AD9575
Rev. A | Page 9 of 16
TYPICAL PERFORMANCE CHARACTERISTICS
–160
–155
–150
–145
–140
–135
–130
–125
–120
–115
110
1k 10k 100k 1M 10M 100M
FREQUENCY (Hz)
PHASE NOISE (dBc/Hz)
08462-006
Figure 5. Phase Noise at LVPECL, 100 MHz Clock Output
–160
–155
–150
–145
–140
–135
–130
–125
–120
–115
110
1k 10k 100k 1M 10M 100M
FREQUENCY (Hz)
PHASE NOISE (dBc/Hz)
08462-007
Figure 6. Phase Noise at LVPECL, 106.25 MHz Clock Output
–160
–155
–150
–145
–140
–135
–130
–125
–120
–115
110
1k 10k 100k 1M 10M 100M
FREQUENCY (Hz)
PHASE NOISE (dBc/Hz)
08462-008
Figure 7. Phase Noise at LVPECL, 125 MHz Clock Output
–160
–155
–150
–145
–140
–135
–130
–125
–120
–115
110
1k 10k 100k 1M 10M 100M
FREQUENCY (Hz)
PHASE NOISE (dBc/Hz)
08462-009
Figure 8. Phase Noise at LVPECL, 155.52 MHz Clock Output
–160
–155
–150
–145
–140
–135
–130
–125
–120
–115
110
1k 10k 100k 1M 10M 100M
FREQUENCY (Hz)
PHASE NOISE (dBc/Hz)
08462-010
Figure 9. Phase Noise at LVPECL, 156.25 MHz Clock Output
–160
–155
–150
–145
–140
–135
–130
–125
–120
–115
110
1k 10k 100k 1M 10M 100M
FREQUENCY (Hz)
PHASE NOISE (dBc/Hz)
08462-011
Figure 10. Phase Noise at LVPECL, 159.375 MHz Clock Output
AD9575
Rev. A | Page 10 of 16
–160
–155
–150
–145
–140
–135
–130
–125
–120
–115
110
1k 10k 100k 1M 10M 100M
FREQUENCY (Hz)
PHASE NOISE (dBc/Hz)
08462-027
Figure 11. Phase Noise at LVPECL, 161.13 MHz Clock Output
–160
–155
–150
–145
–140
–135
–130
–125
–120
–115
110
1k 10k 100k 1M 10M 100M
FREQUENCY (Hz)
PHASE NOISE (dBc/Hz)
08462-012
Figure 12. Phase Noise at LVPECL, 312.5 MHz Clock Output
08462-021
90
100
110
120
130
140
SUPPLY CURRENT (mA)
80
1234
MODE
5678
LVPECL
LVDS
Figure 13. Typical Supply Current vs. Mode (see Table 12)
M2
M2 50mV 2ns
M3 50mV 2ns
08462-022
Figure 14. 156.25 MHz LVDS Output
M2
M2 100mV 1ns
M3 100mV 1ns
0
8462-023
Figure 15. 312.5 MHz LVPECL Output
M2
M2 100mV 10ns
M3 100mV 10ns
08462-024
Figure 16. 62.5 MHz LVCMOS Output
AD9575
Rev. A | Page 11 of 16
TERMINOLOGY
Phase Jitter
An ideal sine wave can be thought of as having a continuous
and even progression of phase with time from 0° to 360° for
each cycle. Actual signals, however, display a certain amount of
variation from ideal phase progression over time. This phenom-
enon is called phase jitter. Although many causes can contribute
to phase jitter, one major cause is random noise, which is charac-
terized statistically as Gaussian (normal) in distribution.
This phase jitter leads to a spreading out of the energy of the
sine wave in the frequency domain, producing a continuous
power spectrum. This power spectrum is usually reported as
a series of values whose units are dBc/Hz at a given offset in
frequency from the sine wave (carrier). The value is a ratio
(expressed in decibels) of the power contained within a 1 Hz
bandwidth with respect to the power at the carrier frequency.
For each measurement, the offset from the carrier frequency
is also given.
Phase Noise
It is meaningful to integrate the total power contained within
some interval of offset frequencies (for example, 10 kHz to
10 MHz). This is called the integrated phase noise over that
frequency offset interval and can be readily related to the time
jitter due to the phase noise within that offset frequency interval.
Phase noise has a detrimental effect on error rate performance
by increasing eye closure at the transmitter output and reducing
the jitter tolerance/sensitivity of the receiver.
Time Jitter
Phase noise is a frequency domain phenomenon. In the time
domain, the same effect is exhibited as time jitter. When
observing a sine wave, the time of successive zero crossings is
seen to vary. In a square wave, the time jitter is seen as a
displacement of the edges from their ideal (regular) times of
occurrence. In both cases, the variations in timing from the
ideal are the time jitter. Because these variations are random in
nature, the time jitter is specified in units of seconds root mean
square (rms) or 1 sigma of the Gaussian distribution.
Additive Phase Noise
Additive phase noise is the amount of phase noise that is attrib-
utable to the device or subsystem being measured. The phase
noise of any external oscillators or clock sources is subtracted.
This makes it possible to predict the degree to which the device
affects the total system phase noise when used in conjunction
with the various oscillators and clock sources, each of which
contributes its own phase noise to the total. In many cases, the
phase noise of one element dominates the system phase noise.
Additive Time Jitter
Additive time jitter is the amount of time jitter that is attribut-
able to the device or subsystem being measured. The time jitter
of any external oscillators or clock sources is subtracted. This
makes it possible to predict the degree to which the device affects
the total system time jitter when used in conjunction with the
various oscillators and clock sources, each of which contributes
its own time jitter to the total. In many cases, the time jitter of
the external oscillators and clock sources dominates the system
time jitter.

AD9575ARUZPEC

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Clock Generators & Support Products PCI-Express PLL Core 2 Outputs
Lifecycle:
New from this manufacturer.
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