PUMP LIGHT GENERATION APPARATUS, OPTICAL AMPLIFIER AND PUMP LIGHT GENERATION METHOD
A pump light generation device including: a first multi-mode laser that outputs first pump light; a second multi-mode laser that outputs second pump light; a first pump current/temperature controller that controls a temperature and a pump current of the first multi-mode laser; a second pump current/temperature controller that controls a temperature and a pump current of the second multi-mode laser; a first polarization maintaining variable optical attenuator that adjusts a light intensity while keeping a polarization state in a linearly polarized wave and outputs the first pump light; a second polarization maintaining variable optical attenuator that adjusts a light intensity while keeping a polarization state in a linearly polarized wave and outputs the second pump light; and a polarization multiplexing circuit that polarization-multiplexes and output the pump light, in which the first pump current/temperature controller and the second pump current/temperature controller perform control such that the longitudinal modes in the first pump light and the second pump light do not overlap each other, and the first polarization maintaining variable optical attenuator and the second polarization maintaining variable optical attenuator perform control such that intensities are equal to each other.
1 - 8 . (canceled)
9 . An optical amplification device comprising:
a first single-mode laser configured to output continuous wave light having a light frequency of fc1;
a second single-mode laser configured to output continuous wave light having a light frequency of fc2 of a value different from fc1;
a first wavelength number changer configured to change output light of the first single-mode laser and generates first pump light having a plurality of emission-line spectra whose light frequency is fc1+n×δf1 (n is an integer including a negative); and
a second wavelength number changer configured to change output light of the second single-mode laser, generates second pump light having a plurality of emission-line spectra whose light frequency is fc2+n×δf2, and sets a frequency interval δf2 of a longitudinal mode to be as close as possible to a frequency interval δf1 of the longitudinal mode;
a polarization-multiplexing circuit configured to polarization-multiplex and outputs the first pump light and the second pump light; and
a gain medium, to which all of an optical signal and the first pump light and second pump light output from the polarization-multiplexing circuit are input, the gain medium amplifying and then outputting the optical signal.
10 . The optical amplification device according to claim 9 ,
wherein the first wavelength number changer generates the plurality of emission-line spectra by periodically modulating the output light of the first single-mode laser, and
the second wavelength number changer generates the plurality of emission-line spectra by periodically modulating the output light of the second single-mode laser.
11 . The optical amplification device according to claim 9 ,
wherein in a case where the optical signal is a digital signal with a baud rate fB, the n×δf1 and n×δf2 are different from the baud rate fB.
12 . The optical amplification device according to claim 9 , wherein the optical signal is a wavelength multiplexed signal in which a light frequency interval of an adjacent wavelength channel is fWDM, and the longitudinal mode frequency intervals δf1 and δf2 are values that are different from a light frequency interval fWDM of the adjacent wavelength channel.
13 - 16 . (canceled)
17 . A pump light generation method comprising:
by a first single-mode laser, outputting continuous wave light having a light frequency of fc1;
by a second single-mode laser, outputting continuous wave light having a light frequency of fc2 of a value different from fc1;
by a first wavelength number changer, changing output light of the first single-mode laser and generates first pump light having a plurality of emission-line spectra whose light frequency is fc1+n×δf1 (n is an integer including a negative); and
by a second wavelength number changer, changing output light of the second single-mode laser, generates second pump light having a plurality of emission-line spectra whose light frequency is fc2+n×δf2, and sets a frequency interval δf2 of a longitudinal mode to be as close as possible to a frequency interval δf1 of the longitudinal mode;
by a polarization-multiplexing circuit, polarization-multiplexing and outputs the first pump light and the second pump light; and
a gain medium, to which all of an optical signal and the first pump light and second pump light output from the polarization-multiplexing circuit are input, the gain medium amplifying and then outputting the optical signal.