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Related Concept Videos

Super-resolution Fluorescence Microscopy01:37

Super-resolution Fluorescence Microscopy

Super-resolution fluorescence microscopy (SRFM) provides a better resolution than conventional fluorescence microscopy by reducing the point spread function (PSF). PSF is the light intensity distribution from a point that causes it to appear blurred. Due to PSF, each fluorescing point appears bigger than its actual size, and it is the PSF interference of nearby fluorophores that causes the blurred image. Various approaches to achieving higher resolution through SRFM have recently been developed.

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Related Experiment Video

Updated: Jun 16, 2026

Observation and Analysis of Blinking Surface-enhanced Raman Scattering
05:52

Observation and Analysis of Blinking Surface-enhanced Raman Scattering

Published on: January 11, 2018

Nanosecond high radiance standard source.

H Krompholz, H Fischer

    Applied Optics
    |February 4, 2010
    PubMed
    Summary
    This summary is machine-generated.

    High-intensity spark channels generated by Nanolite sources exhibit high spectral radiance and luminance. Pulse charging significantly enhances these optical properties compared to slow charging, reaching temperatures over 60,000 K.

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    Last Updated: Jun 16, 2026

    Observation and Analysis of Blinking Surface-enhanced Raman Scattering
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    Excitation-Scanning Hyperspectral Imaging Microscopy to Efficiently Discriminate Fluorescence Signals

    Published on: August 22, 2019

    Area of Science:

    • Physics
    • Optical Engineering
    • Plasma Physics

    Background:

    • Nanolite sources produce high-density spark channels with significant optical emissions.
    • Understanding these emissions is crucial for applications requiring intense light sources.

    Purpose of the Study:

    • To systematically study spectral radiances and luminances of Nanolite spark channels.
    • To compare optical properties under different charging conditions and gas environments.
    • To determine equivalent blackbody temperatures and spectral radiant intensity.

    Main Methods:

    • Comparison of Nanolite spark channel emissions with a calibrated dc-carbon arc.
    • Systematic measurement of spectral radiances R(lambda) and luminances B.
    • Varying gas pressures (air, argon, helium) and charging methods (slow, pulse).

    Main Results:

    • Maximum spectral radiance R(lambda) reached over 70 W cm(-2) A(-1) sr(-1) in air with pulse charging.
    • Equivalent blackbody temperatures exceeded 62,000 K in air (pulse charged).
    • Reproducible results with an absolute error estimated below +/-20%.

    Conclusions:

    • Nanolite spark channels are powerful, tunable light sources.
    • Pulse charging dramatically enhances spectral radiance and temperature.
    • The study provides quantitative data for optimizing Nanolite source applications.