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GC2011A Datasheet(PDF) 23 Page - Texas Instruments

Part # GC2011A
Description  3.3V DIGITAL FILTER CHIP
PDF  50 Pages
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Manufacturer  TI [Texas Instruments]
Direct Link  http://www.ti.com
Logo TI - Texas Instruments

GC2011A Datasheet(HTML) 23 Page - Texas Instruments

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Texas Instruments Incorporated
- 19 -
GC2011A 3.3V DIGITAL FILTER CHIP
SLWS129A
This document contains information which may be changed at any time without notice
3.7
DHILBERT TRANSFORM FILTERS
A Hilbert transform filter converts real signals to complex signals by passing the signal’s positive spectral
frequencies and rejecting its negative frequencies. For example, a sinewave of frequency “w” has both the positive
frequency component ejwt and the negative frequency component e-jwt. The Hilbert transform of the sinewave will be
just the positive component ejwt.
The coefficients for a Hilbert transform can be generated by designing a linear phase low pass filter with a
passband from 0 to FS/4 and a stopband from FS/4 to FS/2, where FS is the signal’s sample rate. The low pass filter’s
impulse response is then mixed up to be centered on FS/4 by multiplying the coefficients by the sequence: (j, -1, -j, 1, j,
-1, -j,
…).
For example, the coefficients:
(h0,h1,h2,h3,h4,h5,h6,h7,h6,h5,h4,h3,h2,h1,h0)
would become:
(jh0,-h1,-jh2,h3,jh4,-h5,-jh6,h7,jh6,-h5,-jh4,h3,jh2,-h1,-jh0).
These coefficients then split into the real coefficients:
( 0, -h1,
0, h3, 0, -h5,
0, h7,
0, -h5,
0, h3,
0, -h1,
0)
and the imaginary coefficients:
(h0,
0, -h2,
0, h4,
0, -h6,
0, h6,
0, -h4,
0, h2,
0, -h0).
As seen in this example, the real coefficients of a Hilbert transform filter have odd symmetry with the center
tap non-zero and every other tap equal to zero. The imaginary coefficients have negative odd symmetry.
A special, but important, version of the Hilbert transform exists when the filter has half-band symmetry.
Half-band symmetry forces all of the real coefficients except the center tap to be zero. The real half filter, for the
half-band Hilbert Transform, is, therefore, just a delay line.
The following table shows how to configure the GC2011A chip for the Hilbert Transform. The A-path is used
for the real part and the B-path for the imaginary part.
Since the coefficients are symmetric, only 32 of the 63 low pass filter coefficients are stored in the chip. If the
low-pass filter coefficients are h(k), for k=0 to 31, where h(31) is the center tap, then coefficient register 0 of each filter
cell is loaded as:
Store -h(4k)
in memory address 192+8*k for k=0 to 7
Store -h(4k+1) in memory address 128+8*k for k=0 to 7
Store +h(4k+2) in memory address 196+8*k for k=0 to 7
Store +h(4k+3) in memory address 132+8*k for k=0 to 7
Note that the odd coefficients are stored in the A-path, and that the even coefficients are stored in the B-path. Also note
that every other odd and every other even coefficient are negated. In the half-band Hilbert transform only h(31) will be
non-zero in the A-path.
Table 8: Hilbert Transform Mode Control Register Settings
Dual Path or
Cascaded
# of Taps
(N)
A-PATH
B-PATH
Cascade
Latency
REG0
REG1
REG0
REG1
REG
Dual
63
60C8
2E84
20C8
2E78
2000
45



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