Polarimeters
Polarimetry
Measurement of all 4 Stokes parameters, display on Poincaré sphere and in oscilloscope mode. Also available: power, normalized Stokes vector and degree-of-polarization (DOP).
Three choices for the normalization of Stokes parameters/vectors:
Standard: Normalized Stokes vectors are normalized to unit length. Regardless of power and DOP, they appear at the surface of the Poincaré sphere.
Exact: Normalized Stokes vectors are normalized only with respect to optical power. For DOP<1 they appear inside the Poincaré sphere. Unpolarized light is displayed at the coordinate origin.
Non-normalized: Display of the non-normalized Stokes parameters. This means, the DOP and the optical power determine the length of the displayed S1-S2-S3 Stokes vector.
Only the PM1000 polarimeter is needed.
Mueller and Jones matrix measurement
In addition to the PM1000 polarimeter, an device for generating a number of polarization states is needed.
This can be the EPS1000 polarization scrambler/transfomer or any other polarization state generator or scrambler which generates a repeatable sequence of polarization states and can be synchronized with the PM1000, for example by a trigger output or input or via USB. For simplicity you can use a PMS1000 polarimeter and polarization scrambler/transfomer(= combination of PM1000 and EPS1000).
With PMS1000 or additional EPS1000, any specified polarization state can be generated.
The Mueller matrix of the device under test is thus determined. Subsequent calculations yield:
Mueller-Jones matrix (= the Mueller matrix made non-depolarizing) and Jones matrix
Eigenmodes, retardation, mean loss and polarization-dependent loss (PDL)
Decomposition of Mueller and Jones matrices into sequences SBA + PPPS + SBA. Definitions: PPPS = horizontal partial polarizer and phase shifter. SBA = Soleil-Babinet analog = retarder having a retardation between 0 and π and eigenmodes anywhere on the S2-S3 great circle of the Poincaré sphere. See also here (Section II.A). An SBA does to horizontal polarization the same as a Soleil-Babinet compensator to circular polarization: partial or full mode conversion with adjustable phase shift.
PMD measurement
An optional tunable laser is built into the PM1000 polarimeter or PMS1000 polarimeter and polarization scrambler/transformer. Else, an available tunable laser is suitably controlled.
This way Mueller and Jones matrices can be measured as a function of optical frequency, and PMD is determined.
Model # | Band | Sampling Rate | Trigger Gating | Type |
---|---|---|---|---|
PM1000 | C+L | 100M SOP samples/sec | internal/external | Desktop, Module, IP Core |