High throughput analysis of single molecule events

By splitting the excitation radiation beam in the optical diffraction element and irradiating the sample point with the evanescent field, the problem of overlapping excitation radiation paths and emission radiation paths in the existing technology is solved, and efficient single-molecule event high-throughput analysis and nucleic acid molecule sequence detection are achieved.

CN120659891APending Publication Date: 2025-09-16GNOTHIS HLDG
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Patent Information

Application Number
CN202380090376.3
Authority / Receiving Office
CN · China
Patent Type
Applications(China)
Current Assignee / Owner
Priority Date
2022-11-29
Filing Date
2023-11-24
Publication Date
2025-09-16

AI Technical Summary

Technical Problem

Existing high-throughput sequencing technologies have difficulty detecting mutations in a minority of sequences present in a nucleic acid population because they are masked by the majority of sequences present in the population, and existing single-molecule analysis methods fail to effectively solve the problem of overlap between excitation radiation paths and emission radiation paths.

Method used

An optical diffraction element is used to split the excitation radiation into multiple separate radiation beams, which are then used to illuminate the sample point through the optically transparent substrate of the carrier. The excitation radiation path does not overlap with the emission radiation path. The evanescent field is used to illuminate the sample point, and the detection device captures and analyzes the emission radiation.

Benefits of technology

It achieves high-throughput analysis of single-molecule events, increases the number and flexibility of analyzable sample points, improves detection efficiency, and is suitable for sequence analysis of single nucleic acid molecules.

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Abstract

The present disclosure relates to analysis of single molecule events (40) as observed by irradiating a sample (18) with excitation radiation (14) and detecting emitted radiation (22) from the sample induced by the excitation radiation, wherein the excitation radiation path from the radiation source (12) to the plurality of samples does not overlap the emitted radiation path from the plurality of samples to the detection device (26).
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