JP2010219568A - Semiconductor optical element device - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide a semiconductor optical element device improving the degree of freedom of design of a nonreflective film even when a total film thickness of a plurality of films is a value different from λ/4. <P>SOLUTION: The nonreflective film is formed with a plurality of films each having a refractive index higher than 1 and formed using high-reflectivity films (a first film 7, a third film 9, a fifth film 11) each having a refractive index higher than a square-root value of an effective refractive index of a semiconductor optical element, and low-refractive index films (a second film 8, a fourth film 10, a sixth film 12, a seventh film 13) each having a refractive index lower than a square-root value of an effective refractive index of a semiconductor laser 31. The plurality of films are formed to have at least three compositions while each film is formed with a single composition, and to set both a real part and an imaginary part of an amplitude reflectance to zero as a whole. <P>COPYRIGHT: (C)2010,JPO&INPIT

Description

  The present invention relates to a semiconductor optical device including a semiconductor optical device that emits light, and a semiconductor laser module using the semiconductor optical device.

First, the configuration of a conventional semiconductor optical device disclosed in Japanese Patent Application Laid-Open No. 2001-196685 will be described with reference to FIG. Conventional semiconductor optical device apparatus, as shown in FIG. 19, a nonreflective film exemplary effective refractive index of the semiconductor optical element is provided in contact with the exit surface of the light of the semiconductor laser 101 and the semiconductor laser 101 of n _c It has.

The non-reflective film is provided in contact with the end face of the semiconductor laser 101 and is provided in contact with the end face of the first film 102 and the first film 102 having a refractive index of n ₁ and a film thickness of d _1. A second film 103 having a refractive index of n ₂ and a film thickness of d ₂ , and an end face of the second film 103, having a refractive index of n ₃ and a film thickness of d 2. ₃ is a third film 104.

Japanese Patent Laid-Open No. 2001-196685

FIG. 20 shows the wavelength dependency data of the reflectance of the non-reflective film used in the semiconductor laser having an effective refractive index of n _c = 3.2. The data shown in FIG. 20 is data on the wavelength dependence of the reflectance of the non-reflective film when the semiconductor laser emits light having a wavelength λ = 1.3 μm.

Data 105 in FIG. 20 indicates that the refractive index is n ₁ = 1.6 and the film thickness is d ₁ = 106.2 nm, the refractive index is n ₂ = 3.2 and the film thickness is d ₂ = 10.6 nm. This is data showing the wavelength dependence of the reflectance of an antireflective film composed of amorphous silicon and quartz having a refractive index n ₃ = 1.45 and a film thickness d ₃ = 73.9 nm.

Further, data 106 in FIG. 20 indicates that the refractive index n ₁ = 1.6 and the film thickness d ₁ = 512.5 nm of alumina, the refractive index n ₂ = 3.2 and the film thickness d ₂ = 10.6 nm. The data shows the wavelength dependence of the reflectance of an antireflective film made of amorphous silicon and quartz having a refractive index n ₃ = 1.45 and a film thickness d ₃ = 73.9 nm.

When the effective refractive index n _c of the semiconductor laser 101 is 3.2, the square root refractive index is n _f = 1.78885. For light with a wavelength λ = 1.3 μm, ¼ of the wavelength λ is 325 nm.

When the total film thickness (d ₁ × n ₁ + d ₂ × n ₂ + d ₃ × n ₃ ) of the above three types of films is substantially equal to ¼ of λ, as shown in the data 105 indicating the wavelength dependence. In addition, the wavelength range in which the antireflective film functions with a low reflectance of 1% or less is 257 nm.

On the other hand, when the total film thickness (d ₁ × n ₁ + d ₂ × n ₂ + d ₃ × n ₃ ) of the three types of films is set to about 961 nm in order to increase the thermal conductivity of the non-reflective film, data showing wavelength dependence. As shown at 106, the wavelength range in which the antireflective film functions with a low reflectance of 1% or less is 78 nm.

  In the conventional semiconductor optical device, the above-described three types of films are used as the non-reflective film of the semiconductor laser as an example of the semiconductor optical device. However, when the total film thickness of these three types of films (the sum of the film thickness and the refractive index for each layer) is set to a value that is an integral multiple of λ / 4 other than λ / 4, the non-reflective film is 1%. The range of wavelengths that function at the following low reflectivity is extremely narrow. More specifically, there is a problem that it is difficult to set the wavelength range in which the antireflective film functions at a low reflectance of 1% or less to 100 nm or more. Therefore, in the conventional semiconductor optical device disclosed in Japanese Patent Laid-Open No. 2001-196685, the total film thickness cannot be different from λ / 4.

  Therefore, as means for solving the problems that occur in the conventional semiconductor optical device disclosed in the above-mentioned Japanese Patent Application Laid-Open No. 2001-196585, the inventors of the present application have disclosed a composition as a technique undisclosed at the time of filing the present application. We are investigating the formation of an antireflective film by a design method in which the real part and the imaginary part of the amplitude reflectivity of two different types of films are set to zero. According to this design method, the total film thickness of two types of films having different compositions can be set to a value different from λ / 4.

  However, in this design method, since there are only two types of films constituting the non-reflective film, the degree of freedom in designing the non-reflective film of the semiconductor optical device cannot be improved. In this design method, for example, in addition to the two types of films in which the real part and the imaginary part of the amplitude reflectance are each zero, it is possible to efficiently radiate the heat of the semiconductor laser as a third type film. A film cannot be provided.

  The present invention has been made in view of the above problems, and its purpose is to improve the degree of freedom in designing an anti-reflective film even when the total film thickness of a plurality of films is different from λ / 4. It is an object of the present invention to provide a semiconductor optical device that can be used and a semiconductor laser module using the same.

  The semiconductor optical device according to the present invention includes a semiconductor optical device, an outgoing light emitted from the semiconductor optical device, and an incident light and a reflected light obtained by reflecting the incident light with respect to light having a specific wavelength. A non-reflective film that interferes and makes the reflectance of light substantially zero.

  The non-reflective film is a plurality of films each having a refractive index greater than 1, and a high refractive index film having a refractive index higher than the square root of the effective refractive index of the semiconductor optical device; And a plurality of films formed by using a low refractive index film having a refractive index lower than the value of the square root of the effective refractive index of the semiconductor optical device.

  In addition, each of the plurality of films has a single composition, the number of composition types of the plurality of films is three or more, and the real part and the imaginary part of the amplitude reflectivity are both zero as a whole. It is comprised so that.

  According to said structure, only two types of film | membranes with which only the refractive index is known and the film thickness is unknown among the several films | membranes with which the kind of composition of the film | membrane was 3 or more, and film thickness and refractive index A design that determines the film thickness of each of the two specific types of films described above so that both the real part and the imaginary part of the overall amplitude reflectance of the plurality of films are both zero using known films. Techniques can be used.

  According to this design technique, the inventors of the present application who design the non-reflective film to be composed of two kinds of films and that the real part and the imaginary part of the amplitude reflectivity of the two kinds of films are both zero. The degree of freedom in designing the antireflective film is improved as compared with the methods that have been studied previously.

  The plurality of films preferably have a total sum of products of film thickness and refractive index larger than a quarter wavelength of light emitted from the semiconductor optical device.

  As described above, when the total sum of the product of the film thickness and the refractive index of each of the plurality of films is larger than ¼ wavelength of the light emitted from the semiconductor optical device, the above-described non-reflective film design method is used. The wavelength range in which the antireflective film functions at a low reflectance of 1% or less can be easily made wider than that of the conventional antireflective film.

  Moreover, it is desirable that the adjacent film provided so as to be adjacent to the semiconductor optical element among the plurality of films has a higher thermal conductivity than the other films. As the adjacent film, aluminum nitride is suitable.

  According to said structure, the semiconductor optical element apparatus implement | achieved which discharge | releases the heat | fever of a semiconductor optical element efficiently can be designed easily using the said design method.

  Further, the first layer film, which is an adjacent film provided so as to be adjacent to the semiconductor optical element among the plurality of films, is made of a material having a refractive index smaller than the value of the square root of the effective refractive index of the semiconductor optical element. Is desirable.

  Furthermore, each of the first layer film and the second layer film provided so as to be adjacent to the first layer film is a material having a refractive index smaller than the value of the square root of the effective refractive index of the semiconductor optical element. It is desirable to comprise.

  According to said structure, absorption of the light in each of 1st layer film and 2nd layer film and absorption of light in the interface of a 1st layer film and a 2nd layer film can be suppressed. Therefore, it is possible to easily design a semiconductor optical device that is unlikely to deteriorate due to light absorption between the first layer film and the second layer film by using the above design method.

Further, the wavelength range in which the non-reflective film functions at a low reflectance of 1% or less is 100 nm or more.
According to said structure, it can adapt flexibly to the change of the wavelength of the light which the semiconductor optical element in a normal state radiate | emits.

  Further, the semiconductor optical element described above may be any of a semiconductor laser, a semiconductor amplifier, a superluminescent diode, and a semiconductor optical modulator.

  The semiconductor laser module of the present invention is a semiconductor laser module using a semiconductor optical device in which the semiconductor optical device is a semiconductor laser. The semiconductor laser module includes a first reflective film having a higher reflectance than a non-reflective film provided outside the semiconductor element device, and a side different from an end surface on which the non-reflective film of the semiconductor element device is provided. And a second reflective film having a reflectance higher than that of the non-reflective film with respect to light having a predetermined wavelength.

  Moreover, the light of the specific wavelength reflected by each of the first reflective film and the second reflective film passes through the non-reflective film. Thereby, light oscillates between the first reflective film and the second reflective film.

  According to the above configuration, the gain of the semiconductor laser itself and the non-reflective film can be obtained by using the non-reflective film whose wavelength range that functions at a low reflectance of 1% or less is wider than that of the conventional non-reflective film. Oscillation determined by the reflectance can be suppressed.

  In the semiconductor laser module of the present invention, it is preferable that the first reflective film is a fiber grating or a filter provided in the optical fiber.

  According to the present invention, even when the total film thickness of a plurality of films has a value different from λ / 4, the degree of freedom in designing an antireflective film can be improved.

It is a figure for demonstrating the non-reflective film of the 2 layer structure from which a reflectance becomes zero at the wavelength (lambda) regarding this invention. It is a figure for demonstrating the non-reflective film of the 4 layer structure from which the reflectance becomes zero at the wavelength (lambda) regarding this invention. 4 is a diagram for explaining a non-reflective film of the semiconductor laser according to the first embodiment. FIG. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of Embodiment 1. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the other example of Embodiment 1. FIG. FIG. 6 is a diagram for explaining a non-reflective film of the semiconductor laser according to the second embodiment. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of Embodiment 2. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the other example of Embodiment 2. FIG. FIG. 10 is a diagram for explaining a non-reflective film of the semiconductor laser according to the third embodiment. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of Embodiment 3. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the other example of Embodiment 3. FIG. FIG. 10 is a diagram for explaining a non-reflective film of a semiconductor laser of still another example of the third embodiment. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the further another example of Embodiment 3. FIG. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of another semiconductor laser of Embodiment 3. FIG. It is a figure which shows the semiconductor laser module provided with the semiconductor laser which has the non-reflective film of Embodiment 4, and a fiber grating. FIG. 10 is a diagram showing the relationship between the gain and loss of a semiconductor laser in the semiconductor laser module of the fourth embodiment. In the semiconductor laser module of the fourth embodiment, when a non-reflective film having a narrow wavelength range that functions at a low reflectance of 1% or less is used, the semiconductor laser when the gain distribution moves to the smaller wavelength side It is the figure which showed the relationship between the gain and loss. In the semiconductor laser module of Embodiment 4, it is the figure which showed the relationship between the gain and loss of a semiconductor laser when the range of the wavelength which a non-reflective film functions with the low reflectance of 1% or less is wide. It is a figure for demonstrating the non-reflective film of the conventional semiconductor optical element. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the conventional semiconductor optical element. FIG. 10 is a diagram for explaining a non-reflective film of the semiconductor laser according to the fifth embodiment. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the 1st example of Embodiment 5. FIG. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the 2nd example of Embodiment 5. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the 3rd example of Embodiment 5. FIG. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the 4th example of Embodiment 5. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the 5th example of Embodiment 5. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the 6th example of Embodiment 5. It is a figure for demonstrating the non-reflective film of the semiconductor laser of Embodiment 6. FIG. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the 1st example of Embodiment 6. FIG. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the 2nd example of Embodiment 6. FIG. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the 3rd example of Embodiment 6. FIG. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the 4th example of Embodiment 6. FIG. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the 5th example of Embodiment 6. FIG. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the 6th example of Embodiment 6. FIG. 10 is a diagram for explaining a non-reflective film of a semiconductor laser according to a seventh embodiment. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the 1st example of Embodiment 7. FIG. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the 2nd example of Embodiment 7. FIG. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the 3rd example of Embodiment 7. FIG. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the 4th example of Embodiment 7. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the 5th example of Embodiment 7. FIG. It is a figure which shows the wavelength dependence of the reflectance of the non-reflective film of the semiconductor laser of the 6th example of Embodiment 7. FIG.

A semiconductor optical device according to an embodiment of the present invention will be described below with reference to the drawings.
Embodiment 1.
Hereinafter, the “two-layered non-reflective film that becomes non-reflective at a specific wavelength λ” which is the basis of the semiconductor optical device according to the present embodiment will be described.

Antireflection coating having a two-layer structure as shown in FIG. 1, the first film 1 and a refractive index of n ₂ and thickness refractive index is and thickness a n ₁ is d ₁ is d ₂ a 2-layer structure film consisting of two films 2 which, and the semiconductor laser 31 effective refractive index of n _c is the refractive index is provided in the space 32, such as air or nitrogen is 1.

When the wavelength of light is λ and the phases of the first film 1 and the second film 2 that are unknown are φ ₁ and φ ₂ , the following equations (1a) and (1b) are established.

  At this time, the amplitude reflectance r is expressed by the following equation (2).

When the real part and the imaginary part of the amplitude reflectance r become zero, the unknown film thickness d ₁ and film thickness d ₂ of the first film 1 and the second film 2 are calculated. In other words, a film having a two-layer structure having the calculated film thicknesses d ₁ and d ₂ of the first film 1 and the second film 2 is a non-reflective film having zero amplitude reflectance. .

The power reflectivity R is represented by | r | ² . At this time, the power reflectance R is zero when the following expressions (3a) and (3b) are satisfied.

For example, the effective refractive index n _c of the semiconductor laser 31 is n _c = 3.37, the first film 1 is Ta ₂ O ₅ (n ₂ = 2.057), and the second film 2 is Al ₂ O ₃ ( n ₁ = 1.62), and when the light wavelength is 980 nm, when the film thickness d ₁ of the _first film ₁ and the film thickness d ₂ of the second film are 71.34 nm and 86.20 nm, respectively, A film having a two-layer structure including the first film 1 and the second film 2 has zero real part and imaginary part of amplitude reflectance.

Next, a non-reflective film having a four-layer structure in which two-layer non-reflective films composed of the first film 1 and the second film 2 described above are further stacked will be described. As shown in FIG. 2, a semiconductor laser 31 effective refractive index of n _c, and a non-reflection film of the four-layer structure, the refractive index is provided in the space 32, such as air or nitrogen is 1.

The non-reflective film having a four-layer structure includes a first film 3 having a refractive index of n ₁ and a film thickness of Ad ₁ , and a second film 4 having a refractive index of n ₂ and a film thickness of Ad _2. The third film 5 has a refractive index of n ₁ and a film thickness of Bd ₁ , and the fourth film 6 has a refractive index of n ₂ and a film thickness of Bd ₂ .

The aforementioned A and B are predetermined parameters. When the real part and the imaginary part of the amplitude reflectance of the four-layer structure non-reflective film are zero, the calculation method of the film thickness of each film of the four-layer structure non-reflective film includes the above two-layer structure. It is possible to use the same method as in the case of the non-reflective film. That is, using the following equations (3c) and (3d), the film thickness d ₁ and the film thickness d ₂ when the real part and the imaginary part of the amplitude reflectance r are each zero are calculated.

For example, it is assumed that the effective refractive index n _c of the semiconductor laser is n _c = 3.37. Further, it is assumed that the first film 3 and the third film 5 are composed of Al ₂ O ₃ (n ₁ = 1.62), respectively. The second film 4 and the fourth film 6 are each composed of Ta ₂ O ₅ (n ₂ = 2.057).

The wavelength of light is assumed to be 980 nm. Further, for example, assume that the parameters are A = 1.2 and B = 0.8. The first film and the thickness d ₂ of the third film having a thickness d ₁ and the second film and the fourth film, when 36.20nm and 27.17nm each of which is unknown, a four-layer structure free The reflection film has an amplitude reflectance r of zero.

Further, a non-reflective film in which another material having a refractive index n ₃ and a film thickness d ₃ is further added to the two-layer structure will be described. In the design of this non-reflective film, the value of the film thickness d ₃ of another film is given in advance. In other words, in the design of this non-reflective film, the phase φ ₃ of other materials represented by the following expressions (4) and (5) is handled as known.

Further, the phase φ ₁ and the phase φ ₂ of the first film and the second film, respectively, are unknown numbers. Even in a non-reflective film in which another material is added to the two-layer structure, a technique similar to the above-described method of designing a non-reflective film having a two-layer structure, that is, the real part and the imaginary part of the amplitude reflectance r are each zero. By using this method, the film thickness d ₁ and the film thickness d ₂ are calculated.

  Thereby, one specific type of other film having a known refractive index and a known film thickness is added to two particular types of films having a known refractive index and an unknown film thickness, and having a specific wavelength. The film thicknesses of the two specific types of films constituting the non-reflective film in which the amplitude reflectance r is almost zero with respect to λ are determined.

In the design method of the five-layer structure non-reflective film, the formula (6) is used. Even when this equation (6) is used, the film thickness d ₁ and the film thickness d ₂ are calculated so that the real part and the imaginary part of the amplitude reflectivity r shown in the expression (3c) are each zero. .

  Thereby, a specific one kind of film having a known refractive index and a known film thickness is added to a four-layer structure in which two specific kinds of films having a known refractive index and unknown film thickness are stacked in two stages. Is added, and the film thicknesses of the two specific types of films constituting the non-reflective film in which the amplitude reflectance becomes substantially zero with respect to the specific wavelength λ are determined.

Further, in the design method of the non-reflective film having the seven-layer structure, Expression (7) is used. Even when this equation (7) is used, the film thickness d ₁ and the film thickness d ₂ are calculated so that the real part and the imaginary part of the amplitude reflectivity r shown in the expression (3c) become zero, respectively. .

  Thus, a specific one kind of film having a known refractive index and a known film thickness is added to a six-layer structure in which two specific kinds of films having a known refractive index and an unknown film thickness are stacked in three stages. Is added, and the film thicknesses of the two specific types of films constituting the non-reflective film in which the amplitude reflectance becomes substantially zero with respect to the specific wavelength λ are determined.

Hereinafter, a semiconductor optical device having a non-reflective film having a seven-layer structure according to this embodiment will be described.
As shown in FIG. 3, in the semiconductor optical device having a seven-layer structure according to the present embodiment, the semiconductor laser 31 and three specific types of films having a known refractive index and an unknown film thickness are stacked in three stages. A non-reflective film in which a specific type of film having a known refractive index and a known film thickness is added to the six-layer structure is provided in a space 32 such as air or nitrogen having a refractive index of 1. It is configured to be.

The non-reflective film includes a tantalum oxide (Ta ₂ O ₅ ) first film 7 (refractive index n ₁ = 2.057, film thickness = Ad ₁ ), and alumina (Al ₂ O ₃ ) second film 8 ( Refractive index n ₂ = 1.62, film thickness = Ad ₂ ), tantalum oxide (Ta ₂ O ₅ ) third film 9 (refractive index n ₁ = 2.057, film thickness = Bd ₁ ), alumina (Al ₂ O ₃ ) fourth film 10 (refractive index n ₂ = 1.62, film thickness = Bd ₂ ), tantalum oxide (Ta ₂ O ₅ ) fifth film 11 (refractive index n ₁ = 2.057) , Film thickness = Cd ₁ ), and six-layer structure of alumina (Al ₂ O ₃ ) sixth film 12 (refractive index n ₂ = 1.62, film thickness = Cd ₂ ) and quartz (SiO ₂ ). The seventh film 13 (refractive index n ₃ = 1.45 and film thickness d ₃ = 50 nm). In addition, the algebra A, B, and C in the formula which shows a film thickness are the predetermined parameters mentioned above.

According to the above-described non-reflective film having a seven-layer structure, A = 2.85, B = 2.0, and C = 2.0, and the phase φ ₁ and the phase φ _{2 of} tantalum oxide and alumina are 0.485352 and When 0.872841, at the wavelength λ = 980 nm, the real part and the imaginary part of the amplitude reflectance r of the non-reflective film can be made zero.

At this time, the thickness of each layer is as follows: first film / second film / third film / fourth film / fifth film / sixth film / seventh film = Ad ₁ / Ad ₂ / Bd ₁ / Bd ₂ / Cd ₁ / Cd ₂ / d ₃ = 104.89 nm / 239.50 nm / 73.60 nm / 168.07 nm / 73.60 nm / 168.07 nm / 50 nm.

  Therefore, the total film thickness, which is the sum of the product of the film thickness of each layer and the refractive index, is 1532.59 nm. This value is about 6.2 times the film thickness of 245 nm, which is ¼ of the light wavelength λ. Therefore, the total film thickness is very thick as compared with the prior art.

  At this time, the wavelength dependence of the reflectance of the non-reflective film is close to a bathtub shape as shown in FIG. The wavelength range in which the antireflective film functions with a low reflectance of 1% or less is 177 nm. Therefore, the wavelength range in which the antireflective film of the present embodiment functions with a low reflectance of 1% or less is compared with the wavelength range in which the conventional antireflective film functions with a low reflectance of 1% or less, It is very wide.

  As will be described later, when a semiconductor laser and a fiber grating are combined, it is desirable to set the desired wavelength λ (for example, 980 nm) at the center of the bathtub-shaped reflectance distribution.

In this case, the antireflection film may be designed so that the phase φ ₁ and the phase φ ₂ of tantalum oxide and alumina are 0.488994 and 0.859283, respectively, and the reflectance is zero at the wavelength λ = 940 nm.

At this time, the thickness of each film is as follows: first film / second film / third film / fourth film / fifth film / sixth film / seventh film = Ad ₁ / Ad ₂ / a _{Bd 1 / Bd 2 / Cd 1} / Cd 2 / d 3 = 101.36nm / 226.16nm / 71.13nm / 158.71nm / 71.13nm / 158.71nm / 50nm.

  FIG. 5 shows the wavelength dependence of the reflectance of the non-reflective film in which the desired wavelength λ (for example, 980 nm) is the center of the bathtub-shaped reflectance distribution. The wavelength range in which the antireflective film functions at a low reflectance of 1% or less is 166 nm. Therefore, the wavelength range in which this non-reflective film functions at a low reflectance of 1% or less is much wider than the wavelength range in which the conventional non-reflective film functions at a low reflectance of 1% or less. ing.

Embodiment 2.
Next, the semiconductor optical device according to the second embodiment will be described with reference to FIGS.

  The semiconductor optical device according to the present embodiment has a known refractive index in a six-layer structure in which a semiconductor laser 31 and two specific types of films whose refractive index is known and whose film thickness is unknown are stacked in three stages. A non-reflective film to which a specific kind of film having a known film thickness is added is provided in a space 32 such as air or nitrogen having a refractive index of 1.

As shown in FIG. 6, the non-reflective film includes a first film 14 (refractive index n ₁ = 2.057, film thickness = Ad ₁ ) of tantalum oxide (Ta ₂ O ₅ ), alumina (Al ₂ O). ₃ ) second film 15 (refractive index n ₂ = 1.62, film thickness = Ad ₂ ), tantalum oxide (Ta ₂ O ₅ ) third film 16 (refractive index n ₁ = 2.057, film) Thickness = Bd ₁ ), alumina (Al ₂ O ₃ ) fourth film 17 (refractive index n ₂ = 1.62, film thickness = Bd ₂ ), tantalum oxide (Ta ₂ O ₅ ) fifth film 18 (Refractive index n ₁ = 2.057, film thickness = Cd ₁ ), alumina (Al ₂ O ₃ ) sixth film 19 (refractive index n ₂ = 1.62, film thickness = Cd ₂ ), and nitriding A seventh film 20 (refractive index n ₃ = 2.072, film thickness d ₃ = 50 nm) of aluminum (AlN) is provided. The algebra A, B, and C in the formula indicating the film thickness are predetermined parameters.

According to the above configuration, when A = 2.7, B = 3.0, and C = 2.0, and the phase φ ₁ and phase φ _{2 of} tantalum oxide and alumina are 0.671597 and 0.482534, respectively. At the wavelength λ = 980 nm, the real part and the imaginary part of the amplitude reflectance of the non-reflective film can be made zero.

At this time, the thickness of each layer is as follows: first film / second film / third film / fourth film / fifth film / sixth film / seventh film = Ad ₁ / Ad ₂ / a _{Bd 1 / Bd 2 / Cd 1} / Cd 2 / d 3 = 137.49nm / 125.44nm / 152.77nm / 139.37nm / 101.85nm / 92.92nm / 50nm. Therefore, the total film thickness is 1489.7 nm. This value is about 6.1 times the value 245 nm corresponding to λ / 4. The film thickness is much thicker than that of a conventional semiconductor optical device.

  At this time, the wavelength dependence of the reflectance of the non-reflective film is close to a bathtub shape as shown in FIG. The wavelength range in which the antireflective film functions with a low reflectance of 1% or less is 145 nm. Therefore, the wavelength range in which the antireflective film of the present embodiment functions with a low reflectance of 1% or less is compared with the wavelength range in which the conventional antireflective film functions with a low reflectance of 1% or less, It is very wide.

When the desired wavelength λ = 980 nm is set to the center of the bathtub-shaped reflectance distribution, the phase φ ₁ and the phase φ ₂ of tantalum oxide and alumina are set to 0.685788 and 0.470145, respectively, and the wavelength λ is 938 nm. What is necessary is just to design an anti-reflective film so that a reflectance may be set to zero.

At this time, the thickness of each film is as follows: first film / second film / third film / fourth film / fifth film / sixth film / seventh film = Ad ₁ / _{Ad 2 / Bd 1 / Bd 2} / Cd 1 / Cd 2 / d 3 = 134.38nm / 116.98nm / 149.31nm / 129.88nm / a 99.54nm / 86.65 / 50nm.

  FIG. 8 shows the wavelength dependence of the reflectance of the non-reflective film. The wavelength range in which this antireflective film functions with a low reflectance of 1% or less is 141 nm. Therefore, the wavelength range in which this non-reflective film functions at a low reflectance of 1% or less is much wider than the wavelength range in which the conventional non-reflective film functions at a low reflectance of 1% or less. ing.

Embodiment 3.
Next, the semiconductor optical device according to the third embodiment will be described with reference to FIGS.

  As shown in FIG. 9, the semiconductor optical device of the present embodiment has a six-layer structure in which a semiconductor laser 31 and three specific types of films having a known refractive index and an unknown film thickness are stacked in three stages. In addition, a non-reflective film to which a specific kind of film having a known refractive index and a known film thickness is added is provided in a space 32 having a refractive index of 1, such as air or nitrogen.

The non-reflective film includes an aluminum nitride (AlN) first film 21 (refractive index n ₃ = 2.072, film thickness d ₃ = 50 nm) and a tantalum oxide (Ta ₂ O ₅ ) second film 22. (Refractive index n ₁ = 2.057, film thickness = Ad ₁ ), alumina (Al ₂ O ₃ ) third film 23 (refractive index n ₂ = 1.62, film thickness = Ad ₂ ), tantalum oxide ( Ta ₂ O ₅ ) fourth film 24 (refractive index n ₁ = 2.057, film thickness = Bd ₁ ), alumina (Al ₂ O ₃ ) fifth film 25 (refractive index n ₂ = 1.62) , Film thickness = Bd ₂ ), tantalum oxide (Ta ₂ O ₅ ) sixth film 26 (refractive index n ₁ = 2.057, film thickness = Cd ₁ ), and alumina (Al ₂ O ₃ ) 7 film 27 (refractive index n ₂ = 1.62, film thickness = Cd ₂ ). The film thickness of aluminum nitride (AlN) constituting the first film 21 is 50 nm.

  Three types of materials of aluminum nitride, tantalum oxide, and alumina are used for the antireflection film of the present embodiment. The thermal conductivity of aluminum nitride is about 1.8 W / cm / ° C. The thermal conductivity of tantalum oxide is about 0.1 W / cm / ° C. The thermal conductivity of alumina is about 0.2 W / cm / ° C. Therefore, aluminum nitride has the highest thermal conductivity among the three materials.

Also, when A = 2.0, B = 2.0 and C = 2.0, and the phase φ ₁ and phase φ _{2 of} tantalum oxide and alumina are 0.449531 and 0.991758, respectively, the wavelength λ = 980 nm In the non-reflective film, the real part and the imaginary part of the amplitude reflectance are zero. At this time, the thickness of each layer is as follows: first film / second film / third film / fourth film / fifth film / sixth film / seventh film = d ₃ / Ad ₁ / a _{Ad 2 / Bd 1 / Bd 2} / Cd 1 / Cd 2 = 50nm / 68.17nm / 190.97nm / 68.17nm / 190.97nm / 68.17nm / 190.97nm.

  Therefore, the total film thickness is 1452.26 nm. The total film thickness is about 5.9 times 245 nm, which is a quarter value of the wavelength λ. The wavelength dependence of the reflectance of this non-reflective film is close to a bathtub shape as shown in FIG. The wavelength range in which the non-reflective film functions at a low reflectance of 1% or less is 152 nm.

When the desired wavelength λ = 980 nm is the center of the bathtub-shaped reflectance distribution, the phase φ ₁ and phase φ ₂ of tantalum oxide and alumina are set to 0.449325 and 1.00016, respectively, and the wavelength λ = 962 nm What is necessary is just to design a non-reflective film so that the real part and imaginary part of the amplitude reflectance of a reflective film may be set to zero, respectively.

At this time, the thickness of each film is as follows: first film / second film / third film / fourth film / fifth film / sixth film / seventh film = d ₃ / Ad ₁ / a _{Ad 2 / Bd 1 / Bd 2} / Cd 1 / Cd 2 = 50nm / 55.89nm / 189.05nm / 66.89nm / 189.05nm / 66.89nm / 189.05nm. FIG. 11 shows the wavelength dependence of the reflectance of this non-reflective film. The wavelength range in which this non-reflective film functions with a low reflectance of 1% or less is 151 nm.

  Next, FIG. 12 shows a non-reflective film in which the first film, aluminum nitride (AlN), is 120 nm.

In FIG. 12, the non-reflective film includes a first film 28 of aluminum nitride (AlN) (refractive index n ₃ = 2.072, film thickness d ₃ = 120 nm), and a _second film of tantalum oxide (Ta ₂ O ₅ ). Film 29 (refractive index n ₁ = 2.057, film thickness = Ad ₁ ), alumina (Al ₂ O ₃ ) third film 30 (refractive index n ₂ = 1.62, film thickness = Ad ₂ ), oxidation Tantalum (Ta ₂ O ₅ ) fourth film 41 (refractive index n ₁ = 2.057, film thickness = Bd ₁ ), alumina (Al ₂ O ₃ ) fifth film 42 (refractive index n ₂ = 1) .62, film thickness = Bd ₂ ), tantalum oxide (Ta ₂ O ₅ ) sixth film 43 (refractive index n ₁ = 2.057, film thickness = Cd ₁ ), and alumina (Al ₂ O ₃ ) The seventh film 44 (refractive index n ₂ = 1.62, film thickness = Cd ₂ ) is provided.

When A = 0.9, B = 2.0, and C = 2.0, and the phase φ ₁ and phase φ _{2 of} tantalum oxide and alumina are 0.726468 and 0.860316, respectively, the wavelength λ = 980 nm In the non-reflective film, the real part and the imaginary part of the amplitude reflectivity are each zero.

At this time, the thickness of each layer is as follows: first film / second film / third film / fourth film / fifth film / sixth film / seventh film = d ₃ / Ad ₁ / a _{Ad 2 / Bd 1 / Bd 2} / Cd 1 / Cd 2 = 120nm / 49.58nm / 74.55nm / 110.17nm / 165.66nm / 110.17nm / 165.66nm. Therefore, the total film thickness of the above-described non-reflective film is 1461.38 nm. That is, the total film thickness is about 6.0 times 245 nm, which is λ / 4. Therefore, compared with the conventional non-reflective film, it is a non-reflective film whose total film thickness is very thick.

  The wavelength dependence of the reflectance of this non-reflective film is close to a bathtub shape as shown in FIG. The range in which the antireflective film functions with a low reflectance of 1% or less is 150 nm. Therefore, the range in which the non-reflective film functions with a low reflectance of 1% or less as compared with the conventional non-reflective film is very wide.

When the desired wavelength λ = 980 nm is the center of the bathtub-shaped reflectance distribution, the phase φ ₁ and phase φ _{2 of} tantalum oxide and alumina are set to 0.700522 and 0.891134, respectively, and the wavelength λ = 947 nm What is necessary is just to design a non-reflective film so that the reflectance of a reflective film may be set to zero.

The film thickness of each film at this time is as follows: first film / second film / third film / fourth film / fifth film / sixth film / seventh film = d ₃ / Ad ₁ / a _{Ad 2 / Bd 1 / Bd 2} / Cd 1 / Cd 2 = 120nm / 46.20nm / 74.62nm / 102.66nm / 165.82nm / 102.66nm / 165.82nm. FIG. 14 shows the wavelength dependence of the reflectance of this non-reflective film. The range in which the antireflective film functions at a low reflectance of 1% or less is 153 nm.

  In the nonreflective film of the present embodiment, the first aluminum nitride film has a thickness of 50 nm and 120 nm. However, the thickness of the first aluminum nitride film is limited to this value. However, the same effect can be obtained with other values.

  The plurality of films constituting the non-reflective films of the first to third embodiments have a total sum of the product of the film thickness and the refractive index larger than a quarter wavelength of the light emitted from the semiconductor optical laser. In this case, if the design method for the non-reflective film is used, the wavelength range in which the non-reflective film functions at a low reflectance of 1% or less can be easily made wider than that of the conventional non-reflective film.

  Further, as described above, it is desirable that the adjacent film provided so as to be adjacent to the semiconductor optical element among the plurality of films has a higher thermal conductivity than the other films. In the semiconductor element device of the present embodiment, an example in which aluminum nitride is used as the adjacent film is shown, but the present invention is not limited to this. In this way, it is possible to easily design a semiconductor optical device that has been realized to efficiently release the heat of the semiconductor laser by using the above design method.

  Moreover, it is desirable that the wavelength range in which the non-reflective film functions with a low reflectance of 1% or less is 100 nm or more. In this way, it is possible to flexibly adapt to changes in the wavelength of light emitted from the semiconductor optical device in a normal state.

Embodiment 4.
Next, a semiconductor laser module according to an embodiment of the present invention will be described with reference to FIGS. FIG. 15 shows a semiconductor laser module including a semiconductor laser and a fiber grating.

As shown in FIG. 15, the semiconductor laser module of the present embodiment includes a semiconductor laser 201, a non-reflective film 203 provided on the front end face side of the semiconductor laser 201, and the reflectance of R _f and the semiconductor laser 201. A semiconductor element device 200 comprising an optical waveguide region 204; a reflective film 202 having a reflectivity of R _r; provided on the rear end face side of the semiconductor laser 201; a lens 205 through which light emitted from the optical waveguide region 204 passes; , An optical fiber 206 through which the light that has passed through the lens 205 is guided, and a fiber grating 207 having a reflectance of R _fg provided in the optical path of the optical fiber 206.

  In the semiconductor laser module of the present embodiment, a fiber grating 207 is provided in the optical fiber 206 in order to stabilize the oscillation wavelength of the semiconductor laser 201. Therefore, the light of a specific wavelength guided into the optical fiber 206 is reflected by the fiber grating 207.

  Further, the non-reflective film 203 is formed of any of the non-reflective films in the first to third embodiments. The reflective film 202 is made of a film having a higher reflectance than the non-reflective film 203. Further, the fiber grating 207 is made of a film having a higher reflectance than the non-reflective film 203. Thereby, a resonator is configured by the fiber grating 207 and the reflection film 202 so that light resonates between the fiber grating 207 and the reflection film 202. The lens 205 is used to efficiently guide the light emitted from the semiconductor laser 201 into the optical path of the optical fiber 206.

FIG. 16 shows the relationship between the gain and loss of the semiconductor laser in the semiconductor laser module of the present embodiment provided with the fiber grating 207. The fiber grating 207 has a reflectance R _fg for a specific wavelength λ _fg . However, the fiber grating 207 has substantially zero reflectivity for wavelengths other than the specific wavelength λ _fg . For this reason, as shown in FIG. 16, the loss of the semiconductor laser becomes extremely small locally at a specific wavelength λ _fg . The gain data shown in FIG. 16 and the portion of the loss data that are locally small intersect. As a result, normally, the semiconductor laser module oscillates at a specific wavelength λ _fg .

However, for example, when the ambient temperature is low, the gain distribution of the semiconductor laser moves to the smaller wavelength side. Therefore, as shown in FIG. 17, the loss of the semiconductor laser determined by the non-reflective film 203 may be smaller than the loss of the semiconductor laser determined by the fiber grating 207. At this time, the gain data and the loss data shown in FIG. 17 intersect with portions other than the portion that is locally small. Therefore, the semiconductor laser module oscillates at the wavelength λ _LD instead of the wavelength λ _fg . As a result, the side mode suppression ratio, which is the ratio of the light intensity of the wavelength λ _{LD to} the light intensity of the wavelength λ _fg , becomes small, or a wavelength other than the wavelength determined by the loss of the fiber grating 207 as described above. There is a disadvantage that the semiconductor laser oscillates at a wavelength.

In the semiconductor laser module of the present embodiment, as shown in FIG. 18, a non-reflective film 203 having a function range with a low reflectance of 1% or less is 100 nm or more is provided on the front end face side of the semiconductor laser 201. . Therefore, the loss data shown in FIG. 18 is not a curve having a steep warp like the loss data in FIGS. 16 and 17, but a gentle land-like curve. As a result, the loss of the semiconductor laser determined by the fiber grating 207 in a wide range of wavelengths can be made smaller than the loss of the semiconductor laser determined by the reflectance of the non-reflective film 203. That is, regardless of whether the gain distribution moves to the side where the wavelength is slightly smaller or moves toward the side where the wavelength is somewhat larger, the gain data and the portion of the loss data that are locally small intersect. Accordingly, oscillation at the wavelength λ _LD shown in FIG. 17 can be suppressed, and the side mode suppression ratio of the semiconductor laser 201 can be prevented from becoming small.

  The semiconductor optical device of each of the first to fourth embodiments has been described by taking the non-reflective film as a seven-layer structure as an example. However, the structure of the non-reflective film of the present invention is not limited to the seven-layer structure, and a nine-layer structure or an eleven-layer structure as long as a plurality of films having three or more kinds of refractive indexes are provided. Any number of layers may be used.

  In addition, A, B, and C, which are parameters of the antireflective films in the first to fourth embodiments, indicate predetermined numerical values as examples in each of the antireflective films in the actual embodiments. However, the parameters of the antireflective film of the present invention are not limited to the predetermined numerical values used for the antireflective film of each actual embodiment. Even if the parameter of the non-reflective film is another numerical value, it is the same as the non-reflective film of the first to fourth embodiments as long as the real part and the imaginary part of the amplitude reflectance can be made zero An effect can be obtained.

  The semiconductor optical device of each of the first to fourth embodiments has been described by taking as an example a case where the plurality of films constituting the non-reflective film have three kinds of refractive indexes. However, if the phase conditions of the films other than the specific two kinds of films among the plurality of films, that is, the film thickness is set in advance, the refractive indexes of the plurality of films constituting the non-reflective film have four or more kinds. Even if it is a case, the specific two types of films may be non-reflective films whose film thickness is determined by the above-described method, that is, the method of zeroing the real part and the imaginary part of the amplitude reflectance of a plurality of films. For example, the same effect as the non-reflective film of Embodiments 1 to 4 can be obtained.

  Further, in each of the semiconductor optical element devices of the first to third embodiments, an example in which a semiconductor laser is used as an example of the semiconductor optical element is shown. As the semiconductor optical element, a semiconductor amplifier, a superluminescent diode, or Even in the case of a semiconductor optical device such as an optical modulator, the same effect as in the case of a semiconductor laser can be obtained.

  In the semiconductor optical device according to the first to fourth embodiments, a value near 980 nm is used as the wavelength of the light emitted from the semiconductor optical device, but the wavelength of the light emitted from the semiconductor optical device is this value. The present invention is not limited to this, and the same effects as those of the semiconductor optical device of each of the first to fourth embodiments can be obtained even with visible light, far infrared light, infrared light, or the like.

  In the first to third embodiments as described above, the semiconductor optical device is configured using a film formed by EB (Electron Beam) vapor deposition. However, the controllability of the film thickness may not be good in the EB vapor deposition method. Therefore, in the following fifth to seventh embodiments, semiconductor optical element devices in which controllability such as film thickness is improved by using an ECR (Electron Cyclotron Resonance) sputtering method will be described.

However, when the ECR sputtering method is used, the cause is unknown, but the bonding property between alumina (Al ₂ O ₃ ) and tantalum oxide (Ta ₂ O ₅ ) is not good. Therefore, in the _{fifth to} seventh embodiments, a semiconductor optical device using a junction of quartz (SiO ₂ ) and tantalum oxide (Ta ₂ O ₅ ) is used.

  When the semiconductor optical device of the fifth to seventh embodiments is used for the semiconductor laser described in the fourth embodiment, the semiconductor optical device of the first to third embodiments is the semiconductor of the fourth embodiment. The same effect as that obtained by the laser can be obtained.

Each of the following Embodiments 5 to 7 is an antireflection film in which two types of films are added in addition to the two-layer structure described in Embodiments 1 to 3. Similarly, by using the same method as the design method of the non-reflective film having the two-layer structure described in the first to third embodiments, that is, the method of setting the real part and the imaginary part of the amplitude reflectance r to zero, respectively. A film thickness d ₁ and a film thickness d ₂ described later are calculated.

Embodiment 5 FIG.
Next, the semiconductor optical device according to the fifth embodiment will be described with reference to FIGS.

  As shown in FIG. 21, in the semiconductor optical device of the present embodiment, the semiconductor laser 31 and the non-reflective film are provided in a space 32 such as air or nitrogen having a refractive index of 1. The non-reflective film has a known refractive index and two specific types of known film thicknesses in a four-layer structure in which two specific types of films with known refractive indices and unknown film thicknesses are stacked in two stages. A membrane is added.

More specifically, as shown in FIG. 21, the non-reflective film includes an alumina (Al ₂ O ₃ ) first film 45 (refractive index n ₃ = 1.629, film thickness d ₃ ), quartz (SiO ₂ ). ₂ ) second film 46 (refractive index n ₂ = 1.484, film thickness = Ad ₂ ), tantalum oxide (Ta ₂ O ₅ ) third film 47 (refractive index n ₁ = 2.072, film) Thickness = Bd ₁ ), quartz (SiO ₂ ) fourth film 48 (refractive index n ₂ = 1.484, film thickness = Bd ₂ ), tantalum oxide (Ta ₂ O ₅ ) fifth film 49 (refraction) And a sixth film 50 (refractive index n ₂ = 1.484, film thickness = Cd ₂ ) of quartz (SiO ₂ ) and a ratio n ₁ = 2.072, film thickness = Cd ₁ ). The algebra A, B, and C in the formula indicating the film thickness are predetermined parameters as in the first to third embodiments.

First, the non-reflective film when the film thickness d _{3 of} alumina (Al ₂ O ₃ ) as the first film 45 is 10 nm will be described. In the present embodiment and the following embodiments, an example of the refractive index of each layer when the film is formed by the ECR sputtering method is shown.

According to the antireflective film of the present embodiment, A = 0.18, B = 1.99, and C = 2.00, and the phase φ ₁ and the phase φ _{2 of} tantalum oxide and quartz are 0.581355 and 0, respectively. .8993, both the real part and the imaginary part of the amplitude reflectance of the non-reflective film can be made zero at the wavelength λ = 980 nm.

At this time, the thickness of each layer is as follows: first film / second film / third film / fourth film / fifth film / sixth film = d ₃ / Ad ₂ / Bd ₁ / the _{bd 2 / Cd 1 / Cd 2} = 10 / 17.01 / 87.08 / 188.07 / 87.52 / 189.02nm.

  Therefore, the total film thickness is 962.91 nm. This value is about 3.9 times the film thickness of 245 nm, which is ¼ of the light wavelength λ. At this time, the wavelength dependence of the reflectance of the non-reflective film is close to a bathtub shape as shown in FIG. Therefore, the wavelength range in which the above-mentioned non-reflective film functions at a low reflectance of 1% or less is 217 nm, compared with the wavelength range in which the conventional non-reflective film functions at a low reflectance of 1% or less. It is very wide.

When the desired wavelength λ = 980 nm is set to the center of the bathtub-shaped reflectance distribution, the phase φ ₁ and phase φ ₂ of tantalum oxide and quartz are set to 0.580136 and 0.908343, respectively, and the wavelength λ = 945 nm. What is necessary is just to design an anti-reflective film so that a reflectance may be set to zero.

At this time, the thickness of each film is as follows: first film / second film / third film / fourth film / fifth film / sixth film = d ₃ / Ad ₂ / Bd ₁ / a _{Bd 2 / Cd 1 / Cd 2} = 10 / 16.57 / 83.80 / 183.20 / 84.22 / 184.12nm.

  FIG. 23 shows the wavelength dependence of the reflectance of the non-reflective film. The wavelength range in which this antireflective film functions with a low reflectance of 1% or less is 213 nm.

Next, an antireflective film in which the film thickness d _{3 of} alumina (Al ₂ O ₃ ) as the first film 45 is 20 nm will be described. According to the above-described non-reflective film, A = 0.12, B = 1.90 and C = 2.00, and the phase φ ₁ and the phase φ _{2 of} tantalum oxide and quartz are 0.601513 and 0.911814, respectively. In some cases, the reflectance is zero at the wavelength λ = 980 nm.

At this time, the thickness of each layer is as follows: first film / second film / third film / fourth film / fifth film / sixth film = d ₃ / Ad ₂ / Bd ₁ / the _{bd 2 / Cd 1 / Cd 2} = 20 / 11.50 / 86.03 / 182.08 / 90.56 / 191.67nm. The total film thickness is 970.19 nm, which is approximately 4.0 times 245 nm, which is a quarter value of the wavelength λ.

  Therefore, the above-described non-reflective film has a very large total film thickness as compared with the conventional non-reflective film. At this time, the wavelength dependence of the reflectance of the non-reflective film is close to a bathtub shape as shown in FIG. In addition, the range in which the above-described non-reflective film functions at a low reflectance of 1% or less is 220 nm. Therefore, the above-mentioned non-reflective film has a very wide range in which the non-reflective film functions at a low reflectance of 1% or less as compared with the conventional non-reflective film.

When the desired wavelength λ = 980 nm is set to the center of the bathtub-shaped reflectance distribution, the phase φ ₁ and phase φ ₂ of tantalum oxide and quartz are set to 0.596734 and 0.925211 respectively, and no reflection occurs at the wavelength λ = 935 nm. What is necessary is just to design a non-reflective film so that the reflectance of a film | membrane may be set to zero.

At this time, the thickness of each film is as follows: first film / second film / third film / fourth film / fifth film / sixth film = d ₃ / Ad ₂ / Bd ₁ / a _{Bd 2 / Cd 1 / Cd 2} = 20 / 11.13 / 81.43 / 176.28 / 85.71 / 185.55nm. FIG. 25 shows the wavelength dependence of the reflectance of the non-reflective film. The wavelength range in which the antireflective film functions with a low reflectance of 1% or less is 215 nm.

Further, a non-reflective film in which the film thickness d _{3 of} alumina (Al ₂ O ₃ ) as the first film 45 is 40 nm will be described. The antireflective film has a wavelength when A = 0.02, B = 1.50 and C = 2.00, and the phase φ ₁ and phase φ _{2 of} tantalum oxide and quartz are 0.789974 and 0.884697, respectively. The reflectance becomes zero at λ = 980 nm.

At this time, the thickness of each layer is as follows: first film / second film / third film / fourth film / fifth film / sixth film = d ₃ / Ad ₂ / Bd ₁ / Bd ₂ / Cd ₁ / Cd ₂ = 40 / 1.86 / 89.20 / 139.48 / 118.93 / 185.97 nm. The total film thickness of this non-reflective film is 982.13 nm, which is about 4.0 times 245 nm which is a quarter of the wavelength λ. Therefore, this total film thickness is very thick compared with the total film thickness of the conventional non-reflective film.

  The wavelength dependence of the reflectance of the non-reflective film at this time is close to a bathtub shape as shown in FIG. This non-reflective film has a wavelength range of 218 nm that functions at a low reflectance of 1% or less, and this range is compared with a wavelength range that functions at a low reflectance of 1% or less of a conventional non-reflective film. And very wide.

When the desired wavelength λ = 980 nm is set to the center of the bathtub-shaped reflectance distribution, the phase φ ₁ and phase φ ₂ of tantalum oxide and quartz are set to 0.774569 and 0.901877, respectively, and no reflection occurs at the wavelength λ = 927 nm. The antireflection film is designed so that the reflectance of the film is zero.

At this time, the thickness of each film is as follows: first film / second film / third film / fourth film / fifth film / sixth film = d ₃ / Ad ₂ / Bd ₁ / a _{Bd 2 / Cd 1 / Cd 2} = 40 / 1.79 / 82.73 / 134.50 / 110.31 / 179.33nm. FIG. 27 shows the wavelength dependence of the reflectance of the non-reflective film. The non-reflective film has a wavelength range of 208 nm that functions at a low reflectance of 1% or less.

In the design method for the non-reflective film having the six-layer structure described above, the following equation (8) is used. Even when this equation (8) is used, the film thickness d ₁ and the film thickness d ₂ are calculated so that the real part and the imaginary part of the amplitude reflectance r shown in the expression (3c) are each zero. .

Embodiment 6 FIG.
Next, the semiconductor optical device of the sixth embodiment will be described with reference to FIGS.

  As shown in FIG. 28, in the semiconductor optical device of this embodiment, the semiconductor laser 31 and the non-reflective film are provided in a space 32 such as air or nitrogen having a refractive index of 1. The non-reflective film is a six-layer structure in which two specific types of films having a known refractive index and unknown film thickness are stacked in three stages. A membrane is added.

As shown in FIG. 28, the antireflective film of the present embodiment includes an alumina (Al ₂ O ₃ ) first film 51 (refractive index n ₃ = 1.629, film thickness d ₃ ), quartz (SiO ₂ ). ) Second film 52 (refractive index n ₂ = 1.484, film thickness = Ad ₂ ), tantalum oxide (Ta ₂ O ₅ ) third film 53 (refractive index n ₁ = 2.072, film thickness) = Bd ₁ ), quartz (SiO ₂ ) fourth film 54 (refractive index n ₂ = 1.484, film thickness = Bd ₂ ), tantalum oxide (Ta ₂ O ₅ ) fifth film 55 (refractive index) n ₁ = 2.072, film thickness = Cd ₁ ), quartz (SiO ₂ ) sixth film 56 (refractive index n ₂ = 1.484, film thickness = Cd ₂ ), tantalum oxide (Ta ₂ O ₅ ) The seventh film 57 (refractive index n ₁ = 2.072, film thickness = Dd ₁ ) and quartz (SiO ₂ ) eighth film 58 (refractive index n ₂ = 1.484, film thickness = Dd ₂₎ ) It is.

First, a non-reflective film in which the film thickness d _{3 of} alumina (Al ₂ O ₃ ) as the first film 51 is 10 nm will be described.

The non-reflective film described above has A = 0.50, B = 2.00, C = 2.00 and D = 2.00, and the phase φ ₁ and phase φ _{2 of} tantalum oxide and quartz are 0.356965 and When 1.03993, the reflectance can be made zero at the wavelength λ = 980 nm.

At this time, the film thickness of each layer is as follows: first film / second film / third film / fourth film / fifth film / sixth film / seventh film / eighth film _{= d 3 / Ad 2 / Bd} 1 / Bd 2 / Cd 1 / Cd 2 / Dd 1 / Dd 2 = 10 / 54.65 / 53.74 / 218.60 / 53.74 / 218.60 / 53.74 /218.60 nm. The total film thickness of this non-reflective film is 1406.45 nm, which is approximately 5.7 times as large as 245 nm, which is a quarter of the wavelength λ.

  Therefore, this total film thickness is very thick compared with the total film thickness of the conventional non-reflective film. At this time, the wavelength dependence of the reflectance of the non-reflective film is close to a bathtub shape as shown in FIG. In addition, the non-reflective film has a wavelength range of 116 nm that functions at a low reflectance of 1% or less, and this range is compared with the wavelength range that functions at a low reflectance of 1% or less of a conventional non-reflective film. It is very wide.

When the desired wavelength λ = 980 nm is set to the center of the bathtub-shaped reflectance distribution, the phase φ ₁ and phase φ ₁ of tantalum oxide and quartz are set to 0.357013 and 1.0386, respectively, and no reflection occurs at the wavelength λ = 971 nm. What is necessary is just to make the reflectance of a film | membrane into zero.

The thickness of each film at this time is as follows: first film / second film / third film / fourth film / fifth film / sixth film / seventh film / eighth film Membrane = d ₃ / Ad ₂ / Bd ₁ / Bd ₂ / Cd ₁ / Cd ₂ / Dd ₁ / Dd ₂ = 10 / 54.08 / 53.26 / 216.31 / 53.26 / 216.31 / 53. 26 / 216.31 nm. FIG. 30 shows the wavelength dependence of the reflectance of the non-reflective film. This non-reflective film has a wavelength range of 115 nm that functions at a low reflectance of 1% or less.

Next, an antireflective film in which the film thickness d _{3 of} alumina (Al ₂ O ₃ ) as the first film 51 is 20 nm will be described. The antireflective film has A = 0.42, B = 2.00, C = 2.00 and D = 2.00, and the phase φ ₁ and phase φ _{2 of} tantalum oxide and quartz are 0.355425 and 1. When 03088, the reflectance becomes zero at the wavelength λ = 980 nm.

The film thickness of each layer at this time is as follows: first film / second film / third film / fourth film / fifth film / sixth film / seventh film / eighth film _{= d 3 / Ad 2 / Bd} 1 / Bd 2 / Cd 1 / Cd 2 / Dd 1 / Dd 2 = 20 / 45.51 / 53.51 / 216.70 / 53.51 / 216.70 / 53.51 /216.70 nm. The total film thickness is 1397.48 nm, which is approximately 5.7 times 245 nm, which is a quarter of the wavelength λ.

  Therefore, this total film thickness is a very large value compared with the total film thickness of the conventional non-reflective film. The wavelength dependence of the reflectance of the non-reflective film at this time is close to a bathtub shape as shown in FIG. This non-reflective film has a wavelength range of 116 nm that functions at a low reflectance of 1% or less, and this value is compared with a wavelength range that functions at a low reflectance of 1% or less of a conventional non-reflective film. It is a very large value.

When the desired wavelength λ = 98 nm is set to the center of the bathtub-shaped reflectance distribution, the phase φ ₁ and phase φ ₂ of tantalum oxide and quartz are set to 0.35537 and 1.02959, respectively, and no reflection occurs at the wavelength λ = 975 nm. The antireflection film is designed so that the reflectance of the film is zero.

The thickness of each film at this time is as follows: first film / second film / third film / fourth film / fifth film / sixth film / seventh film / eighth film Membrane = d ₃ / Ad ₂ / Bd ₁ / Bd ₂ / Cd ₁ / Cd ₂ / Dd ₁ / Dd ₂ = 20 / 45.22 / 53.23 / 215.32 / 53.23 / 215.32 / 53. It is 23 / 215.32 nm. FIG. 32 shows the wavelength dependence of the reflectance of the non-reflective film. This non-reflective film has a wavelength range of 115 nm that functions at a low reflectance of 1% or less.

Further, a non-reflective film in which the film thickness d _{3 of} alumina (Al ₂ O ₃ ) as the first film 51 is 40 nm will be described. The antireflective film has A = 0.30, B = 1.95, C = 2.00 and D = 2.00, and the phase φ ₁ and phase φ _{2 of} tantalum oxide and quartz are 0.356112 and 1 respectively. .00038, the reflectance becomes zero at the wavelength λ = 980 nm.

At this time, the film thickness of each layer is as follows: first film / second film / third film / fourth film / fifth film / sixth film / seventh film / eighth film _{= d 3 / Ad 2 / Bd} 1 / Bd 2 / Cd 1 / Cd 2 / Dd 1 / Dd 2 = 40 / 31.54 / 52.27 / 205.03 / 53.61 / 210.28 / 53.61 /210.28 nm. The total film thickness is 1370.80 nm, which is about 5.6 times as large as 245 nm, which is a quarter of the wavelength λ.

  Therefore, this total film thickness is very thick compared with the total film thickness of the conventional non-reflective film. At this time, the wavelength dependence of the reflectance of the non-reflective film is close to a bathtub shape as shown in FIG. This non-reflective film has a wavelength range of 110 nm that functions at a low reflectance of 1% or less, and this range is compared with a wavelength range that functions at a low reflectance of 1% or less of a conventional non-reflective film. Very wide.

When the desired wavelength λ = 980 nm is the center of the bathtub-shaped reflectance distribution, the phase φ ₁ and the phase φ ₂ of tantalum oxide and quartz are 0.356344 and 1.0013, respectively, and the wavelength λ = 983 nm The antireflection film is designed so that the reflectance of the reflection film is zero.

The thickness of each film at this time is as follows: first film / second film / third film / fourth film / fifth film / sixth film / seventh film / eighth film Membrane = d ₃ / Ad ₂ / Bd ₁ / Bd ₂ / Cd ₁ / Cd ₂ / Dd ₁ / Dd ₂ = 40 / 31.67 / 52.47 / 205.85 / 53.81 / 211.12 / 53. 81 / 211.12 nm. FIG. 34 shows the wavelength dependence of the reflectance of the non-reflective film. The non-reflective film has a wavelength range of 111 nm that functions at a low reflectance of 1% or less.

Further, in the above-described design method for the non-reflective film having the eight-layer structure, the following formula (9) is used. Even when this equation (9) is used, the film thickness d ₁ and the film thickness d ₂ are calculated so that the real part and the imaginary part of the amplitude reflectivity r shown in the expression (3c) are each zero. .

Embodiment 7 FIG.
Next, the semiconductor optical device of the seventh embodiment will be described with reference to FIGS.

  As shown in FIG. 35, in the semiconductor optical device of this embodiment, the semiconductor laser 31 and the non-reflective film are provided in a space 32 such as air or nitrogen having a refractive index of 1. The non-reflective film is an eight-layer structure in which a specific two kinds of films having a known refractive index and an unknown film thickness are stacked in four stages, and a specific two kinds of films having a known refractive index and a known film thickness. A membrane is added.

As shown in FIG. 35, a first film 59 (refractive index n ₃ = 1.629, film thickness d ₃ ) of alumina (Al ₂ O ₃ ), a second film 60 (refractive index) of quartz (SiO ₂ ). n ₂ = 1.484, film thickness = Ad ₂ ), tantalum oxide (Ta ₂ O ₅ ) third film 61 (refractive index n ₁ = 2.072, film thickness = Bd ₁ ), quartz (SiO ₂ ) The fourth film 62 (refractive index n ₂ = 1.484, film thickness = Bd ₂ ), tantalum oxide (Ta ₂ O ₅ ) fifth film 63 (refractive index n ₁ = 2.072, film thickness = Cd ₁ ), quartz (SiO ₂ ) sixth film 64 (refractive index n ₂ = 1.484, film thickness = Cd ₂ ), tantalum oxide (Ta ₂ O ₅ ) seventh film 65 (refractive index n) ₁ = 2.072, film thickness = Dd ₁ ), quartz (SiO ₂ ) eighth film 66 (refractive index n ₂ = 1.484, film thickness = Dd ₂ ), tantalum oxide (Ta ₂ O ₅ ) Ninth membrane 6 And a (refractive index n ₁ = 2.072, film thickness = Ed _1), and quartz layer 68 of the tenth (SiO ₂₎ (refractive index n ₂ = 1.484, film thickness = Ed ₂₎ .

First, an antireflective film in which the film thickness d _{3 of} alumina (Al ₂ O ₃ ) as the first film 59 is 10 nm will be described.

The non-reflective film described above has A = 0.62, B = 2.00, C = 2.00, D = 2.00 and E = 2.00, and the phase φ ₁ and phase φ _{2 of} tantalum oxide and quartz. Is 0.276571 and 1.1374, respectively, the reflectance is zero at the wavelength λ = 980 nm.

At this time, the film thickness of each layer is as follows: first film / second film / third film / fourth film / fifth film / sixth film / seventh film / eighth film / 9th film / 10th film = d ₃ / Ad ₂ / Bd ₁ / Bd ₂ / Cd ₁ / Cd ₂ / Dd ₁ / Dd ₂ / Ed ₁ / Ed ₂ = 10 / 74.12 / 41.64 /239.09/41.64/239.09/51.64/239.09/41.64/239.09 nm. The total film thickness is 1890.63 nm, which is approximately 7.7 times 245 nm, which is a quarter of the wavelength λ. Therefore, this total film thickness is a very large value compared with the total film thickness of the conventional non-reflective film.

  The wavelength dependency of the reflectance of the non-reflective film at this time is close to a bathtub shape as shown in FIG. This non-reflective film has a wavelength range of 79 nm that functions at a low reflectance of 1% or less, and the value is compared with a wavelength range that functions at a low reflectance of 1% or less of a conventional non-reflective film. It is a big value.

When the desired wavelength λ = 980 nm is set to the center of the bathtub-shaped reflectance distribution, the phase φ ₁ and the phase φ ₂ of tantalum oxide and quartz are 0.276804 and 1.13636, respectively, and there is no reflection at the wavelength λ = 971 nm. The antireflection film is designed so that the reflectance of the film is zero.

The thickness of each film at this time is as follows: first film / second film / third film / fourth film / fifth film / sixth film / seventh film / eighth film Film / 9th film / 10th film = d ₃ / Ad ₂ / Bd ₁ / Bd ₂ / Cd ₁ / Cd ₂ / Dd ₁ / Dd ₂ / Ed ₁ / Ed ₂ = 10 / 73.37 / 41. 29 / 236.67 / 41.29 / 236.67 / 41.29 / 236.67 / 41.29 / 236.67 nm. FIG. 37 shows the wavelength dependence of the reflectance of the non-reflective film. This non-reflective film has a wavelength range of 77 nm that functions at a low reflectance of 1% or less.

Next, an antireflective film in which the film thickness d _{3 of} alumina (Al ₂ O ₃ ) as the first film 59 is 20 nm will be described. The non-reflective film described above has A = 0.54, B = 2.00, C = 2.00, D = 2.00 and E = 2.00, and the phase φ ₁ and phase φ _{2 of} tantalum oxide and quartz. Is 0.27554045 and 1.1399, respectively, the reflectance is zero at the wavelength λ = 980 nm.

At this time, the film thickness of each layer is as follows: first film / second film / third film / fourth film / fifth film / sixth film / seventh film / eighth film / 9th film / 10th film = d ₃ / Ad ₂ / Bd ₁ / Bd ₂ / Cd ₁ / Cd ₂ / Dd ₁ / Dd ₂ / Ed ₁ / Ed ₂ = 20 / 64.70 / 41.41 /239.61/41.41/239.61/41.41/239.61/41.41/239.61 nm. The total film thickness is 1894.13 nm, which is about 7.7 times as large as 245 nm, which is a quarter of the wavelength λ. Therefore, this total film thickness is a very large value compared with the total film thickness of the conventional non-reflective film.

  The wavelength dependence of the reflectance of the non-reflective film at this time is close to a bathtub shape as shown in FIG. This non-reflective film has a wavelength range of 80 nm that functions at a low reflectance of 1% or less, and this value is compared with a wavelength range that functions at a low reflectance of 1% or less of a conventional non-reflective film. It is a big value.

When the desired wavelength λ = 980 nm is the center of the bathtub-shaped reflectance distribution, the phase φ ₁ and the phase φ ₂ of tantalum oxide and quartz are 0.275567 and 1.13754, respectively, and the wavelength λ = 971 nm The antireflection film is designed so that the reflectance of the reflection film is zero.

The thickness of each film at this time is as follows: first film / second film / third film / fourth film / fifth film / sixth film / seventh film / eighth film Film / 9th film / 10th film = d ₃ / Ad ₂ / Bd ₁ / Bd ₂ / Cd ₁ / Cd ₂ / Dd ₁ / Dd ₂ / Ed ₁ / Ed ₂ = 20 / 63.97 / 41. It is 11 / 236.92 / 41.11 / 236.92 / 41.11 / 236.92 / 41.11 / 236.92 nm. FIG. 39 shows the wavelength dependence of the reflectance of this non-reflective film. This non-reflective film has a wavelength range of 79 nm that functions with a low reflectance of 1% or less.

Next, an antireflective film in which the film thickness d _{3 of} alumina (Al ₂ O ₃ ) as the first film 59 is 40 nm will be described. The non-reflective film described above has A = 0.40, B = 2.00, C = 2.00, D = 2.00 and E = 2.00, and the phase φ ₁ and phase φ _{2 of} tantalum oxide and quartz. Is 0.275565 and 1.11479 respectively, the reflectance is zero at the wavelength λ = 980 nm.

At this time, the film thickness of each layer is as follows: first film / second film / third film / fourth film / fifth film / sixth film / seventh film / eighth film / 9th film / 10th film = d ₃ / Ad ₂ / Bd ₁ / Bd ₂ / Cd ₁ / Cd ₂ / Dd ₁ / Dd ₂ / Ed ₁ / Ed ₂ = 40 / 46.87 / 41.49 /234.34/41.49/234.34/41.49/234.34/41.49/234.34 nm. The total film thickness is 1869.63 nm, which is about 7.6 times 245 nm, which is a quarter of the wavelength λ. Therefore, this total film thickness is a very large value compared with the total film thickness of the conventional non-reflective film.

  The wavelength dependency of the reflectance of the non-reflective film at this time is close to a bathtub shape as shown in FIG. This non-reflective film has a wavelength range of 79 nm that functions at a low reflectance of 1% or less, and this value is compared with a wavelength range that functions at a low reflectance of 1% or less of a conventional non-reflective film. It is a big value.

When the desired wavelength λ = 980 nm is the center of the bathtub-shaped reflectance distribution, the phase φ ₁ and phase φ ₂ of tantalum oxide and quartz are 0.275663 and 1.11367, respectively, and the wavelength λ = 977 nm The antireflection film is designed so that the reflectance of the reflection film is zero.

The thickness of each film at this time is as follows: first film / second film / third film / fourth film / fifth film / sixth film / seventh film / eighth film Film / 9th film / 10th film = d ₃ / Ad ₂ / Bd ₁ / Bd ₂ / Cd ₁ / Cd ₂ / Dd ₁ / Dd ₂ / Ed ₁ / Ed ₂ = 40 / 46.68 / 41. 37 / 233.38 / 41.37 / 233.38 / 41.37 / 233.38 / 41.37 / 233.38 nm. FIG. 41 shows the wavelength dependence of the reflectance of this non-reflective film. This non-reflective film has a wavelength range of 78 nm that functions at a low reflectance of 1% or less.

Further, in the design method of the above-described non-reflective film having the 10-layer structure, the following formula (10) is used. Even when this equation (10) is used, the film thickness d ₁ and the film thickness d ₂ are calculated so that the real part and the imaginary part of the amplitude reflectance r shown in the expression (3c) become zero, respectively. .

  In addition, A, B, C, D, and E, which are parameters of the antireflective films in the respective fifth to seventh embodiments, are predetermined numerical values as examples in the respective antireflective films in the respective actual embodiments. However, the parameters of the antireflective film of the present invention are not limited to the predetermined numerical values used for the antireflective film of each actual embodiment. Even if the parameters of the non-reflective film are other numerical values, as long as the real part and the imaginary part of the amplitude reflectivity can be zero, the same as the non-reflective film of the fifth to seventh embodiments. An effect can be obtained.

  Further, the semiconductor optical device of each of the fifth to seventh embodiments has been described by taking as an example the case where the refractive indexes of the plurality of films constituting the non-reflective film are three types. However, if the phase conditions of the films other than the specific two kinds of films among the plurality of films, that is, the film thickness is set in advance, the refractive indexes of the plurality of films constituting the non-reflective film have four or more kinds. Even if it is a case, the specific two types of films may be non-reflective films whose film thickness is determined by the above-described method, that is, the method of zeroing the real part and the imaginary part of the amplitude reflectance of a plurality of films. For example, the same effects as those of the nonreflective films of the fifth to seventh embodiments can be obtained.

  In the fifth to seventh embodiments, the non-reflective film is shown when the alumina film thickness of the first film is 10 nm, 20 nm, and 40 nm. However, the alumina film thickness is not limited to these values. Absent.

  In the fifth to seventh embodiments, the non-reflective film has a six-layer structure, an eight-layer structure, and a ten-layer structure. The effect similar to the effect acquired by the non-reflective film of -7 can be acquired.

  Further, in the semiconductor optical device of the fifth to seventh embodiments, the value near 980 nm is used as the wavelength of the light emitted from the semiconductor optical device, but the wavelength of the light emitted from the semiconductor optical device is this value. The present invention is not limited to this, and the same effects as those of the semiconductor optical element devices of the fifth to seventh embodiments can be obtained even with visible light, far infrared light, infrared light, or the like.

  Further, in each of the semiconductor optical device devices of the fifth to seventh embodiments, an example in which a semiconductor laser is used as an example of the semiconductor optical device is shown. However, as the semiconductor optical device, a semiconductor amplifier, a super luminescent diode, or Even in the case of a semiconductor optical device such as an optical modulator, the same effect as in the case of a semiconductor laser can be obtained.

  The embodiment disclosed this time should be considered as illustrative in all points and not restrictive. The scope of the present invention is defined by the terms of the claims, rather than the description above, and is intended to include any modifications within the scope and meaning equivalent to the terms of the claims.

  1, 3, 7, 14, 21, 28 First film 2, 4, 8, 15, 22, 29 Second film 5, 9, 16, 23, 30 Third film 6, 10, 17, 24 4th film, 11, 18, 25, 42 5th film, 12, 19, 26, 43 6th film, 13, 20, 27, 44 7th film, 31 semiconductor laser, 32 space , 200 semiconductor element device, 201 semiconductor laser, 202 reflective film, 203 non-reflective film, 204 optical waveguide region, 205 lens, 206 optical fiber, 207 fiber grating.

Claims (10)

A semiconductor optical device;
The outgoing light emitted from the semiconductor optical element is incident, and the incident light and the reflected light reflected from the incident light are made to interfere with light of a specific wavelength, thereby substantially reducing the reflectance of the light. With anti-reflective film to zero,
The antireflective film is
A plurality of films each having a refractive index greater than 1, a high refractive index film having a refractive index higher than the value of the square root of the effective refractive index of the semiconductor optical element, and the semiconductor optical element It is composed of a plurality of films configured using a low refractive index film having a refractive index lower than the value of the square root of the effective refractive index,
Each of the plurality of films has a single composition, and the number of composition types of the plurality of films is 3 or more, and the real part and the imaginary part of the amplitude reflectivity are both zero as a whole. A semiconductor optical device configured to be   2. The semiconductor optical device according to claim 1, wherein the plurality of films have a sum total of products of respective film thicknesses and refractive indexes larger than a quarter wavelength of light emitted from the semiconductor optical device.   The semiconductor optical device according to claim 1, wherein an adjacent film provided so as to be adjacent to the semiconductor optical element among the plurality of films has a higher thermal conductivity than other films.   The semiconductor optical device according to claim 3, wherein the adjacent film is aluminum nitride.   5. The semiconductor optical device according to claim 1, wherein a wavelength range in which the non-reflective film functions with a low reflectance of 1% or less is 100 nm or more.   3. The semiconductor optical device according to claim 1, wherein the first layer film adjacent to the semiconductor optical device is made of a material having a refractive index smaller than a square root of an effective refractive index of the semiconductor optical device.   The first layer film in contact with the semiconductor optical element and the second layer film in contact with the first layer film are each made of a material having a refractive index smaller than the square root of the effective refractive index of the semiconductor optical element. Or a semiconductor optical device according to 2;   The semiconductor optical device according to claim 1, wherein the semiconductor optical device is any one of a semiconductor laser, a semiconductor amplifier, a superluminescent diode, and a semiconductor optical modulator. The semiconductor optical element device according to any one of claims 1 to 7, wherein the semiconductor optical element is a semiconductor laser;
A first reflective film having a reflectance higher than that of the non-reflective film provided outside the semiconductor element device;
A second reflective film provided on an end face different from the end face on which the non-reflective film of the semiconductor element device is provided and having a reflectivity higher than that of the non-reflective film with respect to light of a predetermined wavelength; With
The light having a specific wavelength reflected by each of the first reflective film and the second reflective film transmits through the non-reflective film and oscillates between the first reflective film and the second reflective film. Semiconductor laser module.   The semiconductor laser module according to claim 9, wherein the first reflective film is a fiber grating or a filter provided in an optical fiber.

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