研究目的
To improve the cell efficiency of CIGS solar cells by fabricating Cu-poor CIGS thin films with a strongly (220)/(204) preferred orientation using RF magnetron sputtering from a single quaternary target.
研究成果
The one-step sputtered CIGS absorber layer, which has excellent crystallographic and chemical properties, can considerably improve the device performance. The optimized CIGS thin-film solar cell fabricated using the one-step sputtering process showed the cell efficiency of 10.02%. These results demonstrated that one has to pay attention to the control of Cu composition of CIGS quaternary target as well as (220)/(204) preferential orientation of the fabricated CIGS films in order to enhance the cell efficiency in one-step sputtering process.
研究不足
The study is limited by the technical constraints of the one-step sputtering process and the potential for optimization in controlling the crystal orientation and composition distribution of the CIGS thin films.
1:Experimental Design and Method Selection:
RF magnetron sputtering was used to deposit Cu-poor CIGS thin films on a soda-lime glass substrate with a high strain point (SS-1) using a Cu-poor CIGS target with a composition ratio of
2:
3:
4:
2 for Cu, In, Ga, and Se, respectively.
5:Sample Selection and Data Sources:
CIGS thin films were fabricated as a function of the substrate temperatures, which have different film properties.
6:List of Experimental Equipment and Materials:
RF magnetron sputtering system (ULVAC MB07-4501), 4-inch sputtering gun, Cu-poor CIGS single target (LTS chemical Co., USA), SS-1 substrate.
7:Experimental Procedures and Operational Workflow:
The sputtering chamber was evacuated to a base pressure of 2 (cid:3) 10-6 Pa. The optimized deposition conditions were as follows: RF power (300 W), ambient gas (argon), gas flow rate (30 sccm), working pressure (
8:43 Pa), and the distance between target and substrate (150 mm). Data Analysis Methods:
The crystalline structure of CIGS thin films was analyzed by X-ray diffraction (XRD, PANalytical X'pert MPD). The phase analysis was performed by Raman spectroscopy with a HeeNe laser with a wavelength of 632 nm (Jobin Yvon SAS). Plane-view and cross-section images of the CIGS thin films were examined by field-emission scanning electron microscopy (FE-SEM, Quanta 200). Optical properties were measured using a UV-VIS-IR spectrometer (Varian Cary 5000). Compositions of the CIGS thin films were measured by inductively coupled plasma (ICP, Agilent Technologies 7700x). The depth profile was analyzed by secondary ion mass spectroscopy (SIMS) system (Cameca-IMS-7f) with O2+ source ions with 150 (cid:3) 135 mm2 raster size. Finally, the photovoltaic (PV) parameters of the CIGS solar cells were measured under the simulated illumination (Solar simulator: WXS-1555S-L2, WACOM) with a light intensity of 100 mW/cm2.
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X-ray diffractometer
PANalytical X'pert MPD
PANalytical
Used for analyzing the crystalline structure of CIGS thin films.
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Field-emission scanning electron microscope
Quanta 200
FEI
Used for examining plane-view and cross-section images of the CIGS thin films.
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Inductively coupled plasma
Agilent Technologies 7700x
Agilent Technologies
Used for measuring compositions of the CIGS thin films.
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RF magnetron sputtering system
ULVAC MB07-4501
ULVAC
Used for depositing Cu-poor CIGS thin films on a soda-lime glass substrate.
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Raman spectrometer
Jobin Yvon SAS
Jobin Yvon
Used for phase analysis of CIGS thin films.
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UV-VIS-IR spectrometer
Varian Cary 5000
Varian
Used for measuring optical properties of the CIGS thin films.
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Secondary ion mass spectroscopy
Cameca-IMS-7f
Cameca
Used for analyzing the depth profile of the CIGS thin films.
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Solar simulator
WXS-1555S-L2
WACOM
Used for measuring the photovoltaic parameters of the CIGS solar cells.
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