Method of designing semiconductor laser device, method of designing raman amplifier, methods of manufacturing semiconductor laser device, semiconductor laser device, raman amplifier, and optical communication system

Patent metadata

Field	Value
Publication number	US-9711945-B2
Application number	US-201615177175-A
Country	US
Kind code	B2
Filing date	Jun 8, 2016
Priority date	Dec 27, 2013
Publication date	Jul 18, 2017
Grant date	Jul 18, 2017

Abstract

A method of designing a semiconductor laser device includes: controlling a distance between the output-side reflection unit and the second reflection unit and an effective optical feedback κ to the semiconductor laser element, the effective optical feedback κ defined by a below-presented formula (1) including a circulating time τ of the light in the semiconductor laser element, a reflectivity R 1 of the output-side reflection unit, and a reflectivity R 2 of the second reflection unit; selecting a semiconductor laser device in which an LFF period is equal to or smaller than 20 ns as a semiconductor laser device in which high speed switching occurs between an FBG mode and an FP mode; and using the selected semiconductor laser device as an semiconductor laser device oscillating in a coherent collapse mode.

κ=(1/τ)×(1− R 1 )×( R 2 /R 1 ) 1/2   (1)

First claim

What is claimed is:

1. A method of designing a semiconductor laser device used for a pumping light source for Raman amplification and including: a semiconductor laser element including an optical cavity including a semiconductor light-emitting unit and a first reflection unit reflecting a light outputted by the semiconductor light-emitting unit; and a second reflection unit disposed at a laser-light-output side of the semiconductor laser element, wherein the first reflection unit includes an output-side reflection unit provided at the laser-light-output side and a rear-end-side reflection unit provided at an opposite side to the laser-light-output side, the method of designing comprising:
controlling: a physical distance L (cm) between the output-side reflection unit and the second reflection unit; and an effective optical feedback κ(1/ps) to the semiconductor laser element, the effective optical feedback κ(1/ps) defined by a below-presented formula (1) including a circulating time τ of the light in the semiconductor laser element, a reflectivity R 1 of the output-side reflection unit, and a reflectivity R 2 of the second reflection unit;
selecting the semiconductor laser device in which a Low Frequency Fluctuation (LFF) period is equal to or smaller than 20 ns as the semiconductor laser device in which a high speed switching occurs between a Fiber Bragg Grating (FBG) mode and a Fabry-Perot (FP) mode; and
using the selected semiconductor laser device as a semiconductor laser device oscillating in a coherent collapse mode,
wherein the controlling is performed while measuring a relationship between an intensity of the laser light outputted from the semiconductor laser device and time to perform the selecting by finding out the semiconductor laser device in which the high speed switching occurs between the FBG mode and the FP mode,
when measuring the relationship between the intensity of the laser light outputted from the semiconductor laser device and the time to perform the selecting, the LFF period is defined as an interval between a reference peak at which a decrease in the intensity is greatest in a predetermined time period and a nearest adjacent peak of which absolute value of the intensity is equal to or greater than 60% of the reference peak, and
the semiconductor laser device at a time the defined LFF period is equal to or smaller than 20 ns is determined and selected as the semiconductor laser device to be used
κ=(1/τ)×(1− R 1 )×( R 2 /R 1 ) 1/2   (1).

2. The method of designing according to claim 1 , wherein the intensity of the laser light outputted from the semiconductor laser device is set at equal to or smaller than 50 mW.

3. The method of designing according to claim 1 , wherein the intensity of the laser light outputted from the semiconductor laser device is set at equal to or greater than 20 mW.

4. The method of designing according to claim 1 , wherein
a wavelength of the laser light outputted from the semiconductor laser element is within a range of 1.3 μm to 1.6 μm, and
a relationship between the physical distance L (cm) between the output-side reflection unit and the second reflection unit and the effective optical feedback κ(1/ps) satisfies a relationship of L>5333×κ−33.

5. A semiconductor laser device used for a pumping light source for Raman amplification and including: a semiconductor laser element including an optical cavity including a semiconductor light-emitting unit and a first reflection unit reflecting a light outputted by the semiconductor light-emitting unit; and a second reflection unit disposed at a laser-light-output side of the semiconductor laser element, wherein the first reflection unit includes an output-side reflection unit provided at the laser-light-output side and a rear-end-side reflection unit provided at an opposite side to the laser-light-output side, wherein
a wavelength of a laser light outputted from the semiconductor laser element is within a range of 1.3 μm to 1.6 μm,
by controlling: a physical distance L (cm) between the output-side reflection unit and the second reflection unit; and an effective optical feedback κ(1/ps) to the semiconductor laser element so that a relationship between the physical distance L (cm) and the effective optical feedback κ(1/ps) defined by a below-presented formula (1) including a circulating timer τ of the light in the semiconductor laser element, a reflectivity R 1 of the output-side reflection unit, and a reflectivity R 2 of the second reflection unit satisfies a relationship of L>5333κ−33, the semiconductor laser device is a semiconductor laser device in which a Low Frequency Fluctuation (LFF) period is equal to or smaller than 20 ns selected as a semiconductor laser device in which a high speed switching occurs between a Fiber Bragg Grating (FBG) mode and a Fabry-Perot (FP) mode to oscillate in a coherent collapse mode,
in order to find out, and conduct the selection of, the semiconductor laser device in which the high speed switching occurs between the FBG mode and the FP mode, the controlling is conducted while measuring a relationship between an intensity of the laser light outputted from the semiconductor laser device and time to conduct the selection,
when measuring the relationship between the intensity of the laser light outputted from the semiconductor laser device and the time to conduct the selection, the LFF period is defined as an interval between a reference peak at which a decrease in the intensity is the greatest in a predetermined time period and a nearest adjacent peak of which absolute value of the intensity is equal to or greater than 60% of the reference peak, and
the semiconductor laser device at a time when the defined LFF period is equal to or smaller than 20 ns is determined and selected to be used
κ=(1/τ)×(1− R 1 )×( R 2 /R 1 ) 1/2   (1).

6. The semiconductor laser device according to claim 5 , wherein the intensity of the outputted laser light is set at equal to or smaller than 50 mW.

7. The semiconductor laser device according to claim 5 , wherein the intensity of the outputted laser light is set at equal to or greater than 20 mW.

Assignees

• Furukawa Electric Co Ltd

Inventors

• Hasegawa Hideaki
• Yokouchi Noriyuki
• Sawamura Taketsugu
• Irino Satoshi
• Yoshida Junji

Classifications

• H01S5/0652

  Coherence lowering or collapse, e.g. multimode emission by additional input or modulation · CPC title

• H01S5/146 Primary

  using a fiber as external cavity · CPC title

• H01S2301/03

  Suppression of nonlinear conversion, e.g. specific design to suppress for example stimulated brillouin scattering [SBS], mainly in optical fibres in combination with multimode pumping · CPC title

• H01S3/094096

  Multi-wavelength pumping · CPC title

• H01S5/02208

  characterised by the shape of the housings · CPC title