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 WIRELESS COMMUNICATIONS DIVISION
GND
RF IN
TQ5631
DATA SHEET
GND
VDD
3V PCS Band CDMA RFA/Mixer IC
IF out
VDD
GIC
LO IN
Features
Small size: SOT23-8 Single 3V operation Low-current operation
Product Description
The TQ5631 is a 3V, RFAmplifier/Mixer IC designed specifically for PCS band CDMA applications. It's RF performance meets the requirements of products designed to the IS-95 standards. The TQ5631 is designed to be used with the TQ3631 (CDMA LNA) which provides a complete CDMA receiver for 1900MHz phones. The RFA/Mixer incorporates on-chip switches which determine gain select states. When used with the TQ3631 (CDMA LNA), four gain steps are available. The RF input port is internally matched to 50 , greatly simplifying the design and keeping the number of external components to a minimum. The TQ5631 achieves good RF performance with low current consumption, supporting long standby times in portable applications. Coupled with the very small SOT23-8 package, the part is ideally suited for PCS band mobile phones. Electrical Specifications1
Parameter Frequency Gain Noise Figure Input 3rd Order Intercept DC supply Current Min Typ 1960 15.0 5.7 1.0 20.0
LO input -4dBm, CDMA High Gain state.
Gain Select High IP3 performance Few external components
Applications
IS-95 CDMA Mobile Phones
Max
Units MHz dB dB dBm mA
Note 1: Test Conditions: Vdd=2.8V, RF=1960MHz, LO=1750MHz, IF=210MHz, Ta=25C,
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1
TQ5631 Data Sheet
Electrical Characteristics
Parameter RF Frequency IF Frequency LO Frequency Conditions PCS band Min. 1800 100 1600 Typ/Nom 1960 210 1750 Max. 2200 300 2300 Units MHz MHz MHz
CDMA Mode-High Gain
Gain Noise Figure Input IP3 Supply Current -1.0 12.2 15.0 5.7 1.0 20.0 25.5 6.8 dB dB dBm mA
CDMA Mode-High Gain Low Linearity
Gain Noise Figure Input IP3 Supply Current 17.0 21.0 5.3 -3.0 20.0 dB dB dBm mA
CDMA Mode-Mid Gain
Gain Noise Figure Input IP3 Supply Current 1.0 3.0 12.0 18.0 15.0 dB dB dBm mA
CDMA Mode-Low Gain
Gain Noise Figure Input IP3 Supply Current Supply Voltage
Note 2: Min/Max limits are at +25C case temperature, unless otherwise specified.
6.2
8.0 10.0 13.5 15.0
dB dB dBm mA 2.9 V
2.7
2.8
Note 1: Test Conditions: Vdd=2.8V, RF=1960MHz, LO=1750MHz, IF=210MHz, TC = 25 C, LO input -4dBm, unless otherwise specified.
Absolute Maximum Ratings
Parameter DC Power Supply Power Dissipation Operating Temperature Storage Temperature Signal level on inputs/outputs Voltage to any non supply pin Value 5.0 500 -30 to 85 -60 to 150 +20 +0.3 Units V mW C C dBm V
2
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TQ5631 Data Sheet
Typical Performance, Note:HG=High Gain, LL=High Gain Low Linearity, LG=Low Gain
Test Conditions, unless otherwise specified: Vdd=2.8V, Ta=25C, RF=1960MHz, LO=1750MHz, IF=210MHz, LO input=-4dBm , Conversion Gain vs. Freq. 25.00 20.00 Gain (dB) IDD (mA) 15.00 10.00 5.00 0.00 1930
LG Mode HG Mode LL Mode
IDD vs. Freq. 21.00 20.00 19.00 18.00 17.00 16.00 15.00 14.00 1990 13.00 1930 1940 1950 1960 Freq. (MHz) 1970 1980 1990
LG Mode HG Mode LL Mode
1940
1950
1960 1970 Freq. (MHz)
1980
IIP3 vs. Freq. 16.00 11.00 IIP3 (dBm) 6.00 1.00 -4.00 1930 Gain (dB)
LG Mode HG Mode LL Mode
Conversion Gain vs. Temp. 25.00 20.00 15.00 10.00 5.00 0.00
LG Mode HG Mode LL Mode
1940
1950
1960 1970 Freq. (MHz)
1980
1990
-30
-15
0
15
30 Temp. (C)
45
60
75
90
Noise Figure vs. Freq. 11.00 10.00 9.00 NF (dB) 8.00 7.00 6.00 5.00 4.00 1920 1940 1960 Freq. (MHz) 1980 2000 IIP3 (dBm)
LG Mode HG Mode LL Mode
IIP3 vs. Temp. 15.00 13.00 11.00 9.00 7.00 5.00 3.00 1.00 -1.00 -3.00 -5.00 -30 -15 0 15 30 45 Temp. (C)
LG Mode HG Mode LL Mode
60
75
90
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3
TQ5631 Data Sheet
Noise Figure vs. Temp. 12.00 11.00 10.00 9.00 8.00 7.00 6.00 5.00 4.00 3.00 2.00 -30 -15 0 15 30 45 Temp. (C) 60 20.00 15.00 IIP3 (dBm) 10.00 5.00 0.00 -5.00 75 90 -7 -5 -3 LO Power (dBm) -1
LG Mode HG Mode LL Mode
IIP3 vs. LO Power
NF (dB)
LG Mode HG Mode LL Mode
IDD vs. Temp. 24.00 22.00 20.00 IDD (mA) 18.00 16.00 14.00 12.00 -30 -15 0 15 30 Temp. (C) 45 60 75 90
LG Mode HG Mode LL Mode
Noise Figure vs. LO Power 10.00 9.00 8.00 NF (dB) 7.00 6.00 5.00 4.00 -7 -5 -3 LO Power (dBm) -1
LG Mode HG Mode LL Mode
Conversion Gain vs. LO Power 25.00 20.00 Gain (dB) IDD (mA) 15.00 10.00 5.00 0.00 -7
LG Mode HG Mode LL Mode
IDD vs. LO Power 23.00 21.00 19.00 17.00 15.00 13.00
LG Mode HG Mode LL Mode
-5
-3 LO Power (dBm)
-1
-7
-5
-3 LO Power (dBm)
-1
4
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TQ5631 Data Sheet
Conversion Gain vs. VDD 23.00 21.00 19.00 Gain (dB) IDD (mA) 17.00 15.00 13.00 11.00 9.00 7.00 2.7 2.8 2.9 VDD (V) 3 3.1 3.2
LG Mode HG Mode LL Mode
IDD vs. VDD 24.00 22.00 20.00 18.00 16.00 14.00 12.00 2.7 2.8 2.9 VDD (V) 3 3.1 3.2
LG Mode HG Mode LL Mode
IIP3 vs. VDD 16.00 14.00 12.00 10.00 8.00 6.00 4.00 2.00 0.00 -2.00 -4.00 2.7 2.8 2.9 VDD (V) 3
IIP3 (dB)
LG Mode HG Mode LL Mode
3.1
3.2
Noise Figure vs. VDD 10.00 9.00 8.00 NF (dB) 7.00 6.00 5.00 4.00 2.6 2.7 2.8 2.9 3 3.1 3.2 3.3 VDD (V)
LG Mode HG Mode LL Mode
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5
TQ5631 Data Sheet
Application/Test Circuit
Control 2 RF AMP Gain R9 Select GND RF IN L2 RF input C10 VDD MXR R10 L3 VDD MXR C15 LO IN
GND C11 IF Out C13 VDD C12 C14 L4 GIC IF out
VDD C19 VDD
LO IN R7 C20
R8
IF AMP Gain Select Control 3
Bill of Material for TQ5631 RF AMP/Mixer
Component Receiver IC Capacitor Capacitor Capacitor Capacitor Capacitor Resistor Resistor Resistor Inductor Inductor Inductor Filter Reference Designator U1 C11 C12, C14, C15, C19 C13 C10 C20 R8 R7, R9 R10 L2 L3 L4 U2 L2XB Part Number TQ5631 22pF 1000pF 12pF 1.5pF 68pF 27 5.1K 20 2.7nH 4.7nH 56nH Value Size SOT23-8 0402 0402 0402 0402 0402 0402 0402 0402 0402 0402 0603 Panasonic Panasonic Panasonic Fijitsu Manufacturer TriQuint Semiconductor
6
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TQ5631 Data Sheet
TQ5631 Product Description Simplified theory of operation
The TQ5631 contains an RF amp, mixer, IF amp, and RF switches. Pin count is reduced by doubling the function of several pins, where dc control bias and RF signal are present at the same time. (Figure 1) In the low gain modes, the RF amp is disabled and the the input signal is routed directly to the mixer. In the high gain modes, a cascode amp is switched in before the mixer. Control for this function is made via a dc signal on the RF input pin 8. A number of switches are used internally to eliminate any parasitic signal paths. The IF amp gain can be stepped as well via a control line at pin 5. The general IF amp gain and current draw can be set using external components at the GIC pin 4. The TQ5631 uses an off chip inductor with a bypass capacitor at pin 6 for tuning the LO buffer. Although the device can be connected directly to 50 at the RF input, a better match is obtained by using a small series inductor and shunt capacitor at the RF input .
Logic truth table and logic control functions
TABLE 1
CONTROL LINES Receiver Mode RFA Gain Select C2 CDMA HG CDMA HGLL CDMA MG CDMA LG 0 0 1 1 IFA Gain Select C3 0 HG CDMA Idd 1 HG Low Idd 0 HG CDMA Idd 1 Bypassed HG HG Bypassed Bypassed LG HG LG HG LNA State Mixer State RFA IFA
TRUTH TABLE
HG=High Gain; HGLL=High Gain Low Linearity; MG=Mid Gain; LG=Low Gain
TABLE 1
When used in conjunction with the TQ3631, the TQ5631 down convert mixer can be set to a variety of different gain states. This allows the receiver (LNA + downconvert mixer) to operate with a wide dynamic range, while optimizing current draw and overall receiver performance. Two external control lines set the LNA + downconverter into any one of the four states, described below. a) CDMA Low Gain Mode: This mode is selected in very high signal environment. The current draw in this case is 16mA for the receive chain. b) CDMA High Gain Mode: This mode is selected in very weak signal environment. The receiver is in it's maximum sensitivity. c) CDMA High Gain Low Linearity Mode: This mode is selected when the phone is in standby mode. The phone power amplifier will be off in this state, removing the possibility of self jamming.
RFA GAIN SELECT, C2
RF IN
RF IN GND
VDD
1 2
8
VDD
d)
CDMA Mid Gain Mode. This mode is selected in a medium signal strength environment.
GND
7
LO TUNE VDD
IF OUT
IF
3
GIC
6
LO/C3
4
VDD
5
IF GAIN SELECT, C3
DOWNCONVERTER APPLICATION HINTS: Printed Circuit Board Layout guidelines for stability
With good layout practices the circuit will be stable. However, poor layout may lead to oscillation problems. Good grounding is especially important for the TQ5631 since it uses an off-chip LO
LO IN GIC ADJUST
FIGURE 3 TQ5631 SIMPLIFIED CIRCUIT
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7
TQ5631 Data Sheet
tuning inductor which provides a potential ground loop path. One could use the evaluation board as an example of proper layout techniques. It is important to position the LO tuning and the GIC components as close to the chip as possible. If the components are placed too far from the chip the PC board traces can act as quarter wave resonators in the 5-10GHz region. If both the GIC and the LO paths to ground resonate at the same frequency, oscillation can result, especially if Q is very high. It is most important that the ground on the GIC bypass cap, the LO tuning bypass capacitor, and the IF shunt cap return back to chip pins 1 and 2 with minimal inductance. This requires that ground returns utilize vias at a number of locations. Solid grounding of the LO tuning inductor and bypass capacitor will result in higher tuning circuit Q. The higher the Q, the greater the LO drive to the mixer will be and IIP3 performance will also improve with higher Q.
PORT 1
MEASURE S21
RF IN GND
from the die out to the pin which much be subtracted off of the needed inductance value.
1 2
IF
8
VDD
COAXIAL PROBE
VDD
GND
7
LO TUNE
3
GIC
6
LO/C3
4
5
IF GAIN SELECT, C3
LO IN
NETWORK ANALYZER
LO Buffer Tuning
Because of the broadband input match of the L0 buffer amplifier, thermal and induced noise at other frequencies can be amplified and injected directly into the L0 port of the mixer. Noise at the IF frequency, and at L0 +/- IF will be downconverted and emerge at the IF port, degrading the downconverter noise figure. For maximum flexibility the high band TQ5631 device has the output node of the L0 buffer amplifier brought out to Pin 6. By connecting an external inductor between the pin and Vdd, LO tuning can be varied. This inductor is selected to resonate with internal capacitance at the L0 frequency in order to roll off outof-band gain and improve noise performance. This approach allows selectivity in the L0 buffer amplifier along with the ability to use the TQ5631 with multiple IF's.
Figure 2 LO Tuning Setup
The inductor is selected that would resonate with the total capacitance at the L0 frequency using the following equation: 1 L = ---------------- - 1.3nH C (2*pi*F)2 To fine tune the LO, two methods have been proven to work well: a) Select the inductance (next standard value) which is higher than the calculated value derived from the equation above. Then select a bypass capacitor that forms a resonant circuit with the inductor. The bypass capacitor can be used to fine tune the resonant frequency. b) The second method relies on moving the bypass capacitor relative to the tuning inductor. This varies the amount of inductance in the circuit and provides a means to fine tune the LO. This method is utilized on the test boards. where C=1.6pF
Calculation of Nominal L Value
The proper inductor value must be determined during the design phase. The internal capacitance at Pin 6 is approximately 1.6 pF. Stray capacitance on the board surrounding Pin 6 will add to the internal capacitance, so the nominal value of inductance can be calculated, but must be confirmed with measurements on a board approximating the final layout (see Figure 2). Additionally, there is already approximately 1.3nH of inductance
8
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TQ5631 Data Sheet
Verification of Proper LO Buffer Amp Tuning Using a Network Analyzer
Connect port 1 to the L0 input (Pin 5) of the TQ5631 with the source power set to deliver -4 dBm. Connect the coaxial probe to Port 2 and place the probe tip approximately 0.1 inch away from the inductor. The magnitude of S21 represents the L0 buffer frequency response (figure 3). The test can be done in any of the CDMA modes, but both the rf and IF ports should be terminated to 50 ohms.
Half IF Spur Rejection Considerations
Because the TQ5631 does not contain a balanced mixer, Half IF spur rejection is completely set by the image filter. Thus we do not recommend using an IF that is less than 2.5 times the bandwidth of the image filter.
Downconverter IF Match Design
The Mixer IF output (pin 3) is an "open-drain" configuration, allowing for flexibility in efficient matching to various filter types and at various IF frequencies. An optimum lumped-element matching network must be designed for maximum power gain and output third order intercept. When designing the IF output matching circuit, one has to consider the output impedance (pin 3) of the IF Amplifier. It will vary somewhat depending on the quiescent current, which is set with the GIC pin. The IF frequency can be tuned from 100 to 300 MHz by varying component values of the IF output matching circuit. The IF output pin also provides the DC bias for the output FET's.
Figure 3 LO Buffer Response
The absolute value isn't important, since it depends on the probe's distance from the pin (it is usually around -30 dB), but the peak of the response should be centered in the slightly to the right of the L0 frequency band center, in this case 1750Mhz. Increasing the inductance will lower the center frequency, and vice versa. Try to keep the probe away from the LO input as it will interfere with the measurement. We have found experimentally that optimum mixer performance is achieved when the LO is tuned slightly higher than the band center. Additionally, since the curve is much steeper on the high-side of the LO tuning curve, it is best to tune the device to a slightly higher frequency to ensure that the application is never operated in that region of the curve. Small variations in the application circuit due to inductor tolerances and pc board trace capacitance will then have less affect on the circuit. Lower than expected IIP3 is the major symptom of improper LO tuning in an application. The internal passive mixer FET needs some minimum LO voltage at its gate in order to achieve satisfactory IP3, which does not occur if the LO is untuned.
In the user's application, the IF output is most commonly connected to a narrowband SAW or crystal filter with impedance from 300 -1000 with 1 - 2 pF of capacitance. A conjugate match to a higher filter impedance is generally less sensitive than matching to 50. When verifying or adjusting the matching circuit on the prototype circuit board, the LO drive should be injected at the nominal power level (-4 dBm), since the LO level does have an impact on the IF port impedance.
Suggested Matching Networks
There are several networks that can be used to properly match the IF port to the SAW or crystal IF filter. The IF FET current is applied through the IF output pin 3, so the matching circuit topology must contain either an RF choke or shunt inductor as shown in Figure 4. For purposes of evaluation, the shunt L, series C, shunt C circuit shown below is the simplest and requires the fewest components. DC current can be easily injected through the shunt inductor and the series C provides a DC block, if needed. The shunt C, in particular can be used to improve the return loss and to reduce the LO leakage. Generally the shunt C should be equal or larger than the series C. Furthermore, for best stability,
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9
TQ5631 Data Sheet
the ground end of the shunt cap should be as close to the chip ground as is possible.
Vdd
bypass
GIC PIN
Chip GND
GIC PIN
Chip GND
L Cseries IF OUT
0 to 5 ohms 0 to 5 ohms AC degen 20 to 60 ohms sets IF current 20 to 60 ohms Zc bypass at IF Freq sets IF current Zc bypass at IF Freq AC degen
50 ohms
Cshunt
Minimize Board Ground Return Inductance
Minimize Board Ground Return Inductance
Figure 4 IF Output Match Figure 5 GIC Pin Networks GIC Component Selection
The GIC pin on the TQ5631 is connected internally to the source of the IF output stage. By adding two resistors and a capacitor to this pin, it is possible to vary both the IF stage AC gain, and the IF stage quiescent current. However, there is a limit to the amount of gain increase that is possible, since there always exists some package and bond wire inductance back to the die. Furthermore, although some additional IP3 performance may be gained by increasing the quiescent current, in practice it makes no sense to increase Idd beyond that which provides maximum input intercept. At some point IP3 is limited by the mixer FET, and no further increase in input intercept can be obtained by adjusting the IF stage. There are two GIC schemes that are recommended for the CDMA devices (Figure 5). The first uses a small resistor in series with a larger bypassed resistor. The AC gain is set by the unbypassed resistor, while the DC IF current is then set by the sum of the two resistors.
band pass
IF
The Image Filter to Mixer RF input Path
We recommend evaluating the CDMA downconverter by considering it and the image filter as a block, since there is a very complicated non-linear interaction between the mixer and image filter. Especially in the LG and MG receiver modes, some LO energy leaks out through the RF input, reflects off the image filter, and then returns back into the mixer (Figure 6). The reflection at the filter occurs because most SAW and dielectric filters look like a short circuit outside of the passband. Depending on the phase of the reflected signal, noise figure, gain, and IP3 can be negatively affected. Thus system simulation can be inaccurate if the downconverter and filter are treated separately.
LO Leakage LNA in Bypass Mode Mixer
The second scheme, which is recommended for the high band device, uses a resistor in parallel with a series combination of resistor and capacitor. The first resistor sets the DC current, while the equivalent parallel resistance sets the AC gain. The presence of a resistor directly from the GIC pin to ground tends to dampen the Q of any resonance in the 5-10ghz range which might be formed by the GIC circuitry.
LO Leakage +
LO
Figure 6 Mixer-Filter Interaction
The issue also raises a dilemma with regard to the specification of SSB noise figure. An image filter is needed for measurement; yet how does one go about specifying the SSB noise figure (CG
10
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TQ5631 Data Sheet
and IIP3 as well) of the downconverter alone, realizing that it depends somewhat upon the type of image filter used and the delay between it and the mixer? The most pragmatic approach measures the NF, CG, and IIP3 with the filter in place. The downconverter to filter distance(in pS) is set to be similar to that which would be used in the end application. Then filter I.L. is simply subtracted off of the system noise figure in order to arrive at the downconverter NF. Similarly, the filter I.L. is subtracted off of the IIP3 and added to the CG in order to arrive at those numbers.
Use correct RF input power levels for accurate test results
Because the CDMA devices have a number of gain states, it important to make sure that IP3 measurements are not taken in a state of compression. Additionally, using too low of a power puts the IMD products too close to the noise floor for accurate results. Figure 7 shows the automated test setup that is used for evaluation. Table 2 lists the RF input powers that we are using to evaluate the devices, which has proved to be effective for automated measurement. For bench measurement, it is possible to use much lower input powers, since no hardware routines are needed for peak searching.
RF Input Power (dBm) Mode CDMA HGLL CDMA HG CDMA MG CDMA LG Downconverter plus Filter -20 -20 -5 -10
Table 2 Suggested RF Input Test Levels
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11
TQ5631 Data Sheet
Package Pinout
GND
RF IN
GND
VDD
IF out
VDD
GIC
LO IN
Pin Descriptions
Pin Name GND GND IF OUT GIC LO IN VDD VDD RF IN Pin # 1 2 3 4 5 6 7 8 Description and Usage Ground Ground IF Output and IF Vdd Off chip tuning for gain/IP3/current LO Input, and Control 3 input LO Buffer Vdd Mixer Vdd RF input, and Control 2 input
12
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TQ5631 Data Sheet
Package Type: SOT23-8 Plastic Package
Note 1
PIN 1 FUSED LEAD
b A c
E E1
Note 2
DIE
e
A1
L
DESIGNATION A A1 b c D e E E1 L Theta
DESCRIPTION OVERALL HEIGHT STANDOFF LEAD WIDTH LEAD THICKNESS PACKAGE LENGTH LEAD PITCH LEAD TIP SPAN PACKAGE WIDTH FOOT LENGTH FOOT ANGLE
METRIC 1.20 +/-.25 mm .100 +/-.05 mm .365 mm TYP .127 mm TYP 2.90 +/-.10 mm .65 mm TYP 2.80 +/-.20 mm 1.60 +/-.10 mm .45 +/-.10 mm 1.5 +/-1.5 DEG
ENGLISH 0.05 +/-.250 in .004 +/-.002 in .014 in .005 in .114 +/-.004 in .026 in .110 +/-.008 in .063 +/-.004 in .018 +/-.004 in 1.5 +/-1.5 DEG
NOTE 3 3 3 3 1,3 3 3 2,3 3
Notes 1. The package length dimension includes allowance for mold mismatch and flashing. 2. The package width dimension includes allowance for mold mismatch and flashing. 3. Primary dimensions are in metric millimeters. The English equivalents are calculated and subject to rounding error.
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13
TQ5631 Data Sheet
Additional Information
For latest specifications, additional product information, worldwide sales and distribution locations, and information about TriQuint: Web: www.triquint.com Tel: (503) 615-9000 Fax: (503) 615-8900
For technical questions and additional information on specific applications:
The information provided herein is believed to be reliable; TriQuint assumes no liability for inaccuracies or omissions. TriQuint assumes no responsibility for the use of this information, and all such information shall be entirely at the user's own risk. Prices and specifications are subject to change without notice. No patent rights or licenses to any of the circuits described herein are implied or granted to any third party. TriQuint does not authorize or warrant any TriQuint product for use in life-support devices and/or systems. Copyright (c) 1998 TriQuint Semiconductor, Inc. All rights reserved. Revision A, March, 2000
14
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