Polarization mode dispersion

Specifications

Definition of Terms

Measurement: either with a fiber-loop type polarization controller using the polarization scanning method, or with a wavelength type polarization controller using the Mueller method.

The change of transit time caused by changing the input polarization state, expressed in fs (10-15seconds).

Conditions: Generation of all polarization states (covering the entire Poincar sphere.

Measurement: with the Agilent Technologies polarization analyzer.

Repeatability

The random uncertainty in reproducing the attenuation after changing and re-setting the attenuation. The repeatability is ± half the span between the maximum and the minimum attenuations, expressed in dB.

Conditions: uninterrupted line voltage, constant wavelength setting, temperature within ± 1 K, constant input polarization state.

Measurement: with an optical power meter.

Return loss

The ratio of the incident power to the reflected power, expressed in dB.

Conditions: jumper cables with high-quality connectors on both attenuator ports. Arbitrary attenuation setting. Applicable to both attenuator ports, with the respective second port terminated (zero reference).

Measurement: with a return loss meter, using a Fabry-Perot type laser source. The measurement result includes attenuator-internal reflectances and reflectances from both attenuator ports.

Wavelength range The range of wavelengths to which the specifications apply.

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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.

Agilent Technologies 8156A manual Polarization mode dispersion, Repeatability, Return loss

Models: 8156A

Definition of Terms