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日本レーザー

EstablishmentApril 16, 1968
capital3000Ten thousand
number of employees70
addressTokyo/Shinjuku-ku/Nishi Waseda 2-14-1
phone03-5285-0861
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last updated:Aug 14, 2026
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Light source for confocal and spinning disk confocal microscopes. Light source for confocal and spinning disk confocal microscopes.
Light source for fluorescence microscopy Light source for fluorescence microscopy
Light source for super-resolution microscopy Light source for super-resolution microscopy
Light source for fluorescence lifetime imaging (FLIM) Light source for fluorescence lifetime imaging (FLIM)
Light

Light source for fluorescence lifetime imaging (FLIM)

■Since multiple wavelengths can be synchronized, complex excitations such as PIE (Pulse Interleaved Excitation) are possible. 【Multi-wavelength output pico-second pulse laser system】 ■A pico-second pulse light source with low pulse-to-pulse jitter, high stability, and low noise. It allows for precise control of delay time, achieving optimal fluorescence lifetime imaging. 【QuixX series】 ■Capable of oscillating from white light to specific wavelengths. Due to pulse driving, time-resolved measurements are possible (optional). With tunable wavelength sweeping, it can accommodate any dye. 【SuperK series】

Multi-wavelength output capable picosecond pulse laser

Multiple wavelengths can be synchronized, allowing for complex excitations such as PIE (Pulse Interleaved Excitation).

Pulse-driven, capable of time-resolved measurements. Due to the ability for multi-wavelength synchronization, complex excitations such as PIE (Pulse Interleaved Excitation) are possible. Multiple diode laser heads can be combined using a combiner, and each head can be individually or synchronously controlled with a multi-channel driver. ■ Light Source ● Diode laser-based picosecond pulse laser ■ Driver ● Multi-channel pulse pattern with ultimate flexibility ● Flexible modular system compatible with laser heads ● Pulse, burst, and CW operation ■ Laser Combiner ● Capable of combining up to 5 laser wavelengths and outputting through a single fiber *For more details, please download the PDF or contact us.

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Picosecond pulse & CW oscillation diode laser QuixX series

A compact diode laser capable of both picosecond and continuous wave oscillation. Wavelengths are available in the range of 375 to 2090 nm. Maximum CW output is 500 mW.

- Picosecond pulse oscillation: Minimum pulse width 50 ps, repetition frequency Single-Shot ~ 100 MHz - Continuous wave (CW) oscillation: ACC & APC mode - Wavelength lineup: 375 to 2090 nm - Maximum output: 500 mW (CW), 2.5 W peak output (picosecond pulse) - User-friendly RS-232 & USB interface included - Variable pulse shape - Low jitter programmable with built-in frequency generator: 1 Hz to 100 MHz - Programmable delay generator: Easily synchronize with external devices - High beam quality & high-efficiency fiber coupling This semiconductor laser is capable of both picosecond pulse oscillation and CW (continuous wave) oscillation with modulation functions. In pulse oscillation, the minimum pulse width is 50 ps, with a maximum repetition frequency of 100 MHz. The adoption of the latest high-performance electronics ensures high stability and low noise. The inter-pulse jitter in picosecond pulse oscillation is <2 ps. It features high-precision temperature control, a programmable frequency generator, an optical system with aberration correction for beam shaping, and a high-resolution SYNC delay generator integrated. *For more details, please download the PDF or contact us.

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Supercontinuum light source 390–2400nm single mode

Outputs high-brightness diffraction-limited light across the entire wavelength range of 390 to 2400 nm. Also supports the construction of wavelength-tunable laser systems.

The "SuperK FIANIUM" is a supercontinuum light source that supports single-mode output across a wavelength range of 390 to 2400 nm, with a simple operating method. By combining it with plug-and-play options, it can form a wavelength-tunable laser system. 【Features】 ■ High beam quality comparable to single-frequency lasers (Gaussian, M2<1.1) ■ Additional wavelength-variable filter option allows for tunable wavelength sweeping ■ Can replace white light sources and broadband multi-wavelength sources ■ Capable of time-resolved measurements due to pulse operation ■ Intuitive operation via PC, allowing parameter changes without turning off the power (*For more product details, please download the catalog) A series of products is also available, including options for industrial applications and compact types, and a new product, the broadband wavelength-tunable laser "SuperK CHROMATUNE," which can oscillate in the wavelength range of 400 to 1000 nm without gaps, is also scheduled for release.

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Single frequency CW DPSS laser for quantum research.

Compact and highly stable single-frequency diode-pumped solid-state (DPSS) laser. Ideal for Raman spectroscopy, interference experiments, lithography, and quantum research.

Wavelengths of 320, 349, 532, 640, and 780 nm, narrow line width (< 0.5 MHz), very low intensity noise (< 0.1% RMS), and diffraction-limited TEM00 beam. The unique optical architecture and hermetically sealed package ensure very stable operation and performance over long periods. It demonstrates high robustness and durability for demanding embedded applications. Additionally, it is ideal for advanced research applications requiring high precision, stability, and spectral purity, such as Raman spectroscopy, interference experiments, holography, and quantum technology development.

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Time-resolved photoluminescence microscope "Solira"

Achieve material property evaluation all in one! Flexible measurement configuration.

"Solira" is a flexible time-resolved photoluminescence (TRPL) microscope that can evaluate the optical properties of materials in a single device. By integrating multiple measurement methods into one system, it enables precise and efficient analysis. It is suitable for the evaluation of materials such as semiconductors, nanomaterials, solar cells, and LEDs. 【Features】 ■ All-in-one solution for material property evaluation ■ Flexible measurement configuration ■ Sensitivity at the single emitter level ■ Excellent system design for expandability ■ Reduction of experimental complexity ■ Application support from experts *For more details, please download the PDF or feel free to contact us.

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