JP4098812B2 - Optical semiconductor device - Google Patents

Description

  The present invention generally relates to an optical semiconductor device, and more particularly to an optical semiconductor device including a temperature control mechanism.

  In a large-capacity optical fiber communication system using optical wavelength multiplexing communication technology, a large number of light sources with stable wavelengths are required. For this reason, in optical wavelength division multiplexing communication, an optical semiconductor module having a wavelength locker such as a temperature control mechanism that can keep the oscillation wavelength constant with respect to temperature change by feedback control is used.

  FIG. 1 shows a configuration of an optical semiconductor module 10 having a conventional wavelength locker.

  Referring to FIG. 1, the optical semiconductor module 10 includes a package body 2, and a semiconductor laser 1 held on a temperature control unit 3 provided on the package body 2 via a carrier member 4, The semiconductor laser is fed through a wire 1C connected to an electrode on the package body 2 to form an output light beam 1A. The formed output light beam 1A is injected through a window 2A on the package body 2 into an optical fiber (not shown) optically coupled thereto.

  Further, the semiconductor laser 1 forms another output light beam 1B in the opposite direction to the output light beam 1A. The output light beam 1B passes through the beam splitter 5 and the wavelength filter 6 and is then transmitted by the first photodiode 7. Detected. Further, the intensity of the output light beam 1B branched by the beam splitter 5 is detected by the second photodiode 8. Further, the carrier member 4 carries a thermistor 4A, and the thermistor 4A measures the temperature of the semiconductor laser 1 and supplies an output signal representing the result to the outside of the package body 2 via a wire 4B.

  In the optical semiconductor module 10, although not shown, a first collimator lens is provided between the semiconductor laser 1 and the window 2A on the optical path of the outgoing light beam 1A, and also on the optical path of the outgoing light beam 1B. A second collimator lens is provided between the semiconductor laser 1 and the beam splitter 5.

  Further, the external control circuit cooperates with the optical semiconductor module 10, and the control circuit allows the intensity of the output light beam 1 B detected by the second photodiode 8 to be constant. To control. That is, the second photodiode 8 is used for APC control. The control circuit further includes the temperature control unit 3 based on the intensity of the output light beam 1B detected by the first photodiode 7 and whose output intensity is controlled to be constant after passing through the wavelength filter 5. Is controlled to compensate for a change in the oscillation wavelength of the semiconductor laser 1.

  FIG. 2 shows an example of the relationship between the oscillation wavelength of the semiconductor laser 1 and the operating temperature.

  Referring to FIG. 2, the oscillation wavelength of the semiconductor laser shifts to the longer wavelength side as the temperature increases mainly due to a change in optical resonator length or a change in refractive index accompanying a change in temperature.

  On the other hand, FIG. 3 shows the wavelength transmission characteristics of the wavelength filter 6. However, the wavelength filter 6 is formed of an optical medium such as glass having parallel opposing surfaces and has an etalon property.

  Referring to FIG. 3, since the wavelength filter 6 has a transmission characteristic that changes sinusoidally with respect to the wavelength, the wavelength filter 6 has an inclined portion of the transmission characteristic at the oscillation wavelength of the output light beam 1B. By designing so as to correspond, it becomes possible to detect the change in the oscillation wavelength with high sensitivity by the photodiode 7.

  Therefore, for example, when the intensity of the output light beam 1B detected by the photodiode 7 is reduced, the semiconductor laser 1 itself is APC controlled using the photodiode 8, and therefore, from the relationship of FIG. It is determined that the operating temperature of the semiconductor laser 1 has increased, and the control circuit controls the temperature control unit 3 to lower the operating temperature of the semiconductor laser 1. That is, in the optical semiconductor module 10 of FIG. 1, a wavelength locker is formed by each component formed on the temperature control unit 3.

  The optical semiconductor module 10 shown in FIG. 1 can detect and compensate for the change in the oscillation wavelength of the semiconductor laser 1 due to the temperature change as described above. However, the environment in which the optical semiconductor module 10 is used is shown in FIG. When the temperature changes, a temperature difference is generated between the semiconductor laser 1 whose temperature is controlled by the temperature control unit 3 and other components on the temperature control unit 3, such as the wavelength filter 6, and as a result, An error may occur in the operation of the wavelength locker described above.

  More specifically, in the optical semiconductor module 10 of FIG. 1, the thermal influence of the environmental temperature is transmitted to the temperature control unit 3 through the package body 2, and thus the temperature control is performed. When the temperature of the semiconductor laser 1 is controlled by the temperature control unit 3 on the carrier 4, the thermal conductivity of the temperature control unit 3 is infinite. Therefore, there may be a temperature difference with the wavelength filter 6.

  FIG. 4 shows the wavelength transmission characteristics of the wavelength filter 6 when the temperature of the filter 6 is 25 ° C. and when it is 75 ° C. In FIG. 4, the solid line indicates the transmittance at 25 ° C., and the broken line indicates the transmittance at 75 ° C.

  Referring to FIG. 4, it can be seen that the transmittance at 75 ° C. is shifted to the longer wavelength side than at 25 ° C. due to thermal expansion and refractive index change of the wavelength filter 6.

  For this reason, in the conventional optical semiconductor module 10 of FIG. 1, the temperature of the semiconductor laser 1 is correctly controlled on the carrier member 4 by the temperature control unit 3, and output light beams 1A and 1B having a predetermined wavelength λ are obtained. Even when the temperature of the wavelength filter 6 is 75 ° C., the output of the photodiode 7 increases, and as a result, it is erroneously determined that the temperature of the semiconductor laser 1 is decreased. . In this case, the temperature control unit 3 is driven to raise the temperature of the semiconductor laser 1, and the actual laser oscillation wavelength is shifted from the desired value of λ to λ ′ on the longer wavelength side.

  Thus, the conventional optical semiconductor module 10 has a problem that the operation of the wavelength locker causes an error when the environmental temperature changes.

  In order to solve this problem, a configuration of an optical semiconductor module that separately controls the temperature of the semiconductor laser 1 and the optical filter has been proposed in Japanese Patent Laid-Open No. 10-79551. However, since the conventional configuration requires two temperature control units, the number of parts is complicated and the power consumption is large.

  Accordingly, it is a general object of the present invention to provide a novel and useful optical semiconductor device and a control method thereof that solve the above-described problems.

  A more specific object of the present invention is to provide a configuration and control capable of performing a highly accurate wavelength locker operation when an environmental temperature changes in an optical semiconductor device having a temperature control unit for forming a wavelength locker. .

The present invention solves the above problems.
The present invention solves the above-described problems by providing a package, a semiconductor laser housed in the package and forming a light beam, a thermal control element connected to the semiconductor laser, and a temperature control element. A temperature control unit that controls the optical control, an optical filter that is thermally connected to the temperature control unit and has a wavelength transmittance characteristic having a predetermined inclination with respect to a wavelength, and a light beam from the semiconductor laser A light receiving unit that receives light through the optical filter and detects the intensity of the light beam that has passed through the optical filter, and a power supply that supplies driving power to the semiconductor laser.
A heat transfer body provided separately from the power supply body and transmitting the temperature of the package to the semiconductor laser, the heat transfer body from the bottom surface of the package where the temperature control unit is provided This is solved by an optical semiconductor device characterized by being connected to the package at a high position.

  According to the present invention, a temperature difference generated between an optical component constituting the wavelength locker and the semiconductor laser in the package due to a change in environmental temperature in which the optical semiconductor device is used causes the package and the semiconductor laser. Is reduced by a simple configuration in which a heat transfer body is provided between them, and as a result, malfunction of the wavelength locker is avoided.

  According to the present invention, in an optical semiconductor module having a wavelength locker, a semiconductor laser housed in the package body and whose oscillation wavelength is locked by the wavelength locker is heated to the package body and further to the external environment via the heat transfer body. By making contact with each other, a stable wavelength locking operation can be ensured even when the components of the wavelength locker, particularly the wavelength filter, are affected by the external environment temperature.

[First embodiment]
5A and 5B are a plan view and a cross-sectional view, respectively, showing the configuration of the optical semiconductor module 20 according to the first embodiment of the present invention. However, in FIGS. 5A and 5B, portions corresponding to the portions described above are denoted by the same reference numerals, and description thereof is omitted.

  5A and 5B, the optical semiconductor module 20 according to the present embodiment has a configuration similar to that of the conventional optical semiconductor module 10 described above, but the carrier 4 is composed of a plurality of wires 9. , Mechanically and thermally coupled to the package body 2. In the illustrated optical semiconductor module 20, a parallel plate beam splitter 5 </ b> A described later is used instead of the beam splitter 5 configured by combining two prisms used in the optical semiconductor module 10.

  In the optical semiconductor module 20, as shown in the sectional view of FIG. 5B, the carrier 4, the beam splitter 5A, the wavelength filter 6 forming the wavelength locker, the photodiode 7 and the photodiode 8 are supported. The temperature control unit 3 is provided in a space 2 </ b> B formed in the package body 2. The temperature control unit 3 includes a Peltier element 3A.

FIG. 5B is a view of the optical semiconductor module 20 as viewed from the direction of the optical window 2A. In FIG. 5B, the beam splitter 5A, the wavelength filter 6, and the photodiodes 7 and 8 are not shown. The temperature control unit 3 has a structure in which the Peltier element 3A is sandwiched between a metal such as Al having excellent thermal conductivity or a ceramic substrate such as Al ₂ O ₃ .

  Further, as shown in FIG. 5A, a control circuit 21 for driving the semiconductor laser 1 is connected to the optical semiconductor module 20 via the wire 1C, and the control circuit 21 is further connected to the thermistor 4A. The temperature of the semiconductor laser 1 is also controlled by driving the Peltier element 3A via the wire 3B based on the output.

  Next, the principle of operation of the optical semiconductor module 20 of this embodiment will be described with reference to FIGS. 6 (A) and 6 (B). However, also in this embodiment, the wavelength filter 6 has the temperature dependence of the wavelength transmittance characteristics shown in FIG. 4, and FIGS. 6A and 6B are a part of the wavelength transmittance characteristics of FIG. It is a figure which expands and shows. As in FIG. 4, the solid line indicates the transmittance characteristic at 25 ° C., and the broken line indicates the transmittance characteristic at 75 ° C.

  Referring to FIG. 6A, when the temperature of the wavelength filter 6 changes from the initial 25 ° C. to 75 ° C. as the environmental temperature increases, the wavelength transmittance characteristic is also indicated by an arrow in the figure. It shifts to the long wavelength side as shown.

  On the other hand, in the optical semiconductor module 20 of the present embodiment, the carrier 4 that carries the semiconductor laser 1 is connected to the package body 2 by a plurality of wires 9, so that heat from the outside travels through the wires 9 and passes through the wires 9. As a result, the temperature of the semiconductor laser 1 rises.

Since the semiconductor laser 1 has the temperature characteristics as described above with reference to FIG. 2, the oscillation wavelength of the semiconductor laser 1 is changed from the initial wavelengths λ ₁ to λ as the temperature rises as shown in FIG. ₂ and further shifted to the longer wavelength side to λ ₃ , and as a result, the intensity of the output light beam 1 B that has passed through the wavelength filter 6 decreases from the initial level L ₁ by ΔL.

Strength reduction ΔL of the output light beam 1B is detected by the photodiode 7, as a result the control circuit 21, so that the output of the photodiode 7 to restore the original level L _1, drives the Peltier element 3A Then, the carrier 4 and the semiconductor laser 1 thereon are cooled. As a result, as shown in FIG. 6B, the oscillation wavelength of the semiconductor laser 1 is shifted from the λ ₃ to the short wavelength side.

By the way, the wavelength filter 6 is also cooled via the temperature control unit 3 by driving the Peltier element 3A in the cooling mode. Accordingly, the wavelength transmittance characteristic of the wavelength filter 6 is also shifted to the short wavelength side as indicated by an arrow in FIG. 6B. As a result, at the wavelength close to the initial wavelength λ ₁ , the predetermined level is reached. L ₁ is recovered. That is, FIG. 6B shows the wavelength locker recovery operation that occurs in the optical semiconductor module 20 according to this embodiment.

  In the wavelength locker recovery operation of FIG. 6B, since heat is supplied to the semiconductor laser 1 from the high temperature operating environment by the heat transfer body during cooling by the Peltier element 3A, the semiconductor laser 1 As a result, only the semiconductor laser 1 is not cooled, and the wavelength locker malfunction as described above with reference to FIG. 4 does not occur.

  As described above, in the optical semiconductor module 20 according to the present embodiment, the temperature of the wavelength filter 6 is increased by thermally coupling the semiconductor laser 1 to the ambient temperature in which the package, that is, the optical semiconductor module 20 is used. In this case, the problem that the wavelength locker malfunctions is solved. In the present embodiment, a plurality of wires are used as the heat transfer body 9, but in this way, the thermoelectricity can be finely controlled by changing the number of wires, and workability is good. For example, if about 10 Au wires having a diameter of 380 μm are used, a desired heat transfer effect can be obtained.

  Although the wire 1C for driving the semiconductor laser 1 also contributes to the heat transfer effect, a single wire alone cannot sufficiently transfer heat from the operating environment to the semiconductor laser 1, and the effect of the present invention is as follows. I can't show it.

FIG. 7 shows the wavelength locker when the temperature of the wavelength filter 6 is changed from a predetermined temperature T ₀ to a higher temperature T ₁ and to a lower temperature T ₂ as in the previous embodiment. It is a figure explaining operation | movement.

The operation of the wavelength locker when the temperature of the wavelength filter 6 rises to T ₁ due to the influence of the environmental temperature is as described above. However, when the temperature drops to T ₂ , The Peltier element 3A is driven in the heating mode, and the original wavelength λ ₁ and the original level L ₁ are restored.

  Incidentally, since the wavelength filter 6 has a sine wave type periodic wavelength transmittance characteristic as described above with reference to FIG. 3 or FIG. 4, excessive heat is supplied from the operating environment via the heat transfer body 9. Then, as shown in FIG. 8, the operating point of the wavelength locker is the region where the wavelength transmittance characteristic is inverted from the region A where the slope of the initial wavelength transmittance characteristic is negative, that is, the slope of the wavelength transmittance characteristic is positive. Therefore, the wavelength locker does not operate correctly. In the region B, contrary to the region A, the control device 21 heats the semiconductor laser 1 when the output of the photodiode 7 decreases, and cools the semiconductor laser 1 when the output increases.

  From this, the heat transfer body 9 has the same polarity as the temperature control direction determined by the wavelength locker control device 21 when the wavelength of the semiconductor laser 1 changes, that is, the polarity of heating or cooling. It is preferable that the ambient temperature of the package body is transmitted to the semiconductor laser 1 within the range shown.

5A and 5B is closed by a lid member (not shown), and the semiconductor laser 1, the carrier 4, the thermistor 4A, the Peltier element 3A, the temperature controller 3, and the beam. The splitter 5A, the wavelength filter 6, the photodiode 7 and the photodiode 8, together with the wires 1C and 4B and the heat transfer body 9, are sealed in a space 2B in the package body 2 in a vacuum or reduced pressure state. . Alternatively, a gas having a smaller thermal conductivity than air, such as N ₂ or Ar, may be enclosed in the space. By doing in this way, since external temperature cannot be easily transmitted to a wavelength filter, the effect of the present invention can be heightened further.

  FIGS. 9A and 9B are a front view and a side view, respectively, showing the configuration of the wavelength filter 6 used in the optical semiconductor module 20 according to this embodiment.

Referring to FIGS. 9A and 9B, the wavelength filter 6 is formed of a multilayer filter 6A and is not shown on the surface, but in order to minimize the influence of the environmental temperature due to radiation from the package body 2. An infrared reflecting film made of SiO ₂ or resin is formed. This also contributes to enhancing the effect of the present invention. The multilayer filter 6A is held on the temperature control unit 3 by a heat transfer holder 6B made of a metal such as Al having a high thermal conductivity. Therefore, the degree of heat transfer by cooling or heating through the temperature control unit 3 by the Peltier element 3A is increased, and the control of the temperature of the Peltier element is stronger than the external temperature, so that it is not easily affected by the external temperature, It can contribute to enhancing the effect of the present invention. The heat conductive holder 6B is also preferably formed with an infrared reflecting film.

  FIG. 10 shows a configuration of a beam splitter 5A used in the optical semiconductor module 20 of the present embodiment.

Referring to FIG. 10, the beam splitter 5A is composed of a parallel flat glass plate 5A ₀ , and the glass plate 5A ₀ carries a reflection film 5B on the incident surface and a transmission film 5C on the emission surface, and serves as a half mirror. Works.

[Second Embodiment]
FIGS. 11A and 11B show the configuration of the optical semiconductor module 30 according to the second embodiment of the present invention. However, in FIGS. 11A and 11B, the same reference numerals are given to the portions described above, and description thereof is omitted.

  11A and 11B, in this embodiment, a ground electrode pattern 4C connected to the semiconductor laser 1 is formed on a part of the carrier 4, and the semiconductor is formed on the ground electrode pattern 4C. Laser 1 is formed. Furthermore, instead of the heat transfer body 9 made of Au wire used in the previous embodiment, a plate material made of a metal having a high thermal conductivity such as Al or Au is used as the heat transfer body 9A.

  In the present embodiment, a heat conductive metal plate material used as the heat transfer body 9A in combination with the ground electrode pattern 4C can efficiently transfer heat from the package body 2 in the operating environment to the semiconductor laser 1. A desired high-precision wavelength locker operation can be obtained.

In this embodiment, as the heat transfer body 9A, a metal thin film having a high thermal conductivity, such as an Au ribbon or an Al ribbon, or a material coated with a metal thin film on a substrate can be used.

[Third embodiment]
12A shows the configuration of the optical semiconductor module 40 according to the third embodiment of the present invention, and FIG. 12B shows the configuration of the beam splitter 5G used in the optical semiconductor module 40 of FIG. 12A. . However, the parts described above are denoted by the same reference numerals, and description thereof is omitted.

  Referring to FIG. 12A, the optical semiconductor module 40 has a configuration similar to that of the previous optical semiconductor module 20, but the beam splitter 5A used in the optical semiconductor module 20 is similar to that shown in FIG. Is replaced by a beam splitter 5G which shows details. FIG. 12A shows a collimator lens 1a disposed in the optical path of the outgoing light beam 1A, and a collimator lens 1b disposed in the optical path of the outgoing light beam 1B. The collimator lens is actually provided also in the optical semiconductor module 20.

Figure 12 Referring to (B), of the beam splitter 5G is wedge-shaped in the present embodiment, i.e. made of a glass plate 5G ₀ main surface are not parallel to each other facing, on the plane of incidence on the glass plate 5G ₀ In addition, a reflective film 5H is formed, and a transmissive film 5I is formed on the exit surface.

  In the beam splitter 5G of FIG. 12B, since both main surfaces of the glass plate 5G constituting the entrance surface and the reflection surface are not parallel, incident light is between the entrance surface and the exit surface in the glass plate 5G. As a result, the overlapping space due to multiple reflection is reduced, and a substantially constant transmittance with respect to the wavelength is guaranteed.

In the previous embodiment, since the beam splitter uses the parallel flat glass plate 5A ₀ , the multiple reflection of the light beam generated inside the beam splitter causes interference and has an etalon property similar to a wavelength filter. This means that the light intensity incident on the wavelength filter fluctuates depending on the wavelength of the light beam, and its characteristics are also easily affected by temperature. Obstructs wavelength lock operation.

  As described above, the beam splitter of the present embodiment can be said to be a suitable beam splitter for the wavelength locker because multiple reflections are suppressed and the properties of the etalon are suppressed and a certain transmittance can be secured. The effect can be exhibited even when the non-parallelism of the beam splitter of the present embodiment is about 0.2 to 10 degrees.

  As long as the beam splitter of the present embodiment detects a wavelength and performs feedback as a wavelength lock mechanism, the beam splitter other than the one using a wavelength-intensity conversion mechanism using a wavelength filter as in the embodiment, and wavelength control A method other than that using temperature control can also be adopted.

  The non-parallel beam splitter itself is known from Japanese Patent Laid-Open No. 5-136513. However, this means that if the laser wavelength fluctuates due to temperature or the like, the light intensity incident on the APC PD changes even if the laser intensity is constant, and it is erroneously detected that the laser output has changed. This is to prevent it. On the other hand, this embodiment is a technology related to the wavelength locker, and since the mechanism for fixing the wavelength is mounted, the problem described in the known example, that is, “the variation of the wavelength of the laser” itself does not occur. For this reason, there is no positive reason to adopt a wedge-type beam splitter for the wavelength locker.

  Although the present invention has been described with reference to the preferred embodiments, the present invention is not limited to such specific embodiments, and various modifications and changes can be made within the scope described in the claims.

  According to the present invention, in an optical semiconductor module having a wavelength locker, a semiconductor laser housed in the package body and whose oscillation wavelength is locked by the wavelength locker is heated to the package body and further to the external environment via the heat transfer body. By making contact with each other, a stable wavelength locking operation can be ensured even when the components of the wavelength locker, particularly the wavelength filter, are affected by the external environment temperature.

It is a figure which shows the structure of the conventional optical semiconductor module with a built-in wavelength locker. It is a figure which shows the temperature characteristic of a semiconductor laser. It is a figure explaining operation | movement of a wavelength locker. It is a figure which shows the transmittance | permeability temperature dependence of a wavelength filter. (A), (B) is a figure which shows the structure of the optical semiconductor module by 1st Example of this invention. (A), (B) is a figure explaining operation | movement of the optical semiconductor module of FIG. It is another figure explaining operation | movement of the optical semiconductor module of FIG. FIG. 6 is a diagram showing a wavelength lock operation region in the optical semiconductor module of FIG. 5. (A), (B) is a figure which shows the structure of the wavelength filter in the optical semiconductor module of FIG. It is a figure which shows the structure of the beam splitter in the optical semiconductor module of FIG. (A), (B) is a figure which shows the structure of the optical-semiconductor module by 2nd Example of this invention. (A), (B) is a figure which shows the structure of the optical semiconductor module by 3rd Example of this invention.

Explanation of symbols

DESCRIPTION OF SYMBOLS 10, 20, 30, 40 Optical semiconductor module 1 Semiconductor laser 1A, 1B Optical beam 1C Feeding wire 1a, 1b Lens 2 Package main body 2A Optical window 2B Space 3 Temperature control part 3A Peltier element 3B Peltier element drive wire 4 Carrier 4A Thermistor 4B Wire 5, 5A Beam splitter 5A ₀ , 5G ₀ Glass plate 5B, 5H Reflective film 5C, 5I Transmission film 6 Wavelength filter 6A Multilayer film 6B Holder 7, 8 Photodiode 9 Heat transfer element 21 Control circuit

Claims (13)

Package,
A semiconductor laser housed in the package and forming a light beam;
A temperature control unit that is thermally connected to the semiconductor laser, includes a temperature control element, and controls the semiconductor laser to a predetermined temperature;
An optical filter thermally connected to the temperature control unit and having a wavelength transmittance characteristic having a predetermined inclination with respect to the wavelength;
A light receiving unit that receives a light beam from the semiconductor laser through the optical filter and detects an intensity of the light beam transmitted through the optical filter;
A feeder for supplying driving power to the semiconductor laser;
A heat transfer body provided separately from the power supply body and transmitting the temperature of the package to the semiconductor laser;
The optical semiconductor device, wherein the heat transfer body is connected to the package at a position higher than a bottom surface of the package where the temperature control unit is provided.   The optical semiconductor device according to claim 1, wherein the wavelength filter has a wavelength transmittance characteristic that varies in a wavelength direction depending on a temperature of the wavelength filter.   2. The optical semiconductor device according to claim 1, wherein the temperature control unit controls the temperature of the light receiving unit so that the light receiving unit has a predetermined light beam intensity.   2. The optical semiconductor device according to claim 1, wherein the heat transfer body is made of a metal wire, a metal foil, a metal plate, or a member carrying a metal film.   The optical semiconductor device according to claim 1, wherein the semiconductor laser is provided on a carrier member, and the heat transfer body is thermally connected to the semiconductor laser through the carrier member.   The carrier member carries a ground electrode, the semiconductor laser is provided on the ground electrode, and the heat transfer body is thermally connected to the semiconductor laser through the ground electrode. Item 6. The optical semiconductor device according to Item 5.   The optical semiconductor device according to claim 1, wherein the wavelength filter is held in a thermally conductive holder, and the thermally conductive holder is thermally connected to the temperature control unit.   2. The optical semiconductor device according to claim 1, wherein the inside of the package is sealed with reduced pressure, vacuum, or a gas whose thermal conductivity is lower than that of air.   A beam splitter for branching a light beam is provided between the semiconductor laser and the light receiving unit, and the beam splitter is made of an optical medium defined by first and second main surfaces that are non-parallel to each other. 2. The optical semiconductor device according to claim 1, wherein the light beam is incident on or emitted from the first or second main surface.   The beam splitter is provided in an optical path between the semiconductor laser and the wavelength filter, and the light beam branched by the beam splitter measures the intensity of the light beam and outputs the output of the semiconductor laser. The optical semiconductor device according to claim 9, wherein the optical semiconductor device is incident on another light receiving unit for control.   Furthermore, a wavelength detection unit for detecting the wavelength of the light beam is provided, and opposing surfaces are defined between the semiconductor laser and the wavelength detection unit by first and second main surfaces that are not parallel to each other. The beam splitter which consists of another optical medium is provided, The said light beam injects or radiate | emits with respect to the said 1st or 2nd main surface, The Claim 1 characterized by the above-mentioned. Optical semiconductor device.   The wavelength detection unit includes a wavelength filter and a light intensity detection unit. After the wavelength-intensity conversion of the light beam by the wavelength filter, the wavelength detection is performed by detecting the intensity by the light intensity detection unit. The optical semiconductor device according to claim 11, wherein the optical semiconductor device is performed.   The optical semiconductor device further includes an output light intensity control unit that controls the output light intensity of the semiconductor laser, and the beam splitter branches the light beam into the wavelength detection unit and the output light intensity control unit. 13. The optical semiconductor device according to claim 12, wherein the optical semiconductor device is a device.

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