WAVELENGTH SWEPT SOURCE APPARATUS AND CONTROLLING METHOD THEREOF

• US 20150002918A1
• Filed: 01/06/2014
• Published: 01/01/2015
• Est. Priority Date: 06/26/2013
• Status: Abandoned Application

• Current Assignee: Electronics and Telecommunications Research Institute
• Original Assignee: Electronics and Telecommunications Research Institute
• Inventors: KWON, Oh Kee, LEE, Chul-Wook, HAN, Young-Tak, SHIN, Jang Uk, OH, Kwang Ryong, SONG, Minhyup
• Application Number:
  US14/148,086
• Publication Number:
  US 20150002918A1
• Time in Patent Office: Days
• US Class Current: 359/239
• CPC Class Codes: G02F 1/3532 Arrangements of plural nonlinear devices for generating multi-colour light beams, e.g. arrangements of SHG, SFG, OPO devices for generating RGB light beams
• CPC Class Codes: H01S 5/0687 Stabilising the frequency of the laser

Abstract

Provided are a wavelength swept source apparatus and a method for controlling thereof. According to the provided apparatus and method, single mode light is generated, a basic optical comb is generated by modulating the generated single mode light, and a plurality of optical combs having different a frequency band from that of the basic optical comb is generated by modulating the plurality of light rays. The plurality of light rays and light rays included in the plurality of optical combs are sequentially emitted according to frequencies of the plurality of light rays and the light rays included in the plurality of optical combs. A value of a control variable is adjusted based on a characteristic of the generated single mode light, the plurality of light rays, the light rays included in the plurality of optical combs, and the emitted light rays.

Claims

1. A wavelength swept source apparatus comprising:

a light source configured to generate single mode light;

an optical comb generation unit configured to generate a basic optical comb comprising a plurality of light rays having identical frequency differences with adjacent light rays by modulating the generated single mode light;

a frequency band extension unit configured to generate a plurality of optical combs by modulating the plurality of light rays, wherein each of the plurality of optical combs comprises same number of light rays as the plurality of light rays, each of the same number of light rays has identical frequency differences with adjacent light rays, each of the plurality of optical combs does not overlap the basic optical comb and has a different frequency band from that of the basic optical comb, and the plurality of optical combs is distributed in a wider frequency band than that in which the basic optical comb is distributed;

a light emission unit configured to sequentially emit the plurality of light rays and light rays included in the plurality of optical combs according to frequencies of the plurality of light rays and the light rays included in the plurality of optical combs; and

a control unit configured to adjust a value of a control variable for at least one of the light source, the optical comb generation unit, the frequency band extension unit, and the light emission unit, based on a characteristic of light outputted from at least one of the light source, the optical comb generation unit, the frequency band extension unit, and the light emission unit.

2. The wavelength swept source apparatus of claim 1, further comprising:

an optical coupler configured to split output light of at least one of the optical comb generation unit and the light emission unit; and

an optical detector configured to transform intensity of the split output light into an electric signal,

wherein the control unit adjusts a value of a current provided to the light source based on the transformed electric signal.

3. The wavelength swept source apparatus of claim 1, further comprising an optical amplifier or optical attenuator configured to adjust intensity of output light of the optical comb generation unit.

4. The wavelength swept source apparatus of claim 3, further comprising:

an optical coupler configured to split output light of at least one of the optical amplifier or optical attenuator and the light emission unit; and

an optical detector configured to transform intensity of the split output light into an electric signal,

wherein the control unit adjusts a gain value of the optical amplifier or optical attenuator based on the transformed electric signal.

5. The wavelength swept source apparatus of claim 1, further comprising:

an optical coupler configured to split output light of the frequency band extension unit; and

an optical spectrum analyzer configured to calculate a frequency band in which the split output light is distributed,

wherein the control unit adjusts at least one of a value of a current provided to the light source, a value of a voltage applied to the optical comb generation unit, and a modulation frequency that determines the voltage applied to the optical comb generation unit, based on the calculated frequency band.

6. The wavelength swept source apparatus of claim 1, further comprising:

an optical coupler configured to split output light of the light emission unit; and

a real-time scope or linewidth measuring instrument configured to calculate an interval between a time at which light having the highest frequency is emitted from the optical coupler and a time at which light having the lowest frequency is emitted from the optical coupler,

wherein the control unit adjusts modulation signal width that determines a voltage applied to the optical comb generation unit, based on the calculated interval.

7. The wavelength swept source apparatus of claim 1, wherein the light emission unit comprises a dispersion controller configured to adjust an interval between each time at which each of the plurality of light rays and the light rays included in the plurality of optical combs is emitted.

8. The wavelength swept source apparatus of claim 7, further comprising:

an optical coupler configured to split output light of the dispersion controller; and

a real-time scope or linewidth measuring instrument configured to calculate an interval between a time at which a light ray having the highest frequency is emitted from the optical coupler and a time at which a light ray having the lowest frequency is emitted from the optical coupler,

wherein the control unit adjusts a value of a voltage applied to the dispersion controller based on the calculated interval.

9. A method for controlling a wavelength swept source apparatus, the method comprising:

generating single mode light;

generating a basic optical comb comprising a plurality of light rays having identical frequency differences with adjacent light rays by modulating the generated single mode light;

generating a plurality of optical combs by modulating the plurality of light rays, wherein each of the plurality of optical combs comprises same number of light rays as the plurality of light rays, each of the same number of light rays has identical frequency differences with adjacent light rays, each of the plurality of optical combs does not overlap the basic optical comb and has a different frequency band from that of the basic optical comb, and the plurality of optical combs is distributed in a wider frequency band than that in which the basic optical comb is distributed;

sequentially emitting the plurality of light rays and light rays included in the plurality of optical combs according to frequencies of the plurality of light rays and the light rays included in the plurality of optical combs;

determining whether a characteristic of at least one of the generated single mode light, the plurality of light rays, the light rays included in the plurality of optical combs, and the emitted light rays reaches a target value; and

adjusting a value of a control variable for at least one of the generated single mode light, the plurality of light rays, the light rays included in the plurality of optical combs, and the emitted light rays, if the characteristic of at least one of the generated single mode light, the plurality of light rays, the light rays included in the plurality of optical combs, and the emitted light rays does not reach the target value.

10. The method of claim 9, wherein

the determining comprises determining whether intensity of at least one of the plurality of light rays and the emitted light rays reaches the target value, and

the adjusting comprises adjusting at least one of a value of a current for controlling an output of the generated single mode light and a gain value for controlling the intensity of the plurality of light rays.

11. The method of claim 9, wherein

the determining comprises determining whether a frequency band in which the plurality of light rays and the light rays included in the plurality of optical combs is distributed reaches the target value, and

the adjusting comprises adjusting at least one of a value of a current for controlling an output of the generated single mode light, a value of a voltage for controlling an output of the plurality of light rays, and a modulation frequency that determines the voltage for controlling the output of the plurality of light rays.

12. The method of claim 9, wherein

the determining comprises determining whether an interval between a time at which a light ray having the highest frequency among the emitted light rays is emitted and a time at which a light ray having the lowest frequency among the emitted light rays is emitted reaches the target value, and

the adjusting comprises adjusting at least one of modulation signal width that determines a voltage for controlling an output of the plurality of light rays and an interval between each time at which each of the emitted light rays is emitted.