The present invention pertains to a photo-voltaic element.
The present invention further pertains to a method of manufacturing the same.
A photo-voltaic element is disclosed in CN105140398 that comprises a conductive substrate; a uniform electron transport layer; a dielectric layer; a metal layer; and a perovskite layer as a photo-electric conversion layer. The latter has a plurality of channels through the dielectric layer and the metal layer that contact the electron transport layer. Accordingly the perovskite photo-electric conversion layer has its electric contacts for delivering electrical energy at the same side. Therewith it can be avoided that light to be converted has to pass through an electrode layer, as a result of which it would be attenuated before conversion.
The cited document also presents a method of manufacturing the photo-voltaic element disclosed therein. Therein a substrate is provided of a transparent conductive glass and an electron transport layer is deposited thereon by magnetron sputtering ZnO. Subsequently a layer of dispersed PS pellets having an original diameter of 2 um is deposited resulting in a hexagonal close-packed structure of said PS pellets. The PS ball diameter is subsequently reduced to 1 um by dry etching using RIE. A dielectric layer of Al2O3 is deposited thereon using ALD deposition followed by magneton sputtering of an Au layer. Subsequently, using a solvent and an ultrasonic treatment the PS pellets and the portions of the Al2O3 layer and the Au layer deposited thereon are removed, so that an Au mesh is obtained that is insulated from the electron transport layer. A perovskite layer is spin coated thereon that both contacts the Au mesh and the ZnO electron transport layer.
It is a disadvantage of this known process, a lift-off process, that the patterning process is not well controlled. As a result the boundaries of the openings in the insulator layer and the upper electrode layer are jagged and an unreliable or even non-working product is obtained.
It is noted that WO2017/060700, published after the priority date of this document also uses a lift-off process. As shown for example in
It is a first object of the invention to provide a photo-voltaic element with an improved conversion efficiency.
It is a second object of the invention to provide a method of manufacturing this improved photo-voltaic element.
In accordance with said first object, according to a first aspect, a photo-voltaic element is provided as disclosed herein.
In accordance with said second object, according to a second aspect, a method of manufacturing a photo-voltaic element is provided as further disclosed herein.
An exemplary photo-voltaic element comprises a stack of layers that at least include in the order named: a first electrode layer, a first charge carrier transport layer, an insulating layer, a second electrode layer, a second charge carrier transport layer, and a photo-electric conversion layer.
The first electrode layer is provided for receiving charge carriers of a first polarity, for example electrons, or alternatively for receiving holes as the charge carrier. The first charge carrier transport layer is provided for transport of charge carriers having the first polarity. E.g. if the first electrode layer is a cathode provided for receiving electrons as the charge carrier then the first charge carrier transport layer is an electron transport layer. Alternatively, if the first electrode layer is an anode provided for receiving holes as the charge carrier then the first charge carrier transport layer is a hole transport layer. The insulating layer may be provided of any sufficiently insulating organic or inorganic material. The second electrode layer is provided for receiving charge carriers of a second polarity opposite to the first polarity. Hence if the first electrode layer is a cathode then the second electrode layer is an anode and vice versa. The second charge carrier transport layer is provided for transport of charge carriers having the second polarity. Accordingly the second charge carrier transport layer is a hole transport layer if the second electrode layer is an anode and an electron transport layer if the second electrode layer is a cathode. The photo-electric conversion layer comprises a plurality of distributed extensions that extend through the second charge carrier transport layer, the second electrode layer and the insulating layer to the first charge carrier transport layer.
Because the photo-electric conversion layer is the uppermost layer of the stack (apart from e.g. a protection layer or encapsulation), it is not necessary that the various layers are transparent. Therewith one or more of the electrodes may be formed as a metal layer, for example an aluminum or a copper layer, possibly sandwiched between intermediate layers, e.g. as MoAlMo or CrCUCr. Nevertheless, embodiments may be contemplated wherein a transparent electrically conductive material is used for the electrodes, for example a transparent electrically conductive oxide like ITO. This is advantageous in that the device so obtained is bilaterally sensitive. Alternatively, this may be combined with a substrate having a reflecting surface. In this embodiment, light entering the device that is not converted in the photo-electric conversion layer is reflected back to the latter, so that it can still be (partially) converted.
Therewith the photo-electric conversion layer is electrically coupled to both the first charge carrier transport layer and the second charge carrier transport layer. In this arrangement solar radiation R does not need to traverse an electrode layer or a charge carrier transport layer, which contributes to an efficient operation of the photo-voltaic element.
An optimal conversion efficiency is achieved by the presence of a charge carrier transport layer between the first electrode layer and the photo-electric conversion layer as well as between the second electrode layer and the photo-electric conversion layer.
The extensions have an effective cross-section Deff in the range of 0.5 to 10 micron, and have an average pitch in the range of 1.1 to 5 times their effective cross-section. The effective cross-section is defined here as the diameter of a circle having an area corresponding to the cross-sectional area AØ of the extensions.
The extensions are typically cylindrical. Alternatively the extensions may taper inward or outward. The extensions may have any cross-section, such as circular, square or triangular. The circumference O of the extensions is less than 10 times the effective diameter Deff and preferably less than 5 times the effective diameter Deff. Therewith an optimum contact surface between the photo-electric conversion layer and the first charge carrier transport layer is achieved with minimum disruption of the intermediary layers, in particular the second electrode layer and the second charge carrier transport layer.
In an embodiment of the photo-voltaic element the extensions taper outward in a direction from the first charge carrier transport layer to the second charge carrier layer. In an embodiment thereof, material of the second charge carrier transport layer covers a surface of the second electrode surrounding the extensions. Therewith a contact surface provided for the photovoltaic layer is improved.
In an embodiment, the first charge carrier layer is absent in areas of the first electrode layer covered by the insulating layer. Also in this case, the stack formed in the product is deemed to comprise first charge carrier layer and a subsequent insulating layer, as the surface of the insulating layer will be above a surface of the first charge carrier layer, when traversing the layers starting from the substrate on which the layers are deposited.
In an embodiment the photo-electric conversion layer is provided of a perovskite material. Perovskite materials typical have a crystal structure of ABX3, wherein A is an organic cation as methylammonium (CH3NH3)30, B is an inorganic cation, usually lead (II) (Pb2+), and X is a halogen atom such as iodine (I−), chlorine (Cl−) or bromine (Br−). Perovskite materials are particularly advantageous in that they can be processed relatively easily and in that their bandgap can be set to a desired value by a proper choice of the halide content. A typical example is methylammonium lead trihalide (CH3NH3PbX3), with an optical bandgap between 1.5 and 2.3 eV depending on halide content. Another more complex structure example is Cesium-formamidinium lead trihalide (Cs0.05(H2NCHNH2)0.95PbI2.85Br0.15) having a bandgap between 1.5 and 2.2 eV. Other metals such as tin may replace the role of Pb in perovskite materials. An example thereof is CH3NH3SnI3. Also combinations of Sn with Pb perovskites having a wider bandgap in the range of 1.2 to 2.2 eV are possible. In another embodiment the photo-electric conversion layer is made of copper indium gallium selenide (CIGS).
The geometry of the substantially circular cylindrical extensions with an effective cross-section Deff in the range of 0.5 to 10 micron, and with an average pitch in the range of 1.1 to 5 times their effective cross-section makes it possible to optimally tune the contact-surface of the photo-voltaic layer with the first and the second charge carrier transport layer respectively dependent on the type of perovskite material used for the photo-voltaic layer. This is favorable, in that the ratio of mobility for holes and electrons may differ. E.g. if for a certain perovskite the mobility of electrons is 3 time higher than for holes, the surface area of the HTL preferably is approximately 3× the surface area of the ETL for an optimal efficiency.
The presently disclosed methods enable manufacturing the photo-voltaic elements disclosed herein. Exemplary methods comprise the steps of:
The method further comprises depositing a first charge carrier transport layer for transport of charge carriers having the first polarity and depositing a second charge carrier transport layer for transport of charge carriers having said second polarity.
In an embodiment depositing the first charge carrier transport layer is subsequent to depositing the first electrode layer and preceding to depositing the insulating layer and said depositing the second charge carrier layer is subsequent to depositing the insulating layer and preceding depositing the resist layer.
In an embodiment, of the method the second charge carrier transport layer is deposited with an electroplating process and subsequent to removing the resist layer, and preceding depositing and curing a photo-electric conversion layer.
In an embodiment the first charge carrier transport layer is deposited with an electroplating process subsequent to removing the resist layer, and preceding depositing the second charge carrier layer.
The method according to the present invention enables the deposition of a thicker stack of layers on the first charge carrier transport layer than would be possible when using the pellet based approach known from the prior art. In this way the second charge carrier transport layer can be provided, therewith significantly improving efficiency of the photo-voltaic element.
Various methods may be used for depositing and applying layers. These methods may include spin-coating, printing methods, slot-die coating and vapor deposition methods like physical vapor deposition (e.g. E-beam PVD, Sputter PVD), (spatial) Atomic Layer Deposition ((s)ALD), and chemical vapor deposition (e.g. plasma-enhanced chemical vapor deposition (PECVD)).
Etching processes may be applied to remove a material (or a part of the material) from a surface either by a chemical reaction generated by the use of a reactive mix of gases (plasma-etching) or by submerging the substrates in a reactive solution where the layer is removed by dissolution or chemical reaction (wet-etching).
A selective etching is made possible by using a mask that locally protects the underlying layer(s). A patterning in such a mask may be obtained for example by optical lithography wherein light is used to transfer a geometric pattern from a photo-mask to a light sensitive chemical photoresist on the substrate. Also imprinting can be applied to pattern the mask. Alternatively the mask may be directly applied in the desired pattern, for example by printing.
These and other aspects are described in more detail with reference to the drawing. Therein:
The first electrode layer 20 is provided for receiving charge carriers of a first polarity. In the embodiment shown the first electrode layer 20 is an anode, i.e. arranged for receiving holes as the charge carriers. Dependent on the lateral size of the photo-voltaic element 1 the first electrode layer 20 may for example have a thickness in the range of a few tens to a few hundreds of nanometers or even more. In the embodiment shown the first electrode layer 20 includes an aluminum sub layer having a thickness of 190 nm, which is sandwiched between a pair of nickel layers, each having a thickness of 5 nm. In another example the first electrode layer is of molybdenum. In an embodiment where the substrate is provided of a metal, it may also serve as a first electrode layer 20.
In the embodiment shown the first charge carrier transport layer 30 is a hole transport layer, having a thickness in the range of 10 to 200 nm. In the embodiment shown the hole transport layer is formed by a nickeloxide layer having a thickness of 50 nm. In another example the hole transport layer is formed by a MoSe layer.
An insulating layer 40 is provided of an organic, e.g. a polymer, or inorganic insulating material, such as a metal oxide. Also a stack of materials can be used. Dependent on the material selected for the insulating layer, it may have a thickness in the range of 10 to 200 nm for example, but also a substantially thicker insulating layer may be applied. In the embodiment shown the insulating layer 40 is provided as a SiO2 layer having a thickness of 100 nm.
A second electrode layer 50 for receiving charge carriers of a second polarity opposite to said first polarity is arranged on the insulating layer 40. In this case the second electrode layer 50 is a cathode. Any sufficiently conducting material can be used for this purpose at a thickness depending on the lateral size of the photo-voltaic element 1. Typically the thickness of the second electrode layer 50 is of the same order of magnitude as the thickness of the first electrode layer 20, so that they have approximately the same conductivity and neither of them forms a bottleneck. In the embodiment shown the second electrode layer 50 is an aluminum layer with a thickness of 200 nm. In some embodiments the second electrode layer 50 may have a thickness greater than that of the first electrode layer 20, e.g. 1.5 times a thickness of the first electrode layer 20, to compensate for the presence of the openings provided in the second electrode layer 50.
A second charge carrier transport layer 60 for transport of charge carriers having said the second polarity, opposite to the first polarity layer is arranged upon the second electrode layer 50. In this case the second charge carrier transport layer 60 is an electron transport layer. The second charge carrier transport layer 60, here an electron transport layer may have a thickness in the range of a few nm, e.g. 5 nm to a few tens of nm, e.g. 50 nm. In the embodiment shown the second charge carrier transport layer 60 is a TiO2 layer having thickness of 15 nm. Other suitable materials for an electron transport layer are for example SnO2, ZrO2 and ZnO:S.
A photo-electric conversion layer 70 is provided upon the second charge carrier transport layer 60. The photo-electric conversion layer 70 has a plurality of distributed, typically cylindrical, extensions 72 that extend through the second charge carrier transport layer 60, the second electrode layer 50 and the insulating layer 40 to the first charge carrier transport layer 30. Therewith the photo-electric conversion layer 70 is electrically coupled to both the first charge carrier transport layer 30 and the second charge carrier transport layer 60. In this arrangement solar radiation R does not need to traverse an electrode layer or a charge carrier transport layer which contributes to an efficient operation of the photo-voltaic element 1. In the embodiment shown the extensions 72 have an effective cross-section Deff in the range of 0.5 to 10 micron, and have an average pitch in the range of 1.1 to 5 times their effective cross-section. The effective cross-section is defined here as the diameter of a circle having an area corresponding to the cross-sectional area AØ of the extensions.
The extensions may have any cross-section, such as circular, square or triangular. Preferably, a circumference O of the extensions is less than 10 times the effective diameter Deff and even more preferably less than 5 times the effective diameter Deff.
In the embodiment the photo-electric conversion layer is provided of a perovskite material, such as methylammonium lead trihalide (CH3NH3PbX3), or cesium-formamidinum lead trihalide (Cs0.05(H2NCHNH2)0.95PbI2.85Br0.15). Alternatively a tin based perovskite material, such as CH3NH3SnI3 may be used. Also more complex perovskite materials may be applied, for example containing a combination of different cations. Also other materials, such as copper indium gallium selenide (CIGS) are suitable.
In the embodiment shown the second electrode layer 50 has anodized edge surfaces 52 facing the extensions 72 of the photo-electric conversion layer 70. This avoids direct contact between the second electrode layer and the photo-electric conversion layer.
As shown in
As shown in
In the embodiment shown light in coupling is further improved by a light in coupling structure 100 arranged over the barrier 90. In the embodiment shown the light in coupling structure comprises a plurality of light in coupling elements 102A, 102B. For example semi-spherical or pyramidal shaped light in coupling elements may be used.
A method of manufacturing a photo-voltaic element is now disclosed with reference to
Therein a substrate is 10 is provided in a first step ST. Then in a second step S2 a stack of layers is deposited thereon that comprise at least in the order named a first electrode layer 20, a first charge carrier transport layer 30, an insulating layer 40, a second electrode layer 50 and a second charge carrier transport layer.
The first electrode layer 20 is provided for receiving charge carriers of a first polarity. The first electrode layer 20 may for example be an anode, i.e. arranged for receiving holes as the charge carriers. Alternatively the first electrode layer 20 may be a cathode, i.e. arranged for receiving electrons as the charge carriers. In an embodiment the first electrode layer 20 is deposited with a PVD (physical vapor deposition) method, for example using E-beam PVD. In this example the first electrode layer 20 was provided as a stack of sub-layers obtained by subsequently depositing a first sub-layer of nickel having a thickness of 5 nm, an aluminum layer having a thickness of 190 nm and a second sub-layer of nickel also having a thickness of 5 nm. Then spin-coating (1000 rpm) was used to deposit a NiO layer as the first charge carrier transport layer 30, here a hole transport layer.
An insulating layer 40 was then deposited in a first and a second stage. In the first of these stages a first, 100 nm thick, sublayer of SiOx was deposited by electron-beam deposition and in the second stage a second sublayer of SiOx, also having a thickness of 100 nm was deposited by PECVD. Then a second electrode layer 50, here a cathode layer of aluminum at a thickness of 200 nm was formed using the same method and conditions as those applied for the deposition of the aluminum sub-layer of the first electrode layer 20.
A second charge carrier transport layer 60, here an electron transport layer was then deposited. In this case electron-beam vapor deposition was used to deposit a TiOx layer with a thickness of 15 nm of linear titanium dioxide (TiOx).
The insulating layer 40 and the layers 50, 60 form a sub-stack having an upper surface 64. In a third step S3, here using spin coating a resist layer 80, here a photo-resist layer having a thickness of 1.6 micron was deposited on this upper surface 64. In other implementations the resist layer may be an imprint-resist layer.
Instead of patterning an originally homogeneous resist layer, it is alternatively possible to directly depositing the resist layer in the desired pattern, for example using a printing technique.
As shown in
Optional pre-processing steps, S6A and S6B may be performed after removal of the resist layer 80 and before deposition of the photo-electric conversion layer 70.
A first optional pre-processing step S6A is illustrated in
Upon completion the substrate 10 may be removed. For example this may be the case if an electrode layer, e.g. the first electrode layer 20 provides sufficient structural integrity. Alternatively, or in addition mechanical support may be provided by further layers applied on the photo-electric conversion layer 70.
Therein
In a next step S16B, as shown in
In a further step S16C, a second charge carrier transport layer 60, is deposited in an electroplating process, therewith using the layer 50 as the electrode. Due to the curved edge 55 of the opening formed in the electrode 50, an increased electric field is obtained that enhances the deposition speed near the opening. By way of example, a hole transport layer may be deposited as the charge carrier transport layer 60, e.g. CuSCN using a solution of CuSO4/Nitrilotriacetic acid/KSCN. Alternatively, the charge carrier transport layer 60 may be deposited from an ionic liquid.
Then in step S17, which is comparable to step S7 as disclosed with reference to
In the photo-voltaic element so obtained, the extensions 72 taper outward in a direction from the first charge carrier transport layer 30 towards the second charge carrier layer 60. As a result of the electroplating process used for the second charge carrier transport layer 60, the material thereof covers a surface of the second electrode 50 surrounding the extensions 72. Using an isotropic etching process, the openings formed will taper outward towards the second charge carrier layer 60 with an angle of approximately 45 degrees, so that the perimeter of the opening at the contact-surface of the first charge carrier transport layer is displaced with respect to the perimeter at the level of the surface of the second charge carrier transport layer is of the order of magnitude of the total thickness of the layers in which the opening is formed. For example, if the effective cross-section Deff of the opening with which the first charge carrier layer 30 is to be exposed, as defined by the mask used for etching is 1 micron, and the thicknesses of the second electrode layer 50 and the insulating layer 40 are 100 nm and 300 nm respectively, then at the plane surface of the second charge carrier transport layer 60, the cross-section Dout may be about 1.8 micron. As the electroplated second charge carrier layer 60 also has a portion 65 that extends over the tapering wall of the opening the contact surface of the second charge carrier layer 60 available for the photovoltaic layer 70 to be deposited in the next step is increased as compared to the situation in
α=(Dout−Deff)/2H.
This additional surface At is illustrated as the hatched are At in
This is compared with the situation in
Ac=½παDH+πα2H2
Hence the difference in the surface At and the surface Ac is equal to
ΔA=At−Ac=π(1−α/2)DH+πα(1−α)H2
Accordingly, if α is in a range between 0 and 1, the contact surface area of the second charge carrier layer 60 is always improved. Furthermore an improvement may be obtained in the range 1<α<2, provided that:
π(1−α/2)D>πα(1−α)H. It is noted that the height of the second charge carrier transport layer 60 typically is substantially smaller than the height of the second electrode layer. However, for visibility the height of this layer 60 is exaggerated.
An alternative embodiment of the method is illustrated in
The preparatory steps with which the semi-finished product as shown in
It is still further possible that only the first charge-carrier layer 30 is deposited by electro-plating. For example, starting from a semi-finished product, differing from the semi-finished product of
While the invention has been illustrated and described in detail in the drawings and foregoing description, such illustration and description are to be considered illustrative and exemplary and not restrictive; the invention is not limited to the disclosed embodiments. Other variations to the disclosed embodiments can be understood and effected by those skilled in the art in practicing the invention, from a study of the drawings, the disclosure and the appended claims.
In the claims the word “comprising” does not exclude other elements or steps, and the indefinite article “a” or “an” does not exclude a plurality. A single processor or other unit may fulfill the functions of several items recited in the claims. The mere fact that certain measures are recited in mutually different claims does not indicate that a combination of these measures cannot be used to advantage. Any reference signs in the claims should not be construed as limiting the scope.
Number | Date | Country | Kind |
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17166454.3 | Apr 2017 | EP | regional |
This application is a divisional of U.S. application Ser. No. 16/604,756 filed Oct. 11, 2019, which is a U.S. National Stage application under 35 U.S.C. § 371 of International Application PCT/NL2018/050224 (published as WO 2018/190711A1), filed Apr. 12, 2018, which claims the benefit of priority to EP 17166454.3, filed Apr. 13, 2017. Benefit of the filing date of each of these prior applications is hereby claimed. Each of these prior applications is hereby incorporated by reference in its entirety.
Number | Date | Country | |
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Parent | 16604756 | Oct 2019 | US |
Child | 18370622 | US |