MULTI-JUNCTION SOLAR CELL AND MANUFACTURING METHOD OF THE SAME

Abstract

Provided is a multi-junction solar cell in which two or more absorption layers having different bandgaps are stacked on one another. The multi-junction solar cell includes a first cell including a first absorption layer, and a second cell electrically connected in series onto the first cell, wherein the second cell includes a second absorption layer having a higher bandgap compared to the first absorption layer, and a plurality of recesses penetrating through the second absorption layer.

Claims

1. A multi-junction solar cell in which two or more absorption layers having different bandgaps are stacked on one another, the multi-junction solar cell comprising: a first cell comprising a first absorption layer; and a second cell electrically connected in series onto the first cell, wherein the second cell comprises: a second absorption layer having a higher bandgap compared to the first absorption layer; and a plurality of recesses penetrating through the second absorption layer.

2. The multi-junction solar cell of claim 1, wherein the first cell comprises a silicon (Si) solar cell.

3. The multi-junction solar cell of claim 1, wherein the second cell comprises a chalcogenide-based solar cell.

4. The multi-junction solar cell of claim 1, wherein the first and second cells are stacked on one another by a first transparent electrode layer, and wherein at least parts of the first transparent electrode layer or at least parts of an emitter layer are exposed by the plurality of recesses.

5. The multi-junction solar cell of claim 1, wherein the plurality of recesses are designed to have a diameter in such a manner that the first and second cells generate equal photocurrents.

6. The multi-junction solar cell of claim 1, wherein the plurality of recesses penetrate through both of a buffer layer generated on the second absorption layer, and a second transparent electrode layer generated on the buffer layer, and wherein a removal area of the second transparent electrode layer is greater than or equal to a removal area of the second absorption layer.

7. A method of manufacturing a multi-junction solar cell in which two or more absorption layers having different bandgaps are stacked on one another, the method comprising: generating, on a back electrode, a first cell comprising a first absorption layer; and generating a second cell electrically connected in series onto the first cell, wherein the generating of the second cell comprises: generating a second absorption layer having a higher bandgap compared to the first absorption layer; and generating a plurality of recesses penetrating through the second absorption layer.

8. The method of claim 7, wherein the generating of the plurality of recesses comprises: irradiating laser beams having a wavelength band absorbed by the second absorption layer, onto at least partial regions of a buffer layer and a second transparent electrode layer sequentially stacked on the second absorption layer, to remove the buffer layer and the second transparent electrode layer; and irradiating the laser beams onto the second absorption layer exposed by the removed buffer layer and the second transparent electrode layer, to remove the second absorption layer.

9. The method of claim 8, wherein the laser beams have a wavelength band equal to or smaller than 700 nm.

10. The method of claim 8, wherein the laser beams have a wavelength band equal to or smaller than 550 nm.

11. The method of claim 8, wherein the laser beams comprise pulsed laser beams having a pulse range of 2 picoseconds (ps) to 100 ps.

12. The method of claim 7, wherein the generating of the plurality of recesses comprises irradiating laser beams having a wavelength band transmitted through the second absorption layer, onto at least partial regions of a buffer layer and a second transparent electrode layer sequentially stacked on the second absorption layer, to remove the second absorption layer, the buffer layer, and the second transparent electrode layer.

13. The method of claim 12, wherein the laser beams have a wavelength band equal to or greater than 800 nm.

14. The method of claim 12, wherein the laser beams have a wavelength band equal to or greater than 950 nm.

15. The method of claim 7, wherein the generating of the plurality of recesses comprises: generating and patterning a first transparent electrode layer on the first cell before the second absorption layer is generated; sequentially depositing the second absorption layer, a buffer layer, and a second transparent electrode layer on the patterned first transparent electrode layer and the first cell exposed due to the patterning; and generating the plurality of recesses by selectively removing the second absorption layer by de-bonding an interface between the first cell from the second absorption layer due to a process performed in the sequential depositing.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0029] The above and other features and advantages of the present invention will become more apparent by describing in detail embodiments thereof with reference to the attached drawings in which:

[0030] FIGS. 1A and 1B are a cross-sectional view and a plan view of a multi-junction solar cell according to an embodiment of the present invention;

[0031] FIGS. 2A and 2B are graphs showing current density-voltage curves of multi-junction solar cells according to a comparative example and an embodiment of the present invention;

[0032] FIGS. 3A to 3C are cross-sectional views for describing a method of manufacturing a multi-junction solar cell, according to an embodiment of the present invention;

[0033] FIG. 4 is a cross-sectional view for describing a method of manufacturing a multi-junction solar cell, according to another embodiment of the present invention;

[0034] FIG. 5 is a cross-sectional view for describing a method of manufacturing a multi-junction solar cell, according to another embodiment of the present invention;

[0035] FIG. 6 is a graph showing external quantum efficiency (EQE) and reflectance spectrums of a multi-junction solar cell sample according to a comparative example;

[0036] FIG. 7 shows graphs showing transmittance, reflectance, and absorbance spectrums of an indium tin oxide (ITO) thin-film (thickness: 183 nm);

[0037] FIGS. 8A to 8G are images of a silicon (Si)/ITO/CuGaSe.sub.2 (CGSe) structure processed using picosecond (ps) pulsed laser beams irradiated at different average powers;

[0038] FIGS. 9A and 9B are a photographic image and a cross-sectional view of a multi-junction solar cell sample according to a test example of the present invention; and

[0039] FIGS. 10A and 10B are a cross-sectional view showing a cell structure of a general hybrid multi-junction solar cell, and a graph showing EQE spectrums of a top cell and a bottom cell.

DETAILED DESCRIPTION

[0040] Hereinafter, the present invention will be described in detail by explaining embodiments of the invention with reference to the attached drawings. The invention may, however, be embodied in many different forms and should not be construed as being limited to the embodiments set forth herein; rather, these embodiments are provided so that this disclosure will be thorough and complete, and will fully convey the concept of the invention to one of ordinary skill in the art.

[0041] As used herein, a first cell refers to a bottom cell of a multi-junction solar cell, and a second cell refers to a top cell thereof.

[0042] FIGS. 1A and 1B are a cross-sectional view and a plan view of a multi-junction solar cell 100 according to an embodiment of the present invention.

[0043] Referring to FIG. 1A, the multi-junction solar cell 100 in which two or more absorption layers (e.g., first and second absorption layers 20 and 50) having different bandgaps are stacked on one another includes a first cell 110 including the first absorption layer 20, and a second cell 120 electrically connected in series onto the first cell 110. The second cell 120 includes the second absorption layer 50 having a higher bandgap compared to the first absorption layer 20, and a plurality of recesses 90 penetrating through the second absorption layer 50. The first and second cells 110 and 120 are stacked on one another by a first transparent electrode layer 40.

[0044] For example, the first cell 110 includes a silicon (Si) solar cell. The second cell 120 may include a chalcogenide-based solar cell.

[0045] A back electrode 10 including aluminum (Al) or silver (Ag) is provided on a surface of the first cell 110, and the other surface thereof is n-doped and then the first transparent electrode layer 40 is deposited thereon. A selenium (Se)-, sulfur (S)-, or tellurium (Te)-based chalcogenide-based absorption layer serving as the second absorption layer 50, a buffer layer 60, and a second transparent electrode layer 70 are sequentially deposited thereon to manufacture the multi-junction solar cell 100. Herein, the first cell 110 may serve as a p-type Si solar cell or an n-type Si solar cell depending on the type of doping. Although not shown in FIG. 1A, at least one surface of the first cell 110 may be textured to scatter light.

[0046] The first transparent electrode layer 40 may be made of, for example, indium tin oxide (ITO), fluorine-doped tin oxide (FTO), aluminum-doped zinc oxide (AZO), or boron-doped zinc oxide (BZO), and have a layered structure of two or more oxide thin-films. The first transparent electrode layer 40 may have a thickness equal to or less than 100 nm, preferably, a thickness equal to or less than 50 nm, and more preferably, a thickness equal to or less than 20 nm. The second transparent electrode layer 70 may use the same material as the first transparent electrode layer 40. In some cases, the second transparent electrode layer 70 may be made of one of the above-listed materials.

[0047] The second absorption layer 50 may include copper (Cu), silver (Ag), gallium (Ga), or indium (In), and have a bandgap of 1.4 eV to 1.7 eV and a thickness equal to or greater than 0.5 m, and preferably, a thickness equal to or greater than 1.0 m.

[0048] Thereafter, at least a part of the second absorption layer 50, the buffer layer 60, and the second transparent electrode layer 70 is removed such that solar light is not absorbed into the second cell 120 but is absorbed into the first cell 110 in a region corresponding to the removed part.

[0049] Referring to FIG. 1B, the plurality of recesses 90 may have a circular shape or any other shape and may be aligned at equal intervals. Herein, the plurality of recesses 90 may have a diameter D designed in such a manner that the first and second cells 110 and 120 generate equal photocurrents. The plurality of recesses 90 penetrate through both of the buffer layer 60 generated on the second absorption layer 50, and the second transparent electrode layer 70 generated on the buffer layer 60.

[0050] The first transparent electrode layer 40 is exposed by the plurality of recesses 90. However, depending on a manufacturing process, the first transparent electrode layer 40 may be partially or completely removed by the plurality of recesses 90. When the first transparent electrode layer 40 is partially removed, remaining parts of the first transparent electrode layer 40 are exposed. When the first transparent electrode layer 40 is completely removed, parts of an emitter layer 30 are exposed. In this case, to constantly maintain photocurrent collection efficiency of the first cell 110 in the recesses 90, at least of an initially deposited thickness of the Si doping layer, i.e., the emitter layer 30, needs to be remained.

[0051] FIGS. 2A and 2B are graphs showing current density-voltage curves of multi-junction solar cells according to a comparative example and an embodiment of the present invention.

[0052] Referring to FIG. 2A, when a photocurrent j.sub.t of a top cell is higher than a photocurrent j.sub.b of a bottom cell, a photocurrent of a multi-junction solar cell is limited to the lower photocurrent j.sub.b due to serial connection between the two solar cells. On the other hand, referring to FIG. 2B, when an absorbance region of a top cell (i.e., a second cell) is removed by a certain fraction f, absorbance of the top cell is reduced and thus a photocurrent thereof is reduced, and absorbance of a bottom cell (i.e., a first cell) is increased correspondingly and thus a photocurrent thereof is increased.

[0053] The photocurrents after the absorbance region of the top cell is removed by f may be determined as shown in Expressions 1 and 2.

Top cell: j.sub.t(1f)<Expression 1>

Bottom cell: j.sub.b(1f)+j.sub.b.sup.sf<Expression 2>

[0054] Herein, j.sub.b.sup.s denotes a photocurrent of the bottom cell (i.e., the first cell) as a single cell. The photocurrent of the top cell needs to be equal to the photocurrent of the bottom cell in Expressions 1 and 2, the fraction f of the removal region may be determined as shown in Equation 3.

f=(j.sub.tj.sub.b)/(j.sub.tj.sub.b+j.sub.b.sup.s)<Equation 3>

[0055] As such, a photocurrent of a multi-junction solar cell is increased from j.sub.b to j* and thus photoelectric conversion efficiency is increased.

[0056] FIGS. 3A to 3C are cross-sectional views for describing a method of manufacturing a multi-junction solar cell 200, according to an embodiment of the present invention.

[0057] Referring to FIG. 3A, a first recess 92 is generated by irradiating picosecond (ps) pulsed laser beams having a wavelength band equal to or lower than 700 nm corresponding to a short-wavelength band absorbed by the second absorption layer 50, and preferably, a wavelength band equal to or lower than 550 nm, e.g., 532 nm, onto a region D1 of the second transparent electrode layer 70. Laser beams Laser1 may pass through the second transparent electrode layer 70, be locally absorbed into the surface of the second absorption layer 50, and induce thermal expansion to selectively remove the second transparent electrode layer 70. A removal area of the second transparent electrode layer 70 is greater than a removal area of the second absorption layer 50 because a laser beam condition for removing the second transparent electrode layer 70 is different from a laser beam condition for removing the second absorption layer 50 and damage of the emitter layer 30 of a first cell 210 may be caused using the latter laser beam condition.

[0058] Referring to FIGS. 3B and 3C, a second recess 94 is generated by thermally vaporizing and removing the second absorption layer 50 by repeatedly irradiating a plurality of low-energy pulsed laser beams onto a region D2 smaller than the region D1.

[0059] In this case, the first transparent electrode layer 40 under the second absorption layer 50 has a very low absorbance at a wavelength band of 532 nm, and the emitter layer 30 thereunder also has a low absorbance. Therefore, by repeatedly irradiating low-energy laser beams, a third recess 96 may be generated by removing the second absorption layer 50 without damaging the first transparent electrode layer 40 and the emitter layer 30. In this case, the first transparent electrode layer 40 may be partially or completely removed.

[0060] Vaporization of the second absorption layer 50 may be induced by irradiating low-energy laser beams and the second absorption layer 50 may be gradually removed as illustrated in FIGS. 3A to 3C by repeatedly irradiating the low-energy laser beams onto the same region. When the removal of the second absorption layer 50 is completed as illustrated in FIG. 3C, the irradiated laser beams pass through the first transparent electrode layer 40 and are absorbed by the first absorption layer 20. An absorption coefficient of the first absorption layer 20 is remarkably lower than that of the second absorption layer 50 (< 1/50) and thus damage of the first absorption layer 20 by the laser beams may be avoided. In some cases, delamination of the first transparent electrode layer 40 may be caused by thermal expansion due to the laser beams absorbed by the first absorption layer 20. The low-energy laser beams may minimize interference of a vaporized material.

[0061] Herein, the region D2 may have a diameter similar to that of the laser beams when the laser beams are simply overlapped, or have a diameter greater than that of the laser beams when the laser beams are irradiated while moving in a spiral shape. The laser beams may have a pulse range of 2 ps to 100 ps and a pulse overlap ratio of 80% to 100%.

[0062] When short-wavelength ps pulsed laser beams are used, by removing the region D1 of the second transparent electrode layer 70 to be larger than and prior to removal of the region D2 of the second absorption layer 50, damage of the emitter layer 30 of the bottom cell due to laser heating may be prevented.

[0063] FIG. 4 is a cross-sectional view for describing a method of manufacturing a multi-junction solar cell 300, according to another embodiment of the present invention.

[0064] Referring to FIG. 4, long-wavelength pulsed laser beams Laser2 are irradiated onto the second transparent electrode layer 70. The long-wavelength pulsed laser beams Laser2 pass sequentially through the second transparent electrode layer 70, the buffer layer 60, and the second absorption layer 50 and are partially absorbed into the first transparent electrode layer 40. As a result, due to rapid thermal expansion of the first transparent electrode layer 40, impact may be generated at an interface between the first transparent electrode layer 40 and the second absorption layer 50, the second absorption layer 50, the buffer layer 60, and the second transparent electrode layer 70 may be delaminated, and thus the second cell 320 may be partially removed to generate the plurality of recesses 90. In this case, the first transparent electrode layer 40 may be partially or completely removed.

[0065] The laser beams may include ps or nanosecond (ns) pulsed laser beams having a wavelength band equal to or higher than 800 nm corresponding to a long-wavelength band not absorbed by the second absorption layer 50, and preferably, a wavelength band equal to or higher than 950 nm, e.g., 1064 nm.

[0066] Laser beams having a certain or higher energy level and a certain or larger diameter are used to cause thermal impact at the interface between the first transparent electrode layer 40 and the second absorption layer 50 and to lift off thin-film materials on the first transparent electrode layer 40 in a single process. In this case, the laser beams may have a diameter equal to or greater than 50 m, and preferably, a diameter equal to or greater than 70 m. When the laser beams have a sufficiently large diameter, excellent lift-off performance may be achieved and a production speed may be increased based on a high-speed process of 1 m/s to 20 m/s.

[0067] FIG. 5 is a cross-sectional view for describing a method of manufacturing a multi-junction solar cell 400, according to another embodiment of the present invention.

[0068] Referring to FIG. 5, when an electrode pattern 42 is generated by selectively removing the first transparent electrode layer 40 and then the second absorption layer 50, the buffer layer 60, and the second transparent electrode layer 70 are generated thereon, the first transparent electrode layer 40 achieves a high interfacial bonding strength with the second absorption layer 50 but a top surface of the emitter layer 30 exposed due to removal of the first transparent electrode layer 40 has a very low interfacial bonding strength. Due to various types of stress or artificial vibration or heating in subsequent processes, the interface between the emitter layer 30 and the second absorption layer 50 is easily selectively separated and removed and the plurality of recesses 90 are generated.

[0069] Test examples will now be described to promote understanding of the present invention. However, the following test examples are merely to promote understanding of the present invention and the present invention is not limited thereto.

[0070] An ITO transparent electrode layer is generated on a p-type Si-based solar cell in which a back electrode, a first absorption layer, and an emitter layer are sequentially stacked on one another, and a multi-junction solar cell sample is manufactured by sequentially depositing CuGaSe.sub.2 (CGSe), CdS, and AZO thereon. Thereafter, external quantum efficiency (EQE) and reflectance spectrums of a top cell and a bottom cell are measured and compared. In addition, reflectance, transmittance, and absorbance spectrums of the ITO thin-film are measured and compared.

[0071] FIG. 6 is a graph showing EQE and reflectance spectrums of a multi-junction solar cell sample according to a comparative example.

[0072] Referring to FIG. 6, a maximum quantum efficiency (QE) of a CGSe absorption layer is about 80% and a maximum QE of a Si solar cell is also about 80%. However, loss occurs due to strong reflection interference. When compared with surface reflectances, the reflectance is maintained very low at a wavelength band absorbed by the CGSe absorption layer, but reflection loss is greatly increased at a wavelength band equal to or lower than a CGSe bandgap.

[0073] That is, in spite of a sufficient absorbance, QE loss of CGSe is inferred as being caused by large electrical collection loss. On the other hand, QE loss of the Si solar cell is inferred as being mostly caused by absorption loss due to surface and interface reflection. Therefore, a technology capable of suppressing long-wavelength reflection loss need to be developed. However, referring back to FIG. 1B, even when performance of each solar cell is improved, a photocurrent of the Si solar cell in the combination of the Si solar cell and the CGSe solar cell is inevitably low, photocurrent matching is required.

[0074] FIG. 7 shows graphs showing transmittance, reflectance, and absorbance spectrums of an ITO thin-film (thickness: 183 nm).

[0075] Referring to FIG. 7, the ITO thin-film has a very low absorbance at a wavelength band of 532 nm and has a high absorbance at a long-wavelength band equal to or higher than 900 nm. Therefore, when laser beams of the wavelength band of 532 nm are irradiated, the absorbance of the ITO thin-film is remarkably lower than that of a CGSe absorption layer and thus loss of a Si solar cell under the ITO thin-film may be suppressed in a process of vaporizing the CGSe absorption layer based on laser heating. On the other hand, using laser beams of the long-wavelength band, the absorbances of the ITO thin-film and the Si solar cell thereunder are higher than that of the CGSe absorption layer and thus the CGSe absorption layer/a buffer layer/an AZO thin-film may be removed based on interface heating using laser beams.

[0076] FIGS. 8A to 8G are images of a Si/ITO/CGSe structure processed using ps pulsed laser beams irradiated at different average powers. FIG. 8A shows optical microscopic images, and FIGS. 8B to 8G show scanning electron microscopic images.

[0077] FIGS. 8A to 8G are optical microscopic and scanning electron microscopic images of a Si/ITO/CGSe structure processed by irradiating ps laser beams having a wavelength of 532 nm, onto the CGSe absorption layer. Laser beams having a frequency of 100 kHz and a pulse width of 12 ps are focused to 23.6 m and are irradiated by varying average power from 59 mW to 173.7 mW while moving at a speed of 50 mm/s. A pulse overlap ratio of the laser beams is about 98% on the basis of the distance between pulse centers. A removal amount of the CGSe absorption layer is increased as the average power is increased, and the CGSe absorption layer is removed to completely expose ITO at 98.3 mW (0.225 J/cm.sup.2). As the power is increased, damage of the ITO thin-film is slightly increased and ITO starts to be delaminated at 173.7 mW (0.397 J/cm.sup.2). The CGSe absorption layer is selectively removed without damage of ITO at a laser power density ranging from 0.225 J/cm.sup.2 to 0.35 J/cm.sup.2. Although processing conditions may slightly very depending on the diameter and the pulse overlap ratio of the laser beams, a sufficient laser process range may be ensured.

[0078] FIGS. 9A and 9B are a photographic image and a cross-sectional view of a multi-junction solar cell sample 500 according to a test example of the present invention. FIG. 9A is a photographic image of the sample 500 manufactured by selectively etching and patterning an ITO thin-film deposited on a Si solar cell, and then generating a CGSe absorption layer thereon, and FIG. 9B is a cross-sectional view of the sample 500 cut along line A-A of FIG. 9A.

[0079] Referring to FIGS. 9A and 9B, although any external force is not applied after a subsequent process is completed, the CGSe absorption layer is delaminated in a large area of a region where the ITO thin-film is removed to expose Si, which means a Si/CGSe interface is very vulnerable. Using the above-described feature, a top cell may be selectively removed by merely patterning the ITO thin-film without a laser process or a photolithography process.

[0080] Using the above-described method of manufacturing a multi-junction solar cell, according to the present invention, a high-efficiency hybrid multi-junction solar cell may be manufactured at a high production speed by controlling photocurrents of a top cell and a bottom cell to be equal. However, the scope of the present invention is not limited to the above-described effect.

[0081] While the present invention has been particularly shown and described with reference to embodiments thereof, it will be understood by one of ordinary skill in the art that various changes in form and details may be made therein without departing from the scope of the present invention as defined by the following claims.