Symmetry
Linearity
The Fourier Theorems
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Conjugation and Reversal
Theorem: For any
,
Proof:
Theorem: For any
,
Proof: Making the change of summation variable
, we get
Theorem: For any
,
Proof:
Corollary:
For any
,
Proof: Picking up the previous proof at the third formula, remembering that
is real,
when
is real.
Thus, conjugation in the
frequency domain corresponds to reversal in the time domain. Another
way to say it is that
negating spectral phase flips the signal around backwards in
time.
Corollary:
For any
,
Proof: This follows from the previous two cases.
Definition: The property
is called Hermitian symmetry
or ``conjugate symmetry.'' If
, it may be called
skew-Hermitian.
Another way to state the preceding corollary is
Symmetry
Linearity
The Fourier Theorems
Contents
Global Contents
Global Index
  Index
  Search
``Mathematics of the Discrete Fourier Transform (DFT)'',
by Julius O. Smith III,
W3K Publishing, 2003, ISBN 0-9745607-0-7.
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Copyright © 2003-10-09 by Julius O. Smith III
Center for Computer Research in Music and Acoustics (CCRMA),
Stanford University
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