Full metadata record
DC Field | Value | Language |
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dc.contributor.author | Changhyuk Lee | - |
dc.contributor.author | Adriaan J. Taal | - |
dc.contributor.author | Jaebin Choi | - |
dc.contributor.author | Kukjoo Kim | - |
dc.contributor.author | Kevin Tien | - |
dc.contributor.author | Laurent Moreaux | - |
dc.contributor.author | Michael L. Roukes | - |
dc.contributor.author | Kenneth L. Shepard | - |
dc.date.accessioned | 2024-01-12T05:42:06Z | - |
dc.date.available | 2024-01-12T05:42:06Z | - |
dc.date.created | 2021-09-29 | - |
dc.date.issued | 2019-02 | - |
dc.identifier.issn | 2376-8606 | - |
dc.identifier.uri | https://pubs.kist.re.kr/handle/201004/79026 | - |
dc.description.abstract | Optical functional neural imaging has revolutionized neuroscience with optical reporters that enable single-cell-resolved monitoring of neuronal activity in vivo. State-of-the-art microscopy methods, however, are fundamentally limited in imaging depth by absorption and scattering in tissue even with the use of the most sophisticated two-photon microscopy techniques [1]. To overcome this imaging depth problem, we develop a lens-less, optical-filter-less, shank-based image sensor array that can be inserted into the brain, allowing cellular-resolution recording at arbitrary depths with excitation provided by an external laser light source (Fig. 11.5.1). Lens-less imaging is achieved generally by giving each pixel a spatial sensitivity function, which can be introduced by near-field or far-field, phase or amplitude masking. Since probe thickness must be less than 70μm to limit tissue damage and far-field masks are characterized by distances on the order of 200μm between the mask and the detector [2], we employ a near-field amplitude mask formed by Talbot gratings in the back-end metal of the CMOS process, which gives each pixel a diffraction-grating-induced angle-sensitivity [3]. Filter-less fluorescence imaging is achieved with time-gated operation in which the excitation light source is pulsed and pixel-level time-gated circuitry collects photons only after the excitation source has been removed. | - |
dc.language | English | - |
dc.publisher | IEEE SOLID-STATE CIRCUITS SOCIETY | - |
dc.title | 11.5 A 512-Pixel 3kHz-Frame-Rate Dual-Shank Lensless Filterless Single-Photon-Avalanche-Diode CMOS Neural Imaging Probe | - |
dc.type | Conference | - |
dc.identifier.doi | 10.1109/ISSCC.2019.8662408 | - |
dc.description.journalClass | 1 | - |
dc.identifier.bibliographicCitation | Solid-State Circuits Conference-(ISSCC), 2019 IEEE International | - |
dc.citation.title | Solid-State Circuits Conference-(ISSCC), 2019 IEEE International | - |
dc.citation.conferencePlace | US | - |
dc.citation.conferencePlace | San Francisco | - |
dc.citation.conferenceDate | 2019-02-17 | - |
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