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    • 专利摘要:
    DYE SENSITIZED SOLAR CELL AND METHOD FOR SOLAR CELL MANUFACTURING. The present invention relates to a dye-sensitized solar cell including a light absorbing layer (1), a first conductive layer (2) for extracting photogenerated electrons from the light absorbing layer, a counter electrode including a second conductive layer (3), a porous insulating layer (5b) disposed between the first and second conductive layers, and a conductive means for transferring charges between the counter electrode and the operating electrode. The solar cell further comprises a third conductive layer (6b) arranged between the porous insulating layer (5b) and the second conductive layer (3), and in electrical contact with the second conductive layer, and the third conductive layer includes a porous substrate ( 8) made of an insulating material and conductive particles accommodated in the pores of the porous substrate, forming a conductive network (9) across the insulating material.
    公开号:BR112015028867B1
    申请号:R112015028867-7
    申请日:2014-05-16
    公开日:2022-02-01
    发明作者:Henrik Lindstrom；Giovanni Fili
    申请人:Exeger Operations Ab；
    IPC主号:
    专利说明:

    FIELD OF THE INVENTION
    [001] The present invention relates to a dye-sensitized solar cell. Furthermore, the invention relates to a method of manufacturing dye-sensitized solar cells. STATUS OF THE TECHNIQUE
    [002] Dye-sensitized solar cells (DSC) have been the focus of developmental studies for the past 20 years and work on similar principles to photosynthesis. Unlike silicon solar cells, these cells obtain energy from sunlight using dyes that are inexpensive to manufacture, are not harmful to the environment, and can be found in abundance.
    [003] A conventional dye-sensitized solar cell, of the sandwich type, presents a layer of porous TiO2 electrode of a few μm in thickness, deposited on a transparent conductive substrate. The TiO2 electrode comprises interconnected metal oxide (TiO2) particles, stained by dye-absorbing molecules from the surface of the TiO2 particles, thereby forming an operational electrode. The transparent conductive substrate is normally a transparent conductive oxide deposited on a glass substrate. The transparent conductive oxide layer serves the function of an electron collector, extracting photogenerated electrons from the operating electrode. The TiO2 electrode is placed in contact with an electrolyte and another transparent conductive substrate, that is, a counter electrode.
    [004] Sunlight is harvested by the dye, producing photo-excited electrons that are injected into the conduction range of the TiO2 particles, and then collected by the conductive substrate. At the same time, certain ions (I-) in the redox electrolyte reduce the oxidized dye and transport the generated electron acceptor species to the counter electrode. The two conductive substrates are sealed at the edges in order to protect the dye-sensitized solar cell (DSC) modules from the surrounding atmosphere and to prevent evaporation or leakage of the DSC components inside the cell.
    [005] During the last 5-10 years, a new type of DSC has been developed - solid-state dye-sensitized solar cells. In this case, the liquid electrolyte is replaced by one of several solid hollow conductive materials, such as CuI, CuSCN, P3HT or Spiro-OMeTAD. The fabrication of Solid State DSCs with 15% efficiency was achieved using a hybrid organic-inorganic perovskite dye (CH3NH3PbI3).
    [006] Chung et al, in Nature Publication, volume 485, mention a dye-sensitized solar cell having a perovskite semiconductor (CsSnI3) hollow conductor, rather than a liquid electrolyte.
    [007] Patent document WO2013/171520 describes an optoelectric device having a photoactive layer comprising a porous perovskite material or a porous lattice-like material, coated with a semiconductor comprising perovskite and a charge-carrying material (cast or electron-carrying material). ), which is arranged inside the pores of the porous material, so as to be in contact with the perovskite semiconductor. The perovskite material is reported to typically act as a light-absorbing material as well as a charge-carrying semiconductor. The photoactive layer is placed between a first electrode (return contact) and a second electrode (counter electrode).
    [008] Patent document WO 2011/096154 discloses a sandwich-type DSC module, including a porous insulating substrate, an operating electrode, including a porous conductive metal layer, formed on top of the porous insulating substrate, and creating an electron collector in the form of a return contact, and a porous semiconductor layer containing an adsorbed dye disposed on top of the porous conductive metal layer, a transparent substrate opposing the porous semiconductor layer, adapted to withstand the sun and transmit sunlight to the layer porous semiconductor. The DSC module further includes a counter electrode, including a conductive substrate disposed on a side opposite the porous semiconductor layer of the insulating substrate, and at a distance from the porous insulating substrate, thereby forming a space between the porous insulating substrate and the conductive substrate. An electrolyte is disposed in the space between the working electrode and the counter electrode. The porous conductive metal layer can be created using a paste comprising metallic or metal-based particles, which is applied on top of the porous insulating substrate by etching, followed by heating, drying and baking. An advantage of this type of dye-sensitized solar cell (DSC) module is that the conductive layer of the operating electrode is arranged between the porous insulating substrate and the porous semiconductor layer. Thus, the conductive layer of the operating cell does not need to be transparent, it can be made of a high conductivity material, which increases the current handling capability of the DSC module and guarantees a high efficiency of said module.
    [009] Figure 1 shows an example of a monolithic dye-sensitized solar cell, cited by the state of the art, comprising an operational electrode in the form of a light absorbing layer (1), a first conductive layer (2) for extracting photogenerated electrons from the light-absorbing layer, a porous insulating substrate (4), and a counter electrode, including a second conductive layer (3) disposed on the opposite side of the porous insulating substrate (4). The light absorbing layer (1) may include a porous metal oxide, with light absorbing material deposited on a top side. The porous insulating substrate (4) is, for example, made of a ceramic microfiber. The first conductive layer (2) is a layer of a porous conductive material deposited on one side of the porous insulating substrate (4). The second conductive layer (3) is a layer of a conductive material deposited on the other side of the porous insulating substrate (4). The first and second conductive layers, for example, are etched onto the porous insulating substrate. The porous insulating substrate is electrically insulating. Both conductive layers (2, 3) consist of particles that are large enough not to penetrate the pores of the porous substrate. The substrate (4) serves the function of separating the conductive layers physically and electrically, in order to avoid direct electronic short circuit between the conductive layers (2, 3). Furthermore, to allow the first and second conductive layers (2, 3) to be etched onto the porous substrate, the porous substrate must be suitable for etching.
    [0010] The electrode configuration in figure 1 is infiltrated with an electrically conductive medium into the pores of the light-absorbing layer, the pores of the first and second conducting layers, and the pores of the porous substrate (not shown in figure 1). The conductive medium forms a continuous layer within the pores of the recording layers, and between the conductive layers, within the pores of the porous insulating substrate, thereby enabling the transport of electrical charge between the counter electrode and the operating electrode, including the light-absorbing layer (1). The first conductive layer extracts electrons from the light-absorbing layer and transports the electrons through an electrical circuit external to the counter electrode (not shown in figure 1). The counter electrode is used to transfer electrons to the conducting medium. The conductive medium transfers the electrons back to the light-absorbing layer, thereby completing the electrical circuit.
    [0011] Depending on the nature of the conducting medium, each of the ions, electrons and voids acting as electrons can be transported between the counter electrode and the light-absorbing layer of the operating electrode. Examples of electrolytes include liquid electrolytes (such as those based on (I-/I3-), redox coupling or cobalt complexes such as redox coupling), gel electrolytes, dry polymer electrolytes, and ceramic solid electrolytes. When ionic charge-carrying materials are used as the conductive medium, the counter electrode is normally equipped with a catalytic substance, which is intended to facilitate the transfer of electrons to the electrolyte.
    [0012] Semiconductors can be used as a conducting medium to transport electrons and voids acting as electrons between the counter-electrode a and the light-absorbing layer of the operating electrode. Examples of semiconductors include inorganic semiconductors such as CuSCN or CuI and organic semiconductors such as Spiro-OMeTAD. When semiconductors are used as the conducting medium, the counter electrode is normally equipped with a substance which is intended to create a satisfactory electrical contact, that is, a satisfactory low ohmic resistance contact between the counter electrode and the conducting medium. . Examples of materials for such contacts include, for example, gold, silver, carbon-containing materials such as, for example, graphite or graphene, and highly conductive metal oxides such as aluminum-doped FTO, ITO or ZnO, or conductive polymers, such as PEDOT:PSS, polythiophene, polyacetylene, polyaniline, polypyrrole, etc. An advantage of using semiconductors as the conductive medium in a solar cell is that they are solid, so there is less risk of leakage. A disadvantage of using semiconductors is their poor conductivity.
    [0013] The conductive medium exhibits a certain electrical resistance to the transport of charges. Electrical resistance increases with the distance the charge is carried. Therefore, when electrical charge is carried between the counter electrode and the light-absorbing layer, there will always be some loss of electrical resistance in the conducting medium. By making the thinnest porous substrate, resistive losses can be reduced. However, as the porous substrate becomes thinner, it also becomes mechanically more fragile.
    [0014] Certain conductive media, such as semiconductors, ionic liquid based electrolytes and cobalt complex electrolytes, may have a very low electrical conductivity, which results in large electrical resistive losses. PURPOSE AND SUMMARY OF THE INVENTION
    [0015] The objective of the present invention is to provide a monolithic dye-sensitized solar cell, having reduced resistive losses in the conductive medium.
    [0016] This objective is achieved by means of a dye-sensitized solar cell, as defined by the description of claim 1.
    [0017] The dye-sensitized solar cell comprises:- a light-absorbing layer;- a first conductive layer for extracting photogenerated electrons from the light-absorbing layer;- a counter electrode including a second conductive layer; - a porous insulating layer arranged between the first and second conductive layers; and- a third conductive layer disposed between the porous insulating layer and the second conductive layer, and in electrical contact with the second conductive layer, and the third conductive layer includes a porous substrate made of an insulating material and conductive particles forming a conductive network through the insulating material; and - a conductive means for transferring charges between the counter electrode and the light absorbing layer.
    [0018] The expression "conductive particles forming a conductive network through the insulating material" here means that the particles form one or more electrically conductive paths through the insulating material in the layer.
    [0019] Due to the conductive network in the porous substrate, the distance between the counter electrode and the light absorbing layer no longer depends on the thickness of the porous substrate. Thus, the thickness of the insulating layer can be reduced and due to this, the distance between the counter electrode and the light absorbing layer can be reduced. Consequently, resistive losses in the conducting medium are reduced. Due to the fact that the distance between the counter electrode and the light absorbing layer no longer depends on the thickness of the porous substrate, it is also possible to use a substrate that is thick enough to guarantee mechanical handling.
    [0020] The conductive network provides an extension of the counter electrode, which extends into the porous substrate. The present invention makes it possible to provide a minimum distance between the light absorbing layer and the counter electrode, in order to obtain minimum resistive electrical losses in the conductive medium.
    [0021] The porous substrate manipulated during the manufacture of the solar cell will be the porous substrate of the third conductive layer, or an integral substrate comprising the porous substrate of the third conductive layer and the porous insulating layer. Thus, the substrate to be manipulated can have an adequate thickness and the porous insulating layer that prevents short circuits between the first and second conductive layers can be thin and resistive electrical losses can be minimized.
    [0022] The porous insulating layer prevents short circuit between the first and second conductive layers. The conductive particles in the third conductive layer form a conductive network across the insulating material of the substrate. The conductive network is in electrical contact with the second conductive layer of the counter electrode and will therefore significantly increase the conductive surface area of the counter electrode. The conductive surface area serves the function of transferring electrons or voids acting as electrons from the counter electrode to the conducting medium. A conductive network in the substrate and thus an increase in the conductive surface area of the counter electrode decreases the charge transfer resistance between the conductive medium and the counter electrode. Furthermore, since the third conductive layer forms a conductive network extending through the insulating material of the substrate, the distance between the light-absorbing layer and the third conductive layer is shorter than the distance between the light-absorbing layer. and the second conductive layer. Consequently, since the third and second conductive layers are in electrical contact, the effective distance between the light absorbing layer and the second conductive layer is shorter and the resistive losses in the conductive medium are therefore reduced.
    [0023] The present invention makes it possible to design the porous insulating layer with an optimal thickness, depending on the requirements, strength and mechanical properties of the insulating layer. An advantage obtained by the present invention is that it is possible to have a thin porous insulating layer disposed between the first and second conductive layers, and still use a thick porous substrate having sufficient and satisfactory mechanical properties for etching the first and second conductive layers. Thus, the invention enables the use of a thick porous substrate and still manages to obtain minimal resistive electrical losses in the conductive medium.
    [0024] A further advantage of the present invention is that the efficiency of the counter electrode is increased due to the fact that the third conductive layer increases the surface of the counter electrode.
    [0025] Another advantage obtained by the present invention is that the efficiency of the counter electrode is increased due to the fact that the third conductive layer increases the surface of the counter electrode.
    [0026] An additional advantage obtained with the present invention is that the effective distance between the low absorption layer and the second conductive layer is reduced and, therefore, the resistive losses in the conductive medium are reduced, as well as a resulting greater efficiency of the solar cell.
    [0027] Another advantage obtained by the present invention is that it becomes possible to use the conductive medium having low electrical conductivity, such as hollow solid state conductors, ionic liquid based electrolytes or cobalt complex based electrolytes.
    [0028] The size of the conductive particles in the third counter electrode is smaller than the pore size of the porous substrate, and the conductive particles are accommodated in the pores of the porous substrate.
    [0029] Preferably, the porous insulating layer is thinner than the porous substrate. Preferably, the porous insulating layer is also thinner than the third conductive layer.
    [0030] The porous substrate that extends from the second conductive layer to the porous insulating layer comprises infiltrated conductive particles. The porous insulating layer extends from the porous substrate to the first conductive layer and may be formed as an integral part of the porous substrate, or be a separate layer from the porous substrate.
    [0031] The conductive medium for transferring charges between the counter electrode and the light absorbing layer may be any suitable conductive medium. Charges in the form of ions, or electrons, or voids acting as electrons can be transported between the counter electrode and the light-absorbing layer. The conductive medium can be a liquid, for example a liquid electrolyte, a gel, or a solid material such as a semiconductor.
    [0032] The conductive medium for transferring charges is arranged between the pores of the porous materials of the light-absorbing layer, the first conductive layer, the porous insulating layer and the porous substrate.
    [0033] The solar cell preferably is a monolithic dye-sensitized solar cell. A monolithic dye-sensitized solar cell is characterized by the fact that all layers are directly or indirectly deposited on a single porous substrate.
    [0034] The first and second conductive layers are positioned on a dark side of the light absorbing layer, that is, the side opposite to the side that receives the light. Thus, the first and second conductive layers are positioned on the same side as the light absorbing layer.
    [0035] According to an embodiment of the invention, the porous insulating substrate comprises woven microfibers. Woven microfibers are mechanically strong. Preferably, the woven microfibers are ceramic microfibers, such as glass fibers. A microfiber is a fiber having a diameter less than 10 μm and a length greater than 1 nm. Ceramic microfibers are fibers made of a refractory and inert material, such as glass, SiO2, Al2O3 or aluminosilicate. The porous substrate may further comprise non-woven microfibers. The non-woven microfibers may, for example, be organic microfibers. Organic microfibers are fibers made of organic materials, such as polymers, for example, polycaprolactone, PET, PEO, etc., or of cellulose, such as, for example, nanocellulose (MFC) or wood pulp. The non-woven microfibers can also be inorganic, such as, for example, glass, SiO2, Al2O3 or aluminosilicate microfibers.
    [0036] According to an embodiment of the invention, the thickness of the third conductive layer is less than 1 mm, preferably less than 100 μm. Due to the fact that the third conductive layer is quite thin, the conductivity requirement of the third conductive layer is quite low, being lower than the conductivity requirement of the first and second conductive layers. Thus, the network of conductive particles obtains sufficient conductivity.
    [0037] According to an embodiment of the invention, the thickness of the porous insulating layer is between 0.1 μm and 20 μm, preferably between 0.5 μm and 10 μm. Resistive electrical losses in the conductive medium are reduced and, in this way, a short circuit is avoided between the first and third conductive layers.
    [0038] The thickness of the first conductive layer is advantageously also kept thin, in order to have a short distance between the light absorbing layer and the third conductive layer and the counter electrode. The thickness of the first conductive layer can be between 0.1 and 40 μm, preferably between 0.3 and 20 μm.
    [0039] According to an embodiment of the invention, the conductive particles in the third conductive layer are made of the same material used in the second conductive layer. Conductive particles can be made of metal, metal alloy, metal oxide or other conductive materials, for example titanium, titanium alloys, nickel, nickel alloys, carbon-based materials, conductive oxides, conductive nitrides, conductive carbides , conductive silicides, or mixtures thereof. For example, the conductive particles in the third conductive layer are made of a material selected from the group consisting of titanium, titanium alloys, nickel, nickel alloys, carbon-based materials such as, for example, graphene or graphite, or black of smoke, or carbon nanotubes, conductive oxides, conductive nitrides, conductive carbides, conductive silicides, or mixtures thereof. Conductive particles can also be catalytic.
    [0040] Preferably, the first and second conductive layers are made of a material selected from the group consisting of titanium, titanium alloys, nickel, nickel alloys, graphite and amorphous carbon, or mixtures thereof. More preferably, the conductive layers (2, 3) are made of titanium or titanium alloy, or mixtures thereof. Other types of platinized conductive particles can be used instead of FTO, eg ATO, ITO, graphite, carbon black, graphene or carbon nanotubes. Furthermore, it is possible to use particles which are both conductive and catalytic, such as, for example, metal carbides, metal nitrides and metal silicides.
    [0041] According to an embodiment of the invention, the porous insulating layer is a part of the porous substrate. The solar cell comprises a porous substrate made of an insulating material and comprises a first portion including said conductive particles, plus a second portion without any conductive particles, wherein the first portion forms said third conductive layer and the second portion forms the said porous insulating layer. The second portion of the porous substrate may be thinner than the first portion of the porous substrate. In this embodiment, the third conductive layer and the porous insulating layer are different parts of the same porous substrate. Thus, the porous insulating layer may be formed as an integral part of the porous substrate or be a separate layer from the porous substrate. The portion of the substrate comprising the conductive particles extends from the second conductive layer towards the first conductive layer, and terminates at a distance from the top side of the substrate, to form the porous insulating layer. An advantage of this modality is that it is easy to manufacture.
    [0042] According to an embodiment of the invention, the porous insulating layer is arranged on one side of the porous substrate, and the second conductive layer is arranged on the opposite side of the porous substrate. For example, the porous insulating layer is etched onto the porous insulating substrate. In this embodiment of the invention, the porous insulating layer is formed as a separate layer over the porous substrate.
    [0043] According to an embodiment of the invention, the solar cell is characterized in that it comprises a porous substrate extending from the second conductive layer to a porous insulating layer, comprising conductive particles that form a conductive network in electrical contact with the second layer. conductive.
    [0044] According to an embodiment of the invention, the porous substrate and the porous insulating layer are formed as integral layers of an insulating material.
    [0045] According to an embodiment of the invention, the porous insulating layer is a separate layer disposed over the porous substrate, where the porous insulating layer and the porous substrate are made of an insulating material.
    [0046] According to an embodiment of the invention, the porous insulating layer and the porous substrate comprise an insulating material comprising woven microfibers. Woven microfibers include suitable pores to accommodate the conductive particles. The porous insulating layer may include non-woven microfibers.
    [0047] According to an embodiment of the invention, the conductive medium is an electrolyte based on cobalt complex. An advantage of using a cobalt complex based electrolyte is its high efficiency.
    [0048] According to an embodiment of the invention, the conductive medium is an electrolyte based on ionic liquid. An advantage of using an ionic liquid based electrolyte is that it can provide high long term stability for solar cell performance.
    [0049] According to an embodiment of the invention, the conductive medium is a solid-state hollow conductor. A hollow solid-state conductor is, for example, a semiconductor. An advantage of using a hollow conductor is that it is a solid material and consequently the sealing requirement of the solar cell is reduced. Examples of semiconductors include inorganic semiconductors such as CuSCN or CuI and organic semiconductors such as P3HT or Spiro-OMeTAD.
    [0050] According to one embodiment of the invention, the conductive medium is a solid-state hollow conductor or an ionic liquid-based electrolyte or a cobalt complex-based electrolyte. Semiconductors based on perovskites, such as CH3NH3PbI3, CH3NH3PbI3-xClx, or CH3NH3SnI3, or based on other suitable perovskites can be used.
    [0051] According to an embodiment of the invention, the light-absorbing layer comprises a perovskite, such as, for example, CH3NH3PbI3, CH3NH3PbI3-xClx, or CH3NH3SnI3. In addition, other suitable perovskites can be used. An advantage of using perovskite is that high efficiencies of solar cells can be achieved.
    [0052] According to an embodiment of the invention, a layer of perovskite can be applied directly over a first conductive layer of titanium and with the titanium having a surface layer of TiO2. Thus, the separate TiO2 nanoparticle layer can be omitted.
    [0053] According to one embodiment of the invention, the light-absorbing layer is a porous layer of TiO2 nanoparticle with an adsorbed organic dye. Examples of organic dyes include: N719, N907, B11, C101. In addition, other organic dyes can be used.
    [0054] A monolithic dye-sensitized solar cell can be manufactured by depositing a first conductive layer on one side of a porous insulating substrate, and a counter electrode, including a second conductive layer, on the other side of the porous insulating substrate. . The light absorbing layer can be deposited on top of the first conductive layer. This structure has several advantages, such as ease of mass production and provision of a well-defined and constant distance between the second conductive layer and the light-absorbing layer. The choice of a conductive medium for transferring charges between the counter electrode and the light-absorbing layer is limited by the resistive losses in the conductive medium. By minimizing the distance between the counter electrode and the light absorbing layer, it is possible to minimize resistive loss. By making the thinner porous substrate, resistive losses can be reduced and the use of conductive medium for transferring charges having high resistive losses will not be restricted. However, very thin porous substrates are difficult to handle and may not have adequate mechanical strength for handling in a production facility.
    [0055] Another object of the present invention is to provide a method of manufacturing a monolithic dye-sensitized solar cell as described by the invention.
    [0056] This object is achieved by a method as defined in claim 17. The method comprises:- depositing a blocking agent on a top side of a porous substrate made of an insulating material, so as to form a blocking layer in a portion of the substrate;- infiltrating the porous substrate from one side of the substrate base with conductive particles having a size smaller than the pore size of the substrate, to form a third conductive layer on a second portion of the substrate;- depositing a ink comprising conductive particles on the upper side of the insulating substrate to form the first conductive layer; - depositing an ink comprising conductive particles on the base side of the porous substrate to form the second conductive layer; e- heat treating the substrate to burn off the blocking layer, thereby forming the porous insulating layer.
    [0057] The order of method steps may vary within the scope of the claims. Thus, for example, the second conductive layer can be made before the first conductive layer.
    [0058] An advantage of this method is that it is easy to manufacture the dye-sensitized solar cell according to the invention.
    [0059] According to an embodiment of the invention, the blocking agent comprises fibers having a diameter between 1 nm and 5 μm.
    [0060] The blocking layer can consist of polymers, ceramic particles, glass fibers, polymer fibers, carbon nanotubes (CNT), nanocellulose or microfibrillated cellulose (MFC). It is advantageous to use fibers as a blocking agent in said blocking layer. Also, it is advantageous to use fibers of very small diameter.
    [0061] This objective is achieved by a method as defined in claim 19.
    [0062] The method comprises:- providing a porous substrate made of an insulating material;- infiltrating the porous substrate from one side of the substrate base;- infiltrating the porous substrate with conductive particles having a size smaller than the pore size of the substrate, so as to form a third conductive layer; - depositing a layer of insulating material on a top side of the porous substrate to form the porous insulating layer; - depositing a porous conductive layer on top of the porous insulating layer, to form the first conductive layer; and - depositing an ink comprising conductive particles on one side of the base of the insulating substrate to form the second conductive layer.
    [0063] The order of the method steps may vary within the scope of the claims. Thus, for example, the second conductive layer can be made before the first conductive layer. For example, the deposition of a porous conductive layer consists of the deposition of an ink comprising conductive particles.
    [0064] The porous insulating layer can be deposited onto the porous substrate by means of screen etching, die groove coating, spraying or wet deposition. The first conductive layer and the second conductive layer can be deposited, for example, by etching. Alternatively, the first conductive layer may be formed by evaporating or sputtering a layer of titanium onto the porous insulating layer, or any other method of depositing a thin layer of titanium onto the porous insulating layer.
    [0065] Alternatively, the first and second conductive layers may be formed by evaporating or sputtering a layer of titanium onto the porous insulating substrate, or by any other method of deposition of a thin layer of titanium onto a porous insulating substrate.
    [0066] The light-absorbing layer is formed, for example, by deposition of a porous layer of TiO2 on the first conductive layer and, after that, adsorbing a dye onto the TiO2 layer.
    [0067] In an alternative embodiment, a layer of perovskite is directly formed over the first conductive layer after the first conductive layer has been treated, so that the surface of the first conductive layer is made of a TiO2 film. BRIEF DESCRIPTION OF THE DRAWINGS
    [0068] The invention will now be explained in more detail by describing different modalities, and referring to the attached figures. Figure 1 shows a dye-sensitized solar cell according to the prior art citation. Figure 2 shows an example. of a dye-sensitized solar cell according to the invention. Figure 3 shows another example of a dye-sensitized solar cell in accordance with the invention. Figure 4 illustrates an example of a method of manufacturing a dye-sensitized solar cell in accordance with the invention. DETAILED DESCRIPTION OF PREFERRED MODALITIES OF THE INVENTION
    [0069] Figure 2 shows a first example of a dye-sensitized solar cell according to the invention. The dye-sensitized solar cell comprises an operating electrode in the form of a light absorbing layer (1), a first conductive layer (2) for extracting photogenerated electrons from the light absorbing layer (1), a counter electrode including a second conductive layer (3), a porous insulating layer (5a) disposed between the first and second conductive layers, and a conductive means (not shown) for transferring charges between the counter electrode and the operating electrode. The solar cell further comprises a third conductive layer (6a) arranged between the porous insulating layer (5a) and the second conductive layer (3), and in electrical contact with the second conductive layer (3).
    [0070] The third conductive layer (6a) includes a porous substrate (4) made of an insulating material and conductive particles (7), forming a conductive network across the porous substrate (4). The conductive particles are arranged in pores of the porous substrate (4). The porous insulating layer (5a) is suitably formed by etching a layer of insulating material onto a top side of the porous substrate (4). The insulating material is, for example, an inorganic material that is positioned between the first and third conductive layers, insulating the first and third conductive layers from each other, and creating a porous insulating layer between the first and third conductive layers, after a heat treatment. . The porous substrate (4) extends from the second conductive layer (3) to the porous insulating layer (5a). In this embodiment, the porous insulating layer (5a) is a separate layer disposed on one side of the porous substrate (4). The first conductive layer (2) is, for example, formed by etching conductive particles onto the porous insulating layer (5a). Suitably, all layers (1, 2, 3 and 5a) are formed by embossing. The porous insulating layer (5a) is, for example, made of ceramic microfibers or materials derived from the delamination of layered crystals, such as 2D materials or nano-blades.
    [0071] Figure 3 shows a second example of a dye-sensitized solar cell according to the invention. The dye-sensitized solar cell comprises an operating electrode in the form of a light-absorbing layer (1), a first conductive layer (2), a counter electrode including a second conductive layer (3), and a porous substrate (8). ) made of an insulating material. The porous substrate (8) comprises a first portion (8a), including conductive particles (9) that form a conductive network in the insulating material of the porous substrate, and a second portion (8b) without any conductive particles, forming a porous insulating layer ( 5b). Thus, the first portion (8a) forms a third conductive layer (6b), and the second portion (8b) forms a porous insulating layer (5b). In this embodiment, the porous insulating layer (8b) is formed as an integral part of the porous substrate (8).
    [0072] The conductive layers (2, 3, 6a, 6b) are porous to allow a conductive medium to penetrate through the conductive layers. Suitably, the conducting medium is a solid-state hollow conductor, or an ionic liquid-based electrolyte or a cobalt complex-based electrolyte.
    [0073] However, the conductive medium may be any suitable conductive medium. The conductive medium may be a liquid, a gel or a solid material, such as a semiconductor. Examples of electrolytes include liquid electrolytes (such as electrolytes based on (I-/I3-), redox coupling or cobalt complexes such as redox coupling), gel electrolytes, dry polymer electrolytes, and ceramic solid electrolytes. Examples of semiconductors include inorganic semiconductors such as CuSCN or CuI and organic semiconductors such as Spiro-OMeTAD.
    [0074] The porous substrate (4, 8) is, for example, made of microfibers. A microfiber is a fiber having a diameter less than 10 μm and a length greater than 1 nm. Suitably, the porous substrate comprises woven microfibers. Ceramic microfibers are fibers made from a refractory, inert material such as glass, SiO2, Al2O3 and aluminosilicate. Organic microfibers are fibers made from organic materials, such as polymers, for example, polycaprolactone, PET, PEO, etc., or cellulose, such as, for example, nanocellulose (MFC) or wood pulp. The porous substrate (4, 8) may comprise microfibers and non-woven microfibers arranged on the woven microfibers. The thickness of the porous substrate (4, 8) is suitably between 10 μm and 1 mm. This type of layer provides the required mechanical strength.
    [0075] The porous substrate (4, 8) is infiltrated by conductive particles (7), so that a conductive network is formed through the insulating material and, due to this, the third conductive layer (6a, 6b) is obtained. The network of electrical particles in the third layer is in electrical contact with the second conducting layer (3). The porous insulating layer (5a, 5b) prevents short circuiting between the first and second conductive layers. The conductive particles must be smaller than the pore size of the substrate (4, 8) in order to be effectively infiltrated. The conductive particles form a conductive network (7, 9) through the insulating material of the substrate. The conductive network (7, 9) is in direct physical and electrical contact with the second conductive layer (3) of the counter electrode. Conducting particles serve the function of transferring electrons from the counter electrode to the conducting medium. Resistive losses in the conductive medium are reduced due to the conductive network in the substrate. Thus, it is possible to use a thick porous substrate and still obtain minimal electrical resistive losses in the conductive medium.
    [0076] Since the network of conductive particles is in direct physical and electrical contact with the counter electrode and at the same time is infiltrated some distance into the substrate, it is possible for the counter electrode to transfer electrons through the particles. conductors to the conductive medium, effectively closer to the light absorbing layer, resulting in a smaller effective distance between the counter electrode and the light absorbing layer. Therefore, electrical losses in the conductive medium can be reduced by infiltrating conductive particles into the substrate. In case a semiconductor with low electronic conductivity is used as the conducting medium, it is necessary to infiltrate the semiconductor through the light absorbing layer and through the current collecting layer and into the porous substrate to a sufficient depth so that the semiconductor is placed in direct physical and electrical contact with the infiltrated conductive particles.
    [0077] Preferably, the thickness (t1) of the third conductive layer (6a, 6b) is less than 1 mm, more preferably less than 100 µm. In this example, the porous substrate (4) was infiltrated with conductive particles on one side of the base. Conductive particles can also be catalytic. Conductive particles can be made of metal, metal alloy, metal oxide, and other conductive materials, for example titanium, titanium alloys, nickel, nickel alloys, carbon-based materials, conductive oxides, conductive nitrides, carbides conductors, conductive silicides, or mixtures thereof.
    [0078] Electrical contact between the first conductive layer and the second conductive layer is prevented by the porous insulating layer (5a, 5b). For example, the thickness(t2) of the porous insulating layer is between 0.1 μm and 20 μm, preferably between 0.5 μm and 10 μm.
    [0079] The conductive layers (2, 3, 6a, 6b) are porous to allow the conductive medium to penetrate through the conductive layers. The material forming the conductive layers (2, 3) must have adequate corrosion resistance to withstand the environment in the solar cell, preferably also be resistant to temperatures above 500°C in air, without loss of adequate conductivity. Preferably, the conductive layers (2, 3) are made of a material selected from the group consisting of titanium, titanium alloys, nickel, nickel alloys, graphite and amorphous carbon, or mixtures thereof. More preferably, the conductive layers (2, 3) are made of titanium or a titanium alloy, or a mixture thereof.
    [0080] Preferably, the thickness (t1) of the first conductive layer (2) is between 0.1 and 40 μm, preferably between 0.3 and 20 μm.
    [0081] The light absorbing layer (1) of the operating electrode may include a porous TiO2 electrode layer, deposited over the first conductive layer (2). The TiO2 electrode layer may comprise TiO2 particles dyed by dye adsorbing molecules on the surface of the TiO2 particles. Alternatively, the first conductive layer has a TiO2 surface layer and the light absorbing layer is a perovskite layer. The porosity of the porous substrate will enable the transport of electrical charge through the substrate.
    [0082] Next, a method of manufacturing a first example of a solar cell according to the invention is described.
    [0083] A porous substrate (4) made of an insulating material is infiltrated with conductive particles having a size smaller than the pore size of the substrate, to form a third conductive layer. The substrate is infiltrated so that a network of conductive particles is formed across the entire length of the substrate. A layer of insulating material is deposited on one side of the porous substrate to form a porous insulating layer. The insulating material consists, for example, of microfibers, made of a ceramic or organic material. An ink comprising conductive particles is deposited on the porous insulating layer to form the first conductive layer, and an ink comprising conductive particles is deposited on the opposite side of the porous substrate to form the second conductive layer. The porous insulating layer is, for example, deposited onto the porous substrate by screen etching, die groove coating, spraying or wet deposition. The first and second porous conductive layers are, for example, deposited onto the porous substrate by means of screen etching or any other suitable etching technique.
    [0084] In the following, an example of a manufacturing method of the second example of a solar cell according to the invention is described with reference to Figure 4. Figure 4 illustrates the deposition sequence in the manufacturing method.
    [0085] Step 1: A blocking agent is deposited onto a top side of a substrate (8) made of an insulating material, to form a blocking layer (10) on a second portion (8b) of the substrate (8). The blocking layer is deposited in order to physically prevent the conductive particles from being infiltrated in any way on the other side of the substrate. Therefore, the blocking layer (10) prevents direct physical and electrical contact between the first conductive layer and the conductive particles. The blocking layer can consist of polymers, ceramic particles, polymer fibers, glass fibers, carbon nanotubes (CNT), nanocellulose or microfibrillated cellulose (MFC). It is advantageous to use fibers as a blocking agent in the blocking layer. Also, it is advantageous to use very small diameter fibers.
    [0086] Step 2: The porous substrate (8) is infiltrated from one side of the substrate base with conductive particles having a size smaller than the pore size of the substrate, to form a third conductive layer (6b) in a first portion (8a) of the substrate. The conductive particles may consist of the same material used in the second conductive layer. Also, it is possible to use other types of particles, such as carbon-based materials (graphite, carbon black, CNT, graphene, etc.). Furthermore, it is also possible to use other types of particles, such as conductive oxides (ITO, FTO, ATO, etc.), or carbides, nitrides or silicides.
    [0087] Step 3: An ink comprising conductive particles is etched onto the top side of the porous substrate (8) to form the first conductive layer (2).
    [0088] Step 4: An ink comprising conductive particles is etched on the base side of the porous substrate (4) to form the second conductive layer (3).
    [0089] Step 5: A layer of TiO2 electrode is deposited over the first conductive layer (2) to form the operating electrode (1).
    [0090] Step 6: the substrate is heat treated to burn off the blocking layer (10), thereby forming the porous insulating layer (5b).
    [0091] Next, two more detailed examples of methods of manufacturing a solar cell according to the invention will be described. EXAMPLE 1:
    [0092] Dye Sensitized Solar Cell (DSC) based on Redox Liquid Electrolyte
    [0093] In the first step, a 28 μm thin glass fabric (MS1037, available from Asahi Kasei E-materials) was obtained wet with a solution of glass microfiber raw material containing C glass microfiber (diameter of 0.5 μm fiber) and water-based colloidal silica. The wet glass fabric was then dried at 110°C for 5 minutes with air in a belt oven.
    [0094] Then, in a second step, the glass fabric deposited as glass microfiber was then wet produced with a solution containing dispersed glass microfibers and nanocellulose on the other side in order to create a blocking layer. The nanocellulose that was added to the second fiberglass raw material serves the function of creating a blocking layer, which prevents conductive particles from passing through said blocking layer. The blocking effect can be intensified by increasing the amount of nanocellulose added to the fiberglass raw material. Thus, particles infiltrated into the third conductive layer can therefore be blocked by the blocking layer.
    [0095] A variation of the second step is to omit the addition of glass microfiber to the solution containing nanocellulose that is used to create the blocking layer. Another variation of the second step is to etch or spray a nanocellulose solution onto one side of the dry glass fabric treated as microfiberglass to create a blocking layer. Another variation of the second step is to use dispersed carbon nanotubes or a dispersed 2D material, instead of nanocellulose, in order to create a blocking layer.
    [0096] Then, in a third step, a paint containing platinized FTO particles was prepared by first mixing 80 mm diameter FTO particles with a solution of hexachloroplatinic acid in isopropanol, then drying the mixture at a temperature of 60°C for 30 minutes, with subsequent heating of the powder treated with air at 400°C for 15 minutes. After heat treatment, the platinized FTO powder was ground together with terpineol in a ball mill to create the final paint containing FTO particles platinized in terpineol. In the next step, the double-sided deposited glass fabric with a blocking layer was infiltrated with conductive catalytic particles by etching, e.g. screen etching, the ink containing FTO particles platinized onto the opposite non-woven glass microfiber side. next to the blocking layer. The etched ink was then allowed to air dry at 120°C for 10 minutes.
    [0097] A variation of the third step is to use other types of platinized conductive particles instead of FTO, such as, for example, ATO, ITO, graphite, carbon black, graphene or carbon nanotubes. Another variation of the third step is to use particles that are both conductive and catalytic, such as particles of metal carbides, metal nitrides and metal silicides.
    [0098] Then, in a fourth step, a paint was prepared by mixing TiH2 with terpineol, using a 50:50 weight ratio. The paint was then milled into a pearl shape for 25 minutes at a speed of 5000 rpm using 0.3 mm zirconia beads. The zirconia beads were then separated from the paint by filtration. The filtered ink was then etched onto the double-sided deposited glass fabric, having a blocking layer and a layer of infiltrated platinized FTO particles and then dried at 200°C for 5 minutes. Then, the filtered ink was etched onto the other side of the glass fabric and then dried at 200°C for 5 minutes. Subsequently, the deposited glass fabric was vacuum sintered at a temperature of 600°C. The pressure during sintering was less than 0.0001 mbar. Consequently, a first conductive layer, a second conductive layer and a third conductive layer were formed after the vacuum heating process.
    [0099] Then, in a fifth step, an ink based on TiO2 (Dyesol 18NR-T) was screen-etched on top of the first conductive layer and then dried at 120°C for 10 minutes.
    [00100] Then, in a sixth step, the treated glass fabric was heated with air at a temperature of 500°C for 20 minutes. Consequently, the deposited TiO2 layer was sintered and the nanocellulose-based blocking layer was removed by combustion.
    [00101] Then, in a seventh step, the treated glass fabric was immersed in a 1mM Z907 dye solution in methoxypropanol, heat treated at 70°C for 120 minutes, and then washed with methoxypropanol and dried. Consequently, the sintered TiO2 film was sensitized by the dye.
    [00102] Then, in an eighth step, a polymer containing a redox electrolyte based on iodide/triiodide (I-/I3-) was deposited on top of the TiO2 layer, in the form of a gel.
    [00103] Then, in a ninth step, the cell was sealed by infiltrating a polymer at the edges around the DSC, covering both sides with glass, while allowing an external electrical connection with the first conductive and second conductive layer. . EXAMPLE 2:
    [00104] Dye Sensitized Solar Cell (DSC) Based on Solid State Leaked Conductor
    [00105] In the first step, the same materials and procedures were used as in the first step of Example 1.
    [00106] Then, in a second step, the same materials and procedures were used relative to the second step of Example 1.
    [00107] Then, in a third step, a paint containing carbon particles was prepared by mixing 75 grams of graphite, 25 grams of carbon black (Super P-Li), and 15 grams of TiO2 (from 20 nm of diameter) with terpineol, with subsequent grinding of the mixture in a ball mill to produce the final ink. In the next step, the double-sided deposited glass fabric with a blocking layer was infiltrated with conductive carbon particles by etching, for example, screen etching the ink onto the non-woven glass microfiber side opposite the blocking layer side. . The engraved ink was then allowed to air dry at 120°C for 10 minutes. A variation of the third step is to use gold-plated carbon particles.
    [00108] Another variation of the third step is to use other types of particles that have sufficient conductivity and also low ohmic resistance to the hollow conductor, such as, FTO or ITO.
    [00109] Then, in a fourth step, a paint was prepared by mixing TiH2 with terpineol, using a ratio of 50:50 by weight. The paint was then milled into a pearl shape for 25 minutes at a speed of 5000 rpm using 0.3 mm zirconia beads. The zirconia beads were then separated from the paint by filtration. The filtered ink was then etched onto the double-sided deposited glass fabric, having a blocking layer and a layer of infiltrated carbon particles and then dried at 200°C for 5 minutes. Then, the filtered ink was etched onto the other side of the glass fabric and then dried at 200°C for 5 minutes. Subsequently, the deposited glass fabric was vacuum sintered at a temperature of 600°C. The pressure during sintering was less than 0.0001 mbar. Consequently, a first conductive layer, a second conductive layer and a third conductive layer were formed after the vacuum heating process.
    [00110] Then, in a fifth step, a TiO2-based ink (Dyesol 18NR-T) was screen-etched on top of the first conductive layer and then dried at 120°C for 10 minutes. The TiO2-based ink was diluted 5-fold with terpineol before etching. A variation would be to omit the fifth step and therefore omit the TiO2-based ink deposition.
    [00111] Then, in a sixth step, the treated glass fabric was heated with air at a temperature of 500°C for 20 minutes. Consequently, the deposited TiO2 layer was sintered and the nanocellulose blocking layer was removed by combustion.
    [00112] In case the TiO2 deposition is omitted in the fifth step, there is no TiO2 layer deposited to be sintered and the nanocellulose will be removed by combustion.
    [00113] Then, in a seventh step, a thin layer of a solution of organic-inorganic perovskite in dimethylformamide (CH3NH3PbI3) was ultrasonic sprayed on the TiO2 layer and dried at 125°C for 30 minutes.
    [00114] In case the TiO2 deposition is omitted in the fifth step, the organic-inorganic perovskite is sprayed directly onto the first conductive layer, after sintering the first conductive layer.
    [00115] A variation of the seventh step is to use mixed halides, eg (CH3NH3PbI3xClx).
    [00116] Another variation of the seventh step is to use tin-based perovskite, such as (CH3NH3SnI3).
    [00117] Another variation of the seventh step is to deposit the perovskite solution by the ink jet method or by die groove coating.
    [00118] Another variation of the seventh step is to deposit the perovskite in a two-step sequential process, first depositing a PbI2 solution, then drying and depositing the CH3NH3I solution with further drying, and finally heating the two dry deposits in order to to complete the reaction between PbI2 and CH3NH3I, to form CH3NH3PbI3.
    [00119] Another variation of the seventh step is to deposit the perovskite through a two-step process, first depositing SnI2 and then drying, then depositing CH3NH3I and drying, with further heating of the two deposits in order to complete the reaction between SnI2 and CH3NH3I to form CH3NH3SnI3.
    [00120] Then, in an eighth step, a solution of spiro-MeOTAD (84 mg of spiro-OMeTAD in 1 mL of chlorobenzene, mixed with 7 microliters of tert-butylpyridine and 15 microliters of LiTFSI(bis(trifluoromethanesulfonyl)imide) lithium) in acetonitrile, was ultrasonic sprayed on top of the TiO2 layer and dried for 5 minutes at 50°C.
    [00121] A variation of the eighth step is to deposit the CuI, CuSCN or P3HT solutions, instead of spiro-OmeTAD, as the hollow conductor.
    [00122] Then, in a ninth step, the cell was sealed by infiltrating a polymer on the edges around the DSC, covering both sides with glass and, at the same time, allowing an external electrical connection with the first conductive layer and second conductive layer.
    [00123] The porous insulating layer (5a) can be deposited onto the porous substrate by any etching process, eg screen etching, die groove coating, spraying or wet laying.
    [00124] The invention is not limited to the above-described embodiment, and may be varied within the scope of the appended claims. Thus, for example, the method of manufacturing a dye-sensitized solar cell can be carried out in several different ways.
    权利要求:
    Claims (21)
    [0001]
    1. Dye-sensitized solar cell, comprising: - a light absorbing layer (1); - a first conductive layer (2) for extracting photogenerated electrons from the light absorbing layer; - a counter electrode including a second conductive layer (3);- a porous insulating layer (5a; 5b) arranged between the first and second conductive layers; e- a conductive means for transferring charges between the counter electrode and the light-absorbing layer, characterized in that the solar cell further comprises a third conductive layer (6a; 6b) arranged between the porous insulating layer and the second conductive layer , and in electrical contact with the second conductive layer, and the third conductive layer includes a porous substrate (4; 8) made of an insulating material and conductive particles accommodated in the pores of the porous substrate forming a conductive network (7) across the insulating material.
    [0002]
    2. Dye-sensitized solar cell, according to claim 1, characterized in that the porous substrate (4; 8) comprises woven microfibers.
    [0003]
    3. Dye-sensitized solar cell, according to any one of the preceding claims, characterized in that the thickness (t2) of the porous insulating layer (5a; 5b) is between 0.1 μm and 20 μm, preferably between 0.5 μm and 10 μm.
    [0004]
    4. Dye-sensitized solar cell, according to any one of the preceding claims, characterized in that the thickness (t1) of the third conductive layer (6a; 6b) is less than 1 mm, preferably less than 100 μm.
    [0005]
    5. Dye-sensitized solar cell, according to any one of the preceding claims, characterized in that said conductive particles are made of the same material used in the second conductive layer (3).
    [0006]
    6. Dye-sensitized solar cell according to any one of the preceding claims, characterized in that said conductive particles are made of a material selected from a group consisting of titanium, titanium alloys, nickel, nickel alloys, carbon-based materials, conductive oxides, conductive nitrides, conductive carbides, conductive silicides, or mixtures thereof.
    [0007]
    7. Dye-sensitized solar cell, according to any one of the preceding claims, characterized in that said porous substrate (8) comprises a first portion (8a), including said network (7) of conductive particles, and a second portion (8b) without conductive particles, and wherein the first portion forms said third conductive layer (6b) and the second portion forms said porous insulating layer (5b).
    [0008]
    8. Dye-sensitized solar cell, according to claim 7, characterized in that said second portion (8b) of the porous substrate is thinner than said first portion (8a) of the porous substrate.
    [0009]
    9. Dye-sensitized solar cell, according to any one of claims 1 to 6, characterized in that the porous insulating layer (5a) is arranged on one side of the porous substrate (4), and the second conductive layer (3) ) is arranged on the opposite side of the porous substrate.
    [0010]
    10. Dye-sensitized solar cell, according to any one of the preceding claims, characterized in that the conductive medium is an electrolyte based on ionic liquid.
    [0011]
    11. Dye-sensitized solar cell, according to any one of the preceding claims, characterized in that the conductive medium is an electrolyte based on a cobalt complex.
    [0012]
    12. Dye-sensitized solar cell, according to any one of the preceding claims, characterized in that the conductive medium is a hollow solid-state conductor.
    [0013]
    13. Dye-sensitized solar cell, according to claim 12, characterized in that the leaked solid-state conductor is perovskite.
    [0014]
    14. Dye-sensitized solar cell, according to any one of the preceding claims, characterized in that the light-absorbing layer (1) comprises perovskite.
    [0015]
    15. Dye-sensitized solar cell, according to any one of the preceding claims, characterized in that the first conductive layer (2) has a surface layer of TiO2 and the light-absorbing layer (1) is a perovskite layer .
    [0016]
    16. Method of manufacturing a dye-sensitized solar cell, comprising a first and a second conductive layer (2; 3) and a porous insulating layer (5b), arranged between the first and second conductive layer, characterized in that the method comprises: - depositing a blocking agent on a top side of a porous substrate (8) made of an insulating material, so as to form a blocking layer (10) on a portion (8b) of the substrate; - infiltrating the porous substrate from one side of the substrate base with conductive particles having a size smaller than the pore size of the substrate, to form a third conductive layer (6b) on another portion (8a) of the substrate; - depositing a porous conductive layer on the top side of the porous substrate to form a first conductive layer; - depositing an ink comprising conductive particles on the bottom side of the porous substrate to form the second conductive layer; e- heat treating the substrate to burn off the blocking layer, thereby forming the porous insulating layer.
    [0017]
    17. Method according to claim 16, characterized in that said blocking agent comprises fibers having a diameter between 1 nm and 5 μm.
    [0018]
    18. Method of manufacturing a dye-sensitized solar cell, comprising a first and a second conductive layer (2; 3) and a porous insulating layer (5a), arranged between the first and second conductive layer, characterized in that the method comprises: - providing a porous substrate (8) made of an insulating material; - infiltrating the porous substrate with conductive particles having a size smaller than the pore size of the substrate, to form a third conductive layer (6a); - depositing a layer of insulating material on a top side of the porous substrate to form the porous insulating layer (5a); - depositing a porous conductive layer on the porous insulating layer (5a), to form a first conductive layer; and - depositing an ink comprising conductive particles onto one side of the base of the insulating substrate to form the second conductive layer.
    [0019]
    19. Method according to claim 18, characterized in that said porous insulating layer (5a) is deposited on the porous substrate by means of screen etching, die groove coating, spray coating and by deposition at wet.
    [0020]
    Method according to any one of claims 16 to 19, characterized in that a light-absorbing layer comprising TiO2 is deposited on the first conductive layer.
    [0021]
    Method according to any one of claims 16 to 20, characterized in that a light-absorbing layer comprising a layer of perovskite is deposited on the first conductive layer.
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    法律状态:
    2018-01-02| B25A| Requested transfer of rights approved|Owner name: EXEGER OPERATIONS AB (SE) |
    2018-11-06| B06F| Objections, documents and/or translations needed after an examination request according [chapter 6.6 patent gazette]|
    2020-02-18| B06U| Preliminary requirement: requests with searches performed by other patent offices: procedure suspended [chapter 6.21 patent gazette]|
    2021-07-13| B350| Update of information on the portal [chapter 15.35 patent gazette]|
    2021-11-09| B09A| Decision: intention to grant [chapter 9.1 patent gazette]|
    2022-02-01| B16A| Patent or certificate of addition of invention granted [chapter 16.1 patent gazette]|Free format text: PRAZO DE VALIDADE: 20 (VINTE) ANOS CONTADOS A PARTIR DE 16/05/2014, OBSERVADAS AS CONDICOES LEGAIS. |
    优先权:
    申请号 | 申请日 | 专利标题
    SE1350611-8|2013-05-17|
    SE1350611|2013-05-17|
    PCT/EP2014/060163|WO2014184379A1|2013-05-17|2014-05-16|A dye-sensitized solar cell and a method for manufacturing the solar cell|
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