{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:VVYWN5R57CWNYDHZZUHNNOEPGC","short_pith_number":"pith:VVYWN5R5","schema_version":"1.0","canonical_sha256":"ad7166f63df8acdc0cf9cd0ed6b88f3082c0ca35a3cdde0c45fe5af42829d9fc","source":{"kind":"arxiv","id":"1308.5958","version":1},"attestation_state":"computed","paper":{"title":"Estimation of mass thickness response of embedded aggregated silica nanospheres from high angle annular dark-field scanning transmission electron micrographs","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Charlotte Hamngren Blomqvist, Christoffer Abrahamsson, Eva Olsson, Magnus Nyd\\'en, Magnus R\\\"oding, Matias Nordin, Mats Rudemo","submitted_at":"2013-08-27T19:40:43Z","abstract_excerpt":"In this study we investigate the functional behavior of the intensity in high-angle annular dark field (HAADF) scanning transmission electron micrograph (STEM) images. The model material is a silica particle (20 nm) gel at 5 wt%. By assuming that the intensity response is monotonically increasing with increasing mass thickness of silica, an estimate of the functional form is calculated using a maximum likelihood approach. We conclude that a linear functional form of the intensity provides a fair estimate but that a power function is significantly better for estimating the amount of silica in t"},"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":"1308.5958","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2013-08-27T19:40:43Z","cross_cats_sorted":[],"title_canon_sha256":"a3622a4957d25758e78bd300cb9dfc7b625d76e21cf7c251e49fc99c3e7a0a68","abstract_canon_sha256":"31ecdb371cbdafaf7742a113f7de24c16f4e2fd23ecc9bd7bb5c9b485d48fa0a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:14:50.666144Z","signature_b64":"Sry4Q4RYH+9si64YLAhuAN0wBh11LmUw5PzpYGmRnS6piQtP+steds5dwOD1szIpfs/RmGQ7pUllLVIc5e77CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ad7166f63df8acdc0cf9cd0ed6b88f3082c0ca35a3cdde0c45fe5af42829d9fc","last_reissued_at":"2026-05-18T03:14:50.665215Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:14:50.665215Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Estimation of mass thickness response of embedded aggregated silica nanospheres from high angle annular dark-field scanning transmission electron micrographs","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Charlotte Hamngren Blomqvist, Christoffer Abrahamsson, Eva Olsson, Magnus Nyd\\'en, Magnus R\\\"oding, Matias Nordin, Mats Rudemo","submitted_at":"2013-08-27T19:40:43Z","abstract_excerpt":"In this study we investigate the functional behavior of the intensity in high-angle annular dark field (HAADF) scanning transmission electron micrograph (STEM) images. The model material is a silica particle (20 nm) gel at 5 wt%. By assuming that the intensity response is monotonically increasing with increasing mass thickness of silica, an estimate of the functional form is calculated using a maximum likelihood approach. We conclude that a linear functional form of the intensity provides a fair estimate but that a power function is significantly better for estimating the amount of silica in t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1308.5958","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1308.5958","created_at":"2026-05-18T03:14:50.665380+00:00"},{"alias_kind":"arxiv_version","alias_value":"1308.5958v1","created_at":"2026-05-18T03:14:50.665380+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1308.5958","created_at":"2026-05-18T03:14:50.665380+00:00"},{"alias_kind":"pith_short_12","alias_value":"VVYWN5R57CWN","created_at":"2026-05-18T12:28:04.890932+00:00"},{"alias_kind":"pith_short_16","alias_value":"VVYWN5R57CWNYDHZ","created_at":"2026-05-18T12:28:04.890932+00:00"},{"alias_kind":"pith_short_8","alias_value":"VVYWN5R5","created_at":"2026-05-18T12:28:04.890932+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/VVYWN5R57CWNYDHZZUHNNOEPGC","json":"https://pith.science/pith/VVYWN5R57CWNYDHZZUHNNOEPGC.json","graph_json":"https://pith.science/api/pith-number/VVYWN5R57CWNYDHZZUHNNOEPGC/graph.json","events_json":"https://pith.science/api/pith-number/VVYWN5R57CWNYDHZZUHNNOEPGC/events.json","paper":"https://pith.science/paper/VVYWN5R5"},"agent_actions":{"view_html":"https://pith.science/pith/VVYWN5R57CWNYDHZZUHNNOEPGC","download_json":"https://pith.science/pith/VVYWN5R57CWNYDHZZUHNNOEPGC.json","view_paper":"https://pith.science/paper/VVYWN5R5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1308.5958&json=true","fetch_graph":"https://pith.science/api/pith-number/VVYWN5R57CWNYDHZZUHNNOEPGC/graph.json","fetch_events":"https://pith.science/api/pith-number/VVYWN5R57CWNYDHZZUHNNOEPGC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VVYWN5R57CWNYDHZZUHNNOEPGC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VVYWN5R57CWNYDHZZUHNNOEPGC/action/storage_attestation","attest_author":"https://pith.science/pith/VVYWN5R57CWNYDHZZUHNNOEPGC/action/author_attestation","sign_citation":"https://pith.science/pith/VVYWN5R57CWNYDHZZUHNNOEPGC/action/citation_signature","submit_replication":"https://pith.science/pith/VVYWN5R57CWNYDHZZUHNNOEPGC/action/replication_record"}},"created_at":"2026-05-18T03:14:50.665380+00:00","updated_at":"2026-05-18T03:14:50.665380+00:00"}