The MAX2101 6-bit quadrature digitizer combines quadrature demodulation with analog-to-digital conversion on
a single bipolar silicon die. This unique RF-to-Bits
TM
function bridges the gap between existing RF downconverters and CMOS digital signal processors (DSPs).
The MAX2101’s simple receiver subsystem is designed
for digital communications systems such as those used
in DBS, TVRO, WLAN, and other applications.
The MAX2101 accepts input signals from 400MHz to
700MHz and applies adjustable gain, providing at least
40dB of dynamic range.
Each baseband is filtered by an on-chip, 5th-order
Butterworth lowpass filter, or the user can select an
external filter path. Baseband sample rate is 60Msps.
The MAX2101 is available in a commercial temperature
range, 100-pin MQFP package.
________________________Applications
Recovery of PSK and QAM Modulated RF Carriers
Direct-Broadcast Satellite (DBS) Systems
Television Receive-Only (TVRO) Systems
Cable Television (CATV) Systems
Wireless Local Area Networks (WLANs)
____________________________Features
♦ ADCs Provide Greater than 5.5 Effective Bits at
fS= 60Msps, fIN= 15MHz
♦ Fully Integrated Lowpass Filters with
Externally Variable Bandwidth (10MHz to 30MHz)
♦ 40dB Dynamic Range
♦ Integrated VCO and Quadrature Generation
Network for I/Q Demodulation
♦ Divide-by-16 Prescaler for Oscillator PLL
♦ Programmable Counter for Variable Sample Rates
♦ Signal-Detection Function
Operating Temperature Range...............................0°C to +70°C
Storage Temperature Range.............................-65°C to +150°C
Lead Temperature (soldering, <10sec)...........................+300°C
Note 1: The digital control inputs are diode protected; however, permanent damage may occur on unconnected units under high-
energy electrostatic fields. Keep unused units in conductive foam or shunt the terminals together. Discharge the conductive
foam to the destination socket before insertion.
Stresses beyond those listed under “Absolute Maximum Ratings” may cause permanent damage to the device. These are stress ratings only, and functional
MAX2101
operation of the device at these or any other conditions beyond those indicated in the operational sections of the specifications is not implied. Exposure to
absolute maximum rating conditions for extended periods may affect device reliability.
ELECTRICAL CHARACTERISTICS
(VCC= 4.75V to 5.25V, TA= +25°C, unless otherwise noted.)
CONDITIONS
DC SPECIFICATIONS (V
Digital Supply Current
ADC Supply Current
RF Blocks Supply Current
IF Port DC Dynamic Range
IF Port Input Resistance
AGC Input Voltage
AGC Input Resistance
AGC Input Capacitance
AGC Control Slope Variation
AGC Control Input Bias Current
Lowpass Filter Tune Input Resistance
Lowpass Filter Tune Input Capacitance
TNKA, TNKB Resonant Port Bias Voltage
LO Resonant Port Input Resistance
LO Resonant Port Input Capacitance
LO Prescaler Output High (Note 3)
LO Prescaler Output Low
LO Prescaler Output Source Current
LO Prescaler Output Sink Current
Baseband Amplifier DC GainA
Baseband Input—Input CapacitanceC
Baseband Amplifier I/Q Offset Match
(VCC= 4.75V to 5.25V, TA= +25°C, unless otherwise noted.)
V
Power Detect Output Minimum
Power Detect Output Maximum
ADC Amplitude Response Match
ADC Input Offset
OFFAD
RF Signal Path DC Gain
Composite I/Q Gain Mismatch
Buffered Reference Voltage
(Zero Temperature Coefficient)
Buffered Reference Voltage
(Proportional to Absolute Temperature)
V
Temperature Coefficient
PTAT
Buffered Reference Voltage
(2 x VREF)
Data Output High (Note 3)
Data Output Low
Data Output Source Current (Note 3)
Data Output Sink Current
Data Clock Output High (Note 3)
Data Clock Output Low
Data Clock Output Source Current (Note 3)
Data Clock Output Sink Current
Master Clock Input Dynamic Range
Master Clock Input Resistance
Master Clock Input Capacitance
Reference Clock Output High (Note 3)
Reference Clock Output Low
Reference Clock Output Source Current
(Note 3)
Reference Clock Output Sink Current
Digital Input High Threshold (Note 5)V
Digital Input Low Threshold (Note 5)V
Digital Input Current High (Note 5)I
Digital Input Current Low (Note 5)I
FLTRSEL Input Current HighI
FLTRSEL Input Current LowI
PWR
PWR
VM
VRF
(IQ)
REF
PTAT
2R5
OH
OL
OH
OL
OH
OL
OH
OL
MCLK
IMCLK
IMCLK
OH
OL
OH
OL
IH
IL
IH
IL
IH
IL
= 0V
p-p
> 2V DC
V
OBB
OBB
Channel to channeldB0.4A
LSB = 24mV, either channel
AGC set to maximum gaindB63A
Entire signal path, DC,
Data Clock Period (Figure 2)
Propagation Delay, Clock to Data (Figure 2)
Data Output Skew (all 12 outputs) Settled within 20% (Figure 2)
Aperture Delay Relative to Data Clock (Figure 2)
Aperture Delay Match, Channel to Channel
Data Output Rise, Fall Time (20% to 80%) (Note 7)
Data Clock Output Rise, Fall Time (20% to 80%) (Note 7)
Reference (Div 6) Clock Output Rise, Fall Time (20% to 80%) (Note 7)
Reference Clock Output Jitter, RMS
VCO Prescaler Output Rise, Fall Time (20% to 80%) (Note 7)
35D1QQ Channel Data Output, bit 1
36D0QQ Channel Data Output, bit 0 (LSB)
39RCLK
41DCLKBData Clock Complementary Output
42DCLKData Clock Output
45D0II Channel Data Output, bit 0 (LSB)
46D1II Channel Data Output, bit 1
49D2II Channel Data Output, bit 2
50D3II Channel Data Output, bit 3
53D4II Channel Data Output, bit 4
54D5II Channel Data Output, bit 5 (MSB)
56BINENBinary Enable
84VSUBRFRF Demodulator Substrate
85PWRII Channel Power Indicator
862R52x VREF Output
87VCCIFIF Signal Processing +5V Supply
88VREF
90IFINIF Amplifier Noninverting Input
91IFINBIF Amplifier Inverting Input
93AGCAutomatic Gain Control Input
94VGNDIFIF Signal-Processing Ground
95FLTRSELBaseband Signal Path Select
96PWRQQ Channel Power Indicator
97VPTATPTAT Reference Voltage Output
100MIXOUTQQ Channel Mixer Output
I Channel Baseband Amplifier,
External Input
High Impedance, connect to VREF
(pin 88)
Bandgap Reference Voltage
Output
______________Detailed Description
The MAX2101 6-bit quadrature digitizer solves one of
the most challenging problems of high dynamic range
digital-receiver design by combining quadrature
demodulation and analog-to-digital (A/D) conversion in
a single device. The MAX2101’s unique RF-to-Bits
function bridges the gap between RF downconverters
and CMOS digital signal processors (DSPs). Figure 1
is a simplified connection diagram.
The MAX2101 accepts input signals from 400MHz to
700MHz and applies gain depending on the input
amplitude. The signal is then split and downconverted
to baseband by two mixers, which are driven by two
local oscillator (LO) signals in quadrature. An internal
voltage-controlled oscillator (VCO) feeds the two LOs.
Each baseband is filtered by an internal 5th-order
Butterworth lowpass filter. The on-board lowpass filters
have an externally variable bandwidth of 10MHz to
30MHz. Each baseband is then converted by a 6-bit
analog-to-digital converter (ADC). The conversion result
is stored in a register and is output using the data
clock. See Figure 2 for the relation between baseband
signal, sample and data clock, and digitized data. The
external master clock is internally divided by six and is
available at RCLK for external system functions, frequency synthesizers, etc. See Figures 3 and 4 for functional diagrams.
IF Input Port (IFIN,
The MAX2101 provides a balanced IF input. The inputs
are self-biasing, so the input signals should be AC terminated, depending on system requirements. To minimize
noise, the unused input should be AC terminated with
25Ω. To minimize distortion, AC terminate the unused
input with a 50Ω resistor.
IFINB
VCO Resonator Tank Ports
(TNKA, TNKB) and Prescaler
The MAX2101 integrates a negative impedance oscillator with balanced inputs. Use a parallel tank network,
as shown in Figure 5. The phase-noise performance of
the oscillator near the carrier is dominated by the resonant network. The resonant inductor must have a sufficiently high Q and a self-resonant frequency (SRF) that
is more than twice the intended LO frequency. Be sure
to minimize parasitic elements surrounding the tank
network by using proper layout techniques. See the
Applications Information
The VCO prescaler output provides phase-lock loop
capability for controlling the VCO frequency. The
prescaler generates the VCO frequency divided by 16.
As a result, the prescaler delivers a 25MHz to
43.75MHz signal over the VCO operating frequency
range of 400MHz to 700MHz. The differential outputs
should have equivalent termination.
Figure 4. Functional Diagram—MAX2101 ADCs and Supporting Sections
Filter Tuning
The MAX2101 integrates two 5th-order Butterworth lowpass filters for anti-alias filtering of the baseband signal. One filter exists for each of the I and Q channels.
The filters’ cutoff frequency is set by driving the FTUNE
pins, pin 77 (I channel) and pin 4 (Q channel). The user
sets the I/Q channel filters independently. Figure 6
shows a typical transfer curve of a filter’s cutoff frequency versus FTUNE voltage.
The MAX2101’s anti-aliasing filtering function provides
superior channel-to-channel matching compared to a
discrete implementation. The filters are realized using a
gyrator topology, which inherently has a strong temperature dependency. The temperature dependency of the
filters must be compensated to achieve a consistent filter response over ambient temperature. This compensation is easily summed with the user-supplied filter
tune signal, with the techniques discussed for both current-drive and voltage-drive implementations later in
this section. Figure 7 shows a typical characteristic of
the FTUNE signal required to provide a constant filter
cutoff frequency over temperature.
Figure 6. Typical Filter Cutoff Frequency vs. FTUNE Input
Voltage
The MAX2101 provides temperature-compensated bias
voltages that, when scaled and summed with the usersupplied filter-control signal, provide the necessary
compensation for the filters. The filter-control signal can
originate in one of two forms: an analog current, or an
analog voltage. The temperature compensation signal
will be added to the control signal as discussed below.
Voltage Drive
A suggested technique of filter drive uses a voltage
source, such as a voltage output DAC. The temperature compensation signals, VPTAT and VREF, are shifted and scaled, then summed with the control voltage,
and the sum is applied to the FTUNE inputs. See Figure
8 for a possible implementation.
The transfer function for Figure 8’s voltage drive configuration can be evaluated as follows:
R
VV
=+−
TCREF
VV
FTUNESET
=+−
F
(VV)
REFPTAT
R
TC
R
F
R
TC
(VV)
REFPTAT
1.90
1.85
FTUNE (V)
1.80
1.75
1.70
Figure 7. Typical Filter Cutoff Frequency Temperature
Dependence
2040100
0140
TEMPERATURE (°C)
80
60
120
Current Drive
An alternate form of filter drive uses a current source,
such as a current-output DAC. The current is transformed to the appropriate voltage via a transresistance
network, which will drive the FTUNE input(s). The temperature compensation signals, VPTAT and VREF, are
shifted and scaled, transformed to current, added to
the user-supplied current, and the sum is transformed
back into the temperature compensated control voltage
(Figure 9).
Amplifier U1A generates a shifted reference signal,
VTC. VTCis transformed into a current through the
resistor RTC. RTCalso scales this signal such that,
when compared to the feedback resistor RF, the proper
temperature dependence is added to the user-supplied
filter control current I
to compensate for the TC of
SET
the filter.
The expression for the final filter tune signal is
expressed as:
R
VI(R )
FTUNESETF
=+−
F
(VV)
REFPTAT
R
TC
Thus, the user-supplied signal V
, which is character-
SET
ized by a very small (ideally 0) temperature coefficient,
will be summed with a small signal (|V
200mV) whose temperature dependence compensates
In both techniques discussed above, the ratio RF/RTCdetermines the compensation required to produce a
filter response with 0TC. As noted in the VPTAT vs.
Temperature graph in the
this ratio should be set at 0.8.
Typical Operating Characteristics
,
Baseband Offset Correction
The MAX2101 integrates a high level of RF signal processing, and applies substantial gain from the IF inputs
to the baseband signals applied to the ADC. Offset in
the signal path can seriously decrease the component’s dynamic range, and variation in offset between I
and Q channels can seriously degrade overall receiver
performance. Several circuit design techniques are
used to minimize offset within the chip. However, two
characteristics of the component contribute to offset in
the signal path.
The off-chip tank network for the VCO resonates the LO
frequency with a relatively large amplitude. If the LO
couples into the IF input, the coupled LO will mix down
to a DC value, which depends on the AGC setting. This
DC signal manifests itself as an offset in the baseband
signal. The second source of offset is the active lowpass anti-aliasing filters. This offset depends on the
cutoff frequency. These two elements represent the
major contributors to DC offset in the signal path.
Offset Adjust Pins OFFI, OFFQ
The MAX2101 offers an offset adjust pin for each of the
I and Q channels, labeled OFFI and OFFQ, respectively. The offset adjust input exhibits an adjustment range
that is sufficient to correct for the errors mentioned
above. The polarity of the OFF_ input is such that a
positive change of the OFF_ voltage results in a negative transition in the baseband signal, BBOUT_. The offset adjust range compensates for up to 5LSBs of offset.
A feedback-controlled, offset-correction network can
be realized that will null any offset detected in the baseband signal applied to the ADCs. The differential baseband signal is sampled at the input to the ADC and
integrated over a sufficiently large period of time (determined by the minimum frequency of the baseband signal), extracting the offset signal. This error signal is
internally applied to the OFF_ input, completing the
feedback loop. The MAX2101 integrates the op amps
and 150kΩ pickoff resistors of the offset correction network. Figure 10 shows a simplified schematic diagram
of the network. Simply connect the appropriate capacitors as shown in Figure 11.
The network in Figure 11 is a lowpass filter with a 5Hz
cutoff frequency. The user can tailor the cutoff frequency
by choosing the appropriate value of capacitance,
according to the following relation:
C
=
where:
C = integrator capacitance
for cutoff frequency
Frequency components of the baseband signal near or
below the cutoff frequency will interfere with the operation of this network. Fortunately, the compressed and
encoded nature of baseband signals at this stage of
the signal chain in typical applications will insure minimal low-frequency components. Hence, this technique
will eliminate all offsets, independent of AGC setting, filter cutoff frequency, or changes in ambient temperature.
Pin 68, ENOPB, is normally connected to ground.
Pulling ENOPB to V
opening the servo loop, and disabling offset correction.
The baseband pins (6, 7, 74, 75) should be left unconnected, or buffered with a high-impedance load (resistive load greater than 10kΩ and capacitive load less
than 3pF).
1
2 f (150k )
π
O
Ω
CC
disables the op amps, thus
Sample Clock Generation
The master sample clock (MCLK) input for the
MAX2101 is typically driven by a low-noise, low-drift
crystal oscillator. The signal should be between 0dBm
and +10dBm, and must be AC coupled to the MCLK
input. This signal is buffered and divided according to
the programmable sample-rate prescaler (PSRP). The
actual sample rates are binary weighted divisors of the
MCLK frequency. Program the sample rates with pins
S0, S1, and S2, as shown in Table 1.
The single-ended, LS-TTL compatible data outputs
from the ADCs are clocked out with respect to the rising edge of the data clock (DCLK). The output drivers
provide sufficient logic levels at speeds up to 60Mbps
into a fanout of 1 with a total load capacitance of 15pF.
All data outputs should have approximately equivalent
loading to ensure proper setup and hold timing.
The data clock outputs are also LS-TTL compatible and
provide a signal to latch the data at rates up to
60Mbps. The outputs are differential to minimize the
harmonic energy that might feed back into the LO or IF
inputs. The balanced outputs should have equivalent
termination to minimize unwanted EMI.
Select either binary or twos-complement output with the
binary enable (BINEN) pin. A logic high will select offset
binary, and a logic low will select a twos-complement
format.
Input Termination Network
The MAX2101 accepts as an input a narrow band IF
whose center frequency is located somewhere in the UHF
range, between 400MHz and 700MHz. The MAX2101
comprises a significant part of a receiver chain characterized by extremely high dynamic range coupled with
demanding intermodulation requirements. As such, it is
imperative to provide proper input termination to the
MAX2101, to minimize effective VSWR and noise figure at
this stage of the system RF signal processing chain.
The input of the MAX2101 is designed to deliver a
VSWR less than 2:1 over the 400MHz to 700MHz range.
The equivalent input network of the input pins IFIN and
IFINB is discussed and illustrated below. However,
standard narrow-band impedance matching techniques can be used to improve on this VSWR for the
intended IF of the system.
Equivalent Input Circuitry
The MAX2101’s input amplifier is designed to provide a
controlled input impedance, provide gain for the signal
path, and provide for the component’s minimum noise
figure. The amplifier uses a feedback topology to provide gain that is insensitive to input frequency, in addition to delivering constant input impedance. Figure 12
illustrates the amplifier’s input portion.
Ideally, the input amplifier will be designed to match to
an anticipated source impedance of 50Ω. The resistive
portion of the input impedance at pin IFIN can be
approximated as follows:
Rr
+
IN
FE
=
(1 A )
+
V
R
where rEis the dynamic resistance at Q3’s emitter, and
AVis the open-loop gain of the differential-pair amplifier
stage.
The amplifier can be designed so the frequency
response does not appreciably affect the input impedance. Details of the amplifier are left out for simplicity.
Figure 12 shows how several parasitic elements contribute to the input impedance over the frequencies of
interest. C
represents the parasitic capacitance
PAD
associated with the bond pad and input metallization.
error to the impedance term. The inductance LBWmodels the bond wire and lead frame in series with the
input amplifier. This inductor represents a significant
portion of the input impedance, and will contribute the
majority of the variation in input impedance as the input
frequency is swept from 400MHz to 700MHz. These
variables combine to produce an actual input impedance versus frequency (Figure 13).
As a result, it is challenging to achieve an extremely low
VSWR for the input of a monolithic amplifier, especially
over a wide range of frequencies. The MAX2101 provides
a VSWR less than 2:1, and delivers this performance over
the wide range of anticipated IFs currently considered.
Fortunately, for DBS, TVRO, and related applications, the
UHF IF is relatively narrow band, allowing the use of standard techniques for narrow-band impedance matching.
Narrow-Band Match
Many references cover narrow-band matching techniques. The match network synthesis is simplified by
assuming the impedance of the source driving the
MAX2101’s IFIN port is positive, real, and equal to 50Ω.
For a given IF, you can simply use a Smith chart to
“map” an impedance to the intended source resistance. Using a two-element matching network, you can
choose the element next to the input (CSHin Figure 14)
to translate the real portion of the impedance to match
the source resistance. The second element (L
SER
in
Figure 14) cancels the reactive component of the network (including the effect of CSH), resulting in a real,
matched input impedance that provides maximum
R
I
Q4Q3
R
F
R
E
E
L
BW
C
PAD
IFINB
(PIN 91)
IFIN (PIN 90) INPUT IMPEDENCE vs.
FREQUENCY
80
60
40
(Ω)
20
IN
Z
0
-20
-40
300 400700
200900
TA = +25°C
= 5V
V
CC
= 50Ω
R
S
IFINB (PIN 91) AC TERMINATED IN 25Ω
500
FREQUENCY (MHz)
600
RE (ZIN)
IM (ZIN)
800
Figure 13. Typical MAX2101 IFIN ZINvs. Frequency (Zs = 50)
power transfer. The transformation uses only reactive
elements so that no additional resistive thermal noise is
added, which would degrade the noise figure.
Figure 14 shows the resulting impedance matching network. The incident signal is AC coupled by C
and CSHare the matching elements. CSHincludes
board layout capacitance. The values of these ele-
Figure 14. Example of Input Network to Minimize VSWR and Noise Figure
ments were calculated assuming a 600MHz source frequency. Capacitor C
for the complementary input IFINB. Resistor R
vides superior noise figure performance by optimizing
the tradeoff between thermal induced noise and the
gain of the input amplifier. This network also provides
ancillary rejection of out-of-band energy, improving the
receiver noise figure and resulting SNR. The topology
shown above produces a VSWR less than 1.7:1 over
the intended UHF band. Do not DC couple the inputs to
ground, as this would result in saturation of the input
stage.
More elaborate matching networks can be designed
depending on the need of the receiver system.
__________Applications Information
Voltage-Controlled Oscillator Equivalent
Input Network and Resonator Issues
The MAX2101 performs the quadrature demodulation
and digitizing functions within a digital receiver system.
A vital component of the quadrature detection function
is the generation of a local oscillator (LO) frequency.
This signal is typically generated by a VCO controlled
by a phase-locked loop. The VCO topology normally
used for high dynamic range receivers is the negative
resistance amplifier and resonator, due to superior
phase-noise performance. The MAX2101 provides the
negative resistance amplifier on-chip, and can be easily interfaced with an off-chip resonant network.
The MAX2101’s VCO amplifier uses a differential topology for several reasons. The differential interface with
provides an AC termination
TERM
TERM
pro-
L
8nH
SER
C
R
TERM
25Ω
TERM
10nF
C
1pF
SH
90
IFIN
MAX2101
91
IFINB
the resonator network provides superior rejection of
spurious signals that might otherwise add to or distort
the resulting LO. The differential interface minimizes the
effect of parasitic package-related elements that affect
the resonant frequency and the loaded Q of the network. The differential-drive network minimizes secondharmonic distortion that might create undesirable
mixing products within the signal chain.
Figure 15 shows the simplified input network of the
negative impedance amplifier, configured as a Wilson
oscillator. The amplifier is a simple differential emitter
coupled pair with emitter degeneration for controlled
open-loop gain. The positive feedback necessary to
create the negative input impedance is performed with
the feedback capacitors, C
, and the coupling capaci-
F
tors, CC. The capacitors ensure operation over the
intended 400MHz to 700MHz spectrum, and add minimal noise to the system. RB1provides a proper bias
voltage for the capacitors (partially constructed with
voltage-dependent pn junctions) and provides for DC
interface with a shunting resonant inductor. Note that
biasing networks are simplified for brevity.
The MAX2101’s negative impedance amplifier expects
a parallel resonant network. Figure 5 shows an example
of a tunable resonant network. The resonator is driven
from the phase-locked loop filter output, as noted. The
loaded Q of the resonant network, and to a lesser
extent the absolute values of the resonant elements,
determine the VCO’s phase-noise performance. As a
result, take care during the design of the resonator to
maximize the loaded Q. To achieve the phase-noise
Figure 15. Simplified Input Network for VCO Resonator Ports
R
B2
R
E
performance in the specification, the resonant network
should exhibit a loaded Q greater than 20.
The resonating inductor L
should exhibit as high a
RES
Q factor as is reasonably possible. The inductor’s selfresonant frequency (SRF) should be well in excess of
the intended frequencies of operation. An air-wound
design is a simple example of an inductor that would fit
these criteria.
A dual varactor topology is recommended for C
VAR
to
compensate for the large-signal amplitude incident
across the resonator ports. The dual varactor in the
arrangement shown in Figure 5 (to first order) allows
cancellation of capacitance modulation due to the large
signals, as the two diodes are driven in a complementary fashion by the LO signal. The dual varactor design
also allows use of devices with larger COvalues, simplifying device selection. The varactor should be driven
with a large reverse bias to increase the MAX2101’s
effective Q.
The resonant frequency is primarily determined by
CSH, which shunts the varactor diodes. CSHis trimmed
(selected) to determine the approximate tuning range
of the phase-locked loop. For applications relevant to
the MAX2101, this frequency range can cover the UHF
R
I
C
F
R
E
I
EE
C
C
TNKB
(PIN 14)
R
B2
R
B1
V
B2
spectrum from 400MHz to 700MHz. The varactor within
the loop will then determine the actual LO frequency
within a much narrower tuning range. Depending on
the expected tuning range variation, CSHcould be
made of a combination of fixed capacitance and
trimmed capacitance. This shunt capacitance will
increase the loaded Q of the resonator and lower the V
to F gain constant, improving the oscillator’s phasenoise performance.
The coupling capacitors CCcouple the variable capacitor network to the tank ports and resonating inductor.
These elements should be selected to present low
impedance (less than 1Ω) at the lowest expected operating frequency. These capacitors should also exhibit
low effective series resistance (ESR) to maintain a high
resonator-loaded Q. R
CHOKE
provides a DC bias for
the varactors, while ensuring a high impedance at the
intended operating frequency. The magnitude of the
choke network’s series impedance should be approximately 10 times the resonant inductor’s impedance at
the operating frequency. Resistors R
provide drive
BUF
for the varactor while ensuring adequate isolation
between the two differential resonator ports. C
combination with R
A direct-broadcast satellite (DBS) receiver consists of
an antenna to receive the X/Ku band carrier from the
satellite, a low-noise block (LNB), an L-band downconverter, and a quadrature demodulator. The system
stages include a dual ADC, a matched filter, clock and
carrier recovery, error detection and correction, and
additional system-dependent DSP. See the
Application Circuit
MAX2101
The LNB provides polar demodulation (vertical and horizontal) and downconversion of the X/Ku band signals
to a first intermediate frequency (IF1) in the 950MHz to
2000MHz range. The L-band downconverter converts
IF1to a second IF (IF2) in the 400MHz to 700MHz
range. The MAX2101 performs the next stages as follows: 1) the quadrature demodulator converts IF2to
two baseband signals, I and Q; and 2) the dual ADCs
digitize the baseband signals, which are then
processed by the various digital blocks to compensate
for transmission distortion and to extract the digital
baseband data.
One interface that causes system designers trouble is
the quadrature demodulator to ADC interface. Power is
needed to drive the low-impedance interconnect
between these two functions. Additionally, this portion
of the signal path can introduce phase and amplitude
errors that complicate back-end error correction. The
integrated MAX2101 solves all of these design problems associated with DBS systems.
The MAX2101 combines bipolar technology with excellent RF and data-converter design to integrate the
quadrature demodulation and ADC functions. The
MAX2101 also includes an IF gain block, a VCO and
prescaler necessary to generate an accurate LO frequency, and fully integrated baseband anti-aliasing filters for both I and Q channels. By integrating several
functions supporting the quadrature demodulation and
A/D block, the MAX2101 replaces several components
and eliminates many board-level design and manufacturing problems.
on the first page of the data sheet.
Layout, Grounding, Bypassing
The MAX2101’s supply pins are separated to isolate
high-current digital noise spikes from sensitive RF and
analog sections. All ground potentials must be DC coupled, and resistive drops should contribute no more
than 50mV difference between the ground pins. A single-point analog ground (“star” ground point) should be
established at the ground supply connection to the PC
Typical
board, separate from the active circuitry. Three ground
planes should be established, connected at the star
ground point. The three ground planes should be dedicated as follows: analog and RF ground plane, digital
ground plane, and output ground plane. The various
ground pins should be connected to this star ground
network according to Table 2. The ground current
return path for all supplies should be low impedance at
frequencies of interest for each supply.
For best performance, use printed circuit boards. Wirewrap boards are not recommended. Board layout
should ensure that digital and analog signal lines are
separated from each other. Do not run analog and digital (especially clock) lines parallel to one another, or
digital lines underneath the MAX2101 package.
The MAX2101 requires +5V ±5% for all supply pins.
Bypass the supply pins with high-quality 0.1µF and
0.001µF ceramic capacitors located as close to the
package as possible. The high-frequency supplies,
VCCIF and VCC2, both require an additional ceramic
surface-mount bypass capacitor nominally valued at
47pF. The baseband supplies (VCCI and VCCQ) need
additional filtering to ensure sufficient channel-to-channel isolation. Place a small-value resistor, such as 5Ω,
between the supply and the pins to create a single-pole
filter with the bypass capacitor. The DC IR drop across
the resistor should not exceed 150mV. Alternatively,
place an RF choke between the supply and the pins.
The SRF of the selected choke must be high enough to
block energy from the other baseband channel.
Maxim cannot assume responsibility for use of any circuitry other than circuitry entirely embodied in a Maxim product. No circuit patent licenses are
implied. Maxim reserves the right to change the circuitry and specifications without notice at any time.
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