Optical amplification

Claim 2

An optical amplification method for an optical communication system which transmits signal light from a transmitting side to a receiving side via an optical transmission medium, comprising: separating the signal light into two orthogonally polarized beams by a first polarizing beam coupler/splitter; amplifying each orthogonally polarized beam by an optical amplifier, each of said optical amplifiers being oriented with respect to each polarized beam to achieve maximum optical gain, and combining together the two orthogonally amplified, polarized beams by a second polarizing beam coupler/splitter.

Claim 3

An optical amplification method according to claim 1, in which each of the optical amplifiers is a travelling-wave semiconductor laser optical amplifier.

Claim 4

An optical amplification method for an optical communication system which transmits signal light having a particular instantaneously fluctuated state of polarization from a transmitting side to a receiving side via an optical transmission medium, comprising: separating the signal light into two orthogonally polarized beams by a first polarizing beam coupler/splitter; amplifying each orthogonally polarized beam by an optical amplifier having a polarization dependency, each of said optical amplifiers being oriented with respect to each polarized beam to achieve maximum optical gain and to provide two orthogonally amplified, polarized beams of substantially the same optical gain level; and combining the two orthogonally amplified, polarized beams by a second polarized beam coupler/splitter.

Claim 5

An optical amplification method for an optical communication system which transmits signal light having a particular instantaneously fluctuated state of polarization from a transmitting side to a receiving side via an optical transmission medium, comprising: separating the signal light into two orthogonally polarized beams by a first polarizing beam coupler/splitter; amplifying each orthogonally polarized beam by an optical amplifier having a polarization dependency, each of said optical amplifiers being oriented with respect to each polarized beam to achieve maximum optical gain and to provide two orthogonally amplified, polarized beams of substantially the same optical gain level; and combining the two orthogonally amplified, polarized beams by a second polarized beam coupler/splitter.

Claim 6

An optical amplification method according to claim 3, in which each of the optical amplifiers is a light travelling wave semiconductor laser, or a Brillouin amplifier or an optical fiber Raman amplifier using a polarization maintaining optical fiber.

Claim 7

An optical amplification system for an optical communication system which transmits signal light having a particular instantaneously fluctuated state of polarization from a transmitting side to a receiving side via an optical transmission medium, comprising: a first polarizing beam coupler/splitter for separating the signal light into two orthogonally polarized beams; a first optical path and a second optical path provided to each transmit one of the two orthogonally polarized beams respectively; two optical amplifiers each having a polarization dependency, wherein one of said optical amplifiers is located in said first optical path and the other optical amplifier is located in said second optical path for amplifying each orthogonally polarized beam, each of said optical amplifiers being oriented with respect to each polarized beam to achieve maximum optical gain and to provide two orthogonally amplified, polarized beams of substantially the same optical gain level from the first path and the second path, respectively; and a second polarizing beam coupler/splitter optically coupled to the first optical path and the second optical path for combining the two orthogonally amplified, polarized beams.

Claim 8

An optical amplification system for an optical communication system which transmits signal light having a particular instantaneously fluctuated state of polarization from a transmitting side to a receiving side via an optical transmission medium, comprising: a first polarizing beam coupler/splitter for separating the signal light into two orthogonally polarized beams; a first optical path and a second optical path provided to each transmit one of the two orthogonally polarized beams respectively; two optical amplifiers each having a polarization dependency, wherein one of said optical amplifiers is located in said first optical path and the other optical amplifier is located in said second optical path for amplifying each orthogonally polarized beam, each of said optical amplifiers being oriented with respect to each polarized beam to achieve maximum optical gain and to provide two orthogonally amplified, polarized beams of substantially the same optical gain level from the first path and the second path, respectively; and a second polarizing beam coupler/splitter optically coupled to the first optical path and the second optical path for combining the two orthogonally amplified, polarized beams.

Claim 9

An optical amplification system according to claim 5, in which each of the optical amplifiers is a light travelling wave semiconductor laser comprising a Brillouin amplifier or an optical fiber Raman amplifier using a polarization maintaining optical fiber.