U.S. patent application number 13/675449 was filed with the patent office on 2013-08-15 for optical semiconductor device.
This patent application is currently assigned to MITSUBISHI ELECTRIC CORPORATION. The applicant listed for this patent is MITSUBISHI ELECTRIC CORPORATION. Invention is credited to Eitaro Ishimura, Keisuke Matsumoto, Takeshi Saito, Yoshifumi Sasahata, Masakazu Takabayashi, Kazuhisa Takagi, Tohru Takiguchi.
Application Number | 20130208350 13/675449 |
Document ID | / |
Family ID | 48945365 |
Filed Date | 2013-08-15 |
United States Patent
Application |
20130208350 |
Kind Code |
A1 |
Saito; Takeshi ; et
al. |
August 15, 2013 |
OPTICAL SEMICONDUCTOR DEVICE
Abstract
An optical semiconductor device includes: semiconductor lasers;
a wave coupling section multiplexing light output by the
semiconductor lasers; an optical amplifying section amplifying
output light of the wave coupling section; a first optical
waveguide optically connecting respective semiconductor lasers to
the wave coupling section; a second optical waveguide optically
connecting the wave coupling section to the optical amplifying
section; a third optical waveguide optically connected to an output
of the optical amplifying section; and a phase regulator located in
at least one of the first, second, and third optical waveguides,
and regulating phase of reflected light that is reflected at a
reflecting point in the optical semiconductor device and that
returns to the semiconductor lasers. The phase regulator adjusts
the phase of the reflected light to decrease line width of the
light output by the semiconductor lasers.
Inventors: |
Saito; Takeshi; (Tokyo,
JP) ; Takabayashi; Masakazu; (Tokyo, JP) ;
Ishimura; Eitaro; (Tokyo, JP) ; Takiguchi; Tohru;
(Tokyo, JP) ; Takagi; Kazuhisa; (Tokyo, JP)
; Matsumoto; Keisuke; (Tokyo, JP) ; Sasahata;
Yoshifumi; (Tokyo, JP) |
|
Applicant: |
Name |
City |
State |
Country |
Type |
MITSUBISHI ELECTRIC CORPORATION; |
|
|
US |
|
|
Assignee: |
MITSUBISHI ELECTRIC
CORPORATION
Tokyo
JP
|
Family ID: |
48945365 |
Appl. No.: |
13/675449 |
Filed: |
November 13, 2012 |
Current U.S.
Class: |
359/341.1 |
Current CPC
Class: |
H01S 5/4062 20130101;
H01S 3/067 20130101; H01S 3/107 20130101; H01S 5/026 20130101; H04B
10/548 20130101; H01S 5/12 20130101; H01S 5/0265 20130101; H04B
10/54 20130101; H01S 5/0654 20130101; H04J 14/02 20130101; H01S
5/14 20130101; H01S 3/10053 20130101 |
Class at
Publication: |
359/341.1 |
International
Class: |
H01S 3/067 20060101
H01S003/067 |
Foreign Application Data
Date |
Code |
Application Number |
Feb 15, 2012 |
JP |
2012-030779 |
Claims
1. An optical semiconductor device comprising: a plurality of
semiconductor lasers; a wave coupling section multiplexing light
output by the plurality of the semiconductor lasers; an optical
amplifying section amplifying output light of the wave coupling
section; a first optical waveguide optically connecting respective
semiconductor lasers to the wave coupling section; a second optical
waveguide optically connecting the wave coupling section to the
optical amplifying section; a third optical waveguide optically
connected to an output of the optical amplifying section; and a
phase regulator located in at least one of the first, second, and
third optical waveguides, and regulating phase of reflected light
that is reflected at a reflecting point located in the optical
semiconductor device and that returns to the plurality of
semiconductor lasers, wherein the phase regulator adjusts the phase
of the reflected light to decrease line width of the light output
by the plurality of semiconductor lasers.
2. The optical semiconductor device according to claim 1, further
comprising a control section adjusting a bias voltage applied to
the phase regulator so that the phase regulator adjusts the phase
of the reflected light to decrease the line width of the light
output by the plurality of semiconductor lasers.
3. An optical semiconductor device comprising: a plurality of
semiconductor lasers; a wave coupling section multiplexing light
output by the plurality of the semiconductor lasers; an optical
amplifying section amplifying output light of the wave coupling
section; an optical waveguide optically connecting respective
semiconductor lasers to the wave coupling section; and a light
intensity lowering section located in the optical waveguide, and
lowering light intensity of reflected light that is reflected at a
reflecting point located in the optical semiconductor device and
that returns to the plurality of semiconductor lasers, wherein the
light intensity lowering section lowers the light intensity of the
reflected light to decrease line width of the light output by the
plurality of semiconductor lasers.
4. The optical semiconductor device according to claim 3, further
comprising a control section adjusting a bias voltage applied to
the light intensity lowering section, and making the light
intensity lowering section lower the light intensity of the
reflected light to decrease the line width of the light output by
the plurality of semiconductor lasers.
5. The optical semiconductor device according to claim 1, further
comprising an optical modulator optically connected to an output of
the optical amplifying section.
6. The optical semiconductor device according to claim 3, further
comprising an optical modulator optically connected to an output of
the optical amplifying section.
Description
BACKGROUND OF THE INVENTION
[0001] 1. Field of the Invention
[0002] The present invention relates to a wavelength-variable
optical semiconductor device used in optical communication systems.
Specifically, the present invention relates to an optical
semiconductor device wherein the increase of spectral line width
due to the reflected light being reflected at the reflecting point
present in the device and returning to the semiconductor laser can
be inhibited.
[0003] 2. Background Art
[0004] In the long distance communication system using relay by an
optical amplifier, DWDM (Dense Wavelength Division Multiplexing) is
used for increasing the transmission volume for one optical fiber.
In this system, optical signals of about 80 different wavelengths
are multiplexed in one fiber. At present, the development of
wavelength-variable lasers that can oscillate at optional
wavelengths from the used wavelength band has progressed, which has
become the mainstream of the light source for long-distance optical
transceivers.
[0005] As a modem method, an IM-DD (Intensity Modulation-Direct
Detection) system has been used in systems having the signal speed
of up to 10 Gbit/s. In recently penetrating 40 Gbit/s system, phase
modulation and differential detection methods are used. In the
digital coherent system adopted in next-generation 100 Gbit/s
systems, phase modulation systems are used. In the signal receiving
side, a coherent detection system wherein local light and signal
light are mixed to detect the intensity and phase information are
used.
[0006] In the conventional IM-DD system, since no phase information
of the light is used, it is enough if the light source oscillates
at a single wavelength, the phase noise causes no problems.
However, in the digital coherent system, the phase noise of the
signal light source and the local light source causes the
deterioration of signal qualities. Although a spectrum line width
is used as the indicator showing the size of the phase noise of the
light source, it is required to narrow the spectrum line width for
lowering the phase noise.
[0007] As a method for realizing the wavelength-variable light
source, an optical semiconductor device wherein a plurality of
semiconductor lasers and optical amplifying sections are
accumulated has been reported. In this method, any one of a
plurality of semiconductor lasers arrayed in parallel is made to
flash, and the output light thereof is output from a waveguide via
a wave coupling section. By amplifying the output light in the
optical amplifying section, light having a desired wavelength is
output at a desired optical power.
[0008] The spectrum line width Vo has generally the relationship
shown in the following numerical expression 1.
v.sub.0.sup..varies.(.kappa.L.sub.DFB).sup.-2(L.sub.DFB).sup.-1(1+.alpha-
..sup.2) [Expression 1]
[0009] For realizing a narrow line width, it is desired to lengthen
the laser length L.sub.DFB. Also in the above described optical
semiconductor device wherein the semiconductor lasers and the
optical amplifying sections are accumulated, it has been reported
that the low line width of 1 MHz or below is realized by
lengthening the laser length. However, there are causes to
deteriorate the spectrum line width. In the case wherein a
reflectivity on the front end surface is limited, the light
reflected by the front end surface is again amplified by the
optical amplifying section, and the reflected light returns to the
semiconductor laser and causes adverse effects.
[0010] When a reflectivity on the front end surface is made to be
R0, the spectrum line width .DELTA..nu. when fed back is
represented the following Numerical Expression 2 (for example,
refer to IEEE JOURNAL OF SELECTED TOPICS IN QUANTUM ELECTRONICS,
Vol. 15, No. 3, May/Jun 2009, pp. 514-520).
.DELTA. v v 0 = 1 ( 1 + C sin { .omega. .tau. / .phi. c + arc tan (
.alpha. ) } ) 2 [ Expression 2 ] ##EQU00001##
Where, there is the relationship of the following numerical
expressions 3 and 4.
C = R ext L ext P DFB P nV L DFB K z 1 / .alpha. 2 [ Expression 3 ]
R ext = R 0 ( P SOA P DFB ) 2 [ Expression 4 ] ##EQU00002##
Where, .nu..sub.0 represents the line width when C=0, i.e. R=0;
.tau. represents the time required for one round trip of the
oscillator exterior to LD.
[0011] From the Numerical expression 2, when there is the feedback
due to reflections, the spectra line width changes periodically,
and becomes maximum when it is nearly
C sin{.omega..tau.+.phi.c/arctan (.alpha.)}=1
When change in the angular frequency for the current value applied
to the laser is approximated as in the following Numerical
expression 5, the line width changes periodically by the current
values applied to the semiconductor laser as shown in FIG. 3 (a) in
IEEE JOURNAL OF SELECTED TOPICS IN QUANTUM ELECTRONICS, Vol. 15,
No. 3, May/Jun 2009, pp. 514-520).
.omega.-.omega..sub.0=aI.sub.DFB.sup.2+bI.sub.DFB [Expression
5]
SUMMARY OF THE INVENTION
[0012] In reality, the end-face reflectivity cannot be 0, but there
is always a limited reflectivity. Therefore, the spectra line
widths of a conventional optical semiconductor device wherein
semiconductor lasers and optical amplifying sections are
accumulated changes periodically depending upon the current values
of the semiconductor lasers, and at times, increase causing
problems on the system may be caused. Furthermore, when modulators
or the like are further accumulated, reflection may occur from each
part or the like to constitute the modulators, and similarly, the
increase of the spectra line width may be caused.
[0013] As long as such a limited reflectivity of a front end
surface or a reflection point present in the device is present, the
reflected light returns to the semiconductor laser after the
reflected light is amplified in the optical amplifying section.
Therefore, there was a problem wherein the increase of the spectra
line width is caused depending on the driving current conditions of
the semiconductor laser.
[0014] In view of the above-described problems, an object of the
present invention is to provide an optical semiconductor device
which can inhibit the increase of the spectra line width by the
reflected light.
[0015] According to the present invention, an optical semiconductor
device includes: a plurality of semiconductor lasers; a wave
coupling section multiplexing output light of the plurality of the
semiconductor lasers; an optical amplifying section amplifying
output light of the wave coupling section; a first optical
waveguide respectively optically connecting the plurality of
semiconductor lasers to the wave coupling section; a second optical
waveguide optically connecting the wave coupling section to the
optical amplifying section; a third optical waveguide optically
connected to an output of the optical amplifying section; and a
phase regulator provided in at least one of the first, second, and
third optical waveguides, and regulating a phase of reflected light
that is reflected at a reflecting point present in the optical
semiconductor device and returns to the plurality of semiconductor
lasers. The phase regulator adjusts the phase of the reflected
light so as to decrease line width of the output light of the
plurality of semiconductor lasers.
[0016] The present invention makes it possible to inhibit the
increase of the spectra line width by the reflected light.
[0017] Other and further objects, features and advantages of the
invention will appear more fully from the following
description.
BRIEF DESCRIPTION OF THE DRAWINGS
[0018] FIG. 1 is a top view showing an optical semiconductor device
according to the first embodiment of the present invention.
[0019] FIG. 2 is a top view showing a modified example 1 of the
optical semiconductor device according to the first embodiment of
the present invention.
[0020] FIG. 3 is a top view showing a modified example 2.
[0021] FIG. 4 is a top view showing an optical semiconductor device
according to the second embodiment of the present invention.
[0022] FIG. 5 is a top view showing the modified example of the
optical semiconductor device according to the second embodiment of
the present invention.
[0023] FIG. 6 is a top view showing an optical modulator according
to the third embodiment of the present invention.
[0024] FIG. 7 is a top view showing the modified example of the
optical semiconductor device according to the third embodiment of
the present invention.
[0025] FIG. 8 is a top view showing an optical semiconductor device
according to the fourth embodiment of the present invention.
[0026] FIG. 9 is a top view showing the modified example of the
optical semiconductor device according to the fourth embodiment of
the present invention.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
[0027] A optical semiconductor device according to the embodiments
of the present invention will be described with reference to the
drawings. The same components will be denoted by the same symbols,
and the repeated description thereof may be omitted.
First Embodiment
[0028] FIG. 1 is a top view showing an optical semiconductor device
according to the first embodiment of the present invention. On an
InP substrate 1, a plurality of semiconductor lasers 2, a wave
coupling section 3, an optical amplifying section 4, optical
waveguides 5a, 5b, 5c, and 5d, and a phase regulator 6 are
accumulated. A plurality of semiconductor lasers 2 are the DFB-LD
(Distributed Feedback Laser Diode) array. The wave coupling section
3 is an MMI coupler (Multi-Mode Interference). The optical
amplifying section 4 is an SOA (Semiconductor Optical Amplifier). A
control section 7 controls the bias applied to the phase regulator
6 and controls the phase regulator 6.
[0029] The wave coupling section 3 multiplexes the output light of
a plurality of the semiconductor lasers 2. The optical amplifying
section 4 amplifies the output light of the wave coupling section
3. The optical waveguide 5a is optically connected to the input
side of the semiconductor lasers 2. A plurality of optical
waveguides 5b respectively optically connect a plurality of
semiconductor lasers 2 to the wave coupling section 3. The optical
waveguide 5c optically connects the wave coupling section 3 to the
optical amplifying section 4. The optical waveguide 5d is optically
connected to the output of the optical amplifying section 4. The
phase regulator 6 is provided in the optical waveguide 5d, and
specifically, an electrode to which a bias is applied to the upper
portion of the optical waveguide 5d is provided. The phase
regulator 6 regulates the phase of the light that is reflected at
reflecting points present in the device and returns to a plurality
of semiconductor lasers 2.
[0030] When the control section 7 applies a forward bias or a
reverse bias to the phase regulator 6, by the carrier plasma effect
in the forward bias applying time, by the quantum confined Stark
effect or the like in the reverse bias applying time, the
reflectivity of the optical waveguide 5d is varied, and the light
path length is varied. Therefore, .tau. in the numerical expression
2 is varied, and the term of sin in the numerical expression 2 can
be optimized (where sin {.omega..tau.+.phi.c+arctan (.alpha.)}=1).
As described above, by adjusting the bias applied to the phase
regulator 6, the spectrum line width .DELTA..nu. can be minimized.
In addition, in the numerical expression 2, although the front end
surface is assumed as the reflecting point, the feedback from the
reflecting point other than the front end surface can be also
expressed by a similar numerical expression by replacing R0 of the
numerical expression 4 with the reflectivity of the reflecting
point.
[0031] Then, the control section 7 adjusts the bias applied to the
phase regulator 6, and makes the phase regulator 6 adjust the phase
of the reflected light so as to decrease the line width of the
output light of a plurality of semiconductor lasers 2. Thereby, the
increase of the spectra line width by the reflected light can be
inhibited.
[0032] FIG. 2 is a top view showing a modified example 1 of the
optical semiconductor device according to the first embodiment of
the present invention. FIG. 3 is a top view showing a modified
example 2. In addition to the configuration in the first
embodiment, an optical modulator 8 is optically connected to the
output of the optical amplifying section 4. In the modified example
1, the phase regulator 6 is provided between the optical amplifying
section 4 and the optical modulator 8. In the modified example 2,
the phase regulator 6 is provided in the optical waveguide 5e in
the output side of the optical modulator 8. In these cases, an
effect similar to the effect of the first embodiment can also be
obtained.
[0033] In this time, the optical waveguide 5a can be omitted. The
layer constructions of the optical waveguides 5a, 5b, 5c, and 5d
can be identical to the semiconductor laser 2 or the optical
amplifying section 4, or can be butt-jointed waveguides having
different construction and configuration. The optical modulator 8
can be a plurality of optical modulators connected in series.
Second Embodiment
[0034] FIG. 4 is a top view showing an optical semiconductor device
according to the second embodiment of the present invention. The
phase regulator 6 is provided in the optical waveguide 5c. In this
case also, an effect similar to that in the first embodiment can be
obtained.
[0035] FIG. 5 is a top view showing the modified example of the
optical semiconductor device according to the second embodiment of
the present invention. In addition to the constitution of the
second embodiment, the optical modulator 8 is optically connected
to the output of the optical amplifying section 4. In this case
also, an effect similar to that in the first embodiment can be
obtained.
Third Embodiment
[0036] FIG. 6 is a top view showing an optical modulator according
to the third embodiment of the present invention. A plurality of
phase regulators 6 are respectively provided in a plurality of
optical waveguides 5b. In this case also, an effect similar to that
in the first embodiment can be obtained.
[0037] FIG. 7 is a top view showing the modified example of the
optical semiconductor device according to the third embodiment of
the present invention. In addition to the configuration of the
third embodiment, the optical modulator 8 is optically connected to
the output of the optical amplifying section 4. In this case also,
an effect similar to that in the first embodiment can be
obtained.
[0038] In first to third embodiments, although the phase regulators
6 are respectively provided in the optical waveguides 5d, 5c, and
5b, the present invention is not limited thereto, but the phase
regulator 6 is not limited thereto, but the phase regulator 6 may
be provided in at least one of the optical wave guides 5b, 5c, and
5d.
Fourth Embodiment
[0039] FIG. 8 is a top view showing an optical semiconductor device
according to the fourth embodiment of the present invention. In
place of the phase regulator 6 to adjust the phase of the reflected
light, a light intensity lowering section 9 to lower the light
intensity of the reflected light is provided in the optical
waveguide 5b.
[0040] The layer configuration of the light intensity lowering
section 9 is identical to the layer configuration of the phase
regulator 6. The control section 7 supplies a larger bias to the
light intensity lowering section 9 than to the phase regulator 6,
and positively generates light absorption. When light absorption
occurs in the light intensity lowering section 9, the intensity of
the light inputted from the semiconductor lasers 2 to the optical
amplifying section 4 is lowered. However, in the optical amplifying
section 4, if the input reaches a constant value or more, the
saturation of the gain occurs. Using this characteristic, by
adjusting current value to the semiconductor lasers 2 so that the
power of light after passing through the light intensity lowering
section 9 is in the region of the gain saturation of the optical
amplifying section 4, the effect of the loss by the light intensity
lowering section 9, the effect of the loss by the intensity
lowering section 9 can be ignored.
[0041] On the other hand, the reflected light from the reflection
point in the device on the front end surface or on the side nearer
to the front end surface than the optical amplifying section 4 is
amplified by the optical amplifying section 4, and returns to the
semiconductor laser 2. Before this, the light intensity lowering
section 9 lowers the light intensity of the reflected light.
Therefore, the effect of the reflected light on the semiconductor
laser 2 is weakened, and the line width of output light of a
plurality of semiconductor lasers 2 is decreased. Therefore, the
control section 7 adjusts the bias applied to the light intensity
lowering section 9, and makes the light intensity lowering section
9 lower the light intensity of the reflected light so that the line
width of the output light. Thereby, the increase of the spectrum
line width by the reflected light can be inhibited.
[0042] In addition, by reversed biasing the light intensity
lowering section 9, the loss of the reflected light occurs, and at
the same time, change in the phase also occurs. Therefore, since
the effect of the third embodiment can also be obtained, the
periodical change of the line width observed in the numerical
expression 2 occurs. As the bias point, in addition to the effect
by the above-described absorption, the bias point to be the most
suitable in the points of the phase must be searched. Furthermore,
the optical waveguide 5a or the optical modulator 8 can be
omitted.
[0043] FIG. 9 is a top view showing the modified example of the
optical semiconductor device according to the fourth embodiment of
the present invention. In addition to the configuration of the
fourth embodiment, phase regulators 6 are respectively provided in
the optical waveguides 5c, 5d, and 5e. The phase regulators 6 can
also be provided in only one or two of the optical waveguides 5c,
5d, and 5e. The control section 7 adjusts the bias applied to these
phase regulators 6, and makes the phase regulators 6 adjust the
phase of the reflected light so that the line width of the output
light of a plurality of semiconductor lasers 2 is decreased.
[0044] Furthermore, in the first to fourth embodiments, an
electrical resistor can be provided on the electrode of the phase
regulator 6 or the light intensity lowering section 9 to make the
resistor produce heat as a heater. Specifically, a forward/reverse
bias is not applied to the phase regulator 6 and the light
intensity lowering section 9 to change the reflectivity, but their
temperatures are varied to change the reflectivity. In this case
also, the same effects of the above-described first to fourth
embodiments can be obtained.
[0045] Obviously many modifications and variations of the present
invention are possible in the light of the above teachings. It is
therefore to be understood that within the scope of the appended
claims the invention may be practiced otherwise than as
specifically described.
[0046] The entire disclosure of Japanese Patent Application No.
2012-030779, filed on Feb. 15, 2012, including specification,
claims, drawings, and summary, on which the Convention priority of
the present application is based, is incorporated herein by
reference in its entirety.
* * * * *