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| | | Weekly Edition | | | Date: 5 March 2026 | | | |
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| New Photonics Products this Week | |
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| 1.25 A - 8 A, LED Driver Modules for LED Lighting Applications | |
LED Driver Module
from Mean Well
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| The LPV-60 Series from Mean Well are LED Driver Modules with an output currents of 1.25 A, 1.67 A, 2.5 A, 4 A, 5A, and 8 A. They deliver output powers of 40 W & 60 W and have output voltages of 5 V, 12 V, 15 V, 24 V, 36 V & 48 V with voltage tolerance of ± 5% & ± 8%. These LED driver modules have a setup time of 500 ms and are ideal for LED decoration & advertisement applications. |
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| 4.3 µm - 4.7 µm, PbSe Photodiode for Thermal Imaging Applications | |
Photodiode
from Opto Diode Corporation
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| The BXT2-17TF from Opto Diode Corporation is a Lead Selenide (PbSe) Photodiode that operates at a wavelength of 4.3 µm - 4.7 µm. It has an active element area of 1 mm2 and a detectivity of 2.4 x 1010 cm.rt(Hz)/W (min). This photodiode is ideal for gas analysis, medical, industrial, emissions monitoring, spectroscopy, process control systems, defense, and security applications. |
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| 400 nm - 700 nm, Plate Beam Splitter | |
Beam Splitter
from Edmund Optics
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| The 43-359 from Edmund Optics is a Plate Beam Splitter that operates at a wavelength of 400 nm - 700 nm. It has a clear aperture of 85% and thickness of 1 mm. This beam splitter has a surface flatness of 4 lambda - 6 lambda and surface quality of 80-50. It has a dimensional tolerance ± 0.38 mm and reflection/transmission ratio of 50/50. This beam splitter has a float glass substrate and dielectric coating with reflectance/transmittance of ± 5%. |
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| 800 nm Acousto-Optic Mode Locker for Digital Switching Applications | |
Acousto-Optic Mode Locker
from Laser 2000
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| The FSML-44-20-BR-800 from Laser 2000 is a Fused Silica Acousto-Optic Mode Locker that operates at a wavelength of 800 nm. It has an active aperture of 3 mm x 3 mm and a carrier frequency of 44 MHz. This acousto-optic mode locker is ideal for low-power lasers, MHz/GHz RF frequency modulation rate, analog light intensity modulation, and digital switching on/off applications. |
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| 1480 nm Fiber Optic Circulator for Dispersion Compensation Applications | |
Fiber Optic Circulator
from OZ Optics Ltd.
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| The FOC-12N-111-9/125-SSS-1480-55-XXX-1-1 from OZ Optics Ltd. is a Fiber Optic Circulator with a wavelength of 1480 nm. It has a slow axis transmission with an extinction ratio of 20 dB, 25 dB & 30 dB and peak isolation of less than 40 dB. This fiber optic circulator is ideal for DWDM networks, chromatic dispersion compensation, fiber amplifiers, fiber sensors, and OCT systems. |
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| Multi Rate Fiber Optic Transceiver for Network Applications | |
Fiber Optic Transceiver
from Oplink Communications
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| The TXC3XGJL2x000x0G from Oplink Communications is a Fiber Optic Transceiver that operates at a coarse wavelength division multiplexing (CWDM) wavelength. It is designed for multiple standard rates with a data rate of 10 Gbps and reach (distance) of 80 Km. This fiber optic transceiver is compatible with LC connectors and is ideal for telecommunication network applications. |
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| 1310 nm Bidirectional Fiber Optic Transceiver for SONET Applications | |
Fiber Optic Transceiver
from Teradian
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| The TBE6X20 from Teradian is an Asymmetric Bidirectional Fiber Optic Transceiver that operates at a wavelength of 1310 nm. It has a transmit data rate of 155 Mbps and link distance of up to 40 km. This fiber optic transceiver is compatible with SC, FC or ST connectors and supports single-mode fiber. It is ideal for ATM/SONET OC-3 and SDH STM-1 communication systems. |
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| 850/1310/1550 nm, Single-Channel Electrical to Optical Converters | |
Electrical to Optical Converters
from Highland Technology
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| The J724 from Highland Technology are Single-Channel Electrical to Optical Converters that operate at a wavelength of 850 nm, 1310 nm, or 1550 nm. They deliver a nominal output power of 1 mW and have a bandwidth from DC to 180 MHz. These electrical-to-optical converters have an optical rise time below 250 ps and a propagation delay of 1.2 ns. |
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| Transimpedance Amplifier for Quadrature Amplitude Modulation | |
Transimpedance Amplifier
from Qorvo
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| The TGA4872 from Qorvo is a Transimpedance Amplifier with a bandwidth of 30 GHz. It has a baud rate of up to 128 Gbps and an equivalent input noise of 20 pA/rtHz. This transimpedance amplifier has a differential transimpedance gain of 100 Ohm - 7500 Ohm and is ideal for dual polarization quadrature phase shift keying and quadrature amplitude modulation applications. |
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| 5 µm - 14 µm, Optical Frequency Comb for Spectroscopy Applications | |
Optical Frequency Comb
from Menlo Systems
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| The MID-IR COMB 5 to 14 um from Menlo Systems is an Optical Frequency Comb that operates at a wavelength of 5 μm - 14 μm. It delivers an average output power above 0.5 mW and has a repetition rate of 100 MHz. This optical frequency comb is ideal for Fourier-transform spectroscopy, chemical & biomolecular sensing of molecules, and detection of atmospheric gases. |
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| 1270 nm - 1610 nm, CWDM Optical Power Meter for Testing Applications | |
Optical Power Meter
from Kingfisher International
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| The KI6501 from Kingfisher International is an Optical Power Meter with wavelengths of 1270 nm, 1290 nm, 1310 nm, 1330 nm, 1350 nm, 1370 nm, 1390 nm, 1410 nm, 1430 nm, 1450 nm, 1470 nm, 1490 nm, 1510 nm, 1530 nm, 1550 nm, 1570 nm, 1590 nm, and 1610 nm. It has a measurement speed below 0.8 s and is ideal for testing multi-λ single mode fiber optic systems. |
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| 375 nm - 12 µm, Laser Spectrum Analyzers for Research Applications | |
Optical Spectrum Analyzer
from Bristol Instruments
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| The 771 Series from Bristol Instruments are Laser Spectrum Analyzers with wavelengths of 375 nm - 1100 nm (VIS), 520 nm - 1700 nm, 1 μm - 2.6 μm (NIR), 1 μm - 5 μm (IR) & 1 μm - 12 μm (MIR). They have an accuracy from ± 0.2 ppm to ± 225 MHz and a spectral resolution of 4 GHz - 8 GHz. These optical spectrum analyzers are ideal for applied research and production test applications. |
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| Featured Article | | What is Raman Spectroscopy? | | Raman spectroscopy is a spectroscopic technique that utilizes scattered light to probe the vibrational energy modes present within a sample. It is named after C. V. Raman who pioneered its observation in 1928 alongside his collaborator K. S. Krishnan. Originally, the Raman effect was observed using sunlight and mercury arc lamps. Click here to read the full article. | | | |
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