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Related Concept Videos

Overview of Electron Microscopy01:25

Overview of Electron Microscopy

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The wavelengths of visible light ultimately limit the maximum theoretical resolution of images created by light microscopes. Most light microscopes can only magnify 1000X, and a few can magnify up to 1500X. Electrons, like electromagnetic radiation, can behave like waves, but with wavelengths of 0.005 nm, they produce significantly greater resolution up to 0.05 nm as compared to 500 nm for visible light. An electron microscope (EM) can create a sharp image that is magnified up to 2,000,000X.
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A scanning electron microscope (SEM) is used to study the surface features of a sample by using an electron beam that scans the sample surface in a two-dimensional manner. Typically, areas between ~1 centimeter to 5 micrometers in width can be imaged. SEM can be used to image bacteria, viruses, tissues as well as larger samples like insects. Conventional SEM gives a magnification ranging from 20X to 30,000X and spatial resolution of 50 to 100 nanometers.
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The early pioneers of microscopy opened a window into the invisible world of microorganisms. In 1830, Joseph Jackson Lister created an essentially modern light microscope. The 20th century saw the development of microscopes that leveraged nonvisible light, such as fluorescence microscopy that uses an ultraviolet light source and electron microscopy that uses short-wavelength electron beams. These advances significantly improved magnification, image resolution, and contrast. By comparison, the...
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Related Experiment Video

Updated: May 2, 2026

Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators
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Optically sampled superconducting-nanostrip photon-number resolving detector for non-classical quantum state

Mamoru Endo, Kazuma Takahashi, Takefumi Nomura

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    |July 30, 2025
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    Superconducting nanowire single-photon detectors (SNSPDs) can now resolve photon numbers. A novel optical sampling technique achieves picosecond resolution, enabling practical applications for these photon-number-resolving detectors (PNRDs).

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    Area of Science:

    • Quantum Optics
    • Photonics
    • Superconducting Devices

    Background:

    • Photon-number-resolving detectors (PNRDs) are crucial for quantum optics.
    • Superconducting nanowire single-photon detectors (SNSPDs) exhibit inherent photon number resolving capabilities.
    • Practical application of SNSPD-based PNRDs is hindered by challenges in detecting small signals with low signal-to-noise ratios.

    Purpose of the Study:

    • To develop a method for practical photon number resolution using SNSPDs.
    • To overcome the limitations of low signal-to-noise ratios and sub-nanosecond time frames in SNSPD measurements.
    • To enable real-time photon number resolution for enhanced quantum state generation and analysis.

    Main Methods:

    • Utilized optical sampling with a dual-output Mach-Zehnder modulator (DO-MZM).
    • Employed an ultra-short pulsed laser synchronized with the SNSPD.
    • Adjusted DO-MZM bias voltage for sensitive detection of picosecond-level signal differences.

    Main Results:

    • Achieved a temporal resolution of 1.9 picoseconds.
    • Enabled sensitive detection of tiny signal differences crucial for photon number resolution.
    • Demonstrated real-time photon number resolution capabilities.

    Conclusions:

    • The developed optical sampling method significantly enhances SNSPD performance for PNRD applications.
    • This advancement transitions SNSPD-based PNRDs from theoretical potential to practical implementation.
    • Facilitated the generation and enhancement of non-classical quantum states through precise photon number resolution.