Oscillation polarization selective semiconductor laser and optical communication system using the same

Claim 2

An oscillation polarization selective semiconductor laser for switching an oscillation polarization mode between two different polarization modes, said semiconductor laser comprising: a distributed reflector; and an active layer, said active layer having at least two quantum well structures, each of which includes a quantum well and barriers, and a bandgap of a quantum well of one of said quantum well structures being different from a bandgap of a quantum well of the other of said quantum well structures such that a distribution of gain spectra generated in said active layer for said two different polarization modes induced in a layer structure of said laser is varied by varying a density of carriers injected into said active layer.

Claim 3

A semiconductor laser according to claim 1, wherein the layer structure of said laser includes at least a first clad layer, a light guide layer, said active layer and a second clad layer formed in this order, and said distributed reflector comprises a grating reflector formed in said light guide layer.

Claim 4

A semiconductor laser according to claim 1, wherein a strain perpendicular to a layering direction is imparted to at least one of said quantum well structures.

Claim 5

A semiconductor laser according to claim 3, wherein a strain perpendicular to the layering direction is imparted to said at least two quantum well structures.

Claim 6

A semiconductor laser according to claim 3, wherein a strain perpendicular to a layering direction is imparted to at least one of said barriers of said at least two of said quantum well structures.

Claim 7

A semiconductor laser according to claim 1, wherein said laser is divided into a plurality of regions in a resonance direction, electrodes are respectively formed on said regions and a level of injected carriers is varied by independently injecting carriers into said regions.

Claim 8

A semiconductor laser according to claim 1, wherein said reflector has a first Bragg wavelength for one of said two different polarization modes and a second Bragg wavelength for the other of said two different polarization modes, and said first and second Bragg wavelengths are set to values which are substantially equal to values corresponding to said bandgaps of said quantum wells.

Claim 9

A semiconductor laser according to claim 1, wherein said reflector has a first Bragg wavelength for one of said two different polarization modes and a second Bragg wavelength for the other of said two different polarization modes, and at least one of said first and second Bragg wavelengths is set to a value which is substantially equal to a a value corresponding to one of said bandgaps of said quantum wells.

Claim 10

A semiconductor laser according to claim 1, wherein said laser is constructed as a distributed feedback semiconductor laser.

Claim 11

A semiconductor laser according to claim 1, wherein said laser is constructed as a distributed Bragg reflector semiconductor laser.

Claim 12

A semiconductor laser according to claim 1, wherein said laser is constructed as a tunable semiconductor laser.

Claim 13

A semiconductor laser according to claim 3, wherein said strain is a tensile strain.

Claim 14

A semiconductor laser according to claim 3, wherein said strain is a compressive strain.

Claim 15

A semiconductor laser according to claim 3, wherein said strain is imparted to a quantum well of said at least one of said quantum well structures.

Claim 16

A semiconductor laser according to claim 14, wherein a tensile strain perpendicular to the layering direction is imparted to said quantum well which has a wider bandgap.

Claim 17

A semiconductor laser according to claim 14, wherein a compressive strain perpendicular to the layering direction is imparted to said quantum well which has a narrower bandgap.

Claim 18

A semiconductor laser according to claim 4, wherein a tensile strain perpendicular to the layering direction is imparted to said quantum well which has a wider bandgap, and a compressive strain perpendicular to the layering direction is imparted to said quantum well which has a narrower bandgap.

Claim 19

A semiconductor laser according to claim 1, wherein said two different polarization modes are a transverse electric mode and a transverse magnetic mode.

Claim 20

A semiconductor laser according to claim 18, wherein said reflector has a first Bragg wavelength for said transverse electric mode and a second Bragg wavelength for said transverse magnetic mode, and said first and second Bragg wavelengths are set to values which are substantially equal to values corresponding to said bandgaps of said quantum wells.

Claim 21

A semiconductor laser according to claim 19, wherein said first Bragg wavelength is set to a value which is substantially equal to a value corresponding to the bandgap of the quantum well which has a narrower bandgap, said second Bragg wavelength is set to a value which is substantially equal to a value corresponding to the bandgap of the quantum well which has a wider bandgap.

Claim 22

A semiconductor laser according to claim 1, wherein said reflector has a first Bragg wavelength for one of said two different polarization modes and a second Bragg wavelength for the other of said two different polarization modes.

Claim 23

A semiconductor laser according to claim 1, wherein at least two of said quantum well structures are stacked.

Claim 24

An optical communication system for transmitting a signal from a transmitter side to a receiver side over a transmission line, said communication system comprising: an oscillation polarization selective semiconductor laser for switching an oscillation polarization mode between two different polarization modes, said semiconductor laser including a distributed reflector and an active layer, said active layer having at least two quantum well structures each of which includes a quantum well and barriers, and a bandgap of a quantum well of one of said quantum well structures being different from a bandgap of a quantum well of the other of said quantum well structures such that a distribution of gain spectra generated in said active layer for said two different polarization modes induced in a layer structure of said laser is varied by varying a density of carriers injected into said active layer; and a polarizer disposed in front of a light emission end surface of said semiconductor laser for selecting only a signal having a predetermined polarization mode.

Claim 25

An optical communication system for transmitting a signal from a transmitter side to a receiver side over a transmission line, said communication system comprising: an oscillation polarization selective semiconductor laser for switching an oscillation polarization mode between two different polarization modes, said semiconductor laser including a distributed reflector and an active layer, said active layer having at least two quantum well structures each of which includes a quantum well and barriers, and a bandgap of a quantum well of one of said quantum well structures being different from a bandgap of a quantum well of the other of said quantum well structures such that a distribution of gain spectra generated in said active layer for said two different polarization modes induced in a layer structure of said laser is varied by varying a density of carriers injected into said active layer; and a polarizer disposed in front of a light emission end surface of said semiconductor laser for selecting only a signal having a predetermined polarization mode.