{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:UOHZEMM5MQYBALGNIDRH663V5A","short_pith_number":"pith:UOHZEMM5","schema_version":"1.0","canonical_sha256":"a38f92319d6430102ccd40e27f7b75e8196918a7f879a50cc1bbe941d533c6d2","source":{"kind":"arxiv","id":"1306.2412","version":2},"attestation_state":"computed","paper":{"title":"On the distribution of DNA translocation times in solid-state nanopores: an analysis using Schrodinger's first-passage-time theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.bio-ph","q-bio.BM"],"primary_cat":"cond-mat.soft","authors_text":"Daniel Y. Ling, X. S. Ling","submitted_at":"2013-06-11T03:35:08Z","abstract_excerpt":"In this short note, a correction is made to the recently proposed solution [1] to a 1D biased diffusion model for linear DNA translocation and a new analysis will be given to the data in [1]. It was pointed out [2] by us recently that this 1D linear translocation model is equivalent to the one that was considered by Schrodinger [3] for the Enrenhaft-Millikan measurements [4,5] on electron charge. Here we apply Schrodinger's first-passage-time distribution formula to the data set in [1]. It is found that Schrodinger's formula can be used to describe the time distribution of DNA translocation in"},"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":"1306.2412","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2013-06-11T03:35:08Z","cross_cats_sorted":["physics.bio-ph","q-bio.BM"],"title_canon_sha256":"5f9b5d9a50315e52b872750d47ea3c0ce3d581b9bffaec6ac9a571c8e73fc790","abstract_canon_sha256":"0c22063869e166a58ab025cc4da73b4980cdff8bbe8b8d7d7332dd18e33f630e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:15:20.533858Z","signature_b64":"WD9vb8OxjY5k6qT3adEVWGtL+awQmACryxJiFSKm7Aa7U73gEg9RLfRrGoe2YwkbgLdrRj0y1pneaWfGmYpBCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a38f92319d6430102ccd40e27f7b75e8196918a7f879a50cc1bbe941d533c6d2","last_reissued_at":"2026-05-18T03:15:20.533140Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:15:20.533140Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On the distribution of DNA translocation times in solid-state nanopores: an analysis using Schrodinger's first-passage-time theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.bio-ph","q-bio.BM"],"primary_cat":"cond-mat.soft","authors_text":"Daniel Y. Ling, X. S. Ling","submitted_at":"2013-06-11T03:35:08Z","abstract_excerpt":"In this short note, a correction is made to the recently proposed solution [1] to a 1D biased diffusion model for linear DNA translocation and a new analysis will be given to the data in [1]. It was pointed out [2] by us recently that this 1D linear translocation model is equivalent to the one that was considered by Schrodinger [3] for the Enrenhaft-Millikan measurements [4,5] on electron charge. Here we apply Schrodinger's first-passage-time distribution formula to the data set in [1]. It is found that Schrodinger's formula can be used to describe the time distribution of DNA translocation in"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.2412","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1306.2412","created_at":"2026-05-18T03:15:20.533249+00:00"},{"alias_kind":"arxiv_version","alias_value":"1306.2412v2","created_at":"2026-05-18T03:15:20.533249+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.2412","created_at":"2026-05-18T03:15:20.533249+00:00"},{"alias_kind":"pith_short_12","alias_value":"UOHZEMM5MQYB","created_at":"2026-05-18T12:28:02.375192+00:00"},{"alias_kind":"pith_short_16","alias_value":"UOHZEMM5MQYBALGN","created_at":"2026-05-18T12:28:02.375192+00:00"},{"alias_kind":"pith_short_8","alias_value":"UOHZEMM5","created_at":"2026-05-18T12:28:02.375192+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/UOHZEMM5MQYBALGNIDRH663V5A","json":"https://pith.science/pith/UOHZEMM5MQYBALGNIDRH663V5A.json","graph_json":"https://pith.science/api/pith-number/UOHZEMM5MQYBALGNIDRH663V5A/graph.json","events_json":"https://pith.science/api/pith-number/UOHZEMM5MQYBALGNIDRH663V5A/events.json","paper":"https://pith.science/paper/UOHZEMM5"},"agent_actions":{"view_html":"https://pith.science/pith/UOHZEMM5MQYBALGNIDRH663V5A","download_json":"https://pith.science/pith/UOHZEMM5MQYBALGNIDRH663V5A.json","view_paper":"https://pith.science/paper/UOHZEMM5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1306.2412&json=true","fetch_graph":"https://pith.science/api/pith-number/UOHZEMM5MQYBALGNIDRH663V5A/graph.json","fetch_events":"https://pith.science/api/pith-number/UOHZEMM5MQYBALGNIDRH663V5A/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UOHZEMM5MQYBALGNIDRH663V5A/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UOHZEMM5MQYBALGNIDRH663V5A/action/storage_attestation","attest_author":"https://pith.science/pith/UOHZEMM5MQYBALGNIDRH663V5A/action/author_attestation","sign_citation":"https://pith.science/pith/UOHZEMM5MQYBALGNIDRH663V5A/action/citation_signature","submit_replication":"https://pith.science/pith/UOHZEMM5MQYBALGNIDRH663V5A/action/replication_record"}},"created_at":"2026-05-18T03:15:20.533249+00:00","updated_at":"2026-05-18T03:15:20.533249+00:00"}