Our 45 GHz fiber-optic detectors make ultra high-speed measurements of more than 40 GHz easy. This ultra high-speed photodetector is frequencey domain optimized to provide especially flat frequency responses over wide bandwidths. Each unit is individually tested and shipped with its own frequency-response curve.
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40-ghz-and-45-ghz-photodetectors - Drawings
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Specifications
Detector Material
InGaAs
Detector Diameter
12 µm
Wavelength Range
500-1630 nm
3 dB Bandwidth
DC to 45 GHz (typ)
Maximum Conversion Gain
10 V/W
Responsivity
0.45 A/W
Fiber-Optic Connector
FC/UPC
Fiber Type
Singlemode
Rise Time
9 ps (typ)
NEP
45 pW/√Hz
Output Connector
Wiltron K
Output Impedance
50 Ω
DC Bias Monitor Bandwidth
50 KHz
DC Bias Monitor Transimpedance Gain
1 V/mA
Power Requirements
Internal 9-V battery
Features
Ultra High-Speed Photodetection
This high-speed fiber optic photodetector shows flat response up to 45 GHz and is optimized for frequency-domain applications. For time-domain applications, please see our Time Domain Fiber-Optic Detectors.
Typical frequency response of Model 1014. Input power was 0.45 mW at 1.06 µm. Measurement accuracy is ±1.5 dB up to 40 GHz, and ±3.5 dB from 40 to 60 GHz.
High Sensitivity Throughout Spectrum
Model 1014 utilizes InGaAs providing coverage from 500 to 1630 nm.
Easy-to-use, Self-contained Module
These self-contained modules connect directly to test instruments like digital oscilloscopes, spectrum analyzers, and network analyzers for lightwave time and frequency-domain measurements. The internal housing of the high-speed models is specially designed to preserve the frequency response and phase to give true fidelity in your measurements. Also, the photodetector comes equipped with a DC-bias monitor that has a transimpedance gain of 1 mV/µA and a 50-kHz bandwidth.
Singlemode FC Fiber-optic Connector Input
These modules accept single-mode FC-fiber-optic inputs from your optical apparatus, eliminating the need for lossy and dispersive high-frequency coaxial cables. The fiber-coupled input also prevents signal distortion.
Battery Powered
The photodiodes are powered by an easily accessible 9V battery. The photodiode bias circuit and battery are housed in an RF-shielded case, reducing the risk of damage from excessive voltage or rough handling, and eliminating the need for expensive bias tees. The battery also eliminates an extra power cable to the module.
Applications
Characterizing the frequency response of pulsed lasers, modulators & transmitters
Microwave generation - heterodyne experiments
Characterizing pulse propagation through dispersive optical systems
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