For the purposes of illustrating the various aspects of the invention, wherein like numerals indicate like elements, there are shown in the drawings simplified forms that are presently preferred, it being understood, however, that the invention is not limited by or to the precise arrangements and instrumentalities shown, but rather only by the issued claims. The drawings are not to scale, nor are the aspects of the drawings to scale relative to each other.
Referring to
The conducting window layer 110 is an electrically conductive layer of material that is acting as an ohmic contact. The conducting window layer may be translucent, transparent or semi-transparent. An exemplary material would be indium tin oxide, a material that typically is formed by reactive sputtering of an In—Sn target in an oxidative atmosphere. An alternative to indium tin oxide may include, for instance, aluminium-doped zinc oxide, boron-doped zinc oxide, or even carbon nanotubes. Indium tin oxide (ITO, or tin-doped indium oxide) is a mixture of indium(III) oxide (In2O3) and tin(IV) oxide (SnO2), typically may be 90% In2O3, 10% SnO2 by weight. It is transparent and colorless in thin layers. In bulk form, it is yellowish to grey. Indium tin oxide's main feature is the combination of electrical conductivity and optical transparency. However, a compromise has to be reached during film deposition, as high concentration of charge carriers will increase the material's conductivity, but decrease its transparency. Thin films of indium tin oxide are most commonly deposited on surfaces by electron beam evaporation, physical vapor deposition, or a range of sputtering techniques.
The semiconductor material of the layers 106 and 108 may be in the form of a substantially single-crystal material. The term “substantially” is used in describing the layers 106, 108 to take account of the fact that semiconductor materials normally contain at least some internal or surface defects either inherently or purposely added, such as lattice defects or grain boundaries. The term substantially also reflects the fact that certain dopants may distort or otherwise affect the crystal structure of the semiconductor material. In particular, p-type semiconductor layer 106 includes a p-type doping agent, whereas n-type semiconductor layer 108 includes an n-type doping agent. Note that the p-type layer 106 is thicker than the n-type layer 108 in all cases where it is desired that the majority of the electron hole pairs are created in the p-type layer 106.
For the purposes of discussion, it is assumed that the semiconductor layers 106, 108 are formed from silicon, unless stated otherwise. It is understood, however, that the semiconductor material may be a silicon-based semiconductor or any other type of semiconductor, such as the III-V, II-IV, etc., classes of semiconductors. Examples of these materials include: silicon (Si), germanium-doped silicon (SiGe), silicon carbide (SiC), germanium (Ge), gallium arsenide (GaAs), gallium phosphide (GaP), and indium phosphide (InP).
The back contact layer 104 may be a conductive layer, such as a conductive metal-based or metal oxide-based layer. The back contact layer is an ohmic contact, i.e., a region on a semiconductor device that has been prepared so that the current-voltage (I-V) curve of the device is linear and symmetric. The back contact material may be chosen for its thermal robustness in contact with Si. For instance, back contact layer 104 may be film based on aluminum or a silicide, such as or titanium disilicide, tungsten disilicide or nickel silicide, an example of which is discussed below. A silicide-polysilicon combination has better electrical properties than polysilicon alone and yet does not melt in subsequent processing.
The back contact layer 104 may be created, for example, by deposition, such as LPE, CVD or PECVD. Mesotaxy or epitaxy may be used also. Whereas as epitaxy is the growth of a matching phase on the surface of a substrate, mesotaxy is the growth of a crystallographically matching phase underneath the surface of the host crystal. In this process, ions are implanted at a high enough energy and dose into a material to create a layer of a second phase, and the temperature is controlled so that the crystal structure of the target is not destroyed. The crystal orientation of the layer can be engineered to match that of the target, even though the exact crystal structure and lattice constant may be very different. For example, after the implantation of nickel ions into a silicon wafer, a layer of nickel silicide can be grown in which the crystal orientation of the silicide matches that of the silicon.
Use of epitaxy or mesotaxy to form back contact layer 104 may be thought of as a conceptual interface between the structure 100A described
Moreover, if the back contact layer 104 is deposited on top of PVSF 102 after exfoliation separation (step 210), a PVS 100 of variation 100A may result. Alternatively, if PVSF 102 is doped, before or after mesotaxy, as a p-type semiconductor and back contact layer 104 is formed by mesotaxy, a PVS 100 similar to variation 100A or 100B may result. If the depth of the mesotaxial growth of the back contact layer 104 is within the middle of PVSF 102, a layer of PVSF 102 may remain underneath the back contact layer 104, as in variation 100A. If the depth of the mesotaxial growth of the back contact layer 104 reaches the bonding surface 126 of PVSF 102, little to none of the layer of PVSF 102 may remain underneath the back contact layer 104, as in variation 100B.
Insofar as the conductive layer is formed on or in the exfoliation layer 122, whether formed by epitaxy, mesotaxy, ion implantation, doping, vapor transport, vapor deposition, etc., the conductive layer will be integral to the exfoliation layer 122. If the conductive layer is formed on or in the exfoliation layer 122 before the exfoliation layer 122 is bonded to the insulator substrate 101, the conductive layer will be proximate to the insulator substrate 101 when the exfoliation layer 122 is bonded to the substrate 101. In other words, the conductive layer will have been formed near the side of the exfoliation layer 122 that faces the insulator substrate, such that, for example, the resulting conductive layer may be between the insulator substrate and the exfoliation layer. If the exfoliation layer 122 is bonded to the insulator substrate 101 first and then the conductive layer is formed on or in the exfoliation layer 122 thereafter, the conductive layer will be on or near the side of the exfoliation layer 122 opposite the insulator substrate 101 and thus distal to the insulator substrate 101. Likewise, any photovoltaic device layers formed in, on or above the exfoliation layer 122 after the exfoliation layer 122 has been bonded to the insulator substrate 101 will be distal to the insulator substrate 101.
As will be discussed in more detail in reference to
In contrast to variations 100B and 100C in
The insulator substrate 101, here a glass substrate 101, may be formed from an oxide glass or an oxide glass-ceramic. Although not required, the embodiments described herein may include an oxide glass or glass-ceramic exhibiting a strain point of less than about 1,000 degrees C. As is conventional in the glass making art, the strain point is the temperature at which the glass or glass-ceramic has a viscosity of 1014.6 poise (1013.6 Pa·s). As between oxide glasses and oxide glass-ceramics, the glasses may have the advantage of being simpler to manufacture, thus making them more widely available and less expensive.
By way of example, the glass substrate 101 may be formed from glass substrates containing alkaline-earth ions, such as, substrates made of CORNING INCORPORATED GLASS COMPOSITION NO. 1737 or CORNING INCORPORATED GLASS COMPOSITION NO. EAGLE2000™. These glass materials have other uses, in particular, for example, the production of liquid crystal displays.
The glass substrate may have a thickness in the range of about 0.1 mm to about 10 mm, such as in the range of about 0.5 mm to about 3 mm. For some SOI structures, insulating layers having a thickness greater than or equal to about I micron (i.e., 0.001 mm or 1000 nm) are desirable, e.g., to avoid parasitic capacitive effects which arise when standard SOI structures having a silicon/silicon dioxide/silicon configuration are operated at high frequencies. In the past, such thicknesses have been difficult to achieve. In accordance with the present invention, an SOI structure having an insulating layer thicker than about 1 micron is readily achieved by simply using a glass substrate 101 having a thickness that is greater than or equal to about 1 micron. A lower limit on the thickness of the glass substrate 101 may be about 1 micron, i.e., 1000 nm.
In general, the glass substrate 101 should be thick enough to support the semiconductor layer 106, 108 through the bonding process steps, as well as subsequent processing performed on the photovoltaic SiOG structure 100. Although there is no theoretical upper limit on the thickness of the glass substrate 101, a thickness beyond that needed for the support function or that desired for the ultimate photovoltaic SiOG structure 100 might not be advantageous since the greater the thickness of the glass substrate 101, the more difficult it will be to accomplish at least some of the process steps in forming the photovoltaic SiOG structure 100.
The oxide glass or oxide glass-ceramic substrate 101 may be silica-based. Thus, the mole percent of SiO2 in the oxide glass or oxide glass-ceramic may be greater than 30 mole percent and may be greater than 40 mole percent. In the case of glass-ceramics, the crystalline phase can be mullite, cordierite, anorthite, spinel, or other crystalline phases known in the art for glass-ceramics. Non-silica-based glasses and glass-ceramics may be used in the practice of one or more embodiments of the invention, but are generally less advantageous because of their higher cost and/or inferior performance characteristics.
Similarly, for some applications, e.g., for SOI structures employing semiconductor materials that are not silicon-based, glass substrates which are not oxide based, e.g., non-oxide glasses, may be desirable, but are generally not advantageous because of their higher cost. As will be discussed in more detail below, in one or more embodiments, the glass or glass-ceramic substrate 101 is designed to match a coefficient of thermal expansion (CTE) of one or more semiconductor materials (e.g., silicon, germanium, etc.) of the layer(s) (potentially 102, 104, 106, 108, or 110) that is (are) bonded thereto, directly or indirectly. The CTE match ensures desirable mechanical properties during heating cycles of the deposition process.
For photovoltaic applications, the glass or glass-ceramic 101 may be transparent in the visible, near UV, and/or IR: wavelength ranges, e.g., the glass or glass ceramic 101 may be transparent in the 350 nm to 2 micron wavelength range. Having transparent, or at least translucent, glass is important in particular in variation 100C, where the light enters the insulator substrate 101 before reaching the rest of PV structure 100C. However, in variations 100A and 100B, the light does not enter the insulator substrate 101, so it is largely irrelevant whether the insulator substrate 101 is translucent, let alone transparent, in which case the insulator substrate 101 is chosen based on other criteria, inter alia CTE, not the least of which is cost.
Although the glass substrate 101 may be composed of a single glass or glass-ceramic layer, laminated structures may be used if desired. When laminated structures are used, the layer of the laminate closest to the layer bonded thereto (e.g., 102, 104 or 110) may have the properties discussed herein for a glass substrate 101 composed of a single glass or glass-ceramic. Layers farther from the bonded layer may also have those properties, but may have relaxed properties because they do not directly interact with the bonded layer. In the latter case, the glass substrate 101 is considered to have ended when the properties specified for a glass substrate 101 are no longer satisfied.
Referring to
At action 202 of
At either action 203, for processes 200A and 200B, or action 206, for process 200C, also shown in
The implantation energy may be adjusted using conventional techniques to achieve an approximate thickness of the exfoliation layer 122. By way of example, hydrogen ion implantation may be employed, although other ions or multiples thereof may be employed, such as boron+hydrogen, helium+hydrogen, or other ions known in the literature for exfoliation. Again, any other known or hereinafter developed technique suitable for forming the exfoliation layer 122 may be employed without departing from the spirit and scope of the present invention.
Depending on the parameters of the PV SOI structure 100, the number and thickness of layers on top of the prepared donor surface 121, and the potential use of any intermediate preparation step, such as CMP or FA, the exfoliation layer 122 may be made as thick or thin as desired and/or as feasible. If various design constraints require the exfoliation layer 122 to be thicker than desired, such as for use in microelectronics, a known method of mass removal, such as CMP or polishing, may be used to reduce the thickness of the layer 122 after it is exfoliated in action 210. However, using a mass removal step adds time and expense to the overall manufacturing process and may not be necessary for PVS 100. For instance, in variation 100A, the PVSF 102 layer may not need to be thin or thick; preferably, PVSF 102 is thick enough to serve as a stable foundation for later finishing processes, but otherwise thin to conserve materials, and hence money.
The opposite issue is more likely to arise with PV structure 100, namely that the exfoliation layer may be too thin. In variations 100B and 100C, a thick layer of Si is desirable for a PVS 100 because a thicker layer of Si will absorb more light and increase its efficiency.- The energy needed to create a desirably thick exfoliation layer may exceed available equipment parameters, and hence additional Si may be deposited or grown epitaxially after the exfoliation layer 122 is created. The additional Si may be added to the exfoliation layer 122 before or after it is transferred to the glass substrate 101. If added before, the Si addition becomes part of a creation of a partially completed PVS 124, whereas if added after, the Si addition becomes part of a finishing process. Similarly, semiconductor layers will be added to PVS 100A after PVSF 102 and back contact 104 are on substrate 101.
At either action 204, for processes 200A and 200B, or action 207, for process 200C, also shown in
Action 205 of
With reference to
At action 208, in
Prior to or after the contact, the structure(s) comprising the donor semiconductor wafer 120, the exfoliation layer 122/PVSF 102/partially completed PVS 124, and the glass substrate 101 are heated under a differential temperature gradient. The glass substrate 101 may be heated to a higher temperature than the donor semiconductor wafer 120 and exfoliation layer 122/PVSF 102/partially completed PVS 124. By way of example, the temperature difference between the glass substrate 101 and the donor semiconductor wafer 120 (and the exfoliation later 122/PVSF 102/partially completed PVS 124) is at least 1 degree C, although the difference may be as high as about 100 to about 150 degrees C. This temperature differential is desirable for a glass having a coefficient of thermal expansion (CTE) matched to that of the donor semiconductor wafer 120 (such as matched to the CTE of silicon) since it facilitates later separation of the exfoliation layer 122 from the semiconductor wafer 120 due to thermal stresses. The glass substrate 101 and the donor semiconductor wafer 120 may be taken to a temperature within about 150 degrees C of the strain point of the glass substrate 101.
Once the temperature differential between the glass substrate 101 and the donor semiconductor wafer 120 is stabilized, mechanical pressure is applied to the intermediate assembly. The pressure range may be between about 1 to about 50 psi. Application of higher pressures, e.g., pressures above 100 psi, might cause breakage of the glass substrate 101. The appropriate pressure may be determined in light of the manufacturing parameters, such as materials being used, and their thicknesses.
Next, a voltage is applied across the intermediate assembly, for example with the donor semiconductor wafer 120 at the positive electrode and the glass substrate 101 the negative electrode. The application of the-voltage potential causes alkali or alkaline earth ions in the glass substrate 101 to move away from the semiconductor/glass interface further into the glass substrate 101. This accomplishes two functions: (i) an alkali or alkaline earth ion free interface is created; and (ii) the glass substrate 101 becomes very reactive and bonds strongly to the exfoliation layer 122 of the donor semiconductor wafer 120.
At action 210, of
Referring to
The hybrid region 160 is of enhanced oxygen concentration of thickness T160. When bonding the conducting window layer 110, for instance, this hybrid region 160 may be enhanced by beginning with a composition stoichiometrically depleted of oxygen to enhance oxygen transfer from the glass substrate 101. This thickness may be defined in terms of a reference concentration for oxygen at a reference surface 170 within the exfoliation layer 122/PVSF 102/partially completed PVS 124. The reference surface 170 is substantially parallel to the bonding surface between the glass substrate 101 and the exfoliation layer 122/PVSF 102/partially completed PVS 124 and is separated from that surface by a distance DS1. Using the reference surface 170, the thickness T160 of the hybrid region 160 will typically satisfy the relationship:
T160≦200 nm,
where T160 is the distance between bonding surface 126 and a surface which is: (i) substantially parallel to bonding surface 126, and (ii) is the surface farthest from bonding surface 126 for which the following relationship is satisfied:
CO(x)-CO/Ref≧50 percent, 0≦x≦T160,
where CO(x) is the concentration of oxygen as a function of distance x from the bonding surface 126, CO/Ref is the concentration of oxygen at the above reference surface 170, and CO(x) and CO/Ref are in atomic percent.
Typically, T160 will be substantially smaller than 200 nanometers, e.g., on the order of about 50 to about 100 nanometers. It should be noted that CO/Ref will typically be zero, so that the above relationship will in most cases reduce to:
CO(x)≧50 percent, 0≦x≦T160.
In connection with the depletion region 230, the oxide glass or oxide glass-ceramic substrate 101 preferably comprises at least some positive ions that move in the direction of the applied electric field, i.e., away from the bonding surface 126 and into the glass substrate 101. Alkali ions, e.g., Li+1, Na+1, and/or K+1 ions, are suitable positive ions for this purpose because they generally have higher mobility rates than other types of positive ions typically incorporated in oxide glasses and oxide glass-ceramics, e.g., alkaline-earth ions.
However, oxide glasses and oxide glass-ceramics having positive ions other than alkali ions, e.g., oxide glasses and oxide glass-ceramics having only alkaline-earth ions, can be used in the practice of the invention. The concentration of the alkali and alkaline-earth ions can vary over a wide range, representative concentrations being between 0.1 and 40 wt. % on an oxide basis. Preferred alkali and alkaline-earth ion concentrations are 0.1 to 10 wt. % on an oxide basis in the case of alkali ions. and 0-25 wt. % on an oxide basis in the case of alkaline-earth ions.
The electric field applied in the bonding step (action 208) moves the positive ions (cations) further into the glass substrate 101 forming the depletion region 230. The formation of the depletion region 230 is especially desirable when the oxide glass or oxide glass-ceramic contains alkali ions, since such ions are known to interfere with the operation of semiconductor devices. Alkaline-earth ions, e.g., Mg+2, Ca+2, Sr+2, and/or Ba+2, can also interfere with the operation of semiconductor devices and thus the depletion region also preferably has reduced concentrations of these ions.
It has been found that the depletion region 230 once formed is stable over time even if the PV structure 100 is heated to an elevated temperature comparable to, or even to some extent higher than, that used in the bonding process. Having been formed at an elevated temperature, the depletion region 230 is especially stable at the normal operating and formation temperatures of PV structures. These considerations ensure that alkali and alkaline-earth ions will not diffuse back from the oxide glass or oxide glass-ceramic 101 into the semiconductor material 104 during use or further device processing, which is an important benefit derived from using an electric field as part of the bonding process.
As with selecting the operating parameters to achieve a strong bond, the operating parameters needed to achieve a depletion region 230 of a desired width and a desired reduced positive ion concentration for all of the positive ions of concern can be readily determined by persons skilled in the art from the present disclosure. When present, the depletion region 230 is a characteristic feature of a PV structure 100 produced in accordance with one or more embodiments of the present invention.
As illustrated in
At action 212, in
Another finishing process 130 may include augmenting the semiconductor thickness of the exfoliation layer 122. In the case of variation 100A, semiconductor material may be added, for example, before mesotaxial growth of a back contact layer 104. It is desired in certain embodiments that the final combined thickness of the semiconductor layers 106 and 108 should be, for example, more than 10 microns (i.e., 10000 nm) and less than about 30 microns. Therefore, an appropriately thick exfoliation layer 122 should be created and augmented with an additional semiconductor layer 132 (e.g., of Si) until the desired thickness is created. Augmentation with an additional Si layer 132 may include a doping step as well. Historically, the amorphized silicon layer has been on the order of about 50-150 nm in thickness, and depending on the implantation energy and implantation time, the thickness of the exfoliation layer 122 has been on the order of about 500 nm. As with microelectronic SOI structures, however, a thinner exfoliation layer 122 may be created for the PVSF 102, with the amorphized silicon layer necessarily being thinner as well, with more semiconductor material added in the finishing processes.
Also according to action 212, the cleaved surface 123 may subject to post-cleaving processing which may include subjecting the cleaved surface 123 to a polishing or annealing process to reduce roughness 123A. Moreover, in order to achieve the exemplary embodiment of variation 100B, the finishing process may include application of the conducting window layer 110, such as deposition of indium tin oxide. Conversely, to achieve the exemplary embodiment of variation 100C, the finishing process may include application of the back contact layer 104, a conductive metal-based or metal oxide-based layer, such as an aluminum-based film deposited by LPE, CVD or PECVD. As discussed above, back contact layer 104 also may be formed by epitaxial or mesotaxial growth, such as of nickel silicide.
To the extent that the partially completed PVS 124 has more of the features of the intended final product, fewer finishing processes are necessary. By contrast, insofar as the formation of PVSF 102 on insulator substrate 101 alone does not distinguish the substrate 101-PVSF 102 combination as a photovoltaic structure over any other semiconductor-on-insulator structure of U.S. Patent Application No. 2004/0229444, several PVS-specific finishing processes are necessary. However, having a substantially single crystal layer as the photovoltaic structure foundation 102 relaxes the parameters within which to operate and expands the scope of options and outcomes available from which to choose, in proceeding with the finishing processes.
In particular, formation of the PVSF 102 or the partially completed PVS 124 allows for greater flexibility in the creation of advanced, multi-junction PVS devices. For example, building on a PVSF 102 of crystal-Si, a manufacturer may exploit the different specific heat capacities of crystal-Si versus GaAs, Ge, and GaInP2 to create various multi-junction layers of GaAs, Ge and GaInP2. Optionally, as the preferred embodiments of
Alternative embodiments of the invention will now be described with reference to the aforementioned SiOG processes and further details. For example, a result of separating the exfoliation layer 122 from the donor semiconductor wafer 120 may produce a first cleaved surface of the donor semiconductor wafer 120 and a second cleaved surface 123 of the exfoliation layer 122. As previously discussed, the finishing process 130 may be applied to the second cleaved surface 123 of the exfoliation layer 122. Additionally or alternatively, the finishing process 130 may be applied to the first cleaved surface of the donor semiconductor wafer 120 (using one or more of the techniques described above), such as polishing.
In another embodiment of the present invention, the donor semiconductor wafer 120 may be part of a donor structure, including a substantially single-crystal donor semiconductor wafer 120, and an epitaxial semiconductor layer disposed on the donor semiconductor wafer 120. (Details of an epitaxially grown semiconductor layer in an SOI context may be found in co-pending U.S. patent application Ser. No. 11/159,889, filed Jun. 23, 2005, the entire disclosure of which is incorporated herein by reference.) The exfoliation layer 122, therefore, may be formed-substantially from the epitaxial semiconductor layer (and may also include some of the single-crystal donor semiconductor material from the wafer 120). Thus, the aforementioned finishing process may be applied to the cleaved surface 123 of an exfoliation layer 122 formed substantially of epitaxial semiconductor material and/or a combination of epitaxial semiconductor material and single-crystal semiconductor material.
As depicted in
For example, when the exfoliation layer 122 is prepared, comprising either the PVSF 102 or partially completed PV structure 124 (step 802), the handling assembly could transport and position the PV structures 100 in need of completion within the PVS processing assembly 820 to permit anodic bonding (step 804) to occur. Further transportation and positioning (step 806) of the substrate 101, bonded to PVSF 102 or partially completed PVS 124, within the PVS processing assembly 820 may allow additional actions 210 and 212 of exfoliating and finishing, respectively, to occur (step 808).
Referring to
The glass wafer with the germanium or GaAs/Ge film optionally then may be polished, annealed or healed to remove the damaged germanium or GaAs top layer and a good quality layer surface. This wafer may be used as a substrate to grow epitaxial structures to form the solar cell. Examples of materials may include GaAs, GaInP/GaAs, GaxInyP/Gac, IndAs/Ge and others known in the art. Various processes may be utilized to deposit the epitaxial films including CVST (closed space vapor transport), MOCVD (metallo-organic chemical vapor deposition), MBE (molecular beam epitaxy) and others known in the art. A number of surface passivating window layers such as wide bandgap epilayers of AlGaAs, InGaP or ZnSe may be employed as well as other encapsulating or passivation layers and surface treatments may be used to complete the cell.
The ohmic contacts may be applied in varying configurations, depending on the device design, but the basic requirement is that the produced current flow from one contact to the next contact to allow for a completed electric circuit, the circuit being completed once the two electrodes leading from the device are coupled with a load. As such, the back contact layer need not be the outermost layer relative to the semiconductor layers, as depicted in
Although the invention herein has been described with reference to particular embodiments, it is to be understood that these embodiments are merely illustrative of the principles and applications of the present invention. It is therefore to be understood that numerous modifications may be made to the illustrative embodiments and that other arrangements may be devised without departing from the spirit and scope of the present invention as defined by the appended claims.
The present invention claims the benefit of the filing date of the prior-filed U.S. Provisional Patent Application No. 60/810061 filed on May 31, 2006 by David Francis Dawson-Elli et al. and entitled “SINGLE CRYSTAL THIN FILM PHOTOVOLTAIC STRUCTURE,” the content of which is relied upon and incorporated herein by reference in its entirety.
Number | Date | Country | |
---|---|---|---|
60810061 | May 2006 | US |