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With increasing applied magnetic eld, the superconducting transition temperature is found to shift toward lower temperatures. In Figure 19.2(b), the TConset and TCzero are plotted in the temperature versus magnetic eld diagram to estimate the upper critical eld HC2 and the irreversibility eld Hirr , where HC2 is the maximum magnetic eld in which superconductivity can survive and Hirr is the maximum magnetic eld where zero resistivity can be obtained. Assuming that the superconductivity is in the dirty limit, HC2 is approximated to be 10.4 T using the equation H = HC2WHH (1 T /TC )1.5 . Here, it was found that this equation could be used for an approximation of the WHH theory [33]. The coherent length was also determined from HC2 to be = 5.51 nm using the equation = ( 0/2 HC2 )1/2 . The irreversibility eld was estimated at Hirr = 9.0 T from the linear extrapolation of TCzero . The variation in resistivity with temperature above TC is very at, which suggests that the transport properties are not those of a simple metal. In contrast, for homoepitaxial (100) lms, the superconducting transition temperatures TConset = 6.3 K and TCzero = 3.2 K, which are about half those obtained for the (111) thin lm, were obtained even at the same boron concentration as shown in Figure 19.2(c). From the temperature versus magnetic eld diagram of TConset and TCzero , upper critical eld and irreversibility eld were estimated to be HC2 = 5.27 T and Hirr = 4.47 T, and the coherent length = 7.89 nm (Figure 19.2d). These results indicate that the superconductivity in homoepitaxial (100) lms is signi cantly suppressed [30, 34]. The reason for the signi cant difference in superconductivity observed for the (111) and (100) thin lms is discussed in the next section.

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