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area (2-d) array of photo-electronic detectors  (Sony)

 
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    Structured Review

    Sony area (2-d) array of photo-electronic detectors
    Area (2 D) Array Of Photo Electronic Detectors, supplied by Sony, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
    https://www.bioz.com/product/2d+array+detector/area++2+d++array+of+photo+electronic+detectors+55a/us06997386-1795-77-85
    Average 90 stars, based on 1 article reviews
    area (2-d) array of photo-electronic detectors - by Bioz Stars, 2026-11
    90/100 stars

    Images

    Related Articles

    other:

    Article Title: PLANAR LASER ILLUMINATION AND IMAGING (PLIIM) DEVICE EMPLOYING A LINEAR IMAGE DETECTION ARRAY HAVING VERTICALLY-ELONGATED IMAGE DETECTION ELEMENTS, WHEREIN THE HEIGHT OF THE VERTICALLY-ELONGATED IMAGE DETECTION ELEMENTS AND THE F/# PARAMETER OF THE IMAGE FORMATION OPTICS ARE CONFIGURED TO REDUCE SPECKLE-PATTERN NOISE POWER THROUGH SPATIAL-AVERAGING OF DETECTED SPECKLE-NOISE PATTERNS
    Article Snippet: First Illustrative Embodiment of the PLIIM-Based System of the Present Invention Shown in FIG. 6A The first illustrative embodiment of the PLIIM-based system of FIG. 6A, indicated by reference numeral 80A, is shown in FIGS. 6B1 and 6B2 as comprising: an area-type image formation and detection module 55′′ having an imaging subsystem 55B′′ with a variable focal length imaging lens, a variable focal distance and a variable field of view, and an area (2-D) array of photo-electronic detectors 55A realized using CCD technology (e.g. the Sony ICX085AL Progressive Scan CCD Image Sensor with Square Pixels for B/W Cameras, or the Kodak KAF-4202 Series 2032(H)×2044(V) Full-Frame CCD Image Sensor) for detecting 2-D line images formed thereon by the imaging subsystem 55A; a pair of planar laser illumination arrays 6A and 6B for producing first and second planar laser illumination beams 7A and 7B; and a pair of PLIB folding/sweeping mirrors 57A and 57B, arranged in relation to the planar laser illumination arrays 6A and 6B, respectively, such that the planar laser illumination beams arc folded and swept so that the planar laser illumination beams are disposed substantially coplanar with a section of the FOV of image formation and detection module during object illumination and image detection operations carried out by the PLIIM-based system.

    Imaging:

    Article Title: METHOD OF SPECKLE-NOISE PATTERN REDUCTION AND APPARATUS THEREFOR BASED ON REDUCING THE TEMPORAL-COHERENCE OF THE PLANAR LASER ILLUMINATION BEAM BEFORE IT ILLUMINATES THE TARGET OBJECT BY APPLYING TEMPORAL FREQUENCY MODULATION TECHNIQUES DURING THE TRANSMISSION OF THE PLIB TOWARDS THE TARGET
    Article Snippet: .. First Illustrative Embodiment of the PLIIM-based System of the Present Invention Shown in FIG. 6A The first illustrative embodiment of the PLIIM-based system of FIG. 6A, indicated by reference numeral 80A, is shown in FIGS. 6B1 and 6B2 as comprising: an area-type image formation and detection module 55′′ having an imaging subsystem 55B′′ with a variable focal length imaging lens, a variable focal distance and a variable field of view, and an area (2-D) array of photo-electronic detectors 55A realized using CCD technology (e.g. the Sony ICX085AL Progressive Scan CCD Image Sensor with Square Pixels for B/W Cameras, or the Kodak KAF-4202 Series 2032(H)×2044(V) Full-Frame CCD Image Sensor) for detecting 2-D line images formed thereon by the imaging subsystem 55A; a pair of planar laser illumination arrays 6A and 6B for producing first and second planar laser illumination beams 7A and 7B; and a pair of PLIB folding/sweeping mirrors 57A and 57B, arranged in relation to the planar laser illumination arrays 6A and 6B, respectively, such that the planar laser illumination beams are folded and swept so that the planar laser illumination beams are disposed substantially coplanar with a section of the FOV of image formation and detection module during object illumination and image detection operations carried out by the PLIIM-based system. ..



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    Image Search Results


    Signal amplitude from the CROSSmini detector with signal fitting and zoomed in views. Figures A, B and C, on the left, shows the signal amplitude from the CROSSmini detector of a spill duration for energy level 70.2, 150.2, and 228.7 MeV, respectively, with nominal beam current 8 MU/s. The red line represents the original signal from CROSSmini and the black line represents the piecewise fitting for the edges. On the right is the zoomed in view of the fitting. The piecewise fitting quantifies the risetime ( t rise ) and measured nominal beam current ( I 0 , measured ).

    Journal: International Journal of Particle Therapy

    Article Title: Phenomenological Study of Intra-Spill Break Spots in Dose-Driven Continuous Scanning Proton Therapy

    doi: 10.1016/j.ijpt.2026.101315

    Figure Lengend Snippet: Signal amplitude from the CROSSmini detector with signal fitting and zoomed in views. Figures A, B and C, on the left, shows the signal amplitude from the CROSSmini detector of a spill duration for energy level 70.2, 150.2, and 228.7 MeV, respectively, with nominal beam current 8 MU/s. The red line represents the original signal from CROSSmini and the black line represents the piecewise fitting for the edges. On the right is the zoomed in view of the fitting. The piecewise fitting quantifies the risetime ( t rise ) and measured nominal beam current ( I 0 , measured ).

    Article Snippet: The beam current was measured using a CROSSmini 2D strip ionization chamber detector array (Liverage Biomedical Inc, Taiwan) positioned at the isocenter plane.

    Techniques:

    Signal amplitude from the CROSSmini detector with signal fitting. shows the signal amplitude as a function of time measured by the CROSSmini detector and the piecewise fittings. Figures A, B, and C are measurements for energy level 70.2 MeV with nominal beam current 8, 14, and 20 MU/s, respectively. Figures D, E, and F are the measurements for energy level 228.7 MeV with nominal beam current 8, 14, and 20 MU/s, respectively.

    Journal: International Journal of Particle Therapy

    Article Title: Phenomenological Study of Intra-Spill Break Spots in Dose-Driven Continuous Scanning Proton Therapy

    doi: 10.1016/j.ijpt.2026.101315

    Figure Lengend Snippet: Signal amplitude from the CROSSmini detector with signal fitting. shows the signal amplitude as a function of time measured by the CROSSmini detector and the piecewise fittings. Figures A, B, and C are measurements for energy level 70.2 MeV with nominal beam current 8, 14, and 20 MU/s, respectively. Figures D, E, and F are the measurements for energy level 228.7 MeV with nominal beam current 8, 14, and 20 MU/s, respectively.

    Article Snippet: The beam current was measured using a CROSSmini 2D strip ionization chamber detector array (Liverage Biomedical Inc, Taiwan) positioned at the isocenter plane.

    Techniques:

    t rise comparison between analytical and measured. The blue and red plots represent the analytically derived t rise and CROSSmini measured t rise , respectively, across the various nominal beam current settings.

    Journal: International Journal of Particle Therapy

    Article Title: Phenomenological Study of Intra-Spill Break Spots in Dose-Driven Continuous Scanning Proton Therapy

    doi: 10.1016/j.ijpt.2026.101315

    Figure Lengend Snippet: t rise comparison between analytical and measured. The blue and red plots represent the analytically derived t rise and CROSSmini measured t rise , respectively, across the various nominal beam current settings.

    Article Snippet: The beam current was measured using a CROSSmini 2D strip ionization chamber detector array (Liverage Biomedical Inc, Taiwan) positioned at the isocenter plane.

    Techniques: Comparison, Derivative Assay