Embodiments of the invention relate to semiconductor devices and methods of manufacture, and more particularly to the field of photovoltaic (PV) devices.
Photovoltaic devices generally comprise multiple layers of material deposited on a substrate, such as glass.
An exemplary energy band diagram of a typical thin-film photovoltaic device, such as a CdTe device is depicted in
As depicted in
CdS is the conventional window layer in many types of thin-film photovoltaic devices, including photovoltaic devices employing one of CdTe and Cu(In, Ga)Se2 as an absorber layer. However, as depicted in
This disclosure is directed to photovoltaic devices and methods of production. In one embodiment, Zn1-xMgxO is employed for a window layer of substrate structure.
In one embodiment, substrate structure 300 may include a glass substrate 305, and TCO layer 310. Buffer layer 315 may be optional. Window layer 320 (e.g., Zn1-xMgxO layer) may be directly on top of TCO layer 310, the TCO layer including one or more of a F-doped SnO2, undoped SnO2, and Cd2SnO4. When TCO layer 310 includes an undoped Cd2SnO4, the TCO layer has no extrinsic dopant, however the layer may be highly n-type due to oxygen vacancies.
According to another embodiment, substrate structure 300 may be provided for manufacturing photovoltaic devices. As depicted in
In one embodiment the thickness of Zn1-xMgxO window layer 320 ranges from 2 to 2000 nm. In another embodiment, the composition of x in Zn1-xMgxO is greater than 0 and less than 1. Window layer 320 may be a more conductive material relative to conventional window layer materials, such as CdS. Additionally, window layer 320 may include a window layer material that allows for greatly reduced fill factor (FF) loss in a blue light deficient environment. A Zn1-xMgxO window layer may allow for more solar radiation in the blue region (e.g., 400 to 475 nm) that can reach the absorber leading to higher short circuit current (Isc).
In an alternative embodiment, a photovoltaic device, such as substrate structure 300 may include a Zn1-xMgxO compound material as window layer 320 and one or more of a barrier layer and a CdS window layer, as depicted in
Zn1-xMgxO may be advantageous over a conventional CdS window layers as Zn1-x MgxO has a wider band gap relative to a device having a CdS window layer. As such, more solar radiation can reach a CdTe absorber, which leads to higher Isc. Similarly, an improved conduction band edge alignment can be achieved by adjusting composition of Zn1-xMgxO, which leads to higher Voc. The dopant concentration can be in the range of 1015 to 1019 atoms (or ions) of dopant per cm3 of metal oxide. Carrier density of Zn1-xMgxO can be greater than the carrier density of CdS. As such, a stronger n-p semiconductor heterojunction can be formed increasing the built-in potential of the solar cells and minimizing recombination at the interface. A more conductive window layer can also improve the loss in fill factor in a low light environment (e.g., photoconductivity effect), where the percentage of blue light is reduced greatly as compared to under full sun light.
Referring to
According to another embodiment, Zn1-xMgxO may be employed for a window layer of a photovoltaic device.
More specifically, photovoltaic device 500 may include one or more of glass substrate 505, TCO layer 510 made from SnO2 or Cd2SnO4, buffer layer 515, a Zn1-xMgxO Window layer 520, a CdTe absorber 525, and a metal back contact 530. Buffer layer 515 may relate to a low conductivity buffer layer, such as undoped SnO2. Buffer layer 515 may be used to decrease the likelihood of irregularities occurring during the formation of the semiconductor window layer. Absorber layer 525 may be a CdTe layer. The layer thickness and materials are not limited by the thicknesses depicted in
Photovoltaic device 500 may include one or more of a cadmium telluride (CdTe), copper indium gallium (di)selenide (CIGS), and amorphous silicon (Si) as the absorber layer 525. In one embodiment, a photovoltaic device may be provided that includes a Zn1-xMgxO window layer 520 between a substrate structure, which may or may not include a low conductivity buffer layer 515, and the absorber layer 525. In certain embodiments, the device may additionally include a CdS window layer in addition to Zn1-xMgxO window layer 520.
In an alternative embodiment, photovoltaic device 500 may include a Zn1-xMgxO compound material as window layer 520 and one or more of a barrier layer and a CdS window layer as depicted in
In certain embodiments, photovoltaic device 500 may not include a buffer layer.
Both zinc oxide (ZnO) and magnesium oxide (MgO) are wide band gap oxides. ZnO has a band gap of 3.2 eV and MgO has a band gap of about 7.7 eV. ZnO may further be advantageous as it is highly dopable. The ternary compound Zn1-xMgxO should have a band gap of at least 3 eV as predicted by simulation, which is much larger than that of CdS, and is thus more transparent to blue light. On the other hand, ZnO has a Δ from −0.6 to −1.0 eV relative to CdTe conduction band edge, while MgO has a positive Δ about 2.7 eV. Therefore, the composition of the ternary compound Zn1-xMgxO can be tuned to lead to a Δ that is slightly positive, as shown in
The improvement in device Voc by replacing a CdS window layer with a Zn1-xMgxO window layer may include improved open circuit voltage from 810 mV to 826 mV.
In another aspect, a process is provided for manufacturing photovoltaic devices and substrates to include a Zn1-xMgxO window layer as depicted in
In one embodiment, a process for manufacturing a photovoltaic device may include a sputtering process of a Zn1-xMgxO window layer by one of DC Pulsed sputtering, RF sputtering, AC sputtering, and other manufacturing processes in general. The source materials used for sputtering can be one or more ceramic targets of a Zn1-xMgxO ternary compound, where x is in the range of 0 to 1. In one embodiment, source materials used for sputtering can be one or more targets of Zn1-xMgx alloy, where x is in the range of 0 to 1. In another embodiment, source materials used for sputtering can be two or more ceramic targets with one or more made from ZnO and the one or more made from MgO. In another embodiment, source materials used for sputtering can be two or more metal targets with one or more made from Zn and one or more made from Mg. Process gas for sputtering the Zn1-xMgxO can be a mixture of argon and oxygen using different mixing ratios.
In one embodiment, a Zn1-xMgxO window layer can be deposited by atmospheric pressure chemical vapor deposition (APCVD) with precursors including but not limited to diethyl zinc, bis(cyclopentadienyl)magnesium with reagent such as H2O or ozone.
According to another embodiment, the process for manufacturing a photovoltaic device may result in a conduction band offset with respect to an absorber layer. For example, the conduction band offset of a window (Zn1-xMgxO) layer with respect to the absorber layer can be adjusted between 0 and +0.4 eV by choosing the proper value of x. Further, the conductivity of a Zn1-xMgxO window layer can be adjusted within a range of 1 mOhm per cm to 10 Ohm per cm by doping the zinc magnesium oxide with one of aluminum (Al), manganese (Mn), niobium (Nb), nitrogen (N), fluorine (F), and by introduction of oxygen vacancies. In one embodiment the dopant concentration is from about 1×1014 cm3 to about 1×1019 cm3. In one embodiment, the window layer is formed using a sputter target having a dopant concentration from about 1×1017 cm3 to about 1×1018 cm3.
This application is a continuation of U.S. patent application Ser. No. 13/238,457 filed Sep. 21, 2011, which claims priority under 35 U.S.C. § 119(e) to Provisional Application No. 61/385,399 filed on Sep. 22, 2010, which are hereby incorporated by reference in their entirety.
Number | Name | Date | Kind |
---|---|---|---|
4160678 | Jain et al. | Jul 1979 | A |
4542256 | Wiederman | Sep 1985 | A |
4568792 | Mooney et al. | Feb 1986 | A |
5317583 | Nasibov et al. | May 1994 | A |
5412232 | Ando | May 1995 | A |
6218684 | Kuhara et al. | Apr 2001 | B1 |
6259016 | Negami et al. | Jul 2001 | B1 |
6534704 | Hashimoto et al. | Mar 2003 | B2 |
6559736 | Lu et al. | May 2003 | B2 |
7105868 | Nause et al. | Sep 2006 | B2 |
7439545 | Honda | Oct 2008 | B2 |
7479596 | Hashimoto et al. | Jan 2009 | B2 |
7494546 | Vispute et al. | Feb 2009 | B1 |
7675133 | Burgener, II et al. | Mar 2010 | B2 |
8304804 | Shibata et al. | Nov 2012 | B2 |
8598447 | Yamaguchi et al. | Dec 2013 | B2 |
8759828 | Akasaka et al. | Jun 2014 | B2 |
8823033 | Yamamoto et al. | Sep 2014 | B2 |
8884285 | Lu et al. | Nov 2014 | B2 |
9059417 | Wei et al. | Jun 2015 | B1 |
9064965 | Lu et al. | Jun 2015 | B2 |
9082903 | Shao et al. | Jul 2015 | B2 |
9112074 | Boutwell et al. | Aug 2015 | B2 |
9385264 | Asadi et al. | Jul 2016 | B2 |
9590015 | Lu et al. | Mar 2017 | B2 |
9627439 | Lu et al. | Apr 2017 | B2 |
9666758 | Asadi et al. | May 2017 | B2 |
20040182434 | Hashimoto et al. | Sep 2004 | A1 |
20080115827 | Woods et al. | May 2008 | A1 |
20090020149 | Woods et al. | Jan 2009 | A1 |
20090084438 | den Boer et al. | Apr 2009 | A1 |
20090199894 | Hollars | Aug 2009 | A1 |
20110005591 | Buller et al. | Jan 2011 | A1 |
20110005594 | Powell et al. | Jan 2011 | A1 |
20110226320 | Little | Sep 2011 | A1 |
20150053267 | Lim | Feb 2015 | A1 |
20150303329 | Teraji et al. | Oct 2015 | A1 |
20150325735 | Shao et al. | Nov 2015 | A1 |
20170033150 | Willigan et al. | Feb 2017 | A1 |
Number | Date | Country |
---|---|---|
1531114 | Sep 2004 | CN |
101164966 | Apr 2008 | CN |
10 2007 047 146 | Apr 2008 | DE |
1460692 | Sep 2004 | EP |
1555698 | Jul 2005 | EP |
9528008 | Oct 1995 | WO |
Entry |
---|
Takashi Minemoto, “Cu(In,Ga)Se2 solar cells with controlled conduction band offset of window/Cu(In,Ga)Se2 layers”, Journal of Applied Physics, Jun. 15, 2001, pp. 8327-8330, vol. 89, No. 12. |
Takashi Minemoto et al., “Control of conduction band ofset in wide-gap Cu(In,Ga)Se2 solar cells”, Solar Enerygy Materials & Solar Cells, 2003, pp. 121-126, vol. 75. |
A. Morales-Acevedo, “Thin Film Cds/CdTe Solar Cells: Research Perspective,” Solar Energy, vol. 80, pp. 675-681, (2006). |
N, Naghavi et al., “Buffer Layers and Transparent Conducting Oxides for Chalcopyrite Cu(In,Ga)(S,Se)2 Based Thin Film Photovoltaics: Present Status and Current Developments,” Progress in Photovoltaics: Research and Applications, vol. 18, pp. 411-433, Apr. 2010. |
J. Sites et al., “Strategies to Increase CdTe Solar-Cell Voltage,” Thin Solid Films, vol. 515, pp. 6099-6102, 2007. |
J. Perrenoud et al., “Application of ZNO1-xSx as Window Layer in Cadmium Telluride Solar Cells,” IEEE 978-1-4244-5892-9/10, 2010. |
English Machine Translation of DE 102007047146A1. |
M. Gloeckler, et al., “Efficiency limitations for wide-band-gap chalcopyrite solar cells,” Thin Solid Films 480-481 (205) p. 241-245. |
First Chinese Office Action, Application No. 201610452924.4, dated Dec. 30, 2016. |
Number | Date | Country | |
---|---|---|---|
20150325735 A1 | Nov 2015 | US |
Number | Date | Country | |
---|---|---|---|
61385399 | Sep 2010 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 13238457 | Sep 2011 | US |
Child | 14740501 | US |