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4.8 HILBERT TRANSFORM                            231

           etc. For example, let’s find out the inverse of the  applying a π/2 rad phase difference to each fre-
           wavelet w(t) ¼ (2, 1). The z transform of the  quency component of the input function. The
           wavelet is w(z) ¼ (2 + z) and its inverse is  theoretical basis of the transform depends on
           wzðÞ ¼ 1= 2+ zÞ. In order to determine the   the definition of analytical function. The time-
                   ð
           inverse wzðÞ, derivatives of 1/(2 + z) are calcu-  dependent analytical function u(t) is a complex
           lated.  The    first  four  derivatives  of  function and can be defined as
           wzðÞ ¼ 1= 2+ zÞ are
                   ð
                                                                      utðÞ ¼ xtðÞ + iy tðÞ    (4.29)
                          1             2
                0               00            000
                                                z
               w zðÞ ¼         w zðÞ ¼       w ðÞ       where x(t) and y(t) are real and imaginary com-
                            2              3
                       ð 2+ zÞ        ð 2+ zÞ           ponents, respectively, and are known as the
                          6             24
                                000 0
                                   z
                    ¼          w ðÞ ¼                   Hilbert transform pair (Fig. 4.17A). Bracewell
                            4               5
                       ð 2+ zÞ        ð 2+ zÞ           (1965) suggested that the imaginary component
                                                        y(t) is obtained by the Hilbert transform of the
           Substituting z ¼ 0 into the derivatives of wzðÞ,
           we can obtain the coefficients in Eq. (4.28). Using  real component x(t)by
                                                                                ∗
           a MacLaurin series expansion, the z transform of            ytðÞ ¼ htðÞ xtðÞ       (4.30)
           the inverse of wavelet w(t) ¼ (2, 1) can be
           obtained as                                  where * denotes convolution, h(t) is the Hilbert
                                                        transform operator (Fig. 4.17B) defined by
                       1  1   1  2  1  3  1  4
                wzðÞ ¼   z + z       z +   z  ⋯                                 1
                       2  4   8    16    32                               htðÞ ¼              (4.31)
                                                                               πt
           Getting the coefficients of z, the inverse of the
           wavelet  w(t) ¼ (2,  1)  can  be  found  as  and its Fourier transform H(ω) is described as
           wtðÞ ¼ 1=2,  1=4, 1=8,  1=16, 1=32, …Þ.      (Fig. 4.17C):
                 ð
                                                                                  i ω > 0
                                                                               8
                                                                               >
                                                                               >
                                                                               <
                 4.8 HILBERT TRANSFORM                       H ωðÞ ¼  isgn ωðÞ ¼  +i ω < 0    (4.32)
                                                                               >
                                                                               >
                                                                               :
                                                                                 0  ω ¼ 0
              The Hilbert transform is a useful tool to
           obtain extra information from the seismic data,  where sgn(ω) is the signum function. Substitut-
           known as complex trace attributes, explained  ing Eq. (4.31) into Eq. (4.29), we get (Barnes,
           in Section 12.5. It is a mathematical process  2007):











           FIG. 4.17  (A) Analytical signal, (B) Hilbert transform operator, (C) Fourier transform of (B).
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