The patent badge is an abbreviated version of the USPTO patent document. The patent badge does contain a link to the full patent document.

The patent badge is an abbreviated version of the USPTO patent document. The patent badge covers the following: Patent number, Date patent was issued, Date patent was filed, Title of the patent, Applicant, Inventor, Assignee, Attorney firm, Primary examiner, Assistant examiner, CPCs, and Abstract. The patent badge does contain a link to the full patent document (in Adobe Acrobat format, aka pdf). To download or print any patent click here.

Date of Patent:
Apr. 30, 2002

Filed:

Sep. 03, 1999
Applicant:
Inventors:

Robert Meachem Jopson, Rumson, NJ (US);

Herwig Werner Kogelnik, Rumson, NJ (US);

Lynn Elizabeth Nelson, Eatontown, NJ (US);

Assignee:

Lucent Technologies Inc., Murray Hill, NJ (US);

Attorney:
Primary Examiner:
Assistant Examiner:
Int. Cl.
CPC ...
G02F 1/01 ;
U.S. Cl.
CPC ...
G02F 1/01 ;
Abstract

The present invention consists of a method and apparatus for measuring first and higher order PMD vectors in optical fibers. For each first-order PMD vector determination, two distinct polarization states are sequentially injected into an optical device under test for each of a pair of frequencies &ohgr; and &ohgr;+&Dgr;&ohgr; . A Stokes vector s representing the first polarization state must not be parallel or anti-parallel to a Stokes vector s representing the second polarization state, but the relative angle between s and s need not be known. The frequency interval &Dgr;&ohgr; is large to obtain a high signal-to-noise ratio. Thus, four light beams are injected, the first at frequency &ohgr; and polarization s , the second at frequency &ohgr; and polarization s , the third at frequency &ohgr;+&Dgr;&ohgr; and polarization s , and the fourth light at frequency &ohgr;+&Dgr;&ohgr; and polarization s . The output polarizations of these beams are measured and four corresponding output Stokes vectors are determined. A first-order PMD vector is then calculated from the four input Stokes vectors and four output Stokes vectors. Each subsequent PMD vector determination is then made using a pair of frequencies which differs from the previous pair of frequencies by a frequency interval &Dgr;&ohgr; which is small compared to &Dgr;&ohgr; . Since &Dgr;&ohgr; can be small, high spectral resolution of the PMD vector can be obtained, while still maintaining good signal-to-noise ratio provided by using a large &Dgr;&ohgr; . The good signal-to-noise ratio and high spectral resolution of the PMD vector allow the accurate determination of second- and higher-order PMD vectors.


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