MPC9239 REVISION 2 DECEMBER 18, 2012 7 ©2012 Integrated Device Technology, Inc.
MPC9239 Data Sheet 900 MHz Low Voltage LVPECL Clock Synthesizer
PROGRAMMING INTERFACE
Programming the MPC9239
Programming the MPC9239 amounts to properly configuring
the internal PLL dividers to produce the desired synthesized
frequency at the output. The output frequency can be
represented by this formula:
f
OUT
= (f
XTAL
2) (M 4) (N 2) or (1)
f
OUT
= f
XTAL
M N(2)
where f
XTAL
is the crystal frequency, M is the PLL
feedback-divider and N is the PLL post-divider. The input
frequency and the selection of the feedback divider M is limited
by the VCO-frequency range. f
XTAL
and M must be configured
to match the VCO frequency range of 800 to 1800 MHz in order
to achieve stable PLL operation:
M
MIN
= f
VCO,MIN
(2 f
XTAL
) and (3)
M
MAX
= f
VCO,MAX
(2 f
XTAL
)(4)
For instance, the use of a 16 MHz input frequency requires
the configuration of the PLL feedback divider between M = 25
and M = 56. Table 8 shows the usable VCO frequency and M
divider range for other example input frequencies.
Assuming that a 16 MHz input frequency is used, equation
(2) reduces to:
f
OUT
= 16 M N
Substituting N for the four available values for N (1, 2, 4, 8)
yields:
Example Calculation for an 16 MHz Input Frequency
For example, if an output frequency of 384 MHz was desired,
the following steps would be taken to identify the appropriate M
and N values. 384 MHz falls within the frequency range set by
an N value of 2, so N[1:0]=00. For N = 2, f
OUT
= 8M, and
M=f
OUT
8. Therefore, M = 384 8 = 48, so M[6:0] = 0110000.
Following this procedure a user can generate any whole
frequency between 50 MHz and 900 MHz. The size of the
programmable frequency steps will be equal to:
f
STEP
= f
XTAL
N
APPLICATIONS INFORMATION
Using the Parallel and Serial Interface
The M and N counters can be loaded either through a parallel
or serial interface. The parallel interface is controlled via the
P_LOAD
signal such that a LOW to HIGH transition will latch
the information present on the M[6:0] and N[1:0] inputs into the
M and N counters. When the P_LOAD
signal is LOW the input
latches will be transparent and any changes on the M[6:0] and
N[1:0] inputs will affect the f
OUT
output pair. To use the serial
port the S_CLOCK signal samples the information on the
S_DATA line and loads it into a 12 bit shift register. Note that the
P_LOAD
signal must be HIGH for the serial load operation to
function. The Test register is loaded with the first three bits, the
N register with the next two, and the M register with the final
eight bits of the data stream on the S_DATA input. For each
register the most significant bit is loaded first (T2, N1, and M6).
A pulse on the S_LOAD pin after the shift register is fully loaded
will transfer the divide values into the counters. The HIGH to
LOW transition on the S_LOAD input will latch the new divide
values into the counters. Figure 4 illustrates the timing diagram
for both a parallel and a serial load of the MPC9239 synthesizer.
M[6:0] and N[1:0] are normally specified once at power-up
through the parallel interface, and then possibly again through
the serial interface. This approach allows the application to
come up at one frequency and then change or fine-tune the
clock as the ability to control the serial interface becomes
available.
Using the Test and Diagnosis Output TEST
The TEST output provides visibility for one of the several
internal nodes as determined by the T[2:0] bits in the serial
configuration stream. It is not configurable through the parallel
interface. Although it is possible to select the node that
represents f
OUT
, the LVCMOS output is not able to toggle fast
enough for higher output frequencies and should only be used
for test and diagnosis.
The T2, T1, and T0 control bits are preset to ‘000' when
P_LOAD
is LOW so that the PECL f
OUT
outputs are as jitter-free
as possible. Any active signal on the TEST output pin will have
detrimental affects on the jitter of the PECL output pair. In
normal operations, jitter specifications are only guaranteed if
the TEST output is static. The serial configuration port can be
used to select one of the alternate functions for this pin.
Most of the signals available on the TEST output pin are
useful only for performance verification of the MPC9239 itself.
However, the PLL bypass mode may be of interest at the board
level for functional debug. When T[2:0] is set to 110 the
MPC9239 is placed in PLL bypass mode. In this mode the
S_CLOCK input is fed directly into the M and N dividers. The N
divider drives the f
OUT
differential pair and the M counter drives
the TEST output pin. In this mode the S_CLOCK input could be
used for low speed board level functional test or debug.
Bypassing the PLL and driving f
OUT
directly gives the user more
control on the test clocks sent through the clock tree shows the
functional setup of the PLL bypass mode. Because the
S_CLOCK is a CMOS level the input frequency is limited to 200
MHz. This means the fastest the f
OUT
pin can be toggled via the
S_CLOCK is 100 MHz as the divide ratio of the Post-PLL
divider is 2 (if N = 1). Note that the M counter output on the
TEST output will not be a 50% duty cycle.
Table 9. Output Frequency Range for f
XTAL
= 10 MHz
N
f
OUT
f
OUT
Range f
OUT
Step
1 0 Value
0 0 2 8M 200–450 MHz 8 MHz
0 1 4 4M 100–225 MHz 4 MHz
1 0 8 2M 50–112.5 MHz 2 MHz
1 1 1 16M 400–900 MHz 16 MHz
MPC9239 REVISION 2 DECEMBER 18, 2012 8 ©2012 Integrated Device Technology, Inc.
MPC9239 Data Sheet 900 MHz Low Voltage LVPECL Clock Synthesizer
Figure 4. Serial Interface Timing Diagram
Power Supply Filtering
The MPC9239 is a mixed analog/digital product. Its analog
circuitry is naturally susceptible to random noise, especially if
this noise is seen on the power supply pins. Random noise on
the V
CC_PLL
pin impacts the device characteristics. The
MPC9239 provides separate power supplies for the digital
circuitry (V
CC
) and the internal PLL (V
CC_PLL
) of the device. The
purpose of this design technique is to try and isolate the high
switching noise digital outputs from the relatively sensitive
internal analog phase-locked loop. In a controlled environment
such as an evaluation board, this level of isolation is sufficient.
However, in a digital system environment where it is more
difficult to minimize noise on the power supplies a second level
of isolation may be required. The simplest form of isolation is a
power supply filter on the V
CC_PLL
pin for the MPC9239.
Figure 5 illustrates a typical power supply filter scheme. The
MPC9239 is most susceptible to noise with spectral content in
the 1 kHz to 1 MHz range. Therefore, the filter should be
designed to target this range. The key parameter that needs to
be met in the final filter design is the DC voltage drop that will
be seen between the V
CC
supply and the MPC9239 pin of the
MPC9239. From the data sheet, the V
CC_PLL
current (the
current sourced through the V
CC_PLL
pin) is maximum 20 mA,
assuming that a minimum of 2.835 V must be maintained on the
V
CC_PLL
pin. The resistor shown in Figure 5 must have a
resistance of 10-15 to meet the voltage drop criteria. The RC
filter pictured will provide a broadband filter with approximately
100:1 attenuation for noise whose spectral content is above
20 kHz. As the noise frequency crosses the series resonant
point of an individual capacitor its overall impedance begins to
look inductive and thus increases with increasing frequency.
The parallel capacitor combination shown ensures that a low
impedance path to ground exists for frequencies well above the
bandwidth of the PLL. Generally, the resistor/capacitor filter will
be cheaper, easier to implement and provide an adequate level
of supply filtering. A higher level of attenuation can be achieved
by replacing the resistor with an appropriate valued inductor. A
1000 H choke will show a significant impedance at 10 kHz
frequencies and above. Because of the current draw and the
voltage that must be maintained on the V
CC_PLL
pin, a low DC
resistance inductor is required (less than 15 ).
Figure 5. V
CC_PLL
Power Supply Filter
Table 10. Test and Debug Configuration for TEST
T[2:0]
TEST Output
T2 T1 T0
0 0 0
12-bit shift register out
1
1. Clocked out at the rate of S_CLOCK.
0 0 1 Logic 1
0 1 0 f
XTAL
2
0 1 1 M-Counter out
1 0 0 f
OUT
1 0 1 Logic 0
1 1 0 M-Counter out in PLL-bypass mode
1 1 1 f
OUT
4
Table 11. Debug Configuration for PLL Bypass
1
1. T[2:0] = 110. AC specifications do not apply in PLL bypass mode.
Output Configuration
f
OUT
S_CLOCK N
TEST
M-Counter out
2
2. Clocked out at the rate of S_CLOCK (2 N)
S_CLOCK
S_DATA
S_LOAD
M[6:0]
N[1:0]
P_LOAD
T2 T1 T0 N1 N0 M6 M5 M4 M3 M2 M1
M0
M, N
First
Bit
Last
Bit
V
CC_PLL
V
CC
MPC9239
C
1
, C
2
= 0.01...0.1 F
V
CC
C
F
= 22 F
R
F
= 10-15
C
2
C
1
MPC9239 REVISION 2 DECEMBER 18, 2012 9 ©2012 Integrated Device Technology, Inc.
MPC9239 Data Sheet 900 MHz Low Voltage LVPECL Clock Synthesizer
Layout Recommendations
The MPC9239 provides sub-nanosecond output edge rates
and thus a good power supply bypassing scheme is a must.
Figure 6 shows a representative board layout for the MPC9239.
There exists many different potential board layouts and the one
pictured is but one. The important aspect of the layout in
Figure 6 is the low impedance connections between V
CC
and
GND for the bypass capacitors. Combining good quality general
purpose chip capacitors with good PCB layout techniques will
produce effective capacitor resonances at frequencies
adequate to supply the instantaneous switching current for the
MPC9239 outputs. It is imperative that low inductance chip
capacitors are used; it is equally important that the board layout
does not introduce back all of the inductance saved by using the
leadless capacitors. Thin interconnect traces between the
capacitor and the power plane should be avoided and multiple
large vias should be used to tie the capacitors to the buried
power planes. Fat interconnect and large vias will help to
minimize layout induced inductance and thus maximize the
series resonant point of the bypass capacitors. Note the dotted
lines circling the crystal oscillator connection to the device. The
oscillator is a series resonant circuit and the voltage amplitude
across the crystal is relatively small. It is imperative that no
actively switching signals cross under the crystal as crosstalk
energy coupled to these lines could significantly impact the jitter
of the device. Special attention should be paid to the layout of
the crystal to ensure a stable, jitter free interface between the
crystal and the on—board oscillator. Although the MPC9239
has several design features to minimize the susceptibility to
power supply noise (isolated power and grounds and fully
differential PLL), there still may be applications in which overall
performance is being degraded due to system power supply
noise. The power supply filter and bypass schemes discussed
in this section should be adequate to eliminate power supply
noise related problems in most designs.
Figure 6. PCB Board Layout Recommendation
for the PLCC28 Package
Using the On-Board Crystal Oscillator
The MPC9239 features a fully integrated on-board crystal
oscillator to minimize system implementation costs. The
oscillator is a series resonant, multivibrator type design as
opposed to the more common parallel resonant oscillator
design. The series resonant design provides better stability and
eliminates the need for large on chip capacitors. The oscillator
is totally self contained so that the only external component
required is the crystal. As the oscillator is somewhat sensitive to
loading on its inputs the user is advised to mount the crystal as
close to the MPC9239 as possible to avoid any board level
parasitics. To facilitate co-location surface mount crystals are
recommended, but not required. Because the series resonant
design is affected by capacitive loading on the XTAL terminals
loading variation introduced by crystals from different vendors
could be a potential issue. For crystals with a higher shunt
capacitance it may be required to place a resistance across the
terminals to suppress the third harmonic. Although typically not
required it is a good idea to layout the PCB with the provision of
adding this external resistor. The resistor value will typically be
between 500 and 1K.
The oscillator circuit is a series resonant circuit and thus for
optimum performance a series resonant crystal should be used.
Unfortunately most crystals are characterized in a parallel
resonant mode. Fortunately there is no physical difference
between a series resonant and a parallel resonant crystal. The
difference is purely in the way the devices are characterized. As
a result a parallel resonant crystal can be used with the
MPC9239 with only a minor error in the desired frequency. A
parallel resonant mode crystal used in a series resonant circuit
will exhibit a frequency of oscillation a few hundred ppm lower
than specified, a few hundred ppm translates to kHz
inaccuracies. In a general computer application this level of
inaccuracy is immaterial. Tabl e 12 below specifies the
performance requirements of the crystals to be used with the
MPC9239.
1
C2CF
XTAL
C1 C1
= V
CC
= GND
= Via
Table 12. Recommended Crystal Specifications
Parameter Value
Crystal Cut Fundamental AT Cut
Resonance
Series Resonance
1
1. See accompanying text for series versus parallel resonant
discussion.
Frequency Tolerance 75ppm at 25C
Frequency/Temperature Stability 150pm 0 to 70C
Operating Range 0 to 70C
Shunt Capacitance 5-7pF
Equivalent Series Resistance (ESR) 50 to 80
Correlation Drive Level 100 W
Aging 5ppm/Yr (First 3 Years)

MPC9239FNR2

Mfr. #:
Manufacturer:
IDT
Description:
Clock Synthesizer / Jitter Cleaner FSL 900MHz LVPECL Freq. Synthesizer
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New from this manufacturer.
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