Using the Attenuator

Setting Up the Attenuation

Resetting the Attenuation Factor

To reset the attenuation factor, press and hold ATT until the value resets (this takes approximately two seconds). The attenuation factor resets so that the filter attenuation is zero, that is

Att(dB) = Cal(dB)

Entering a Calibration Factor

The calibration factor is shown at the bottom left of the display

Figure 2-3

The Calibration Factor on the Display

This factor does not affect the filter attenuation. It is used to offset the values for the attenuation factor.

There are two ways of entering the calibration factor.

by editing, and

by transferring

Editing the Calibration Factor

You would use this, for example, to enter an offset to compensate for the insertion loss (attenuation) of your hardware setup.

The filter attenuation stays constant while you edit the calibration factor. This means that the attenuation factor, shown on the display, changes according to the formula below (from equation (1)):

AttNEW(dB) = Attfilter(dB) + CalNEW(dB) = AttOLD(dB) -CalOLD(dB) + CalNEW(dB)

To edit an external calibration factor,

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Agilent Technologies 8156A Entering a Calibration Factor, Resetting the Attenuation Factor, Editing the Calibration Factor

8156A specifications

Agilent Technologies 8156A is a high-performance optical source offering advanced capabilities for testing and characterizing optical systems. Specifically designed for applications in telecommunications and data communications, the 8156A stands out due to its precision, versatility, and reliability, making it an essential tool for engineers and researchers in the telecommunications industry.

One of the main features of the 8156A is its ability to generate a stable, accurate, and tunable optical signal. This optical source operates across a wide wavelength range, typically from 1260 nm to 1675 nm, covering key regions used in fiber optics. The tunable laser module is particularly beneficial for applications requiring the testing of fiber optic components, systems, and networks, enabling users to specify any wavelength within this range.

The device employs advanced technologies, including distributed feedback (DFB) laser technology, offering low noise and high output power while ensuring minimal phase and frequency jitter. This results in precise measurements that are crucial for evaluating the performance of optical devices. The 8156A also features a built-in optical power meter, allowing for seamless integration and real-time monitoring of optical power levels during testing.

Another significant characteristic of the 8156A is its user-friendly interface, which includes easy-to-read displays and intuitive controls. This design simplifies operation, allowing users to set up tests quickly and efficiently. Additionally, it provides various output options, including single-mode and multi-mode fiber interface compatibility, expanding its usability across different applications.

The 8156A is equipped to handle numerous protocols and systems, including passive optical networks (PON), optical transport networks (OTN), and traditional wavelength-division multiplexing (WDM) technologies. Its agility in adapting to various protocols enhances its role in research and development settings.

Moreover, the device offers a range of automation features, enabling users to script complex measurement sequences, making it an adaptable solution for both laboratory and field environments. Combined with its robust build quality, the Agilent Technologies 8156A optical source not only ensures reliable operation but also provides a long service life, making it a valuable investment for any optical testing application.