This disclosure relates to solar photovoltaic conversions devices. More particularly to a method and apparatus for improving the energy conversion efficiency in a solar cell device using solar cell design that enables a higher amount of light to be converted to energy by trapping the light in the solar cell.
Solar photovoltaic conversions devices can convert light into electrical energy using an absorber layer that uses photons from incident light to create electron-hole pairs. Generally, the absorber lay is relatively thin to enable the electrons and holes to reach membrane layer by making the absorber layer thickness smaller than the diffusion lengths of the charge carriers. As a result, light may not be totally absorbed by the absorber layer in a single pass. The absorber layer may be thickened to absorb more light, but this increases cost of the solar cell device. Another approach may be to design a solar cell that diffuses the light more broadly across the absorber layer. However, the random scattering causes the light path to increase which results in a limitation on energy conversion by letting light escape from the solar cell. Accordingly, solar cell designs that prevent light from escaping may be desirable.
Broadly, converting solar energy to electrical energy is based on photons of incident radiation (e.g., light) generating electron-hole pairs within the silicon layer(s) of a solar cell to force charge carriers in the silicon layer(s) to move (e.g., current flow). The silicon layer may include an absorber layer with p-type silicon layer(s) and n-type silicon layer(s) on either side. The electron and holes generated in the absorber layer should reach the p-type or n-type silicon layer. This movement can be accomplished by making the absorber layer thinner than the diffusion lengths of the electrons and holes. Generally, below the silicon layer may be a reflector layer that reflects light back into the silicon layer to generate additional electron-hole pairs. However, the reflected light may escape the silicon layer and may not further contribute to electron-hole pair generation. This disclosure describes systems and methods for trapping reflected light (e.g., photons) within the silicon layer to increase electron-hole pair generation per unit of light. Trapping may be explained using the total internal reflection principle.
Total internal reflection of a propagating wave (e.g., light) can occur when a wave attempts to travel between a propagating medium that has a higher refractive index than an adjacent propagating medium. However, total internal reflection may also depend on the incident angle of the wave. For example, total internal reflection may occur when the incident angle is greater than a critical angle that may be dependent upon the refractive index of each propagating medium. In this way, light may be trapped within a propagating medium as long as the incident angle is greater than the critical angle. As a result, trapped light (e.g., photons) may generate more electron-hole pairs in the silicon layer than a single or double pass of a light through the silicon layer.
In one embodiment, the solar cell may comprise a glass layer or substantially transparent layer, a silicon layer(s), and a reflector layer. The glass layer may also include a light concentration layer or component that directs incident light through the glass layer and the silicon layer to a focal point in the reflector layer. The silicon layer may include a reflection notch that may be substantially filled by the reflector layer and adjacent to the focal point. The reflection notch may be configured to reflect at least a portion of the incident light towards the boundary of the silicon layer and the reflector layer. When the refractive index of the silicon layer may be higher than the refractive index of the reflector layer then total internal reflection may occur. The geometry of the reflection notch may be configured to reflect at least a portion of the incident light such that the incident angle of the reflected light at the silicon-reflector layer boundary is greater than the critical angle. In this way, light may be trapped within the silicon layer per the total internal reflection principle.
The reflection notch may be formed in the silicon layer(s) using a variety of techniques that are optimized to form a reflective surface. The reflective surface may be designed to reflect incident light towards silicon-reflector layer interface so that the reflected light may be totally reflected at the silicon-reflector layer interface. The reflection notch may be generated by selective etching (e.g., wet or dry etch), selective imprinting, or selective formation of topology.
In one embodiment, selective formation of topology may be implemented by altering the substrate surface of a first solar cell layer to impact the formation of a second solar cell layer that may be deposited on the first solar cell layer. For example, the glass substrate layer may be etched to form a 3-dimensional pattern on the surface. Subsequent solar cells layer may conform to the pattern and form a reflection notch that is aligned with the light concentration module on the glass layer surface.
Described herein are several embodiments related to the current density control across the anode assembly. Note that this summary section does not specify every embodiment and/or incrementally novel aspect of the present disclosure or claimed invention. Instead, this summary only provides a preliminary discussion of different embodiments and corresponding points of novelty over conventional techniques. For additional details and/or possible perspectives of the invention and embodiments, the reader is directed to the Detailed Description section and corresponding figures of the present disclosure as further discussed below.
The features within the drawings are numbered and are cross-referenced with the written description. Generally, the first numeral reflects the drawing number where the feature was first introduced, and the remaining numerals are intended to distinguish the feature from the other notated features within that drawing. However, if a feature is used across several drawings, the number used to identify the feature in the drawing where the feature first appeared will be used. Reference will now be made to the accompanying drawings, which are not necessarily drawn to scale and wherein:
Disclosed herein include systems and methods for a solar cell design that reflects light within the silicon layer(s) of the solar cell. The topography of the silicon layer(s) and the reflector layer are configured to reflect incident light along the silicon layer(s).
Of course, the order of discussion of the different steps as described herein has been presented for clarity sake. In general, these steps can be performed in any suitable order. Additionally, although each of the different features, techniques, configurations, etc. herein may be discussed in different places of this disclosure, it is intended that each of the concepts can be executed independently of each other or in combination with each other.
The solar cell design 102 may include, but is not limited to, a light concentration component 112, a substantially transparent layer 114 (e.g., glass), a silicon layer(s) 116 that use light 106 (e.g., photons) to generate electrical energy, and a reflector layer 118.
In this embodiment, a reflection notch 120 may be incorporated into the interface of the silicon layer 116 and the reflector layer 118. The light concentration component 112 may focus, direct, or concentrate the light 106 towards the reflection notch 120. The light 106 may be reflected by the reflection notch 120 towards the silicon-reflector interface. The light 106 may be reflected towards the glass-silicon interface. When the incident angle (not shown) of the light 106 at the glass-silicon interface is greater than a critical angle (not shown) will enable at least a majority of the light 106 to be reflected back within the silicon layer 116. The critical angle (not shown) may be determined based, at least in part, on the principle of total internal reflection which enables propagating waves (e.g., light 106) to completely reflect from an interface of two wave mediums, such as the silicon layer 116 and the reflector layer 118. The principle of total internal reflection will be described in greater detail in the description of the remaining figures.
In other embodiments, the solar cell design 104 may include additional layers (e.g., transparent conductive oxides, etc.) or components to generate electrical energy. The silicon layer 116(s) 116 may include multiple silicon layers 116 that may be used to generate electrical energy and transfer electrical energy from the solar cell 102 to the electrical device. The silicon layers 116 may include different dopant concentrations (e.g., p-type, n-type, intrinsic, etc.), crystal structures (e.g., microcrystalline, amorphous, etc.) and/or surface textures.
In the
The focal point 200 may be the point on the principal axis 202 in which light 106 that passes through the light concentration component may converge together. The location of the focal point 200 may vary horizontally or vertically as shown in
The reflection notch 120, as shown in
They surfaces may include, but are not limited to, a reflector layer surface 402 at the silicon layer 116 and reflector layer 118 interface, a silicon layer surface 404 at the silicon layer 116 and transparent layer 114 (not shown) interface. The reflection notch surface 406 may also be at the silicon layer 116 and reflector layer 118 interface, but may not be on the same plane as the reflector layer surface 402. Although all of the surfaces are shown as planar, they are not required to be absolutely planar and may have significant non-uniformity. In which case, the surface planes may be approximated to a plane that is an average or a mean of the surface that forms the silicon layer 116 and reflector layer 118 interface or the silicon layer 116 and transparent layer 114 (not shown) interface that may refract or reflect light 106.
The reflection notch angle 408 may represent how much the reflection notch 120 may protrude from the reflector layer 118 into the silicon layer 116. In one embodiment, the reflection notch angle 408 may be measured between the intersection of the reflector layer surface 402 and the reflection notch surface 406. The reflection notch angle 408 may range between 15° and 80° and may vary in view of the focal point 200, the light concentration component 112, the incident light angle 410, the reflected angle 412, and the critical angle 414.
The incident light angle 410 may represent the angle between the intersection of the principal axis 202 and the light 106 that is incident upon the reflection notch 120. The intersection may be at the focal point 200. Generally, there may be not set absolute value for each instance of light 106 (e.g., light 106 in
The reflected light angle 412 may represent the angle between the intersection of the reflector layer surface 402 and the reflected light 106 from the reflection notch 120. The incident light angle 410 and the reflection notch angle 408 may have a relatively large impact on the reflected light angle 412. For total internal reflection, the incident light angle 410 may be lower than 2 times the reflection notch angle 408 minus the critical angle 414. The light 106 reflected back into the silicon layer 116 may also induce additional electron-hole pair generation. However, to generate more electron-hole pairs the light 106 may need to be reflected back into the silicon layer 116 when the light intercepts the transparent/silicon layer interface. Under the principle of total internal reflection, the light may intercept the transparent/silicon layer interface at a critical angle 414.
The critical angle 414 determines whether the incident light may reflect back into the silicon layer 116 when the light 106 reaches the silicon-transparent layer interface. The critical angle 414 may be equal to or greater than the critical angle 414 to enable the light 106 to be reflected into the silicon layer 116 and not refracted into the transparent layer 114 (not shown). As noted above in the description of
Wherein n2 is the index of refraction for the transparent layer 114 and n1 is the index of refraction for the silicon layer 116. The critical angle 414 may be measured from a perpendicular plane 416 that extends out from the point of intersection between the light 106 and the silicon-transparent layer 114 interface or the silicon layer surface 404. The material for total internal reflection could be metal or ceramic.
In some embodiments, the solar cell 102 may include multiple reflection notches 120 to enable total internal reflection of light 106 throughout a larger surface area than the solar cell 102 shown in
In one embodiment, the light concentration components 112 may each include a corresponding reflection notch 120 that aligned along the principal axis 202. In this way, each of the reflection notches 120 may be able to reflect light 106 in a way that may enable total internal reflection as described above in the description of
Solar cell 102 is not limited to the layers shown in
Manufacturing the solar cell 600 may be done using selective etching techniques to form the reflection notch 120. The selective etching methods may include patterning processes that may designate which portions of the substrate that may be etched or left in place. Prior to and after the selective etching, one or more cleaning processes may also be used to prepare the substrate for patterning and etching and/or post-etch cleaning. Selective etching or removal of material may be accomplished through photolithography patterning and plasma etching or laser ablation.
Photolithography may include using light sensitive films to put a sacrificial pattern on top of the substrate and plasma etching may be used to remove portions of the substrate that are not covered by the pattern. Laser ablation may include using a laser to etch a pattern into the substrate. This may involve moving the laser along the substrate that may remove portions of the substrate where the laser contacts the substrate.
In view of the aforementioned solar cell 102 design, the alignment of the light concentration component 112 and the reflection notch 120 may be needed. However, selectively etching multiple layers, or even one layer, to align with other features in the solar cell 102 may be costly and time consuming. One embodiment that may reduce manufacturing cost and time may include a self-aligned process that assists with aligning the features of the solar cell 102. One embodiment of the self-aligned solar cell 700 will be described in the description of
In contrast to solar cell 600, the self-aligned solar cell 700 may include an alignment notch 708 in the transparent substrate layer 702 that may be similar to the transparent substrate 114. The alignment notch 708 may be aligned with the light concentration component 112 during the selective etching process (e.g., laser ablation). For example, the laser may be shot through the light concentration component 112 to remove a portion of the transparent layer 702 that is opposite the light concentration component 112. The laser may travel through the transparent layer 702 to remove a portion of material that on the opposite side from the light concentration component.
The alignment notch 708 may include a metal-oxide layer 704 that may be similar to the metal-oxide layer 602 described in the description of
At step 802, a transparent substrate 114 for a solar cell 700 may have a light concentration component 112 formed on one of its surfaces. In the illustrated embodiment, a single light concentration component 112 is shown. However, in other embodiments, two or more light concentration components 112 may be adjacent to each other, as shown in
The light concentration component 112 may have a focal point 200 that needs to be aligned with a reflection notch 120 that may be formed by a blanket film deposition process without selectively etching that the deposited film. In this embodiment, the self-alignment may use the light concentration component 112 to pattern the transparent substrate 114 in a way that forms the reflection notch 120 using a blanket deposition process for the reflector material.
At step 804, a trench may be formed in the transparent layer 702 by using a laser that is focused by the light concentration component 112. The laser ablation may remove a portion of the transparent layer 702 that is on the opposite side from the light concentration component 112. In one embodiment, the laser may be configured to form the trench so that the trench width is greater than the trench depth. The aspect ratio trench depth over trench width may be lower 0.5 and with a depth in the range 0.5 micron to 40 microns. The trench may include two opposing surfaces that form the trench depth and another surface connected to the two opposing surfaces. The connecting surface may represent the trench width. The trench width and depth may vary to accommodate various sizes of the reflection notch 120. A deeper trench may increase the height of the reflection notch 120 and a wider trench may increase the width of the reflection notch 120. Generally, the trench surfaces may be configured to adhere to an overlying film.
At step 806, a transparent electrode layer 704 or metal-oxide layer may be deposited on the transparent substrate 702 and may, at least, partially fill the trench. The fill may be substantially conformal to the trench features and may be a less thickness than the transparent substrate 702 thickness. The transparent electrode layer 704, as described in
At step 808, a silicon layer 706 may be deposited on the transparent electrode layer 704 and may fill the remainder of the trench in a substantially conformal manner. A notch in the silicon layer 706 may be formed by the silicon layer 116 as a result of conforming to the trench. As shown in the corresponding diagram, the notch may be opposing the trench from the upper surface of the silicon layer 116. Although substantially triangular in the cross section illustration, the notch may be substantially conical or pyramid-like in three dimensions. The notch geometry may be based, at least in part, on the trench width, trench depth, trench length, and the deposition rate of the silicon layer(s) 116. As noted in the description of
At step 810, the reflector layer 118 may be deposited over the silicon layer 116 and substantially fills the notch in the silicon layer 116. The reflector layer 118 may form the reflection notch 120 by filling the notch in the silicon layer 116. The reflection notch 120 may reflect substantial portion of light 106 from the silicon layer 116 towards the reflector/silicon interface that may surround the reflection notch 120. As noted in the description of
Although only certain embodiments of this application have been described in detail above, those skilled in the art will readily appreciate that many modifications are possible in the embodiments without materially departing from the novel teachings and advantages of this invention. Accordingly, all such modifications are intended to be included within the scope of this invention.