JPH11266031A - Condenser type solarlight power generator and generator module having diffracting surface - Google Patents

Abstract

PROBLEM TO BE SOLVED: To simplify the macroscopic structure of a condenser type solar beam generator, by a method whereina photodetectors are provided on the surface of a medium filling up the space held by a photodetecting surface and a diffracting surface, while the refractive index of the medium is specified to exceed that of the outer photo- detecting surface. SOLUTION: A condenser type solarlight power generator generates electricity by condensing solar beams 1 in cylindrical photodetectors 6. At this time, a diffracting surface 7 is formed by bonding a sheet in the structure holding an aluminum-made reflecting member between a surface protective member and a backside protective member onto the backside. At this time, a medium 5 is made of a plastic. Since the refractive index of the plastic is about 1.5, the incident angle when the incident light reflecting on the diffracting surface 7 to be entered in the photodetecting surface 4 again does not exceed 41.8 deg.. Therefore, the blaze angle of the diffracting surface 7 is specified to be 45 deg.. In such a constitution, the solar beams having wide wavelength range can be effectively condensed by the diffraction. Accordingly, the condenser having multiple juxtaposed photodetectors 6 in a simple structure can increase the condensing efficiency.

Description

DETAILED DESCRIPTION OF THE INVENTION

[0001]

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a concentrating photovoltaic power generation device having a diffraction surface and a concentrating photovoltaic power generation module.

[0002]

2. Description of the Related Art A light-receiving surface, a light-reflecting device installed so that at least a part thereof is located in a space surrounded by a regular reflection surface and the light-receiving surface and the regular reflection surface, and the space is filled. Examples of the structure of the light collecting device having a medium include:
"New Family 2-D nonimagin Concentrators The Compound Triangular Concentrator (New family 2-D nonimagin
g concentrators the compound triangular concentrat
or) ", APPLIED OPTIC
S), Vol. 24, No. 22 (1985), 3872
３８3876. In such a conventional structure, as shown in FIG. 21A, when the incident light 1 enters the light receiving surface 4 of the light condensing device and is reflected by the regular reflection surface 32 perpendicular to the incident light 2, the medium 5 is refracted. Regardless of the ratio, the reflected light 3 passes through the same optical path as the incident light 2 in the opposite direction and exits from the light receiving surface 4 to the outside.

In order to avoid this, for example, FIG.
As shown in (b), the specular reflection surface 32 is inclined with respect to the light receiving surface 4, and the light 2 incident on the light collector is reflected by the specular reflection surface 32 and is again incident on the light receiving surface 4 at an incident angle 33. To increase. In such a structure, by making the refractive index of the medium 5 larger than the refractive index outside the light receiving surface 4, total reflection can be performed on the light receiving surface. As described above, the incident light can be confined inside the light condensing device using the regular reflection on the inclined surface and the total reflection on the light receiving surface, and can be finally incident on the light receiving device 6. However, as shown in FIG. 21C, the incident angle 33 of the reflected light on the light receiving surface 4 cannot be made sufficiently large depending on the incident angle of the incident light 1, and the light escapes outside the light collecting device. .

[0004]

In the prior art, since the regular reflection surface is used, the ratio of the area of the light-receiving surface of the light-receiving device to the area of the light-receiving surface of the light-receiving device, that is, the ratio of the light-receiving surface of the light-receiving device, Assuming that the area is A and the area B of the incident surface of the light condensing device is B / A, the light condensing magnification is obtained. It is difficult to increase the light use efficiency when the light collection magnification is increased.

An object of the present invention is to provide a technique capable of simplifying a macroscopic structure of a concentrating solar power generation device.

Another object of the present invention is to provide a technique capable of increasing the light-gathering power while keeping the light use efficiency of the light-collecting solar power generation device high.

The above and other objects and novel features of the present invention will become apparent from the description of the present specification and the accompanying drawings.

[0008]

The outline of a typical invention among the inventions disclosed in the present application will be briefly described as follows.

(1) A light-receiving surface, a diffraction surface, a medium filling a space between the light-receiving surface and the diffraction surface, and a light-receiving device in which at least a part of the surface is in contact with the medium. A concentrator photovoltaic power generator wherein the refractive index of the medium is larger than the refractive index outside the light receiving surface.

(2) The diffraction surface is a reflection diffraction surface.

(3) The reflection diffraction surface is a blazed diffraction surface.

(4) The blazed diffraction surface has a blaze angle that is symmetrical to the outside.

(5) The blazed diffraction surface is symmetrically arranged on the left and right sides of the diffraction surface.

(6) A concentrating photovoltaic power generation module obtained by modularizing a plurality of the concentrating photovoltaic power generation devices.

(7) In the concentrating solar power generation module, the medium is continuous between the plurality of concentrating solar power generation devices.

[0016]

Embodiments of the present invention (embodiments) will be described below in detail with reference to the drawings.

An embodiment of the present invention is directed to a light receiving surface, a diffraction surface, a medium filling a space between the light receiving surface and the diffraction surface, and a light receiving device in which at least a part of the surface is in contact with the medium. And a concentrating solar power generation device having a refractive index of the medium larger than a refractive index outside the light receiving surface. As the light receiving device, a solar cell that converts sunlight into electric power is used.

FIG. 1 is a diagram showing a schematic configuration of a concentrating solar power generation device according to an embodiment of the present invention.

In the concentrator photovoltaic power generator of the present embodiment, as shown in the structure having a cross section shown in FIG. Does not reflect only in the specular reflection direction (0-order light direction) of the surface,
According to the microscopic structure of the diffraction surface 7 and the wavelength of the incident light 1,
The light is reflected in the directions of next, −1st, 2nd, and −2nd order. Therefore, even when the light is incident perpendicularly to the diffraction surface 7, the reflected light 3 does not all pass through the same optical path as the incident light 2, and the reflected light 3
Next, the light is divided and reflected in respective directions such as primary, −1, secondary, and −secondary. Therefore, by designing an appropriate diffractive surface 7, the reflected light 3 is totally reflected inward on the light receiving surface 4 and can be efficiently taken into the light collecting device.

Similarly, as shown in FIG. 1B, when the light 1 is obliquely incident on the light receiving surface 4, the reflected light 3 is also reflected by the light receiving surface 4.
Can be designed to be totally reflected. FIG.
Even if the totally reflected light does not immediately enter the light receiving device 6 as in (c), the light can be totally reflected again on the light receiving surface 4 and confined in the light collecting device.

In the above description, the energy distribution of the light of each order when the incident light 2 is diffracted is not mentioned, but the shape of the surface of the diffraction surface viewed microscopically is shown in FIG.
In the case shown in (1), the component of the light of the order having a direction close to the specular reflection direction with respect to the diffraction surface 7 macroscopically becomes large. Therefore, when the light receiving surface 4 and the diffraction surface 7 are arranged in parallel, a large light component is reflected in the specular reflection direction. A blazed diffraction surface having a symmetrical shape shown in FIG. 2C or an asymmetrical shape shown in FIG.

Naturally, these diffractive surfaces 7 are macroscopically flat or curved, and have a periodic triangular shape having a repetitive pitch 9 in a microscopic range about the length of the wavelength of the light to be handled. Has lattice grooves. Further, in order to keep the diffraction efficiency high, it is necessary to use diffracted light of order 10 or less at most.
Therefore, the repetition pitch 9 of the diffraction surface needs to be about 10 times or less the wavelength of light in the medium. Further, it is desirable to use the third or lower order diffracted light.

As shown in FIG. 3A, a flat light receiving device 6 having a rectangular parallelepiped cross section is installed between the light receiving surface 4 and the diffraction surface 7 as shown in FIG. The space surrounded by the surface 4 is the structure filled with the medium 5 and FIG.
As shown in FIG. 1, there is a structure in which a cylindrical or spherical light receiving device 6 having a circular cross section is installed between the light receiving surface 4 and the diffraction surface 7.

FIG. 4A shows an example having a reflection curved surface 13. In this case, the light receiving device 6 having a rectangular parallelepiped cross section is installed on the light receiving surface side in parallel with the light receiving surface. The light reflected by the diffraction surface 7 enters the light receiving device 6 directly or by being reflected by the reflection curved surface 13. In such a shape, the reflection curved surface 13
May be a regular reflection surface, but if it is a diffraction surface, the light can be collected more effectively. Further, as shown in FIG. 4B, the light-collecting efficiency can be increased by arranging the diffraction surface 7 at an angle to the light-receiving surface 4.

FIG. 5A shows a structure in which an inclined diffraction surface 7 is arranged below a flat light receiving surface 4 and the direction 14 of the grating grooves on the diffraction surface is formed in a direction perpendicular to the inclination direction. In this structure, the surface 8 of the diffraction surface 7 has a microscopic cross section as shown in FIG. FIG. 5B shows a structure in which an inclined light receiving surface 4 is arranged above a flat diffraction surface 7. Thus, a high light-collecting efficiency can be obtained with a light-collecting device having a two-dimensional structure.

As shown in FIGS. 6A and 6B,
By forming the diffraction groove in the direction along the slope, a structure having both the light collection effect of the prism structure formed by the light receiving surface 4 and the slope 7 and the light collection effect by diffraction can be obtained. In this structure, the surface 8 of the diffraction surface 7 has a microscopic cross section as shown in FIG.

In these structures shown in FIGS. 5 and 6, the light-receiving device 6 has a plate-like shape. However, the light-receiving device 6 may have a cylindrical shape as shown in FIG. 7, or a sphere or a rectangular parallelepiped. Needless to say, these surfaces may have a secondary structure such as unevenness.

FIG. 8 shows a microscopic structure of the diffraction surface. In the case of a symmetrical configuration as in the structure of FIG. 8, the light incident on the right side 15 from the center is
And the light incident on the left side 16 from the center is the light receiving device 6 on the left side.
The light collection efficiency can be increased by entering the light.
For this purpose, it is desirable that the microscopic shape of the diffraction surface 8 be a shape in which individual asymmetric triangular shapes are symmetrically arranged on the left and right as shown in FIG.

Also, in the structure shown in FIG.
It is desirable to change the microscopic shape of the diffraction surface 8 from the center to the right and left sides of the apparatus.

As shown in FIG. 10A, when the diffraction groove is formed along the slope,
(B) As shown in (A-A 'cross-sectional shape of (a)), the blaze angle for guiding the diffracted light to the light receiving device 6 more effectively by changing the microscopic cross-sectional shape of the diffraction groove on the left and right of the center of the device. It is desirable that

FIG. 11 shows a structure in which the diffraction surface 7 has a wavy shape. In this case, the diffraction grooves 1 extend in the direction along the slope of the diffraction surface 7.
4 is desirable. Further, the light receiving device 6 is shown in FIG.
It may be installed in the direction along the wave shape of the diffraction surface 7 as shown in FIG. 11A, or may be installed in the direction perpendicular to it as shown in FIG. Further, it may be installed in a direction between them.

FIGS. 12A and 12B show a structure in which the cross section of the light receiving surface 4 is curved. As described above, the light receiving surface 4 of the light collector does not necessarily have to be flat. Further, the diffraction surface 7 may have a cross-sectional shape as shown in FIGS. A two-dimensional structure obtained by extending these structures in the front-rear direction of the drawing, or a light condensing device having a structure rotated around the rotation axis 30 is also conceivable. In these, the direction 14 of the diffraction groove may be a direction along the cross section of the diffraction surface 7 or a direction along the circumferential direction.

FIGS. 13A and 13B show examples in which diffraction grooves are two-dimensionally arranged when the diffraction surface is viewed from above. By arranging in this manner, light can be collected not only from the side surface of the light receiving device 6 but also from the periphery thereof toward the light receiving device 6, so that the light collection magnification can be increased. Further, as shown in FIG. 14, a large-area light-collecting module can be formed by modularizing a plurality of light-collecting devices. In addition, as shown in FIG. 15, by using a two-dimensional diffraction grating in which diffraction grooves 14 extending in different directions are combined, light incident around the light receiving device 6 can be effectively collected two-dimensionally.

FIG. 16 shows a sectional structure of the diffraction surface. In the simplest case, as shown in FIG. 16A, there is a structure having desired microscopic irregularities on the diffraction surface side of the medium 5 and a reflective material layer 17 made of metal or the like on the surface.

Further, as shown in FIG.
7 has a back surface protective layer 18 on the back surface, and FIG.
As described above, there is a structure in which a desired intermediate layer 19 is provided between the reflective material layer 17 and the diffraction surface side of the medium 5. This intermediate layer 19
Are an adhesive for bonding the reflective material layer 17 to the medium 5, a protective material for the reflective material layer 17, and a reflective material layer 17.
May be an intermediate layer having a desired refractive index in order to increase the reflectance.

FIG. 16D shows a case where the back surface of the medium 5 is microscopically flat and the intermediate layer 19 is flat on the medium 5 side. FIG. 16E shows a structure having an adhesive layer 20 between the intermediate layer 19 and the medium 5. Further, it is needless to say that the same light-collecting effect as described above can be obtained even in a structure in which an adhesive layer for bonding each layer or a protective material layer is appropriately added to these structures.

In the structure shown in FIG. 3A, since the light receiving device 6 is installed in the light collecting device, the procedure for installing the light receiving device 16 in the light collecting device when actually manufacturing the light receiving device 6 is described. It can be complicated. This can be avoided, for example, by using a structure in which the light receiving device is installed on the surface of the light collecting device as shown in FIG. In this case, a second regular reflection mirror 35 for guiding light to the surface of the light receiving device 6 is required. In addition, it is desirable to place a first regular reflection surface on the end surface where the light receiving device 6 is not installed. Further, by using a diffractive surface instead of the regular reflection surface, the incident angles of the light incident on the light receiving device can be made uniform, so that the light capturing rate of the light receiving device further increases.

Embodiment 1 FIG. 18 is a diagram showing a schematic configuration of a concentrating solar power generation device and a concentrating solar power generation module according to Embodiment 1 of the present invention. As shown in FIG. 18, the concentrating photovoltaic power generation device of the first embodiment was designed for the purpose of collecting sunlight into a cylindrical light receiving device to generate power.

First, the structure shown in FIG. 18A was used as the light collecting device. The diffractive surface 7 was formed by bonding a sheet having a structure in which an aluminum reflective member 17 as shown in FIG. The medium 5 was made of plastic.

Since the refractive index of the plastic is about 1.5, the incident angle when the incident light is reflected on the diffraction surface and re-enters the light receiving surface is arcsin (1 / 1.5) = 41.8 degrees or less. Need to be For this purpose, it is desirable that the blaze angle of the diffractive surface is larger than this. Therefore, in the first embodiment, the blaze angle is set to 45 degrees.

Sunlight has a wide wavelength range from ultraviolet light having a wavelength of about 300 nm to far-infrared light of several μm. In order to effectively condense this light by diffraction, it is necessary to design such that a sufficient diffraction angle can be obtained for short wavelength light for which it is difficult to increase the diffraction angle. The refractive index of the medium 5 is about 1.5
Therefore, the wavelength of light in the medium is 1.5 times the wavelength in air.
It's a fraction.

Since the shortest wavelength of the sunlight is about 400 nm, the second-order diffracted light is used for the shortest wavelength, and the repetition pitch of the microscopic unevenness of the diffraction surface 7 is set to the wavelength of 400 nm / 1.5 in plastic. It was 533 nm, which is twice as large.

An aluminum frame 21 was formed around a condensing device in which a plurality of such light receiving devices were connected, and a plastic support 12 was provided on the back surface. With this structure, a light-collecting module having a simple structure and high light-collecting efficiency can be formed as compared with a conventional light-collecting device using a slope having a large step.

(Embodiment 2) FIG. 19 is a view showing a schematic configuration of a concentrating photovoltaic power generation device and a concentrating photovoltaic power generation module according to a second embodiment of the present invention.

The concentrator photovoltaic power generator of the second embodiment is designed to collect sunlight into a light receiving device 6 composed of a solar cell using a plate-like crystalline silicon semiconductor and to extract electric power.

First, the structure shown in FIG. 19A was used as the light collecting device. The electric power generated by the light receiving device 6 composed of a solar cell was taken out from an electrode provided in a portion 31 continuous with the light receiving device 6. Glass was used for the medium 5. The refractive index of the medium 5 is about 1.5. Since the shortest wavelength of sunlight is about 400 nm, the shortest wavelength is 3
The repetition pitch of the microscopic irregularities on the diffraction surface 7 is set to 3 at a wavelength of 400 nm / 1.5 in the glass.
It was 800 nm twice.

A plurality of such light receiving devices are continuously arranged as shown in FIG.
1 was formed, and a surface cover glass 22 was further placed. The electric power generated by the light receiving device 6 is supplied to the first wiring 26 and the second wiring 2 through the first electrode 24 and the second electrode 25 provided on the portion 31 connected to the light receiving device located outside the diffraction surface.
7.

Further, on the back surface, a support 12 made of plastic and also for protecting the back surface and a protective material 28 for the electrode portion were provided. With this structure, macroscopic structure is simple,
In addition, a light-collecting module with high light-collecting efficiency could be formed. Solar cells include those using a semiconductor device and those using a photochemical reaction. Needless to say, the effects of the present invention do not depend on the type of solar cell.

(Embodiment 3) FIG. 20 is a view showing a schematic configuration of a concentrator photovoltaic power generation apparatus and a concentrator photovoltaic module according to a third embodiment of the present invention.

The concentrator photovoltaic power generator according to the third embodiment of the present invention is designed for the purpose of collecting sunlight into a light receiving device 6 comprising a solar cell using a plate-shaped crystalline silicon semiconductor and extracting electric power. did. First, FIG.
The structure shown in FIG. Electric power generated by the solar cell was taken out from an electrode provided on the back surface of the light receiving device 6. Glass was used for the medium 5. The refractive index of the medium 5 is about 1.5. Since the shortest wavelength of the sunlight is about 400 nm, the second-order diffracted light is used for the shortest wavelength, and the repetition pitch of the microscopic unevenness of the diffraction surface 7 is twice the wavelength of 400 nm / 1.5 in glass. 533 nm.

A plurality of such light receiving devices 6 are arranged continuously as shown in FIG. 20B, and an aluminum frame 21 is formed therearound. The electric power generated by the light receiving device 6 can be extracted from the first wiring 26 and the second wiring 27 through the first electrode 24 and the second electrode 25 provided on the back surface of the light receiving device. Further, a protective material 28 made of plastic was provided on the back surface. In this module, the first reflection surface 34 and the second reflection surface 35 were formed by one reflection plate using a double-sided reflection plate. With this structure, a light-collecting module with a simple macroscopic structure and high light-collecting efficiency could be formed. Solar cells include those using a semiconductor device and those using a photochemical reaction. Needless to say, the effects of the present invention do not depend on the type of solar cell.

The microscopic structure of the surface of the diffractive surface described so far does not need to completely match the illustrated shape, and may have irregularities that do not affect the diffraction. In addition, when actually manufacturing these surfaces, the shape may be deformed due to the limitation of machining accuracy, but the effects of the present invention can be obtained as long as the deformation does not hinder the diffraction of light. Needless to say. Further, these diffraction surfaces can be easily formed by, for example, forming replicas by an embossing method.

As described above, the present invention has been specifically described based on the embodiments (examples). However, the present invention is not limited to the above-described embodiments (examples), and various modifications may be made without departing from the scope of the invention. It goes without saying that it can be done.

[0054]

The effects obtained by typical inventions among the inventions disclosed in the present application are as follows.

(1) The macroscopic structure of the concentrator photovoltaic power generator can be simplified.

(2) The light collection efficiency can be increased while keeping the light use efficiency of the light concentrating solar power generation device high.

[Brief description of the drawings]

FIG. 1 is a diagram showing a schematic configuration of a concentrating solar power generation device according to an embodiment of the present invention.

FIG. 2 is a diagram showing a microscopically viewed shape of the surface of a diffraction surface of the concentrator photovoltaic power generation device of the present embodiment.

FIG. 3 is a diagram illustrating a schematic configuration of a concentrating solar power generation device according to another embodiment of the present invention.

FIG. 4 is a diagram illustrating a schematic configuration of a concentrating solar power generation device according to another embodiment of the present invention.

FIG. 5 is a diagram showing a schematic configuration of a concentrating solar power generation device according to another embodiment of the present invention.

FIG. 6 is a diagram illustrating a schematic configuration of a concentrating solar power generation device according to another embodiment of the present invention.

FIG. 7 is a diagram illustrating a schematic configuration of a concentrating solar power generation device according to another embodiment of the present invention.

FIG. 8 is a diagram showing a schematic configuration of a concentrating solar power generation device according to another embodiment of the present invention.

FIG. 9 is a diagram illustrating a schematic configuration of a concentrating solar power generation device according to another embodiment of the present invention.

FIG. 10 is a diagram illustrating a schematic configuration of a concentrating solar power generation device according to another embodiment of the present invention.

FIG. 11 is a diagram showing a schematic configuration of a concentrating solar power generation device according to another embodiment of the present invention.

FIG. 12 is a diagram illustrating a schematic configuration of a concentrating solar power generation device according to another embodiment of the present invention.

FIG. 13 is a diagram showing a schematic configuration when the diffraction surface of the concentrator photovoltaic power generation device according to the embodiment of the present invention is viewed from above.

FIG. 14 is a diagram showing a schematic configuration when the diffraction surface of the concentrator photovoltaic module of the embodiment of the present invention is viewed from above.

FIG. 15 is a diagram showing a schematic configuration when a diffraction surface of a concentrating solar power generation device according to another embodiment of the present invention is viewed from above.

FIG. 16 is a diagram illustrating a cross-sectional structure of a diffraction surface of the concentrating solar power generation device according to the embodiment of the present invention.

FIG. 17 is a diagram showing a schematic configuration of another concentrating solar power generation device of the present invention.

FIG. 18 is a diagram illustrating a schematic configuration of a concentrating solar power generation device and a concentrating solar power generation module according to a first embodiment of the present invention.

FIG. 19 is a diagram illustrating a schematic configuration of a concentrating solar power generation device and a concentrating solar power generation module according to a second embodiment of the present invention.

FIG. 20 is a diagram illustrating a schematic configuration of a concentrating solar power generation device and a concentrating solar power generation module according to a third embodiment of the present invention.

FIG. 21 is a diagram showing a schematic configuration of a conventional light collecting device.

[Explanation of symbols]

1: incident light, 2: light incident on the light condensing device, 3: reflected light,
4 light receiving surface, 5 medium, 6 light receiving device, 7 diffraction surface, 8
... Diffraction surface surface viewed microscopically, 9 ... Ditch groove pitch, 10 ...
Heat insulating layer, 11: cover, 12: support, 13: reflection curved surface, 14: diffraction groove direction, 15: right side, 16: left side, 17
... reflective material layer, 18 ... backside protective layer, 19 ... surface layer, 20
... adhesive layer, 21 ... frame, 22 ... cover glass, 23
... heat insulating plate, 24 ... first electrode, 25 ... second electrode, 26
... first wiring, 27 ... second wiring, 28 ... protective material, 29
... Rotation direction, 30 ... Rotation axis, 31 ... Continuous part of light receiving device located outside diffraction surface, 32 ... Specular reflection surface, 33 ... Incident angle, 34 ... First reflection surface, 35 ... Second reflection surface , 36
.. Light exiting from the exit surface, 37 ... exit surface.

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[Procedure amendment]

[Submission date] February 22, 1999

[Procedure amendment 1]

[Document name to be amended] Statement

[Correction target item name] Claim 4

[Correction method] Change

[Correction contents]

[Procedure amendment 2]

[Document name to be amended] Statement

[Correction target item name] 0012

[Correction method] Change

[Correction contents]

(4) The blazed diffraction surface has an asymmetric blaze angle.

 ────────────────────────────────────────────────── ─── Continuing on the front page (72) Inventor Yoshiaki Yazawa 1-280 Higashi Koigakubo, Kokubunji-shi, Tokyo Inside the Central Research Laboratory, Hitachi, Ltd. Inside the Central Research Laboratory of the Works (72) Inventor Ken Tsutsui 1-280 Higashi Koigakubo, Kokubunji-shi, Tokyo Inside the Central Research Laboratory of Hitachi, Ltd. (72) Inventor Junko Minemura 1-280 Higashi Koigakubo, Kokubunji-shi, Tokyo Inside Central Research Laboratory, Hitachi, Ltd.

Claims (7)

[Claims] 1. A medium, comprising: a light receiving surface; a diffraction surface; a medium filling a space between the light receiving surface and the diffraction surface; and a light receiving device having at least a part of the surface in contact with the medium. Wherein the refractive index is larger than the refractive index outside the light receiving surface. 2. The concentrator photovoltaic power generator according to claim 1, wherein the diffraction surface is a reflection diffractive surface. 3. The concentrator photovoltaic power generation device according to claim 2, wherein the reflection diffraction surface is a blazed diffraction surface. 4. The concentrator photovoltaic power generator according to claim 3, wherein the blazed diffraction surface has a blaze angle that is symmetrical to the outside. 5. The concentrator photovoltaic power generation device according to claim 4, wherein said blazed diffraction surface has a structure arranged symmetrically on the left and right sides of the diffraction surface. . 6. A concentrating photovoltaic power generation module, wherein a plurality of the concentrating photovoltaic power generation devices according to claim 1 are modularized. 7. The concentrating solar power generation module according to claim 6, wherein the medium is continuous between the plurality of concentrating solar power generation devices. Power generation module.