Keysight (Agilent) 83446A Product Overview

Agilent 83446A Lightwave Clock/Data Receiver
Product Overview
High gain optical receiver for recovering clock and data directly from optical fiber
• OC-48/STM-16 data rate (2.48832 Gb/sec)
• Operates over full range of power levels specified in SONET/SDH standards
• Auxiliary input recovers clock and data from 2.48832 Gb/sec electrical signals
Clock/
Data
Recovery
AGC
Amplifier
Photodiode
Optical
Input
Aux Out
Clock Out
Data Out
Front Panel
Rear Panel
Electrical
Input
Input Select
Switch
Agilent’s 83446A Lightwave Clock/Data Receiver is designed to extract clock and data infor­mation from digitally modulated lightwave signals. The 83446A is for use with OC-48/STM-16 (2.48832 Gb/sec) signals. It incor­porates a high-gain avalanche photo-diode (APD), gain-controlled amplifier, and clock/data recovery hybrid to deliver clean, error­free outputs from optical signals with powers as low as –27 dBm at either 1310 or 1550 nm wave­lengths. The Agilent 83446A is designed especially for use with high speed bit-error-ratio testers (BERTs) such as the Agilent 86130A. By connecting the 83446A clock and data outputs to the corresponding inputs on the BERT’s error detector, bit­error-ratio analysis can be per­formed directly on optical signals, making it easy to do system acceptance and BER floor analysis.
The high sensitivity of the Agilent 83446A assures accu­rate results over the full range of optical powers specified in SONET/SDH standards such as ITU G.957 and Bellcore TA-NWT-000253. It can also be useful for optical eye diagram analysis on sampling oscillo­scopes. In situations where no separate clock signal is available, the clock output of the 83446A can be used to trigger the oscillo­scope. Unlike schemes that use the data pattern as the trigger source, triggering from a recov­ered clock assures that the eye diagram is an accurate represen­tation of all possible bit combina­tions on the incoming data stream.
For analog monitoring of unconditioned data, the Agilent 83446A provides an auxiliary electrical output. This high-gain AGC controlled output is useful for general diagnostic analysis of the incoming waveform. (Because its frequency response does not meet the stringent requirements for eye mask com­pliance testing defined in SONET/SDH standards, mask tests should be done with an appropriate reference receiver.
Another feature of the 83446A is a rear-panel input for recovering clock and data from an electrical waveform. A rear panel switch selects between either the front optical input or the rear electri­cal input. (The electrical input bypasses the internal high-gain amplifier, so external amplifica­tion must be used when operat­ing on low power signals to achieve a level sufficient for proper operation.) The Agilent 83446A uses a 50 µm fiber core diameter which is compatible with either single-mode or multi­mode fibers. The optical input incorporates a universal adapter for use with any of the connector interfaces in the Agilent 81000 series. The standard instrument includes an FC/PC connector interface. Option 010 deletes the FC/PC connector. Interfaces for other optical connector types must be ordered separately.
Example uses of the
Agilent 83446A
Laser Transmitter Optimization
The Agilent 83446A, in con­junction with an Agilent 86130A Error Performance Analyzer and Agilent 8156A High-performance Optical Attenuator, can help determine the optimum bias setting for laser transmitters. The optimum bias is found when the improve­ment in BER, due to higher extinction ratio, is balanced by degradation due to increased nonlinear waveform distortion effects. BER floors are easily identified by monitoring the error rate as the input power level to the 83446A is increased. The Agilent 83446A operates error-free at input powers above –27 dBm, so any residual errors at higher input powers can be associated with the transmitter under test.
2
86130A BERT
83446A
Clock
In
Data
In
Data
Out
DUT
Laser
8156A
Variable Optical
Attenuator
Clock
Out
Data
Out
Optical
In
Optical
Out
Data
In
In Out
Setup for Optimizing
Laser Transmitter Extinction Ratio
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