CN113571594A - Copper indium gallium selenide battery and manufacturing method thereof - Google Patents

Copper indium gallium selenide battery and manufacturing method thereof Download PDF

Info

Publication number
CN113571594A
CN113571594A CN202110805785.XA CN202110805785A CN113571594A CN 113571594 A CN113571594 A CN 113571594A CN 202110805785 A CN202110805785 A CN 202110805785A CN 113571594 A CN113571594 A CN 113571594A
Authority
CN
China
Prior art keywords
cigs
layer
band gap
ggi
gradient
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN202110805785.XA
Other languages
Chinese (zh)
Other versions
CN113571594B (en
Inventor
刘武
宋丹丹
朱成皖
李昊天
赵谡玲
乔泊
徐征
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Beijing Jiaotong University
Original Assignee
Beijing Jiaotong University
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Beijing Jiaotong University filed Critical Beijing Jiaotong University
Priority to CN202110805785.XA priority Critical patent/CN113571594B/en
Publication of CN113571594A publication Critical patent/CN113571594A/en
Application granted granted Critical
Publication of CN113571594B publication Critical patent/CN113571594B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/04Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof adapted as photovoltaic [PV] conversion devices
    • H01L31/06Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof adapted as photovoltaic [PV] conversion devices characterised by at least one potential-jump barrier or surface barrier
    • H01L31/072Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof adapted as photovoltaic [PV] conversion devices characterised by at least one potential-jump barrier or surface barrier the potential barriers being only of the PN heterojunction type
    • H01L31/0749Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof adapted as photovoltaic [PV] conversion devices characterised by at least one potential-jump barrier or surface barrier the potential barriers being only of the PN heterojunction type including a AIBIIICVI compound, e.g. CdS/CulnSe2 [CIS] heterojunction solar cells
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/02Details
    • H01L31/0224Electrodes
    • H01L31/022466Electrodes made of transparent conductive layers, e.g. TCO, ITO layers
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/0248Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by their semiconductor bodies
    • H01L31/0256Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by their semiconductor bodies characterised by the material
    • H01L31/0264Inorganic materials
    • H01L31/032Inorganic materials including, apart from doping materials or other impurities, only compounds not provided for in groups H01L31/0272 - H01L31/0312
    • H01L31/0322Inorganic materials including, apart from doping materials or other impurities, only compounds not provided for in groups H01L31/0272 - H01L31/0312 comprising only AIBIIICVI chalcopyrite compounds, e.g. Cu In Se2, Cu Ga Se2, Cu In Ga Se2
    • H01L31/0323Inorganic materials including, apart from doping materials or other impurities, only compounds not provided for in groups H01L31/0272 - H01L31/0312 comprising only AIBIIICVI chalcopyrite compounds, e.g. Cu In Se2, Cu Ga Se2, Cu In Ga Se2 characterised by the doping material
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/0248Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by their semiconductor bodies
    • H01L31/036Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by their semiconductor bodies characterised by their crystalline structure or particular orientation of the crystalline planes
    • H01L31/0392Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by their semiconductor bodies characterised by their crystalline structure or particular orientation of the crystalline planes including thin films deposited on metallic or insulating substrates ; characterised by specific substrate materials or substrate features or by the presence of intermediate layers, e.g. barrier layers, on the substrate
    • H01L31/03923Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by their semiconductor bodies characterised by their crystalline structure or particular orientation of the crystalline planes including thin films deposited on metallic or insulating substrates ; characterised by specific substrate materials or substrate features or by the presence of intermediate layers, e.g. barrier layers, on the substrate including AIBIIICVI compound materials, e.g. CIS, CIGS
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/18Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof
    • H01L31/1884Manufacture of transparent electrodes, e.g. TCO, ITO
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/50Photovoltaic [PV] energy
    • Y02E10/541CuInSe2 material PV cells
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02PCLIMATE CHANGE MITIGATION TECHNOLOGIES IN THE PRODUCTION OR PROCESSING OF GOODS
    • Y02P70/00Climate change mitigation technologies in the production process for final industrial or consumer products
    • Y02P70/50Manufacturing or production processes characterised by the final manufactured product

Abstract

The invention provides a CIGS battery and a manufacturing method thereof, wherein the CIGS battery comprises a CIGS film, the CIGS film is from the front surface close to the side of a buffer layer to the rear surface close to the side of a back electrode, the Ga gradient comprises two minimum values, and the GGI value and the band gap gradient of the CIGS film are both in W-shaped distribution. Effectively improves the open-circuit voltage VOCImproving carrier collection efficiency and short-circuit current JSCMeanwhile, the W-shaped gradient contains two areas with low GGI, so that the absorption probability of long-wavelength photons is increased.

Description

Copper indium gallium selenide battery and manufacturing method thereof
Technical Field
The invention relates to the technical field of solar cells, in particular to a copper indium gallium selenide cell and a manufacturing method thereof.
Background
In the process of depositing the CIGS thin film by the co-evaporation method, the properties of the thin film material such as uniformity, crystal structure and the like are related to the evaporation rate of the constituent elements. Different kinds of gradient distribution are realized, and the longitudinal distribution of the Ga content in the film can be controlled by changing the evaporation rate of Ga element by changing the evaporation temperature of a Ga source under the condition that the rest evaporation conditions are the same. In a cigs solar cell, the deep band gap variation due to the variation of the Ga content (GGI, i.e., Ga/(Ga + In)) ratio is generally referred to as a Ga gradient. The absorption band gap of the CIGS thin film can change according to a fixed proportion along with the proportion of Ga content to form a band gap gradient, and the change of the Ga gradient in the thin film can bring about the change of the band gap gradient. The GGI gradient distribution categories currently fall into three main categories, flat gradient, single gradient, and "V" double gradient.
Figure 1 shows three band gap curves for a Copper Indium Gallium Selenide (CIGS) cell. The flat gradient bandgap profile, where (a) denotes, is limited in the drift of photo-generated electrons generated in other regions than electrons generated in or near the depletion layer due to the zero gradient of the potential. In contrast, in the case where a band gap gradient exists as shown in (b), (c), photoelectrons can easily reach the depletion region, thereby improving carrier collection efficiency. At present, the copper indium gallium selenide solar cell with a V-shaped double-gradient band gap structure as shown in (c) has the highest efficiency: the increase of the band gaps on the surface and the back surface inhibits the recombination of the absorption region of the battery and effectively improves the open-circuit voltage VOC(ii) a The middle narrow band gap can reduce the spectral response loss of the battery in a long wave band, so that the short-circuit current J is enabledSCThe loss of (2) is minimized.
In the optimization process of the gradient distribution of the band gap of the CIGS battery from a flat band gap to a single band gap to a V-shaped double band gap, the gain optimization of the battery performance is improved all the time. However, in the prior art, compared with the Shockley-Queisser (S-Q) efficiency limit, the loss of the open-circuit voltage of the CIGS battery still reaches more than 350mV, the short-circuit current loss is also the largest in the third-generation thin-film solar battery and reaches more than 10%, and the battery performance also has a great promotion space.
Disclosure of Invention
The invention provides a copper indium gallium selenide battery and a manufacturing method thereof, which aim to solve the defects in the prior art.
In order to achieve the purpose, the invention adopts the following technical scheme.
A CIGS cell includes a CIGS film from a front surface near a buffer layer side to a rear surface near a back electrode side, a Ga gradient includes two minima, and both a GGI value and a band gap gradient of the CIGS film exhibit a W-type distribution.
Preferably, the cell comprises a substrate, a back electrode, a CIGS thin film, a buffer layer, an electron transport layer, and a transparent front electrode.
Preferably, the GGI value of the front surface of the CIGS thin film is 0.25-0.65, and the band gap of the front surface of the CIGS thin film and the conduction band offset value CBO of the n-type buffer layer of the CIGS cell are kept at-0.05-0.1 eV.
Preferably, the minimum value of GGI of the band gap gradient is 0.1-0.5.
Preferably, the rear surface GGI value of the CIGS thin film is 0.5-1.
Another aspect of the present invention provides a method for manufacturing the copper indium gallium selenide battery, including:
preparing a molybdenum electrode layer with the thickness of 100-1000 nanometers on a battery substrate by adopting a direct-current magnetron sputtering method;
depositing a CIGS thin film with the thickness of 0.5-5 microns on the molybdenum electrode layer by adopting a three-step co-evaporation method; GGI is regulated and controlled by controlling the evaporation rates of Ga and In sources at different stages, so that the band gap of CIGS is regulated to form W-shaped band gap gradient distribution;
performing alkali metal post-treatment on CIGS by using NaF, KF, RbF or CsF alkali metal source materials;
depositing an n-type thin film with the thickness of 10-100 nanometers on the CIGS layer subjected to the alkali metal post-treatment by adopting a chemical bath deposition method to serve as a buffer layer;
preparing a zinc oxide layer with the thickness of 50-500 nanometers on the buffer layer by adopting a direct-current magnetron sputtering method to serve as an electron transmission layer;
and preparing an AZO layer with the thickness of 150-1000 nanometers on the electron transmission layer by adopting a direct current magnetron sputtering method to serve as a transparent front electrode.
Preferably, the AZO is aluminum-doped zinc oxide.
The technical scheme provided by the CIGS battery and the manufacturing method thereof can be seen that the invention optimizes the gradient distribution of the band gap aiming at the problem of device performance loss in the conventional CIGS battery, under the condition that the total content of Ga in the CIGS film is the same, the GGI value in the CIGS film is distributed from the front surface close to the buffer layer side to the rear surface close to the back electrode side, the Ga gradient comprises two minimum values, the GGI and the band gap gradient of the CIGS film are in W-shaped distribution, so that the battery is relatively higher than the conventional flat gradient, single gradient and V-shaped double gradient, the GGI value of the front surface and the GGI value of the rear surface of the CIGS film, the combination of the W-shaped gradient on the wide band gap of the CIGS surface and the wide band gap of the back surface of the CIGS film is inhibited, and the open-circuit voltage V is effectively improvedOC(ii) a The increase of the GGI value of the rear surface forms a high back electric field, improves the carrier collection efficiency and improves the short-circuit current JSCAnd an open circuit voltage VOCMeanwhile, the W-shaped gradient contains two areas with low GGI, so that the absorption probability of long-wavelength photons is increased.
Additional aspects and advantages of the invention will be set forth in part in the description which follows, and in part will be obvious from the description, or may be learned by practice of the invention.
Drawings
In order to more clearly illustrate the technical solutions of the embodiments of the present invention, the drawings needed to be used in the description of the embodiments are briefly introduced below, and it is obvious that the drawings in the following description are only some embodiments of the present invention, and it is obvious for those skilled in the art to obtain other drawings based on these drawings without creative efforts.
Fig. 1 is a schematic diagram of three band gap curves for a Copper Indium Gallium Selenide (CIGS) cell;
FIG. 2 is a schematic diagram of an example CIGS thin film band gap gradient design of a CIGS thin film;
fig. 3 is a flowchart of a method for manufacturing a copper indium gallium selenide cell according to an embodiment.
Detailed Description
Reference will now be made in detail to embodiments of the present invention, examples of which are illustrated in the accompanying drawings, wherein like reference numerals refer to the same or similar elements or elements having the same or similar function throughout. The embodiments described below with reference to the accompanying drawings are illustrative only for the purpose of explaining the present invention, and are not to be construed as limiting the present invention.
As used herein, the singular forms "a", "an", "the" and "the" are intended to include the plural forms as well, unless the context clearly indicates otherwise. It will be further understood that the terms "comprises" and/or "comprising," when used in this specification, specify the presence of stated features, integers, steps, operations, elements, and/or components, but do not preclude the presence or addition of one or more other features, integers, steps, operations, elements, components, and/or groups thereof. It should be understood that "connected" or "coupled" as used herein may include wirelessly connected or coupled. As used herein, the term "and/or" includes any and all combinations of one or more of the associated listed items.
It will be understood by those skilled in the art that, unless otherwise defined, all terms (including technical and scientific terms) used herein have the same meaning as commonly understood by one of ordinary skill in the art to which this invention belongs. It will be further understood that terms, such as those defined in commonly used dictionaries, should be interpreted as having a meaning that is consistent with their meaning in the context of the prior art and will not be interpreted in an idealized or overly formal sense unless expressly so defined herein.
For the convenience of understanding of the embodiments of the present invention, the following description will be further explained by taking specific embodiments as examples with reference to the drawings, and the embodiments of the present invention are not limited thereto.
Examples
The present embodiment provides a CIGS cell, including a CIGS thin film, fig. 2 is a schematic diagram illustrating a design of a band gap gradient of the CIGS thin film of the CIGS cell of the present embodiment, referring to fig. 2, a Ga gradient includes two minimum values from a front surface near a buffer layer side to a rear surface near a back electrode side, and both a GGI value and a band gap gradient of the CIGS thin film exhibit a "W" type distribution. GGI is Ga content, GGI ═ Ga/(Ga + In).
The cell of this embodiment includes a substrate, a back electrode, a CIGS thin film, a buffer layer, an electron transport layer, and a transparent front electrode.
The GGI value of the front surface of the CIGS thin film is 0.25-0.65, and the band gap of the front surface of the CIGS thin film and the conduction band detuning value CBO of the n-type buffer layer of the CIGS battery are kept at-0.05-0.1 eV. The CIGS cell band gap gradient design is applicable to different n-type buffer layers including CdS, Zn (O, S) and In2S3、ZnS、Zn1-xMgxO, gain is universal.
The minimum value of GGI of the band gap gradient is 0.1-0.5, and the value of GGI of the rear surface of the CIGS film is 0.5-1.
Another aspect of the present invention provides a method for manufacturing a copper indium gallium selenide battery, and fig. 3 is a flowchart of the method for manufacturing the copper indium gallium selenide battery, and with reference to fig. 3, the method includes the following steps:
s101: and preparing a molybdenum electrode layer with the thickness of 500 nanometers on the battery substrate by adopting a direct-current magnetron sputtering method.
The cell substrate of this example was 3mm glass.
S102: and depositing a W-shaped band gap gradient copper indium gallium selenide film with the thickness of 1 micron on the molybdenum electrode layer by adopting a three-step co-evaporation method.
The GGI ratio is regulated and controlled by controlling the evaporation rates of Ga and In sources at different stages, so that the band gap of CIGS is regulated to form W-shaped band gap gradient distribution.
In particular, the deposition process needs to be carried out in a sufficient amount of Se atmosphere, in a first step, inEvaporating and depositing In, Ga and Se at a lower substrate temperature (260-400 ℃) to form a compound prefabricated layer consisting of the In, Ga and Se; and step two, closing the In source and the Ga source, and opening the Cu source at a higher substrate temperature (550-600 ℃) to prepare a copper-rich CIGS layer, wherein at a high temperature, copper is used as Cu2-xThe Se secondary phase exists in a liquid state; finally, evaporating the In, Ga source, and Cu while the substrate is still at the elevated temperature2-xSe reacts to finally form a CIGS thin film with the thickness of 1 micron.
The step provides a high-efficiency W-shaped Ga gradient distribution value, the total GGI value is 0.58, the ratio of the GGI values of the front surface of the CIGS film is 0.51-0.62, the minimum value ratio of the first GGI value is 0.49-0.51, the ratio of the middle GGI value is 0.51-0.62, the minimum value ratio of the second GGI value is 0.49-0.51, and the ratio of the GGI values of the rear surface of the CIGS film is 0.74-0.96.
S103: and (3) evaporating 5 nm CsF on the top of the CIGS film by thermal evaporation to perform alkali metal post-treatment, and then performing annealing treatment.
Diffusing alkali metal elements to the surface or inside of the CIGS thin film through a post annealing process at 350 ℃;
and S104, depositing cadmium sulfide with the thickness of 50 nanometers on the CIGS thin film subjected to the alkali metal post-treatment by adopting a Chemical Bath Deposition (CBD) method to serve as a buffer layer.
And S105, preparing a zinc oxide layer with the thickness of 100 nanometers on the buffer layer by adopting a direct-current magnetron sputtering method. Wherein the zinc oxide layer is an electron transport layer, the electron transport layer adopts zinc oxide, and the zinc oxide layer with the thickness of 100 nanometers is prepared on the perovskite layer by adopting a magnetron sputtering method.
S106: and preparing an AZO layer with the thickness of 200 nanometers on the electron transmission layer by adopting a direct current magnetron sputtering method to serve as a transparent front electrode.
In the step, the transparent front electrode adopts AZO, the AZO is aluminum-doped zinc oxide, and an AZO layer with the thickness of 200 nanometers is prepared on the electron transmission layer by adopting a magnetron sputtering method.
In summary, the CIGS cell and the method for manufacturing the same according to the present embodiment effectively increase the open-circuit voltage V by suppressing the recombination of the absorption region of the cell by increasing the band gap of the front surface of the CIGS thin filmOC(ii) a The increase of the band gap of the back surface of the CIGS film is utilized to form a high back electric field, the carrier collection efficiency is improved, and the short-circuit current J is improvedSCAnd an open circuit voltage VOC(ii) a The use of two low-GGI regions reduces the loss of spectral response of the cell in the long wavelength band, while increasing the absorption probability of long wavelength photons. Compared with the highest efficiency achieved by the current V-shaped double gradient, the copper indium gallium selenide solar cell can achieve the photoelectric conversion efficiency higher than 23.35%.
The above description is only for the preferred embodiment of the present invention, but the scope of the present invention is not limited thereto, and any changes or substitutions that can be easily conceived by those skilled in the art within the technical scope of the present invention are included in the scope of the present invention. Therefore, the protection scope of the present invention shall be subject to the protection scope of the claims.

Claims (7)

1. A CIGS battery comprises a CIGS film, and is characterized in that the CIGS film is from the front surface close to the side of a buffer layer to the back surface close to the side of a back electrode, the Ga gradient comprises two minimum values, and the GGI value and the band gap gradient of the CIGS film both show W-shaped distribution.
2. The CIGS cell of claim 1, wherein the cell comprises a substrate, a back electrode, a CIGS thin film, a buffer layer, an electron transport layer, and a transparent front electrode.
3. The CIGS cell of claim 1, wherein the GGI value of the front surface of the CIGS thin film is 0.25-0.65, and the band gap of the front surface of the CIGS thin film and the CBO value of the n-type buffer layer of the CIGS cell are maintained at-0.05-0.1 eV.
4. The CIGS battery of claim 1, wherein the GGI minimum value of the band gap gradient is 0.1-0.5.
5. The CIGS cell of claim 1, wherein the rear surface of the CIGS thin film has a GGI value of 0.5 to 1.
6. A method for manufacturing the CIGS battery according to any one of claims 1 to 5, comprising:
preparing a molybdenum electrode layer with the thickness of 100-1000 nanometers on a battery substrate by adopting a direct-current magnetron sputtering method;
depositing a CIGS thin film with the thickness of 0.5-5 microns on the molybdenum electrode layer by adopting a three-step co-evaporation method; GGI is regulated and controlled by controlling the evaporation rates of Ga and In sources at different stages, so that the band gap of CIGS is regulated to form W-shaped band gap gradient distribution;
performing alkali metal post-treatment on CIGS by using NaF, KF, RbF or CsF alkali metal source materials;
depositing an n-type thin film with the thickness of 10-100 nanometers on the CIGS layer subjected to the alkali metal post-treatment by adopting a chemical bath deposition method to serve as a buffer layer;
preparing a zinc oxide layer with the thickness of 50-500 nanometers on the buffer layer by adopting a direct-current magnetron sputtering method to serve as an electron transmission layer;
and preparing an AZO layer with the thickness of 150-1000 nanometers on the electron transmission layer by adopting a direct current magnetron sputtering method to serve as a transparent front electrode.
7. The method of claim 6, wherein the AZO is aluminum-doped zinc oxide.
CN202110805785.XA 2021-07-16 2021-07-16 Copper indium gallium selenium battery and manufacturing method thereof Active CN113571594B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202110805785.XA CN113571594B (en) 2021-07-16 2021-07-16 Copper indium gallium selenium battery and manufacturing method thereof

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202110805785.XA CN113571594B (en) 2021-07-16 2021-07-16 Copper indium gallium selenium battery and manufacturing method thereof

Publications (2)

Publication Number Publication Date
CN113571594A true CN113571594A (en) 2021-10-29
CN113571594B CN113571594B (en) 2023-06-16

Family

ID=78165139

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202110805785.XA Active CN113571594B (en) 2021-07-16 2021-07-16 Copper indium gallium selenium battery and manufacturing method thereof

Country Status (1)

Country Link
CN (1) CN113571594B (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN115498052A (en) * 2022-09-22 2022-12-20 深圳先进技术研究院 CIGS solar cell and preparation method thereof

Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007335792A (en) * 2006-06-19 2007-12-27 Matsushita Electric Ind Co Ltd Thin-film solar cell
CN102418072A (en) * 2011-10-11 2012-04-18 中国科学院深圳先进技术研究院 Preparation method of light absorption layer of Cu-In-Ga-Se (CIGS) film solar cell
CN102509737A (en) * 2011-11-02 2012-06-20 南开大学 Flexible stainless steel substrate copper-indium-gallium-selenium film battery and preparation method thereof
CN103887373A (en) * 2014-04-15 2014-06-25 苏州斯贝孚光伏科技有限公司 Production process of gradient band gap CIGS solar cell light absorption layer by adopting anti-vacuum method
JP2015162524A (en) * 2014-02-26 2015-09-07 富士フイルム株式会社 Photoelectric conversion element, solar battery, and method for manufacturing photoelectric conversion element
CN105633212A (en) * 2015-12-29 2016-06-01 中国电子科技集团公司第十八研究所 Method and device for preparing gradient band gap light absorption layer based on one-step co-evaporation technology
CN106229362A (en) * 2016-09-22 2016-12-14 东莞市联洲知识产权运营管理有限公司 Preparation method of copper indium gallium selenide thin film and copper indium gallium selenide thin film
CN106449816A (en) * 2016-09-22 2017-02-22 东莞市联洲知识产权运营管理有限公司 Preparation method for copper-indium-gallium-selenide thin film
CN111128747A (en) * 2019-12-27 2020-05-08 光之科技发展(昆山)有限公司 Preparation method of laminated absorption layer of double-gradient band gap CIGS solar cell

Patent Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007335792A (en) * 2006-06-19 2007-12-27 Matsushita Electric Ind Co Ltd Thin-film solar cell
CN102418072A (en) * 2011-10-11 2012-04-18 中国科学院深圳先进技术研究院 Preparation method of light absorption layer of Cu-In-Ga-Se (CIGS) film solar cell
CN102509737A (en) * 2011-11-02 2012-06-20 南开大学 Flexible stainless steel substrate copper-indium-gallium-selenium film battery and preparation method thereof
JP2015162524A (en) * 2014-02-26 2015-09-07 富士フイルム株式会社 Photoelectric conversion element, solar battery, and method for manufacturing photoelectric conversion element
CN103887373A (en) * 2014-04-15 2014-06-25 苏州斯贝孚光伏科技有限公司 Production process of gradient band gap CIGS solar cell light absorption layer by adopting anti-vacuum method
CN105633212A (en) * 2015-12-29 2016-06-01 中国电子科技集团公司第十八研究所 Method and device for preparing gradient band gap light absorption layer based on one-step co-evaporation technology
CN106229362A (en) * 2016-09-22 2016-12-14 东莞市联洲知识产权运营管理有限公司 Preparation method of copper indium gallium selenide thin film and copper indium gallium selenide thin film
CN106449816A (en) * 2016-09-22 2017-02-22 东莞市联洲知识产权运营管理有限公司 Preparation method for copper-indium-gallium-selenide thin film
CN111128747A (en) * 2019-12-27 2020-05-08 光之科技发展(昆山)有限公司 Preparation method of laminated absorption layer of double-gradient band gap CIGS solar cell

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN115498052A (en) * 2022-09-22 2022-12-20 深圳先进技术研究院 CIGS solar cell and preparation method thereof
CN115498052B (en) * 2022-09-22 2024-02-09 深圳先进技术研究院 CIGS solar cell preparation method
WO2024060425A1 (en) * 2022-09-22 2024-03-28 深圳先进技术研究院 Cigs solar cell and preparation method therefor

Also Published As

Publication number Publication date
CN113571594B (en) 2023-06-16

Similar Documents

Publication Publication Date Title
US8916767B2 (en) Solar cell and method of fabricating the same
US7632701B2 (en) Thin film solar cells by selenization sulfurization using diethyl selenium as a selenium precursor
US8658890B2 (en) Solar cell and method of manufacturing solar cell
EP1492169A2 (en) Solar cell
US9935211B2 (en) Back contact structure for photovoltaic devices such as copper-indium-diselenide solar cells
US20100243043A1 (en) Light Absorbing Layer Of CIGS Solar Cell And Method For Fabricating The Same
US8283187B2 (en) Photovoltaic device and method for making
US20100200059A1 (en) Dual-side light-absorbing thin film solar cell
KR20140109530A (en) A thin film solar cell
KR20170036596A (en) A solar cell comprising CZTS Thin film with a oxide buffer layer and a method of manufacturing the same
JP2005228975A (en) Solar battery
Nakada et al. Cu (In1-x, Gax) Se2-based thin film solar cells using transparent conducting back contacts
JP3837114B2 (en) Solar cell
CN113571594B (en) Copper indium gallium selenium battery and manufacturing method thereof
EP2738817A2 (en) Solar cell
JP2011023520A (en) P-type semiconductor film and solar cell
KR102015985B1 (en) Method for manufacturing CIGS thin film for solar cell
CN105047737A (en) CIGS-based thin film solar cell manufacturing method
KR102337783B1 (en) Thin film solar cell having tin(ⅱ) sulfide light-absorber layer and method of manufacturing the thin film solar cell
KR102596328B1 (en) Preparation method for CZTS thin film solar cell absorbing layer, CZTS thin film solar cell absorbing layer prepared therefrom
KR102584673B1 (en) Flexible thin film solar cell and method for manufacturing the same
US20120080306A1 (en) Photovoltaic device and method for making
KR102212042B1 (en) Solar cell comprising buffer layer formed by atomic layer deposition and method of fabricating the same
KR102513863B1 (en) Flexible CZTSSe thin film solar cells and manufacturing method thereof
JP2011091249A (en) Solar battery

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant