Jds Uniphase Corporation

Lumentum Operations LLC

John Martinho

Jay A Skidmore

Nicolas Guerin

Yonghong Guo

Yi Liang

Thomas Friessnegg

Xia Hong

Louis B Allard

Huijie Xu

Yaogeng Ding

Lihua Wang

Jonathan Paradis

A pump laser package may include an input fiber to send signal light on a first optical path. A first lens may be arranged on the first optical path. The pump laser package may include a source to send pump light on a second optical path. A second lens and a negative lens may be arranged on the second optical path. The first lens and the negative lens may be arranged to create a virtual image associated with the pump light. The pump laser package may include an output fiber on a third optical path. The first lens may be arranged on the third optical path. The pump laser package may include a combiner to receive the signal light on the first optical path, receive the pump light on the second optical path, and send the signal light and the pump light on the third optical path.

Fiber coupled laser source pump with wavelength division multiplexer

A method for the rapid measurement of polarization dependent properties of an optical device under test uses a novel technique to generate light in four different polarization states in which each state is individually sensed at a different interference frequency. The device for executing this method includes a Mach-Zehnder interferometer (M-Z) having a reference arm and a signal arm. In the signal arm, a device called a 'polarization state frequency multiplexer' (PSFM) splits the light into four ports, transforms each part into one of four predetermined polarization states and then combines the light in the different polarization states together. The combined light is then passed through the device under test and combined/interfered with the light propagating through the reference arm at the output of the M-Z interferometer. Since the optical frequency of the input light to the M-Z interferometer is scanned through a range of wavelengths at a fixed repetition rate, the output light intensity (reference pattern) from the interferometer is modulated. By analyzing the M-Z interferometer output in the frequency domain, the signal levels of each polarization state can be identified and measured.

Polarization state frequency multiplexing

In order to calibrate an apparatus for measuring the polarization dependent loss of an optical device under test, a set of nominal polarization states of incident light are generated with a polarization generator. The incident light is then passed through a dot-product conserving polarization rotator at a first setting. A transmission characteristic is measured through a standard optical component with a known polarization dependent loss value for each polarization state. This step is repeated for a number of different settings of the polarization rotator. A polarization dependent loss value is calculated for the standard optical component based on the measured transmission characteristics at each polarization rotator setting. The calculated polarization dependent loss values are then processed to generate an aggregate error value. The aggregate error value is minimized by adjusting the values of the nominal polarization states to estimate the actual polarization states, which can then be used to calculate the polarization dependent loss of an optical device whose value is unknown.

Polarization dependent loss measurement in photonic devices

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John Martinho