Dynamic magnetic information storage or retrieval – General recording or reproducing
Reexamination Certificate
2000-02-14
2004-08-10
Hudspeth, David (Department: 2651)
Dynamic magnetic information storage or retrieval
General recording or reproducing
C360S051000
Reexamination Certificate
active
06775084
ABSTRACT:
TECHNICAL FIELD OF THE INVENTION
The invention relates generally to electronic circuits, and more particularly to a circuit and method for providing an initial phase difference between a disk-drive read signal and a read-signal sample clock. A digital timing-recovery circuit can use this phase difference to provide an initial coarse alignment between the read signal and the sample clock. By providing an initial coarse alignment, the recovery circuit can reduce the overall alignment-acquisition time.
BACKGROUND OF THE INVENTION
Switching and other types of noise can cause today's high-speed integrated circuits (ICs) to operate improperly. One solution is to electrically isolate a noise-susceptible circuit from a noisy circuit using a ground plane, shielding, or other isolation techniques. Another solution is modify the noisy circuit so that it generates less noise.
In addition, to placate computer users who are demanding faster data-processing and data-transfer rates, IC manufacturers wish to design faster digital ICs that support these faster rates. Typically, one increases data-processing and transfer rates by increasing the clock speed of the ICs that perform these tasks. Unfortunately, merely increasing an IC's clock frequency without redesigning it may cause circuits on the IC to oscillate.
FIG. 1
is a block diagram of a conventional disk-drive read channel
10
having a voltage-controlled oscillator (VCO)
12
, which may inject noise or transients into other circuits within the read channel
10
or elsewhere. The read channel
10
includes a read path
14
, which includes a disk
16
for storing data, a read head
18
for reading the disk
16
and for generating a read signal that represents the read data, a read circuit
20
for sampling the read signal in response to a sample clock, and a Viterbi detector
22
for recovering the stored data from the samples of the read signal. The read channel
10
also includes a phase-locked timing loop
24
for generating the sample clock, for aligning the sample clock with the read signal such that the read circuit
20
samples the read signal at appropriate times, and for maintaining the alignment of the sample clock. The timing loop
24
includes a phase detector
26
for generating an error signal that represents the phase difference between the read signal and the sample clock, a filter
28
for filtering the error signal, the VCO
12
for generating the sample clock at a frequency indicated by the filtered error signal, and a frequency divider
30
for allowing the frequency of the sample clock to be greater than the data rate of the read signal. The read circuit
20
effectively closes the loop
24
, i.e., couples the loop input to the loop output.
FIG. 2
is a timing diagram showing the desired alignment between the sample clock and the preamble portion of the read signal. Referring to
FIGS. 1 and 2
, the preamble is a bit pattern stored at the beginning of every sector (individual sectors not shown) of the disk
16
. The read channel
10
uses the preamble to calibrate the channel timing with respect to the read signal. While reading the preamble, the read head
18
generates a sinusoid (or an approximate sinusoid). The peaks and zero crossings of this preamble sinusoid correspond to the centers of respective data windows
34
. During the subsequent data portion (not shown) of the read signal, the centers of the data windows
34
correspond to the data points of the read signal—the data points are the portions of the read signal that the head
18
generates while positioned directly over the respective storage locations on the surface of the disk
16
. By aligning the sampling edges of the sampling clock with the peaks and zero crossings of the preamble sinusoid, these edges will be aligned with the centers of the data windows
34
during the data portion of the read signal, and thus will cause the read circuit
20
to sample the read signal at the data points.
Referring to
FIGS. 1 and 2
, the timing loop
24
aligns the sample clock with the read signal during the preamble portion and maintains this alignment during the data portion of the read signal. In response to the zero crossing of the preamble sinusoid at time t
0
, a start-up circuit (not shown) causes the VCO to generate a predetermined edge of the sample clock—a falling edge in this example—and thus provides a coarse alignment between the preamble sinusoid and the sample clock. Next, the timing loop
24
uses negative feedback to align the rising edges of the sample clock with the sinusoid peaks and to align the falling edges of the sample clock with the sinusoid zero crossings. That is, if the rising and falling edges are leading the respective peaks and zero crossings, then the loop
24
reduces the frequency of the VCO
12
. Conversely, if the rising and falling edges are lagging the respective peaks and zero crossings, then the loop
24
increases the frequency of the VCO
12
. Thus, the timing loop
24
provides a fine alignment between the preamble sinusoid and the sample clock. At a predetermined time t
1
, the timing loop
24
is deemed to have aligned the sample clock with the preamble sinusoid. To maintain this alignment, however, the loop
24
continues to adjust the VCO frequency as necessary during the remainder of the preamble portion and throughout the data portion of the read signal.
Unfortunately, the timing loop
24
may generate noise that adversely affects other circuits such as those in the read path
14
. Specifically, the adjusting of the VCO frequency to acquire and maintain alignment between the sample clock and the read signal often generates significant amounts of noise. Because the timing loop
24
is often integrated on the same die as noise-sensitive circuits, isolation techniques such as using ground plane or shielding are often unavailable, ineffective, prohibitively complex, or prohibitively expensive.
In addition, the timing loop
24
often has a relatively high latency, which often limits the data-read rate of the read channel
10
. The loop's latency is equivalent to the loop delay, or the time it takes for a signal to travel from an arbitrary starting point in the loop, through the loop, and back to the starting point. For example, starting at the output of the read circuit
20
, the phase detector
26
processes a sample of the read signal, the filtered error signal adjusts the frequency of the sample clock, in response to the phase difference between the sample point of the read signal and the sample clock, the read circuit
20
generates a subsequent sample in response to the adjusted sample clock, and then the process repeats. As the frequency of the sample clock increases, the timing loop
24
effectively responds more slowly to phase changes between the read signal and sample clock, and thus the loop's margin of stability decreases. If the frequency of the sample clock increases beyond the frequency of the loop
24
, then the loop
24
oscillates and causes the read channel
10
to operate improperly. Thus, the relatively high latency of the loop
24
limits the frequency of the sample clock, and thus limits the data-read rate of the read channel
10
.
Fortunately, a conventional digital timing-recovery loop does not suffer from the above-described limitations of the timing loop
24
(FIG.
1
). Generally, a digital timing-recovery loop includes a free-running VCO having a frequency that corresponds to the expected rate at which the read head
18
will read data bits from the disk
16
. But instead of adjusting the VCO frequency to acquire and maintain alignment between the sample clock and the read signal, the digital timing-recovery loop adjusts the values of the read samples to the values they would have had if the sample clock and read signal were aligned.
But unfortunately, using a digital timing-recovery loop instead of the phase-lock timing loop
24
(
FIG. 1
) often requires a reduction in the data-storage density of the disk
16
(FIG.
1
). The digital timing-recovery loop lacks a start-u
Byrne Jason D.
Ozdemir Hakan
Colon Rocio
Hudspeth David
Santarelli Bryan A.
STMicroelectronics Inc.
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