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New Products

New Products

  • 30-meter long optical path gas absorption cell (collimator).

    30-meter long optical path gas absorption cell (collimator).

    Based on Tunable Diode Laser Absorption Spectroscopy (TDLAS), this gas absorption cell utilizes a multi-reflection cavity long optical path design with Herriott cell concave mirrors. The mirrors are coated with high-quality gold, silver, and protective layers, ensuring high reflectivity. With a compact design, it provides a relatively long absorption path and high precision. The entire optical cavity gas cell is made from high-quality, corrosion-resistant materials. Depending on the detection mode, it can be configured as either a closed or open type for detecting and analyzing various gas concentrations. The product can be directly installed with standard optical source collimators, eliminating the need for additional mirrors or adjustment components, making it highly convenient to use. This product is suitable for industrial applications, high-sensitivity gas analysis, academic institutions, scientific research, and online environmental monitoring.

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  • Adjustable Focus Aspheric Fiber Collimator 650-1050nm (Focal Length 4.5mm Beam Waist Diameter 0.98 FC/APC)

    Adjustable Focus Aspheric Fiber Collimator 650-1050nm (Focal Length 4.5mm Beam Waist Diameter 0.98 FC/APC)

    The design uses springs to assemble a suitable optical lens inside the mechanical part, which is used for the collimator output of the optical fiber beam and can also be used for fiber-to-fiber coupling. By rotating the sleeve outside the collimator, the internal optical lens can be translated forward and backward along the optical axis, thereby adjusting the distance between the lens and the end face of the optical fiber to obtain different spot sizes.

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  • 980nm Polarization-Independent Free-Space Isolator

    980nm Polarization-Independent Free-Space Isolator

    Free-space isolators can be divided into two types: polarization-dependent and polarization-independent. The polarization-dependent isolators, also known as Faraday isolators, are mainly composed of three parts: a polarizer, a Faraday rotator, and an analyzer (set at 45?? to the polarizer axis). Polarization-independent isolators typically consist of a birefringent crystal (or polarizer), a Faraday rotator, and a half-wave plate. These are usually used in fiber lasers to effectively maintain the stability of the optical system. Made with high-quality magneto-optic crystals, these isolators offer low absorption, high extinction ratio, and low loss, ensuring excellent and reliable performance. The peak isolation can reach up to 45dB, with an aperture size up to 45mm. The typical transmission rate can reach 95%, and all products are customizable according to customer requirement

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  • 550-880nm Bandwidth Adjustable Polarization-Related Free-Space Isolator

    550-880nm Bandwidth Adjustable Polarization-Related Free-Space Isolator

    Free-space isolators can be divided into two types: polarization-dependent and polarization-independent. The polarization-dependent isolators, also known as Faraday isolators, are mainly composed of three parts: a polarizer, a Faraday rotator, and an analyzer (set at 45° to the polarizer axis). Polarization-independent isolators typically consist of a birefringent crystal (or polarizer), a Faraday rotator, and a half-wave plate. These are usually used in fiber lasers to effectively maintain the stability of the optical system. Made with high-quality magneto-optic crystals, these isolators offer low absorption, high extinction ratio, and low loss, ensuring excellent and reliable performance. The peak isolation can reach up to 45dB, with an aperture size up to 45mm. The typical transmission rate can reach 95%, and all products are customizable according to customer requirement

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  • C-Band Variable Gain Fiber Amplifier (Gain Range 18.5~30.5dB)

    C-Band Variable Gain Fiber Amplifier (Gain Range 18.5~30.5dB)

    Idealphotonics’ C-band variable gain fiber amplifier is a next generation variable gain fiber amplifier, which is a variable gain fiber amplifier with excellent performance and complete functions on the market today. It adopts the current excellent optical performance, advanced electronic technology, and complete software functions. Excellent transient suppression technology and thermal management control technology enable many complex optical functions to be realized. It is a versatile fiber amplifier commonly used in the market today. The next generation variable gain fiber amplifier consists of a variable gain preamplifier (PA) and a variable gain power amplifier (BA), two-stage amplifier. The gain of the two-stage amplifier can be set independently within a certain range. There is an access connector between the two-stage amplifier, which can be used for mid-stage access, such as optical add/drop multiplexing module (OADM), dispersion compensation module (DCM) and other application optical modules. MP4700 is a version with mid-stage access. The product meets the communication technology requirements of C-Band 44-wavelength or 88-wavelength DWDM system and is widely used in long-distance and ultra-long-distance transmission networks. With its complete functions, it can be used as a line amplifier, preamplifier, power amplifier, and add-drop multiplexing amplifier.

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  • C-Band Variable Gain Fiber Amplifier (Gain Range 23~35dB)

    C-Band Variable Gain Fiber Amplifier (Gain Range 23~35dB)

    Idealphotonics’ C-band variable gain fiber amplifier is a next generation variable gain fiber amplifier, which is a variable gain fiber amplifier with excellent performance and complete functions on the market today. It adopts the current excellent optical performance, advanced electronic technology, and complete software functions. Excellent transient suppression technology and thermal management control technology enable many complex optical functions to be realized. It is a versatile fiber amplifier commonly used in the market today. The next generation variable gain fiber amplifier consists of a variable gain preamplifier (PA) and a variable gain power amplifier (BA), two-stage amplifier. The gain of the two-stage amplifier can be set independently within a certain range. There is an access connector between the two-stage amplifier, which can be used for mid-stage access, such as optical add/drop multiplexing module (OADM), dispersion compensation module (DCM) and other application optical modules. MP4700 is a version with mid-stage access. The product meets the communication technology requirements of C-Band 44-wavelength or 88-wavelength DWDM system and is widely used in long-distance and ultra-long-distance transmission networks. With its complete functions, it can be used as a line amplifier, preamplifier, power amplifier, and add-drop multiplexing amplifier.

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  • 532nm Dual-Polarization Related Free-Space Isolator

    532nm Dual-Polarization Related Free-Space Isolator

    Free-space isolators can be divided into two types: polarization-dependent and polarization-independent. The polarization-dependent isolators, also known as Faraday isolators, are mainly composed of three parts: a polarizer, a Faraday rotator, and an analyzer (set at 45° to the polarizer axis). Polarization-independent isolators typically consist of a birefringent crystal (or polarizer), a Faraday rotator, and a half-wave plate. These are usually used in fiber lasers to effectively maintain the stability of the optical system. Made with high-quality magneto-optic crystals, these isolators offer low absorption, high extinction ratio, and low loss, ensuring excellent and reliable performance. The peak isolation can reach up to 45dB, with an aperture size up to 45mm. The typical transmission rate can reach 95%, and all products are customizable according to customer requirement

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  • Adjustable Focus Aspheric Fiber Collimator 650-1050nm (Focal Length 11mm Beam Waist Diameter 2.35 FC/APC)

    Adjustable Focus Aspheric Fiber Collimator 650-1050nm (Focal Length 11mm Beam Waist Diameter 2.35 FC/APC)

    The design uses springs to assemble a suitable optical lens inside the mechanical part, which is used for the collimator output of the optical fiber beam and can also be used for fiber-to-fiber coupling. By rotating the sleeve outside the collimator, the internal optical lens can be translated forward and backward along the optical axis, thereby adjusting the distance between the lens and the end face of the optical fiber to obtain different spot sizes.

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  • 400X400μm Homogenized Fiber Optic Connector

    400X400μm Homogenized Fiber Optic Connector

    Homogenized fiber has unique spot homogenization and scrambling properties. When Gaussian-distributed laser is input, it can obtain a flat-top spot with uniform energy distribution after passing through square/rectangular/octagonal fiber. At the same time, the coupling efficiency is also higher than that of circular fiber. It is an ideal fiber for precision laser processing (welding, cutting, marking), astronomical observation, night vision monitoring, laser biological detection and other application fields. This product link is the related model of homogenized bare optical fiber + connector jumper.

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  • 1030nm 200W Fiber-to-Free Space Isolator

    1030nm 200W Fiber-to-Free Space Isolator

    The fiber-to-free space isolators from IdealPhotonics’ can be divided into three main types: beam-expanding output type, beam-expanding output type with indicator light, and non-beam-expanding output type. They have center wavelengths of 980nm, 1030nm, and 1064nm, with an average power handling capability of up to 200W. These isolators are widely used in the industrial processing field and can effectively maintain the frequency stability of fiber lasers, fiber amplifiers, and optical sensors. This product can be customized according to customer requirements, including operating wavelength, size, and power handling capacity.

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  • 1320nm High-Temperature High-Power DFB Chip 250mW

    1320nm High-Temperature High-Power DFB Chip 250mW

    The 1320nm high-temperature high-power DFB laser chip is suitable for operation in high-temperature environments, offering advantages such as ultra-low RIN noise and high output optical power. The output power can reach up to 250mW. Wavelength customization services are available based on customer requirements.

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  • C-Band Variable Gain Fiber Amplifier (Gain Range 29~41dB)

    C-Band Variable Gain Fiber Amplifier (Gain Range 29~41dB)

    Idealphotonics’ C-band variable gain fiber amplifier is a next generation variable gain fiber amplifier, which is a variable gain fiber amplifier with excellent performance and complete functions on the market today. It adopts the current excellent optical performance, advanced electronic technology, and complete software functions. Excellent transient suppression technology and thermal management control technology enable many complex optical functions to be realized. It is a versatile fiber amplifier commonly used in the market today. The next generation variable gain fiber amplifier consists of a variable gain preamplifier (PA) and a variable gain power amplifier (BA), two-stage amplifier. The gain of the two-stage amplifier can be set independently within a certain range. There is an access connector between the two-stage amplifier, which can be used for mid-stage access, such as optical add/drop multiplexing module (OADM), dispersion compensation module (DCM) and other application optical modules. MP4700 is a version with mid-stage access. The product meets the communication technology requirements of C-Band 44-wavelength or 88-wavelength DWDM system and is widely used in long-distance and ultra-long-distance transmission networks. With its complete functions, it can be used as a line amplifier, preamplifier, power amplifier, and add-drop multiplexing amplifier.

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  • 10+ 10 Years of Experience
  • 50 50 + Countries Bussiness
  • 10000 10k + Diodes sold worldwide
  • 30 30+ Invention patent
  • 10 10+ Advanced Optical Solutions

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