Abstract:
Ge/Si and other nonsilicon film heterostructures are formed by hydrogen-induced exfoliation of the Ge film which is wafer bonded to a cheaper substrate, such as Si. A thin, single-crystal layer of Ge is transferred to Si substrate. The bond at the interface of the Ge/Si heterostructures is covalent to ensure good thermal contact, mechanical strength, and to enable the formation of an ohmic contact between the Si substrate and Ge layers. To accomplish this type of bond, hydrophobic wafer bonding is used, because as the invention demonstrates the hydrogen-surface-terminating species that facilitate van der Waals bonding evolves at temperatures above 600° C. into covalent bonding in hydrophobically bound Ge/Si layer transferred systems.

Description:
RELATED APPLICATIONS  
       [0001]    The present application is related to U.S. Provisional Patent Application, serial No. 60/284,726, filed on Apr. 17, 2001, and claims priority to it under 35 USC 119. 
     
    
     
       BACKGROUND OF THE INVENTION  
         [0002]    1. Field of the Invention  
           [0003]    The invention relates to the field of semiconductor processing of films and in particular to processing nonsilicon films on heterostructures.  
           [0004]    2. Description of the Prior Art  
           [0005]    Group III-V semiconductor layered structures grown on bulk germanium substrates have been used in the prior art to create high efficiency triple-junction solar cells with efficiencies greater than 30%. However, these are prohibitively expensive for all but space applications, because the Ge substrate constitutes a large portion of this cost.  
           [0006]    Therefore, what is needed is some type of methodology whereby Ge and other nonsilicon films can be made on heterostructures, e.g. integrated with silicon substrates.  
         BRIEF SUMMARY OF THE INVENTION  
         [0007]    Ge/Si and other nonsilicon film heterostructures are formed by hydrogen-induced exfoliation or spitting of the Ge or nonsilicon film and then wafer bonded to a cheaper substrate, such a Si, glass, ceramic or the like, as a way to reduce product cost, while, for example, maintaining solar cell device performance from the heterostructures fabricated from such films. The illustrated embodiment of the invention describes a Ge film, but it is to be expressly understood that other semiconductor materials could similarly be employed in a manner consistent with the spirit and scope of the invention. For example, GaAs and InP films might also be employed.  
           [0008]    In the illustrated embodiment by transferring thin, single-crystal layers of Ge to a less expensive Si substrate and reclaiming the donor wafer through a polishing process, a single 300 μm thick Ge wafer serves as a source for transfer of more than one hundred thin Ge layers or films.  
           [0009]    The bond at the interface of the Ge/Si heterostructures is covalent to ensure good thermal contact, mechanical strength, and to enable the formation of an ohmic contact between the Si substrate and Ge layers. To accomplish this type of bond hydrophobic wafer bonding is used, because the hydrogen-surface-terminating species that facilitate van der Waals bonding evolves at temperatures above 600° C. into covalent bonding in hydrophobically bound Ge/Si layer transferred systems.  
           [0010]    Thus, it can now be understood that one embodiment of the invention is defined as a method of forming a Ge-based heterostructure comprising the steps of H +  or He +  doping a Ge substrate by ion implantation, bonding the Ge substrate onto a non-Ge substrate and annealing the bonded structure to exfoliate a Ge film therefrom. Any Ge compatible composition may be used as the substrate with Si being the preferred embodiment. However, InP and GaAs are also expressly contemplated including generally any element or compound which includes elements from Groups III-V of the periodic table.  
           [0011]    The Ge film is bonded onto a Si substrate in the illustrated embodiment. The step of bonding is comprised of the steps of disposing the Ge film in contact with the non-Ge substrate to define an interface between the Ge film and non-Ge substrate; applying at least a first magnitude of pressure across a corresponding first area of the interface; and annealing the interface under a second magnitude of pressure therebetween.  
           [0012]    The step of applying at least a first magnitude of pressure across the interface further comprises the steps of sequentially applying additional magnitudes of pressure across corresponding areas of the interface, e.g. the steps of applying sequentially smaller magnitudes of pressure across sequentially larger areas of the interface. In the illustrated embodiment the step of sequentially applying additional magnitudes of pressure comprises the step of sequentially applying three magnitudes of pressure are applied across three corresponding sized areas of the interface, namely applying a first magnitude of pressure, which is approximately 24 MPa across an approximately 0.64 cm diameter area, followed by approximately 6.1 MPa across an approximately 1.3 cm diameter area, followed by approximately 1.5 MPa across an approximately 2.5 cm diameter area. The step of annealing the bonded structure under a second magnitude of pressure therebetween comprises the step of annealing the interface at approximately 175° C. under approximately 930 kPa of pressure therebetween.  
           [0013]    In another embodiment the method further comprises the step of passivating the non-Ge substrate prior to disposing the Ge film in contact therewith.  
           [0014]    In still another embodiment the method further comprises the step of disposing an anti-bubble layer onto the Ge substrate to create a hydrophilic interface therebetween and thus to reduce hydrogen bubble formation when the Ge substrate is bonded to the non-Ge substrate. Where the substrate is Si, the step of disposing a anti-bubble layer onto the Ge substrate comprises the step of disposing an amorphous Si layer onto the Ge substrate to form a Si/a-Si interface by molecular beam deposition.  
           [0015]    In yet another embodiment the method further comprises the steps of wet chemical cleaning the Ge substrate and non-Ge substrate prior to bonding and then annealing the cleaned Ge substrate and non-Ge substrate prior to bonding, namely annealing the cleaned Ge substrate and non-Ge substrate at approximately 250° C. In N 2 .  
           [0016]    In another embodiment the method further comprises the step of fabricating a semiconductor device onto the Ge-based heterostructure, such as a triple junction solar cell thereon using metal-organic chemical vapor deposition (MOCVD).  
           [0017]    In a further embodiment the method further comprises the step of disposing a smoothing layer onto the exfoliated Ge film, namely a Ge buffer layer using molecular beam epitaxy. Smoothing techniques that may also be applied to the exfoliated film also include CMP and chemical etching processes.  
           [0018]    The invention is also understood to be defined as a Ge-based heterostructure comprising a Ge film, and a non-Ge substrate bonded to the Ge film in which the Ge film has been exfoliated from an H +  ion implanted Ge layer by annealing. Again in the illustrated embodiment the non-Ge substrate is composed of Si, but is expressly meant to include other elements, compounds, and mixtures which include at least in part elements from Groups III-V of the periodic table.  
           [0019]    The Ge substrate and non-Ge substrate are in mutual contact under pressure and annealed to form a covalent bonded interface therebetween. The Ge substrate and non-Ge substrate are brought into mutual contact with each other and subjected to sequential applications of pressure distributed over an area of the interface, namely sequentially smaller magnitudes of pressure across sequentially larger areas of the interface. The non-Ge substrate and Ge substrate are passivated prior to being bonded. As discussed above, an anti-bubble layer may be disposed onto the Ge substrate to create a hydrophilic interface therebetween and thus to reduce hydrogen bubble formation when the Ge film is bonded to the non-Ge substrate, namely where the non-Ge substrate is Si and the anti-bubble layer is amorphous Si. Alternatively, as also discussed above the non-Ge substrate is rendered hydrophilic or hydrophobic by wet chemical cleaning the Ge substrate and non-Ge substrate prior to bonding and then annealing the cleaned Ge film and non-Ge substrate prior to bonding.  
           [0020]    The Ge-based heterostructure is an intermediate structure and generally a semiconductor device will be fabricated on the Ge film. The illustrated embodiment shows the fabrication of a triple junction solar cell thereon using metal-organic chemical vapor deposition (MOCVD). However, what type of semiconductor device can be fabricated on the Ge film is quite arbitrary and should be understood to include any semiconductor device now known or later devised. For example, it is expressly contemplated that in addition to solar cells that GaAs based LEDs and lasers will be fabricated on Ge film heterostructures of the invention  
           [0021]    As discussed the Ge-based heterostructure of the invention also may include a smoothing layer onto the exfoliated Ge film, namely a Ge layer disposed onto the exfoliated Ge film using molecular beam epitaxy.  
           [0022]    While the apparatus and method has or will be described for the sake of grammatical fluidity with functional explanations, it is to be expressly understood that the claims, unless expressly formulated under 35 USC 112, are not to be construed as necessarily limited in any way by the construction of “means” or “steps” limitations, but are to be accorded the full scope of the meaning and equivalents of the definition provided by the claims under the judicial doctrine of equivalents, and in the case where the claims are expressly formulated under 35 USC 112 are to be accorded full statutory equivalents under 35 USC 112. The invention can be better visualized by turning now to the following drawings wherein like elements are referenced by like numerals. 
       
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS  
       [0023]    [0023]FIG. 1 is a graph of a voltage-current curve for a P+Ge/P+Si heterostructure fabricated according to the invention which has been annealed to 350° C. demonstrate ohmic electric contact.  
         [0024]    [0024]FIG. 2 a  is a vertical cross-sectional view of a scanning electron microscope image of a MOCVD triple-junction solar cell structure grown according to the invention on a Ge/Se heterostructure template.  
         [0025]    [0025]FIG. 2 b  is a vertical cross-sectional view of a scanning electron microscope image of a MOCVD triple-junction solar cell structure grown according to the invention on a bulk Ge substrate.  
         [0026]    [0026]FIG. 3 is a graph of the GaAs band-edge emission photoluminescence of MOCVD triple-junction tandem solar cells on Ge/Si heterostructures in Samples 1 and 2 shown in dotted line and on bulk Ge in solid line.  
         [0027]    [0027]FIG. 4 is post-growth RHEED image of a surface showing Bragg rods and a reconstructed Ge surface indicating a smooth top plateau.  
         [0028]    [0028]FIG. 5 a  is an atomic force microscopic view of an exfoliated Ge surface prior to MBE Ge buffer layer growth indicating a surface roughness of about 100 angstrom RMS.  
         [0029]    [0029]FIG. 5 b  is an atomic force microscopic view of the surface of FIG. 5 a  which has been smoothed by the epitaxial growth of a Ge buffer layer to about 20 angstrom RMS roughness with a mesa geometry.  
         [0030]    [0030]FIGS. 6 a - 6   c  are diagrammatic side cross sectional views of the method of fabrication of one embodiment of the invention.  
         [0031]    [0031]FIGS. 7 a - 7   d  are diagrammatic side cross sectional views of the method of fabrication of another embodiment of the invention.  
         [0032]    [0032]FIG. 8 is a diagrammatic side cross sectional view of still another embodiment of the heterostructure. 
     
    
       [0033]    The invention and its various embodiments can now be better understood by turning to the following detailed description of the preferred embodiments which are presented as illustrated examples of the invention defined in the claims. It is expressly understood that the invention as defined by the claims may be broader than the illustrated embodiments described below.  
       DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS  
       [0034]    The invention uses direct wafer bonding in combination with hydrogen-induced layer splitting of germanium to transfer single crystal germanium (100) films  10  to silicon (100) substrates  12  as shown in FIGS. 2 a  and  2   b  without using an intervening metallic bonding layer as is typical in the prior art. The metal-free nature of the bond makes the bonded wafers suitable, for example, for subsequent epitaxial growth of triple-junction GaInP/GaAs/Ge layered solar cells, generally denoted by reference numeral  14 , at high temperatures without concern about metal contamination of the device active region.  
         [0035]    The Exfoliation and Rebonding  
         [0036]    As shown in FIG. 6 a  a germanium crystalline wafer  16  was doped with 1×10 17  cm −2  H +  at 80 keV. These wafers  16  are rendered strongly hydrophobic in the process. The embedded H +  coalesce into hydrogen gas bubbles, which induced an upper film  10  of wafer  16  to split off by a thermal cycle up to more than 350° C. in an N 2  ambient. Layer splitting is achieved by the formation of hydrogen-containing platelets that initiate the propagation of micro-cracks parallel to the Ge surface  18  upon annealing to greater than 350° C. with no external pressure on wafer  16 . Thus, a film  10  is cleaved or exfoliated from wafer  16  and bonded to wafer  20  as diagrammatically shown in FIG. 6 b . The process can be repeated many times and wafer  16  repeatedly split to form a plurality of exfoliated films  10 . Film thickness can be varied by control of the H +  doping concentrations and depths.  
         [0037]    For example, in the illustrated embodiment doped germanium crystalline wafer  16  was used to transfer approximately 700 nm thick films  10  with an area of approximately 1 cm 2 . Ge substrate surface  18  is passivated by removal of any organic contamination by cleaning by acetone and methanol followed by a 1 minute deionized water rinse and a 10 second dip in 5% HF acid followed in turn by surface blow drying to remove any oxide from surface  18  which is left coated with uncontaminated adsorbed hydrophobic H + . Substrate  16  can now be bonded to a different and less costly substrate  20  having the desired electrical or physical properties, e.g. a silicon wafer  20  as shown in FIG. 6 c , and annealed to transfer the film  10 .  
         [0038]    Si (100) wafer  20  was passivated by the same wet process sequence described above and a subsequent rinse followed by a deionized water rinse and a 30 second 80° C. 1:1:3 H 2 O 2 :NH 4 OH:H 2 O (RCA1) cleaning process followed by a deionized water rinse and a brief HF acid dip to remove the grown oxide. The RCA1 cleaning is included to further reduce the organic surface contamination and remove particles. Following surface passivation both Si substrate  20  and Ge substrate  10 , they have an RMS roughness well under 0.5 nm as measured on a 5 μm by 5 μm atomic force microscopy scan.  
         [0039]    After passivation substrate  20  and substrate  16  are brought into surface-to-surface contact with each other as shown in FIG. 6 c  and bonding is initiated by a 3500-psi pressure (24MPa) applied over a 0.25-inch (0.64 cm) diameter region at the center of the wafer. The contact region is then propagated outward using subsequent pressures of 890 psi (6.1 MPa) applied over a 0.5-inch (1.3 cm) diameter region and 220 psi (1.5 MPa) applied over a 1.0-inch (2.5 cm) diameter region. A thermal annealing process to 175° C. with an applied pressure of 135 psi (930 kPa) in a modified Parr Instruments pressure cell is used to strengthen the bonding.  
         [0040]    Hydrophobic surface passivation of film surface  18  and a less than 1 nm RMS roughness of surface  18  as measured by contact mode atomic force microscopy along with more than 3000 psi pressure initiation are suitable conditions for reversible room temperature bonding of substrate  16  to substrate  20  to occur. The low strength room temperature bond is then annealed at 175° C. under 135 psi pressure strengthen the bonding between substrate  16  and substrate  20 . Annealing the bonded structure with or without pressure up to &gt;300 C causes film  10  to transfer to substrate  20 . The covalently bonded heterostructures have been shown to be stable during thermal cycling from room temperature to 750° C.  
         [0041]    Ge-to-Si direct wafer bonding and layer transfer has been achieved as described above, but initial efforts were complicated by gas bubble formation at the bonded Ge/Si interface  36  between film  10  and substrate  20 . These bubbles were likely caused by residual interface contamination present at the time of bonding, either in the form of adsorbed water or organic contamination which subsequently evolved as gas trapped at the interface  36 . These bubbles have been eliminated by two methods.  
         [0042]    The first method is by molecular beam deposition of a 40-Å amorphous Si layer  38  on the H-implanted Ge substrate  16  as diagrammatically shown in FIGS. 7 a - 7   d.  In this case, a hydrophilic or hydrophobic Si—Si wafer bond is later formed with substrate  20  using hydrophilic or hydrophobic surface passivation on both the substrate  20  and the a-Si layer  38  deposited on the Ge substrate  16 . The room-temperature bonding energy for hydrophilic Si surfaces is typically about 100 mJ cm −2  for Si/Si systems. The Ge/Si heterostructures  14  formed by Si/a-Si hydrophilic bonding show a strong reduction in the total number of interfacial bubbles. Bubble reduction is thought to be due to the increased hydrophilic bond strength at the Si/a-Si interface verses the hydrophobic room-temperature bond strength of the Ge/Si interface in the previously mentioned Ge/Si hydrophobic bonding technique. The higher bond strength increases the bubble pressure required to separate the bonded surfaces and to deform the thin Ge transferred film  10 . Additionally, improved organic removal is made possible by the RCA1 cleaning of the a-Si layer  38 .  
         [0043]    The second method to eliminate bubbles at the interface  36  is to use a 250° C. pre-bonding anneal in N 2  following wet chemical cleaning, but prior to bonding the hydrophobic Ge and Si surfaces in the methodology of FIGS. 6 a - 6   c.  This pre-bonding anneal is thought to desorb water and evolve organic contaminants, leaving a more perfectly H-terminated surface. This reduces the bubble defect density in transferred films  10 .  
         [0044]    The Ohmic Contact  
         [0045]    Electrical measurements indicated ohmic I-V characteristics for germanium layers bonded to silicon substrates with less than 35 ohms resistance at the interface such as shown in FIG. 1 and described below.  
         [0046]    The interface electrical properties were measured by defining Al on a Ge/Si heterostructure  14 , prepared by a pre-bonding anneal in N 2  as described above, followed by a layer split anneal at 350° C. The Ge substrate was Ga-doped to 5×10 17  cm −3  and the Si substrate was B doped to 1×10 18  cm −3  in an effort to minimize the junction depletion width formed at the heterojunction interface  36 .  
         [0047]    During initial application of a 10 V bias, the Ge/Si interface 36 exhibited dielectric breakdown followed by ohmic I-V characteristics in subsequent scans as graphically depicted in FIG. 1. These measurements indicate an interfacial resistance of 35-40 Ωover a total interfacial area of about 0.1 cm 2  for a specific interfacial resistance of about 3.5 Ωcm −2 . The Al contact and substrate resistances were determined to be negligible for overall structure resistance. The relatively high interface resistance is attributed to the fact that the bonded Ge/Si sample was annealed at a maximum temperature of 350° C., lower than the temperature required for covalent bond formation, which is 600° C. or greater in Si/Si interfaces.  
         [0048]    The Triple Junction Solar Cell  
         [0049]    Triple-junction solar cell structures grown on these Ge/Si heterostructure templates by metal-organic chemical vacation deposition, MOVCD, as shown in FIGS. 2 a  and  2   b  and described below show comparable photoluminescence intensity and minority carrier lifetime to a control structure grown on bulk Ge as depicted in FIG. 3.  
         [0050]    Metal organic chemical vapor deposition (MOCVD) growth of triple-junction solar cell heterostructures  14  in FIG. 2 a  on bonded Ge/Si substrate  22  was performed using (CH 3 ) 3 Ga and AsH 3  precursors for GaAs cell growth and (CH 3 ) 3 Ga, (CH 3 ) 3 In and PH 3  precursors for GaInP cell growth. The peak temperature during growth was 750° C. and the structure as shown in FIG. 2 a  is comprised of a GaAs buffer layer  24  followed by two active base regions, a GaAs base  24  and a GaInP base  28  separated by a tunnel junction structure  30 .  
         [0051]    Photoluminescence (PL) intensity and time-resolved photoluminescence (TRPL) minority carrier lifetime of the structure of FIG. 2 a  were measured in the heavily doped GaAs top contact layer  32  in a control sample grown on bulk Ge  34  in FIG. 2 b  and structures grown on a Ge/Si heterostructure  14  in FIG. 2 a . Photoluminescence measurements were performed with a pump laser operated at λ=457 nm. Because the heavily doped GaAs contact layer  32  was optically thick to the pump laser, photoluminescence was not observed in the GaInP base  28  or the GaAs base region  26 , both of which are expected to exhibit higher lifetime and superior material quality to the heavily doped GaAs contact layer  32 . Time-resolved photoluminescence measurements were performed at NREL with a 600-nm pump laser operated at a repetition rate of 1000 kHz. The samples were maintained at 293° K during the measurement. The results of the measurement are shown and described in connection with FIG. 3.  
         [0052]    Triple-junction solar cell structures  14  as shown in FIG. 2 a  were grown by metal-organic chemical vapor deposition (MOCVD) on Ge/Si heterostructures fabricated by hydrophobic wafer bonding. Two of these Ge/Si heterostructures were used as templates for growth and labeled Sample 1 and Sample 2, while a control solar cell structure was also grown on bulk Ge in the same process as shown in FIG. 2 b . The RMS surface roughness was measured by contact-mode atomic force microscopy, with the results shown in Table 1. 
                               TABLE 1                                       Ge roughness in Å   Ge roughness in Å           Sample   Pre-MOCVD   Post-MOCVD                           Bulk Ge   &lt;5   147           Sample 1   236   897           Sample 2   225   204                      
 
         [0053]    Sample 1 exhibited RMS surface roughness four-fold greater than that of the GaAs contact layer of Sample 2. These GaAs contact layer roughness values are uncorrelated to the exfoliated Ge surface roughness which was measured, a phenomenon that is not understood at present. Cross-sectional scanning electron micrographs of Sample 1 and the bulk Ge control structure are shown in FIGS. 2 a  and  2   b  respectively. These images show the layer structure of the triple-junction solar cell and the morphology of the interfaces of the various layers and abrupt interfaces within the microscope resolution, about 100 nm. Sample 1 exhibits a rough interface between the layers of the cell structure, with a maximum interface roughness of 0.3 mm located at the GaAs/GaInP interface  30 . Photoluminescence studies of the top GaAs contact layer  32  indicate comparable GaAs band-edge emission at 880 nm for the bulk Ge control and Sample 2, the smoother epitaxial structure on Ge/Si, as indicated in the graph of FIG. 3. Sample 1 exhibits considerably lower photoluminescence intensity than Sample 2. Photoluminescence measurements demonstrate an inverse relationship between the GaAs contact layer  32  surface roughness and GaAs contact layer band-edge photoluminescence intensity, suggesting an increased defect density in the samples with rougher GaAs contact surfaces. Time resolved photoluminescence measurements of the GaAs contact layer  32  indicate short but comparable decay time constants of τ=0.23 ns for the bulk Ge sample and τ=0.20 ns for Sample 2, indicating comparable minority carrier life-times in the two structures, if similar surface recombination velocities are assumed. The GaAs contact is not passivated, thus shortening the minority carrier lifetime of the GaAs contact layer  32 , due to a high recombination velocity at the exposed surface. Additionally, the heavy doping in the GaAs contact layer  32  also limits the minority carrier lifetime in this layer.  
         [0054]    Ge Surface Smoothing  
         [0055]    Contact mode atomic force microscopy images of the transferred germanium surface generated by the formation of micro-bubbles and micro-cracks along the hydrogen-induced layer-splitting interface reveals minimum RMS roughness of between 10 nm and 23 nm.  
         [0056]    The use of a molecular beam epitaxy Ge buffer layer to smooth the cleaved surface of the Ge heterostructure as shown in FIGS. 5 a  and  5   b  has been shown to smooth the surface from about 11 nm to as low as 1.5 nm with a mesa-like morphology that has a top surface roughness of under 1.0 nm giving a promising surface for improved solar cell growth on solar cell structures.  
         [0057]    The triple-junction solar cell optical performance results indicate that without any surface preparation following the H-induced cleavage of the Ge layer  10 , high quality Group III-V photovoltaic materials can be grown with good photoluminescence intensity and minority carrier lifetime properties relative to a cell grown on a bulk Ge substrate  34 . However, to further improve the optical and electrical properties, it is desirable to reduce the exfoliated surface roughness. To smooth the exfoliated Ge surface  18  a 250 nm-thick Ge buffer layer  40  as shown in FIG. 8 was grown on the surface of the Ge/Si heterostructure  14  by molecular beam epitaxy at 450° C. at a rate of 0.1 nm/s. The surface evolution was monitored in situ with reflection high electron energy diffraction. The reflection high energy electron diffraction spectrometer (RHEED) pattern as shown in FIG. 4 following the growth also indicated a smooth (2×1) reconstructed Ge (100) surface. Epitaxial Ge growth reduced the surface RMS roughness of the transferred Ge layer from about 11 to about 1.5 nm. In addition, the morphology of the surface drastically changed to a mesa-like form, with a large relatively smooth layer of less than 1 nm surface roughness, as illustrated in the comparison of the atomic force micrographs of FIGS. 5 a  and  5   b.    
         [0058]    In summary, it can now be appreciated that fabrication of high quality, large, e.g. about 1 cm 2  area Ge (100)/Si (100) heterostructures by hydrophobic wafer bonding and H-induced layer splitting is enabled by the above disclosure. Bonded Ge/Si heterostructures  14  exhibit ohmic interfaces and are suitable as templates for heterostructured devices, such as MOCVD growth of InGaP/GaAs/Ge triple-junction solar cell structures with photoluminescence intensity and decay lifetimes comparable to those found in solar cell structures grown on bulk Ge (100) substrates. Epitaxial growth of Ge buffer layers on transferred Ge/Si layers shows promise as a means of reducing the Ge surface roughness and improving the optical quality of epitaxial GaInP/GaAs/Ge layers.  
         [0059]    Many alterations and modifications may be made by those having ordinary skill in the art without departing from the spirit and scope of the invention. Therefore, it must be understood that the illustrated embodiment has been set forth only for the purposes of example and that it should not be taken as limiting the invention as defined by the following claims. For example, notwithstanding the fact that the elements of a claim are set forth below in a certain combination, it must be expressly understood that the invention includes other combinations of fewer, more or different elements, which are disclosed in above even when not initially claimed in such combinations.  
         [0060]    The words used in this specification to describe the invention and its various embodiments are to be understood not only in the sense of their commonly defined meanings, but to include by special definition in this specification structure, material or acts beyond the scope of the commonly defined meanings. Thus if an element can be understood in the context of this specification as including more than one meaning, then its use in a claim must be understood as being generic to all possible meanings supported by the specification and by the word itself.  
         [0061]    The definitions of the words or elements of the following claims are, therefore, defined in this specification to include not only the combination of elements which are literally set forth, but all equivalent structure, material or acts for performing substantially the same function in substantially the same way to obtain substantially the same result. In this sense it is therefore contemplated that an equivalent substitution of two or more elements may be made for any one of the elements in the claims below or that a single element may be substituted for two or more elements in a claim. Although elements may be described above as acting in certain combinations and even initially claimed as such, it is to be expressly understood that one or more elements from a claimed combination can in some cases be excised from the combination and that the claimed combination may be directed to a subcombination or variation of a subcombination.  
         [0062]    Insubstantial changes from the claimed subject matter as viewed by a person with ordinary skill in the art, now known or later devised, are expressly contemplated as being equivalently within the scope of the claims. Therefore, obvious substitutions now or later known to one with ordinary skill in the art are defined to be within the scope of the defined elements.  
         [0063]    The claims are thus to be understood to include what is specifically illustrated and described above, what is conceptionally equivalent, what can be obviously substituted and also what essentially incorporates the essential idea of the invention.