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Table 6.6: Berlekamp-Massey Algorithm for a Double-Error Correcting Code 1 dm k sk C(X) L Pb) dk 1 1 1 417 1 417 a17 1 + 4 ' 7 x 2 417 1+4'7x 1 1 2 43 0 1+a'7x+a22x2 2 1+a17x 1 4 8 48 3 1 2 48 1+a'7x+422x2 2 1+a'7x 0 4 a6

Example 7.7 For the ( x i , y i ) data of Example 7.1, the execution of the algorithm is as follows (using 1-based indexing):

Method java.lang.Object() 0 return Method boolean equals(java.lang.Object) 0 aload_0 1 aload_1 2 if_acmpeq 9 5 iconst_0 6 goto 10 9 iconst_1 10 ireturn Method void finalize() 0 return Method java.lang.String toString() 0 new #13 <Class java.lang.StringBuffer> 3 dup 4 aload_0 5 invokevirtual #18 <Method java.lang.Class getClass()> 8 invokevirtual #19 <Method java.lang.String getName()> 11 invokestatic #24 <Method java.lang.String valueOf(java.lang.Object)> 14 invokespecial #16 <Method java.lang.StringBuffer(java.lang.String)> 17 ldc #3 <String @ > 19 invokevirtual #17 <Method java.lang.StringBuffer append(java.lang.String)> 22 aload_0 23 invokevirtual #20 <Method int hashCode()> 26 invokestatic #22 <Method java.lang.String toHexString(int)> 29 invokevirtual #17 <Method java.lang.StringBuffer append(java.lang.String)> 32 invokevirtual #23 <Method java.lang.String toString()> 35 areturn

g(xn)

MI].

Before you begin including dynamic data, you need to establish a data source connection and recordset, so be sure you re familiar with the techniques described in 19 before proceeding.

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Theorem 5.39 allows a sequence of equations to be built up for determining Im for any m . Take for example q = 2: k = 1: k = 2: k = 3:

The material dependence of the resonance frequency is given by Equation (186) (Section 18241), which allows either a direct comparison between different materials of identical geometry or, equally, can be used to describe the in uence of geometry on an identical performance material Diamond seems to be the most appropriate material for high frequency applications The in uence of the material parameters in scaling is however only by the square root Therefore, differences are rather moderate and may be overruled by the resolution limits of the respective processing technologies Another important aspect is the quality factor Q, which re ects the losses at resonance; a high Q-factor representing low losses Q will depend on mechanical losses like internal friction, which may be mainly associated with grain boundaries, or external friction such as air damping.

s a ( L - x)

However, at the small geometries needed for high speed applications, inhomogeneities such as surface roughness may become important [204] At sub- m geometries, the boundary conditions, mostly determined by the geometrical layout, need also to allow the resonance to develop with maximum ef ciency Mechanical matching becomes important [205] Therefore microwave resonators have been built with nanoor ultrananocrystalline diamond [206], but may have to compete with single-crystal Si technologies A test structure for diamond resonator performance can be seen in Figure 1836 [206] NCD bridge structures with a length ranging from 1 to 8 m (often also called clamped clamped or double ended beams), are xed within a diamond frame similar to an Euler bar test structure, (see Section 18322).

117 10

However, in contrast to an Euler bar, as a resonator the bridge needs to be stress free (or stress balanced), since built-in stress will lower the resonance frequency It can be seen from the diagram, that with decreasing beam length the resonance frequency increases to 640 MHz for a length of 2 m The lm thickness was 180 nm The square root relationship between length and resonance frequency is well preserved The rst order resonance of double-clamped cantilevers is approximately six times higher than in the case of a single-ended cantilever as discussed in Sections 18241 and 18244 It should be noted that the beams have been covered by a metallisation layer, used for electrostatic actuation with the help of a counter electrode.

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