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LTC6952 Datasheet(PDF) 72 Page - Analog Devices

Part # LTC6952
Description  Ultralow Jitter, 4.5GHz PLL with 11 Outputs and JESD204B Support
PDF  80 Pages
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Manufacturer  AD [Analog Devices]
Direct Link  http://www.analog.com
Logo AD - Analog Devices

LTC6952 Datasheet(HTML) 72 Page - Analog Devices

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LTC6952
72
6952f
For more information www.analog.com
Preliminary Technical Data
Advance Product Information Subject to Change
Rev PrA
APPLICATIONS INFORMATION
The purpose of R1 and R2 in Figure 50 is to force an offset
at the SYSREF inputs equivalent to a CML logic “0” when
the SYSREF output is not active. The resistors’ values are
determined by the supply voltage (VDD) and the receiver
device’s input common mode voltage (VCM)anddifferential
input resistance (RDIFF). Use Equation 26 to calculate R1
and Equation 27 to calculate R2.
R1 = RDIFF • [VCM/0.44 – 0.5]
(26)
R2 = RDIFF • [(VDD – VCM)/0.44 – 0.5]
(27)
For receiver devices with internal 100Ω terminations, the
values of R1 and R2 can be very small and will affect the
overall termination impedance, leading to undesirable
impedance mismatch. For this reason, the use of pulsed
SYSREFs (MODEx = 3) AC coupled into receiver parts with
internal 100Ω terminations is not recommended.
Settling time for pulsed SYSREF connections (Figure 50)
is approximately determined by the AC coupling capaci-
tors (CAC), both the differential and common mode input
resistance of the receiver device (RDIFF and RCM), and
resistors R1 and R2:
tsettleP ≅ 10 • [RDEV • ROS/(RDEV + ROS)] • CAC
where:
RDEV = 2RCM + RDIFF/2
ROS = minimum(R1, R2)
For pulsed mode SYSREFs to work correctly with AC
coupling, tsettleP must be greater than 1000/fSYSREF, where
fSYSREF is the frequency of the SYSREF pulses.
Use the following procedure to achieve correct JESD204B
SYSREF behavior for AC coupled pulsed SYSREFs.
These methods assume that the SYSREF outputs have
already been synchronized and that the SYSREF output
drivers have been disabled for power savings (PDx = 2).
Pulsed SYSREFs (MODEx = 3)
1. Enable the LTC6952 SYSREF output drivers by setting
PDx = 0 and set SRQMD = 1.
2. Wait for a settling period of at least tsettleP.
3. Set the receiver device to accept SYSREFs.
Figure 51. Example of Spurious Measurement Technique
100Ω
50Ω
OUTx+
OUTx–
6952 F51
LTC6952
OUTx+
OUTx–
LTC6955
IN+
IN–
SPECTRUM
ANALYZER
4. Set SSRQ or the EZS_SRQ inputs to “1” for at least
1ms, then set back to “0”.
5. Set the receiver device to stop accepting SYSREFs.
6. Disable the LTC6952 SYSREF output drivers by setting
PDx = 2 and set SRQMD = 0
MEASURING DIFFERENTIAL SPURIOUS SIGNALS
USING SINGLE-ENDED TEST EQUIPMENT
Using a spectrum analyzer to measure spurious signals
on the single-ended output of a clock generation chip will
give pessimistic results, particularly for outputs that ap-
proximate square waves. There are two reasons for this.
First, since the spurious energy is often an AC signal
superimposed on the power supply, a differential output
will reject the spurs to within the matching of the posi-
tive and negative outputs. Observing only one side of the
differential output will provide no rejection.
Second, and most importantly, the spectrum analyzer will
display all of the energy at its input, including amplitude
modulation that occurs at the top and bottom pedestal
voltage of the square wave. However, only amplitude
modulation near a zero crossing will affect the clock.
The best way to remove this measurement error is to
drive the clock generator output differentially into a limit-
ing buffer on a separate clean power supply. One of the
differential outputs of the limiting buffer can then connect
to a spectrum analyzer to correctly measure the spurious
energy. An example of this technique using the LTC6952
as the clock generator and an LTC6955 as the limiter is
shown in Figure 51.



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