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second cmos camera  (Basler)


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    Structured Review

    Basler second cmos camera
    ( a) Schematic of the TD imaging system for S-FLT acquisition, comprising of a gated intensifier connected to a <t>CMOS</t> <t>camera,</t> and a CW camera attached to the intensifier via a beam splitter (BS) for parallel acquisition of CW and time gated images. A pulsed laser source (EXR-20, SuperK Varia, NKT Photonics, 400–850 nm tuning range, 80 MHz repetition rate, < 20 ps pulse width, or FFSMART, Toptica, 780 nm, 78 MHz repetition rate, 120 fs pulse width) coupled to a multimode optical fiber illuminates the sample (S) via a light diffuser (D). Fluorescence is collected using a macro lens coupled with a filter wheel (F) with multiple bandpass filters ( Supplement 1 Table S1). (b) Schematic of the proposed S-FLT method: Typical TD fluorescence decay curve (in log scale) shown with the choice of the single time gate “ T ” used in the S-FLT calculation (Eq. ), which is an explicit formula for the lifetime τ in terms of the single gate measurement I ( T ) and the parallel CW measurement I C W . (c) Mean square error and variance of FLTs estimated from RLD (left) and S-FLT (right), as a function of SNR and true FLT. (See Supplement 1 Section 2.A for details regarding the simulation and a plot of noise performance for a wider range of SNRs).
    Second Cmos Camera, supplied by Basler, used in various techniques. Bioz Stars score: 95/100, based on 35 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
    https://www.bioz.com/result/second cmos camera/product/Basler
    Average 95 stars, based on 35 article reviews
    second cmos camera - by Bioz Stars, 2026-05
    95/100 stars

    Images

    1) Product Images from "High-speed wide-field fluorescence lifetime imaging for intraoperative tumor visualization and in vivo multiplexing"

    Article Title: High-speed wide-field fluorescence lifetime imaging for intraoperative tumor visualization and in vivo multiplexing

    Journal: Biomedical Optics Express

    doi: 10.1364/BOE.568712

    ( a) Schematic of the TD imaging system for S-FLT acquisition, comprising of a gated intensifier connected to a CMOS camera, and a CW camera attached to the intensifier via a beam splitter (BS) for parallel acquisition of CW and time gated images. A pulsed laser source (EXR-20, SuperK Varia, NKT Photonics, 400–850 nm tuning range, 80 MHz repetition rate, < 20 ps pulse width, or FFSMART, Toptica, 780 nm, 78 MHz repetition rate, 120 fs pulse width) coupled to a multimode optical fiber illuminates the sample (S) via a light diffuser (D). Fluorescence is collected using a macro lens coupled with a filter wheel (F) with multiple bandpass filters ( Supplement 1 Table S1). (b) Schematic of the proposed S-FLT method: Typical TD fluorescence decay curve (in log scale) shown with the choice of the single time gate “ T ” used in the S-FLT calculation (Eq. ), which is an explicit formula for the lifetime τ in terms of the single gate measurement I ( T ) and the parallel CW measurement I C W . (c) Mean square error and variance of FLTs estimated from RLD (left) and S-FLT (right), as a function of SNR and true FLT. (See Supplement 1 Section 2.A for details regarding the simulation and a plot of noise performance for a wider range of SNRs).
    Figure Legend Snippet: ( a) Schematic of the TD imaging system for S-FLT acquisition, comprising of a gated intensifier connected to a CMOS camera, and a CW camera attached to the intensifier via a beam splitter (BS) for parallel acquisition of CW and time gated images. A pulsed laser source (EXR-20, SuperK Varia, NKT Photonics, 400–850 nm tuning range, 80 MHz repetition rate, < 20 ps pulse width, or FFSMART, Toptica, 780 nm, 78 MHz repetition rate, 120 fs pulse width) coupled to a multimode optical fiber illuminates the sample (S) via a light diffuser (D). Fluorescence is collected using a macro lens coupled with a filter wheel (F) with multiple bandpass filters ( Supplement 1 Table S1). (b) Schematic of the proposed S-FLT method: Typical TD fluorescence decay curve (in log scale) shown with the choice of the single time gate “ T ” used in the S-FLT calculation (Eq. ), which is an explicit formula for the lifetime τ in terms of the single gate measurement I ( T ) and the parallel CW measurement I C W . (c) Mean square error and variance of FLTs estimated from RLD (left) and S-FLT (right), as a function of SNR and true FLT. (See Supplement 1 Section 2.A for details regarding the simulation and a plot of noise performance for a wider range of SNRs).

    Techniques Used: Imaging, Fluorescence



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    ( a) Schematic of the TD imaging system for S-FLT acquisition, comprising of a gated intensifier connected to a <t>CMOS</t> <t>camera,</t> and a CW camera attached to the intensifier via a beam splitter (BS) for parallel acquisition of CW and time gated images. A pulsed laser source (EXR-20, SuperK Varia, NKT Photonics, 400–850 nm tuning range, 80 MHz repetition rate, < 20 ps pulse width, or FFSMART, Toptica, 780 nm, 78 MHz repetition rate, 120 fs pulse width) coupled to a multimode optical fiber illuminates the sample (S) via a light diffuser (D). Fluorescence is collected using a macro lens coupled with a filter wheel (F) with multiple bandpass filters ( Supplement 1 Table S1). (b) Schematic of the proposed S-FLT method: Typical TD fluorescence decay curve (in log scale) shown with the choice of the single time gate “ T ” used in the S-FLT calculation (Eq. ), which is an explicit formula for the lifetime τ in terms of the single gate measurement I ( T ) and the parallel CW measurement I C W . (c) Mean square error and variance of FLTs estimated from RLD (left) and S-FLT (right), as a function of SNR and true FLT. (See Supplement 1 Section 2.A for details regarding the simulation and a plot of noise performance for a wider range of SNRs).
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    ( a) Schematic of the TD imaging system for S-FLT acquisition, comprising of a gated intensifier connected to a <t>CMOS</t> <t>camera,</t> and a CW camera attached to the intensifier via a beam splitter (BS) for parallel acquisition of CW and time gated images. A pulsed laser source (EXR-20, SuperK Varia, NKT Photonics, 400–850 nm tuning range, 80 MHz repetition rate, < 20 ps pulse width, or FFSMART, Toptica, 780 nm, 78 MHz repetition rate, 120 fs pulse width) coupled to a multimode optical fiber illuminates the sample (S) via a light diffuser (D). Fluorescence is collected using a macro lens coupled with a filter wheel (F) with multiple bandpass filters ( Supplement 1 Table S1). (b) Schematic of the proposed S-FLT method: Typical TD fluorescence decay curve (in log scale) shown with the choice of the single time gate “ T ” used in the S-FLT calculation (Eq. ), which is an explicit formula for the lifetime τ in terms of the single gate measurement I ( T ) and the parallel CW measurement I C W . (c) Mean square error and variance of FLTs estimated from RLD (left) and S-FLT (right), as a function of SNR and true FLT. (See Supplement 1 Section 2.A for details regarding the simulation and a plot of noise performance for a wider range of SNRs).
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    Image Search Results


    ( a) Schematic of the TD imaging system for S-FLT acquisition, comprising of a gated intensifier connected to a CMOS camera, and a CW camera attached to the intensifier via a beam splitter (BS) for parallel acquisition of CW and time gated images. A pulsed laser source (EXR-20, SuperK Varia, NKT Photonics, 400–850 nm tuning range, 80 MHz repetition rate, < 20 ps pulse width, or FFSMART, Toptica, 780 nm, 78 MHz repetition rate, 120 fs pulse width) coupled to a multimode optical fiber illuminates the sample (S) via a light diffuser (D). Fluorescence is collected using a macro lens coupled with a filter wheel (F) with multiple bandpass filters ( Supplement 1 Table S1). (b) Schematic of the proposed S-FLT method: Typical TD fluorescence decay curve (in log scale) shown with the choice of the single time gate “ T ” used in the S-FLT calculation (Eq. ), which is an explicit formula for the lifetime τ in terms of the single gate measurement I ( T ) and the parallel CW measurement I C W . (c) Mean square error and variance of FLTs estimated from RLD (left) and S-FLT (right), as a function of SNR and true FLT. (See Supplement 1 Section 2.A for details regarding the simulation and a plot of noise performance for a wider range of SNRs).

    Journal: Biomedical Optics Express

    Article Title: High-speed wide-field fluorescence lifetime imaging for intraoperative tumor visualization and in vivo multiplexing

    doi: 10.1364/BOE.568712

    Figure Lengend Snippet: ( a) Schematic of the TD imaging system for S-FLT acquisition, comprising of a gated intensifier connected to a CMOS camera, and a CW camera attached to the intensifier via a beam splitter (BS) for parallel acquisition of CW and time gated images. A pulsed laser source (EXR-20, SuperK Varia, NKT Photonics, 400–850 nm tuning range, 80 MHz repetition rate, < 20 ps pulse width, or FFSMART, Toptica, 780 nm, 78 MHz repetition rate, 120 fs pulse width) coupled to a multimode optical fiber illuminates the sample (S) via a light diffuser (D). Fluorescence is collected using a macro lens coupled with a filter wheel (F) with multiple bandpass filters ( Supplement 1 Table S1). (b) Schematic of the proposed S-FLT method: Typical TD fluorescence decay curve (in log scale) shown with the choice of the single time gate “ T ” used in the S-FLT calculation (Eq. ), which is an explicit formula for the lifetime τ in terms of the single gate measurement I ( T ) and the parallel CW measurement I C W . (c) Mean square error and variance of FLTs estimated from RLD (left) and S-FLT (right), as a function of SNR and true FLT. (See Supplement 1 Section 2.A for details regarding the simulation and a plot of noise performance for a wider range of SNRs).

    Article Snippet: A second CMOS camera (Basler acA547217um) was positioned after the emission filter, coupled via a 50:50 beamsplitter (Thorlabs CCM1-BS014), to collect CW images.

    Techniques: Imaging, Fluorescence