVIXu90Ag==","signature_status":"signed_v1","signed_at":"2026-05-18T03:44:02.851834Z","signed_message":"canonical_sha256_bytes"},"source_id":"1106.3160","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:67fe26448b907c87b01eabbc3e8740c9c5986b14df9648ea84982910f58cd08e","sha256:b85a90ab7090ccba33f451d97ea906ec33b4c81f0a65b4b9220a31c35247c478"],"state_sha256":"544fc5926a955bd278e670227c951eced411c575fc6f3777d0dfa3cb0a55501b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0/m4zhPO+Rf+50xJro/u0Q5dMuLuXxKhWFS6AlDDp1KGu6V25TD94lIkIg+Ey4FDhlm2SviLGkKeeDXSn99JDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-24T07:10:23.898668Z","bundle_sha256":"02b7994dc3458615739791473972f2d1daecac3bf7f5089318a3889aa4a537c8"}}