The present invention relates to photoconversion devices such as photovoltaic cells or photodetectors. More in particular, the invention is related to a light transmissive layered photonic structure to enhance light harvesting and tune the color of a transparent photovoltaic device.
Photovoltaic energy sources integration in buildings is of the upmost importance to reduce building emissions. Semi-transparent cells offer a high degree for integration provided they can be incorporated in buildings as windows panes, curtain walls or double skin façades, causing a minimal alteration to the vision of the building users and the exterior appearance of the building. When considering a semitransparent photovoltaic technology there are four important aspects that must be approached: harvesting of those photons which are invisible to the human eye, maximizing transparency to the visible light, device lifetime, and the esthetic appearance from a building wall that incorporates such photovoltaic technology. To increase light harvesting for invisible photons in organic semi-transparent devices several techniques and methods of manufacturing the same have been disclosed:
Y. Galagan et al./Applied Physics Letters 98 (2011) Art. No. 043302 reports on the use of a cholesteric liquid crystal to reflect only in a narrow band of the solar spectrum and remain transparent for the other wavelengths.
R. R. Lunt et al./Applied Physics Letters 98 (2011) Art. No. 113305 reports on the use of a distributed Bragg reflector mirror to increase reflectivity in the infrared which subsequently increases the efficiency of a low efficiency transparent organic solar cell.
To increase transparency in the visible for the top metal electrode, different kinds of electrodes have been disclosed: Pat. No. CN101593812 A and Tao, C. et al./Applied Physics Letters 95 (2009), Art. No. 053303 discloses a transparent anode which adopts a multilayer structure and comprises an anode buffer layer, a metal thin layer and an anti-reflection film. By introducing the anti-reflection film, the energy conversion efficiency of the semitransparent inverse organic solar cell can be improved. By changing the thickness of the anti-reflection film, the transmission spectrum of the transparent anode can be adjusted.
Semi-transparent photovoltaic devices can be made using several kinds of thin film photovoltaic technologies such as CIGS, amorphous silicon, or dye sensitized cells. However, the strong absorption at short visible wavelengths in all such cases leads to a yellowish or reddish color hue to objects that are being observed through such type of devices. On the other hand, the wavelength dependent absorption of some photovoltaic polymer blends such as PBDTTT-C:PCBM or PTB7:PCBM does not exhibit any highly pronounced features in the visible range. Consequently, when looking through a thin layer of such a blend, one does not perceive any significant alteration of the color hue of any kind of image behind. In fact, the only visual effect of such blend to the image being observed through is a reduction in the light intensity received by the eye
Several mechanisms to alter the color or other properties of transparent photovoltaic devices have been disclosed: US 2009/0277500 A1 discloses color tuning of cells by packaging together a transparent solar cell coated on a first transparent substrate with a an optical filter coated on a second transparent substrate. The cell and filter are packaged together using an insulating layer as ethylene vinyl acetate (EVA), polyvinyl butyral (PVB), or another similar material. No fine control (100 nm resoltion or less) can be provided over the thickness of such insulating layer, which prevents any improvement on the performance of the transparent solar cell module. In other words, US 2009/0277500 discloses two separate devices which are bound together with a layer of insulating material. The lack of thickness control over such insulating layer implies that the optical filter acts as a stand alone device having no direct effect on the performance of the solar cell device. KR101140731 B1 discloses a transmission type photovoltaic module of various colors by utilizing interference color of a 3D photonic crystal.
Alternatively one may tune the device color perception to the observer by introducing an absorbing layer to alter the wavelength dependent transmission and eventually modify the color appearance.
The main object of the present invention is to provide a semi-transparent photo conversion device that enhances harvesting of visible sunlight. For this purpose, a semitransparent photovoltaic cell is provided with a multilayer structure that can be used to increase the efficiency, increase the lifetime, and change the color hue appearance of the cell while guaranteeing a minimum change to the light absorption capacity. In particular, the invention discloses a photoconversion device comprising a transparent substrate and a first light transmissive electrical contact overlaying the transparent substrate, a first charge blocking layer, an absorption layer comprising and active organic photosensitive material, a second charge blocking layer overlying the active organic photosensitive material, a second light transmissive electrical contact and a multilayer structure in this order, the multilayer structure comprising at least two layers of different dielectric materials with different index of refraction and wherein the thickness of each layer is between 5 and 500 nm and two adjacent layers have different refractive indexes. Other aspects of the invention are apparent form the dependent claims.
To complete the description and in order to provide for a better understanding of the invention, a set of drawings is provided.
The photo conversion device has a direct or inverted architecture that comprises a first light transmissive electrical contact overlaying a transparent substrate, a charge blocking layer overlying the first light transmissive electrical contact and underlying the active organic photosensitive material, a second charge blocking layer overlying the active organic photosensitive material, a second light transmissive electrical contact overlying the second charge blocking layer, and a multilayer structure overlying the second light transmissive electrical contact. The multilayer structure is composed of two or more layers of dielectric materials. In such multilayer structure, the index of refraction of each layer must be different than the index of refraction of the adjacent layers. A method for manufacturing the photovoltaic cell including the multilayer structure comprises one deposition step for each layer in the device. The manufacturing of the entire device finishes with the deposition of the last dielectric layer from the multilayer structure.
More in particular, in a preferred embodiment the device is an inverted organic solar cell comprising:
1 A substrate of any light transmissive rigid or flexible material on which the photovoltaic cell can be grown upon as glass, crystal, transparent metal, semiconductor or plastic. Examples of these materials are silica (SiO2), borosilicate (BK7) and PET.
2 A first transparent electrode comprising a thin metal layer or nanowire mesh from the elements of the group of Ag, Al, Au, Ti, Ni, Cu, or combinations thereof, or a transparent conductive oxide layer from the group of ITO, ZnO, Al:ZnO, SnO2, FTO, or conductive polymers such as PEDOT, PEDOT:PSS, PEDOT-TMA or a carbon nanotube, or a graphene layer of a thickness between 0.3 nm and 350 nm.
3 Overlying and in contact with the first electrode there is a hole blocking layer comprising a transparent semi-conductor layer as ZnO, PFN, or TiO2 (thickness between 1 nm and 150 nm). The layer comprises either a homogenous or a nanoparticle morphology of the materials listed.
4 An organic active material forming a blend that contains a mixture of two components: a semiconductor conjugated polymer and a fullerene compound. The first component is a conjugated polymer with alternating electron-donor and electron-acceptor monomers. The donor is a derivative of benzo[1,2-b:4,5-b′]dithiophene, whereas as acceptor many different types of compounds can be used, for example, though not exclusively, thiophene, benzothiadiazole or diketopyrrolopyrrole derivatives. Alternatively, the first component is a α-PTPTBT polymer, where the electron donating unit is a thiophene-phenylene-thiophene (TPT) and the acceptor unit is 2,1,3-benzothiadiazole (BT). Alternatively, the first component is a polythiophene polymer (P3HT). The second component of the blend is C60 or a soluble derivative of the fullerene family of compounds. The thickness of the whole active material layer is between 40 nm and 500 nm. Alternatively, the active material may comprise a stack of two or more of such blends forming a tandem organic active layer in a series configuration. The separation between the blends in the stack may comprise an interlayer for facilitating recombination of holes and electrons.
5 An electron blocking layer comprising a transparent semi-conductor layer as MoO3, PEDOT:PSS, WO3, NiO (1 nm and 150 nm). The layer may comprise either a homogenous or a nanoparticle morphology of the materials listed above.
6 A second transparent electrode may comprise a thin metal layer or nanowire mesh from the elements of the group of Ag, Al, Au, Ti, Ni, Cu, . . . or combinations thereof, or a transparent conductive oxide layer from the group of ITO, ZnO, Al:ZnO, SnO2, FTO, or conductive polymers such as PEDOT, PEDOT:PSS, PEDOT-TMA or a carbon nanotube, or a graphene layer. (0.3 nm up to 350 nm)
7 A multilayer structure comprising two or more dielectric layers. In this multilayer structure each dielectric layer may comprise a transparent inorganic material such as MoO3, MgF2, TiO2, SiO2, SiN1.3:H, SiO2:F, Ta2O5, ZnO, Al2O3, ZnS, CaF2, MbO5, ZrO2, Y2O3, SiO2:H, LiF. Each layer may comprise either a homogenous or a nanoparticle morphology of the inorganic materials listed above. Alternatively the layer may comprise transparent polymer materials such as PMMA, Polystyrene, PET. The thickness of each layer within the multilayer structure is between 5 nm and 500 nm. The range of thicknesses is such because the thickness of each one of the dielectric layers has a direct effect on the performance (efficiency, lifetime, transparency and color) of the entire device.
The first layer in the multilayer structure comprises one of the dielectric materials above or a mixture of them. The second layer in the multilayer structure comprises one of the materials above but not the same one or same mixture as in the first layer in the sense that the index of refraction for the second layer must be different than the index of the first layer in the multilayer structure. The third layer in the multilayer structure comprises a material from the list above with an index of refraction different than the index of the second layer in the multilayer structure. This sequence is repeated up to the last layer of the structure. In a preferred embodiment for the multilayer structure the material used in all the odd layers is the same while the material used in all even layers is the same.
In an alternative embodiment, the device is a direct organic cell comprising the same elements as before, but where an electron blocking layer comprising a transparent semi-conductor layer as PEDOT:PSS, NiO, WO3, MoO3 of a thickness between 1 and 150 nm is provided on top of the first transparent electrode and a hole blocking layer comprising a transparent semi-conductor layer as ZnO, PFN, BCP, TiO2, LiF, LiCoO2 of a thickness between 1 and 150 nm is provided on top of the active material.
Below there are three examples where the optimal thicknesses for the dielectric layers in the multilayer structure are provided. As can be seen such optimal thicknesses are different in each case but they are always within the range specified. A fourth example is to demonstrate that the multilayer structure increases the operation lifetime of the device by providing an effective barrier to corrosive elements such as oxygen or moisture.
As it can be seen in the figure, photon absorption by the invention is enhanced for light wavelengths to which the human eye is most insensitive. Photon absorption in the wavelength range (400-600 nm) where the eye sensitivity is the largest is however similar to photon absorption by the semi-transparent cell which does not include the multilayer structure. In other words, the invention is more efficient in converting light to electricity with the same visible transparency.
As it can be seen in the figure the transmission window can be shifted when the thickness of the layers in the multilayer structure is changed. This causes a change in the color of the device but almost no change in the photon collection efficiency of the device.
Number | Date | Country | Kind |
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13166037.5 | Apr 2013 | EP | regional |