LMV232 Dual-Channel Integrated Mean Square Power Detector for CDMA & WCDMA General Description Features The LMV232 dual RF detector is designed for RF transmit power measurement in mobile phones. This dual mean square IC is especially suited for accurate power measurement of RF signals exhibiting high peak-to-average ratios used in 3G and UMTS/CDMA applications. The LMV232 saves calibration steps and system certification and is highly accurate. The circuit operates with a single supply from 2.5 to 3.3V. The LMV232 contains a mean square detector with two sequentially selectable RF inputs. The RF input power range of the device has been optimized for use with a 20 dB directional coupler, without the need for additional external components. A single external RC combination between FB and OUT provides an externally configurable gain and LF filter bandwidth of the device. The device has two digital interfaces. A shutdown function is available to set the device in a low-power shutdown mode. In case SD = HIGH, the device is in shutdown, if SD = LOW the device is active. The Band-Select function controls the selection of the active RF input channel. In case BS = HIGH, RFIN1 is active. In case BS = LOW, RFIN2 is active. The dual mean square detector is offered in an 8-bump micro SMD 1.5 x 1.5 x 0.6 mm package. This micro SMD package has the smallest footprint and height. n n n n n n n > 20 dB square-law detection range 2 sequentially selectable RF inputs Low power consumption shutdown mode Externally configurable gain and LF filter bandwidth. Internal 50 RF termination impedance Optimized for use with 20 dB directional coupler Lead free 8-bump micro SMD package 1.5 x 1.5 x 0.6 mm Applications n n n n n n n n 3G mobile communications UMTS WCDMA CDMA2000 TD-SCDMA RF control Wireless LAN PC Card and GPS modules Typical Application 20127801 (c) 2005 National Semiconductor Corporation DS201278 www.national.com LMV232 Dual-Channel Integrated Mean Square Power Detector for CDMA & WCDMA April 2005 LMV232 Absolute Maximum Ratings (Note 1) Junction Temperature (Note 3) If Military/Aerospace specified devices are required, please contact the National Semiconductor Sales Office/ Distributors for availability and specifications. Mounting Temperature Infrared or Convection (20 sec) Supply Voltage VDD - GND 235C Operating Ratings (Note 1) 3.6V Max Supply Voltage ESD Tolerance (Note 2) Human Body Model 2.5V to 3.3V Operating Temperature Range 2000V Machine Model -40C to +85C RF Frequency Range 200V Storage Temperature Range 150C Max 50 MHz to 2 GHz -65C to 150C 2.7 DC and AC Electrical Characteristics Unless otherwise specified, all limits are guaranteed to VDD = 2.7V; TJ = 25C. Boldface limits apply at temperature extremes. (Note 4) Symbol IDD Parameter Supply Current VLOW BS and SD Logic Low Level (Note 6) VHIGH BS and SD Logic High Level (Note 6) IBS, ISD Current into BS and SD pins VOUT Output Voltage Swing IOUT Output Short Circuit Condition Min Typ Max Units Active Mode: SD = LOW, No RF Input Power Present 9.8 11 13 mA Shutdown: SD = 1.8V, No RF Input Power Present 0.09 5 30 A 0.8 V 1.8 V 5 A From Positive Rail, Sourcing, FB = 0V, IOUT = 1 mA 20 80 90 mV From Negative Rail, Sinking, FB = 2.7V, IOUT = -1 mA 20 60 70 mV Sourcing, FB = 0V, VOUT = 2.6V 3.7 2.7 5.1 Sinking, FB = 2.7V, VOUT = 0.1V 3.7 2.7 5.5 No RF Input Power 235 230 254 VOUT Output Voltage (Pedestal) VPED Pedestal Variation Over Temperature (Note 10) 5.4 IOS Offset Current Variation Over Temperature (Note 10) 1.17 tON Turn-on-Time (Note 9) No RF Input Power Present, Output Loaded with 10 pF 2.0 tR Rise Time (Note 7) Step from No Power to 0 dBm Applied, Output Loaded with 10 pF 4.5 en Output Referred Voltage Noise RF Input = 1800 MHz, -10 dBm, Measured at 10 kHz GBW Gain Bandwidth Product SR Slew Rate RIN DC Resistance PIN RF Input Power Range www.national.com 400 mA 275 280 mV mV A 6.0 s s nV/ 3.7 MHz 3.0 V/s (Note 7) 50.8 RF Input Frequency = 900 MHz -11 +13 dBm -24 0 dBV 1.8 1.0 2 (Continued) Unless otherwise specified, all limits are guaranteed to VDD = 2.7V; TJ = 25C. Boldface limits apply at temperature extremes. (Note 4) Symbol KDET Parameter Detection Slope Condition Min Typ 900 MHz 21 1800 MHz 10 1900 MHz 10 2000 MHz 10 Max Units A/mW fLOW LF Input Corner Frequency Lower -3 dB Point of Detection Slope 60 MHz fHIGH HF Input Corner Frequency Upper -3 dB Point of Detection Slope 1.0 GHz AISO Channel Isolation 900 MHz 58 1800 MHz 62 1900 MHz 58 2000 MHz 55 dB Note 1: Absolute Maximum Ratings indicate limits beyond which damage to the device may occur. Operating Ratings indicate conditions for which the device is intended to be functional, but specific performance is not guaranteed. For guaranteed specifications and the test conditions, see the Electrical Characteristics. Note 2: Human body model: 1.5 k in series with 100 pF. Machine model, 0 in series with 100 pF. Note 3: The maximum power dissipation is a function of TJ(MAX) , JA and TA. The maximum allowable power dissipation at any ambient temperature is PD = (TJ(MAX) - TA)/JA. All numbers apply for packages soldered directly into a PC board. Note 4: Electrical Table values apply only for factory testing conditions at the temperature indicated. Factory testing conditions result in very limited self-heating of the device such that TJ = TA. No guarantee of parametric performance is indicated in the electrical tables under conditions of internal self-heating where TJ > TA. Note 5: Power in dBV = dBm + 13 when the impedance is 50. Note 6: All limits are guaranteed by design or statistical analysis. Note 7: Typical values represent the most likely parametric norm. Note 8: Device is set in active mode with a 10 k resistor from VDD to RFIN/EN. RF signal is applied using a 50 RF signal generator AC coupled to the RFIN/EN pin using a 100 pF coupling capacitor. Note 9: Turn-on time is measured by connecting a 10 k resistor to the RFIN/EN pin. Be aware that in the actual application on the front page, the RC-time constant of resistor R2 and capacitor C adds an additional delay. Note 10: Typical numbers represent the 3-sigma value of 10k units. 3-sigma value of variation between -40C / 25C and variation between 25C / 85C. 3 www.national.com LMV232 2.7 DC and AC Electrical Characteristics LMV232 Connection Diagram 8-Bump micro SMD 20127802 Top View Pin Description Pin Name Power Supply B3 VDD Positive Supply Voltage B1 GND Power Ground Digital Inputs C3 SD Schmitt-triggered Shutdown. The device is active for SD = LOW. For SD = HIGH, it is brought into a low-power shutdown mode. C2 BS Schmitt-triggered Band Select pin. When BS = HIGH, RFIN1 is selected, when BS = LOW, RFIN2 is selected. A1 RFIN1 C1 RFIN2 Feedback A2 FB Connected to inverting input of output amplifier. Enables user-configurable gain and bandwidth through external feedback network. Output A3 Out Amplifier output Analog Inputs Description RF Input connected to the coupler output with optional attenuation to measure the Power Amplifier (PA) / Antenna RF power levels. Both RF inputs of the device are internally terminated with a 50 resistance. Ordering Information Package 8-Bump micro SMD Part Number Package Marking Transport Media LMV232TL A I 02 250 Units Tape and Reel LMV232TLX 3k Units Tape and Reel Note: This product is only offered with lead free bumps. www.national.com 4 NSC Drawing TLA08AAA LMV232 Block Diagrams 20127864 LMV232 5 www.national.com LMV232 Typical Performance Characteristics Unless otherwise specified, VDD = 2.7V, TJ = 25C, R1 = 6.2 k and C1 = 1.5 nF (See typical application on the frontpage). VOUT - VPEDESTAL vs. RF Input Power Supply Current vs. Supply Voltage 20127877 20127867 VOUT - VPEDESTAL vs. RF Input Power @ 900 MHz Input Referred Error vs. RF Input Power @ 900 MHz 20127868 20127869 VOUT - VPEDESTAL vs. RF Input Power @ 1800 MHz Input Referred Error vs. RF Input Power @ 1800 MHz 20127870 www.national.com 20127871 6 LMV232 Typical Performance Characteristics Unless otherwise specified, VDD = 2.7V, TJ = 25C, R1 = 6.2 k and C1 = 1.5 nF (See typical application on the frontpage). (Continued) VOUT - VPEDESTAL vs. RF Input Power @ 1900 MHz Input Referred Error vs. RF Input Power @ 1900 MHz 20127872 20127873 VOUT - VPEDESTAL vs. RF Input Power @ 2000 MHz Input Referred Error vs. RF Input Power @ 2000 MHz 20127874 VOUT -VPEDESTAL 20127875 vs. RF Input Power @ 1900 MHz Input Referred Error vs. RF Input Power @ 1900 MHz 20127882 20127883 7 www.national.com LMV232 Typical Performance Characteristics Unless otherwise specified, VDD = 2.7V, TJ = 25C, R1 = 6.2 k and C1 = 1.5 nF (See typical application on the frontpage). (Continued) RF Input Impedance vs. Frequency @ Resistance and Reactance Gain and Phase vs. Frequency 20127804 20127876 Sourcing Current vs. Output Voltage Sinking Current vs. Output Voltage 20127878 20127879 Output Voltage vs. Sourcing Current Output Voltage vs. Sinking Current 20127880 www.national.com 20127881 8 The LMV232 mean square power detector is particularly suited for accurate power measurement of RF modulated signals that exhibit large peak to average ratios, i.e. large variations of the signal envelope. Such noise-like signals are encountered e.g. in CDMA and Wide-band CDMA cellphones. Many power detection circuits, particularly those devised for constant-envelope modulated signals as in GSM, are based on peak detection and provide accurate power measurements for constant envelope or low-crest factor (ratio of peak to RMS) signals only. Such detectors are therefore not particularly suited for CDMA and WCDMA applications. PEAK TO AVERAGE RATIO SENSITIVITY The LMV232 power detector provides an accurate power measurement for arbitrary input signals, low and high peakto-average ratios and crest factors. This is because its operation is not based on peak detection, but on direct determination of the mean square value. This is the most accurate power measurement, since it exactly implements the definition of power. A mean-square detector measures VRMS2 for all waveforms. Peak detection is less accurate because the relation between peak detection and mean square detection depends on the waveform. A peak detector measures P = VPEAK2 for all waveforms, while it should measures P = VPEAK2/2 (for R = 1) for a sine wave and P = VPEAK2/3 for a triangle wave for instance. For a CDMA signal, the measurement error can be in the order of 5 to 6 dB. For many wave forms, specially those with high peak-to-average ratios, peak detection is not accurate enough and therefore a mean square detector is recommended. TYPICAL APPLICATION The LMV232 is especially suited for CDMA and WCDMA applications with 2 Power Amplifiers (PA's). A typical setup is given in Figure 1. The output power of one PA is measured at a time, depending on the bandselect pin (BS). If the BS = High RFIN1 is used for measurements, if BS = Low RFIN2 is used. The measured output voltage of the LMV232 is read by the ADC of the baseband chip and the gain of the PA gain is adjusted if necessary. With an input impedance of 50, the LMV232 can be directly connected to a 20 dB directional coupler without the need for an additional external attenuator. The setup can be adjusted to various PA output ranges by selection of a directional coupler or insertion of an additional (resistive) attenuator between the coupler outputs and the LMV232 RF inputs. The LMV232 conversion gain and bandwidth are configured by a resistor and a capacitor. Resistor R1 sets the conversion gain from RFIN to the output voltage. A higher resistor value will result in a higher conversion gain. The maximum dynamic range is achieved when the resistor value is as high as possible, i.e. the output signal just doesn't clip and the MEAN SQUARE CONFORMANCE ERROR The LMV232 is a mean square detector and therefore should have an output voltage (in Volts) that linearly relates to the RF input power (in mW). The input referred error, with respect to an ideal linear mean square detector, is determined as a measure for the accuracy of the detector. 20127801 FIGURE 1. Typical Application 9 www.national.com LMV232 voltage stays within the baseband ADC input range. The filter bandwidth is adjusted by capacitor C1. The capacitor value should be chosen such that the response time of the device is fast enough and modulation on the RF input signal is not visible at the output (ripple suppression). The -3 dB filter bandwidth of the output filter is determined by the time constant R1*C1. Generally a capacitor value of 1.5 nF is a good choice. Application Notes LMV232 Application Notes (Continued) The detection curves of Figure 2 show the detector response to RF input power. To show the complete dynamic range on a logarithmic scale, the pedestal voltage (VPEDESTAL) is subtracted from the output. The pedestal voltage is defined as the output voltage in the absence of an RF input signal (at 25C). The best-fit ideal mean square response is represented by the fitted curve in Figure 2. The input referred error of the detection curves with respect to this best-fit mean square response is determined as follows: * Determine the best-fit mean square response. * Determine the output referred error between the actual detector response and the ideal mean square response. * Translate the output referred error to an input referred error. 20127869 FIGURE 3. Input referred Error vs. RF Input Power Analyzing Figure 3 shows that three sections can be distinguished: * At higher power levels the error increases. * A middle section where the error is constant and relatively small. * At lower power levels the error increases again. These three sections are leading back to three error mechanisms. At higher power levels the detectors output starts to saturate because the output voltage approaches the maximum signal swing that the detector can handle. The maximum output voltage of the device thus limits the upper end of the detection range. Also the maximum allowed ADC voltage of the baseband chip can limit the detection range at higher power levels. By adjusting the feedback resistor RFB of Figure 1 the upper end of the range can be shifted. This is valid until the detector cell inside the LMV232 is the limiting factor. 20127884 FIGURE 2. Detection Curve The best-fit linear curve is obtained from the detector response by means of linear regression. The output referred error is calculated with the formula: ErrordBV = 20*log[ (VOUT-VPEDESTAL)/(KDET*PIN) ] Where, Conversion gain of the ideal fitted curve KDET is in V/mW and the RF input power PIN in mW. To translate this output referred error (in dB) to an input referred error, it has to be divided by a factor of 2. This is due to the mean square characteristic of the device. The response of a mean square detector changes by 2 dB for every dB change of the input power. Figure 3 depicts the resulting curve. www.national.com The middle section of the error curve shows a small error variation. This is the section where the detector is used and is called the detection range of the detector. This range is limited on both sides by a maximum allowed error. For low input power levels, the variation of output voltage is very small. Therefore the measurement resolution ADC is important in order to measure those small variations. Offsets and temperature variation impact the accuracy at low power levels as well. DETECTION ERROR OVER TEMPERATURE Like any power detector device, the output signal of the LMV232 mean square power detector shows some residual variation over temperature that limits it's dynamic range. The variation determines the accuracy and range of input power levels for which the detector produces an accurate output signal. The error over temperature is mainly caused by the variation of the pedestal voltage. Besides this, a minimal error contribution leads back to the conversion gain variation of the detector. This conversion gain error is visible in the midpower range, where the temperature error curves of Figure 3 run parallel to each other. Since the conversion gain variation is acceptable, the focus will be on the pedestal voltage variation over temperature. 10 level is digitally subtracted from the measured output signal of the LMV232 during normal operation. The procedure is thus: * Measure the detector output in the absence of RF power during manufacturing. * Store the output voltage value in the cell phone memory (after it is analog-to-digital converted). * Subtract the stored value from each detector output reading. (Continued) The pedestal voltage at 25C is subtracted from the output voltage of each curve. Variations of the pedestal voltage over temperature are thus included in the error. The pedestal voltage variation itself consists of 2 error sources. One is the variation of the reference voltage VREF. The other is an offset current IOS that is generated inside the detector. This depicted in Figure 4. Depending on the measurement strategy one or both error sources can be eliminated. The error sources of the pedestal voltage can be shown in a formula for VOUT: VOUT = VREF + (IOS + IDET) * RFB Where IDET represents the intended detector output signal. In the absence of RF input power IDET equals zero. The formula for the pedestal voltage can therefore be written as: VPEDESTAL = VREF + IOS * RFB 20127806 FIGURE 5. Strategy 1: Room Temperature Calibration The advantage of this strategy is that calibration is required only once during manufacturing and not during normal operation. The disadvantage is the fact that this method neither compensates for the residual temperature drift of the reference voltage VREF nor for offset current variations. Only part-to-part variations at room temperature are eliminated by this strategy. Especially the residual temperature drift negatively affects the measurement accuracy. 20127805 FIGURE 4. Pedestal Voltage Strategy 2: Elimination of Temperature Spread in VREF If software changes need to be reduced to a minimum and the baseband chip has a differential ADC, strategy 2 can be used to eliminate temperature variations of the reference voltage VREF. One pin of the ADC is connected to FB and one is connected to OUT (Figure 6). For low input power levels, the pedestal variation VPEDESTAL is the dominant cause of error. Besides temperature variation of the pedestal voltage, which limits the lower end of the range, the pedestal voltage can also vary from part-to-part. By applying a suitable measurement strategy, the pedestal voltage error contribution can be significantly reduced or eliminated completely. POWER MEASUREMENT STRATEGIES This section describes the measurement strategies to reduce or eliminate the pedestal voltage variation. Which strategy is chosen depends on the possibilities for a factory trim and implementation of calibration procedures. Since the pedestal voltage is the reference level for the LMV232, it needs to be calibrated/measured at least once to eliminate part-to-part spread. This is required to determine the exact detector output signal. Because of process tolerances, the absolute part-to-part variation of the output voltage in the absence of RF input power will be in the order of 5 - 10%. All measurement strategies discussed eliminate this part-to-part spread. 20127807 FIGURE 6. Strategy 2: Differential Measurement Strategy 1: Elimination of Part-to-Part Spread at Room Temperature Only In this strategy, the pedestal voltage is determined once during manufacturing and stored into the memory of the phone. At each power measurement this stored pedestal The power measurement is independent of the reference voltage VREF, since the ADC reading is: VOUT-VFB = (IOS + IDET) * RFB 11 www.national.com LMV232 Application Notes LMV232 Application Notes (Continued) The calibration measurement procedure can be explained with the aid of Figure 1, which depicts a typical power measurement setup using the LMV232. In normal operation, the two PA's in the setup will never be active at the same time. One PA will produce the required transmit power, while the other one is off, (disabled) and produces no power. The pedestal voltage should be measured in the absence of RF power. This can be achieved by switching the Band Select (BS) pin such that the LMV232 input is selected where the disabled PA is connected to. The pedestal voltage at no input power can be read at the output pin. The reading of the ADC obviously doesn't contain the reference voltage source VREF anymore, but the contribution of the offset current remains present. This measurement is performed during normal operation. Therefore, it eliminates voltage reference variations over temperatures, as opposed to strategy 1. Also offset variations in the op amp are eliminated in this strategy. Strategy 3: Complete Elimination of Temperature Spread in Pedestal Voltage The most accurate measurement is strategy 3, which eliminates the temperature variation of both the reference voltage VREF and the offset current IOS. In this strategy, the pedestal voltage is measured regularly during operation of the phone, and stored in the phone memory. For each power measurement, the stored value is digitally subtracted from the (analog-to-digital converted) detector output signal. Since it measures the pedestal voltage itself for calibration it compensates both for the reference voltage VREF as well as for the offset current variation IOS. The frequency of the `calibration measurement' can be significantly lower than those of power measurements, depending on how fast the temperature of the device changes. Using the Band Select (BS) control pin of the LMV232: * Select the RF input that is connected to the disabled PA, by the BS pin. * Measure the detector output. * Store the result in the phone memory. * Important advantages of this approach are that no factory trim is required and the temperature drift of the pedestal can be cancelled almost completely as well as the part-to-part spread. The remaining error is determined by the resolution of the ADC. A slight disadvantage is that on average more than one detector reading is required per power measurement. This overhead though can be made almost negligible in normal circumstances. 20127808 FIGURE 7. Strategy 3: Calibration during normal operation www.national.com Subtract the stored value from each detector power reading, until a new update is performed. 12 inches (millimeters) unless otherwise noted NOTES: UNLESS OTHERWISE SPECIFIED 1. EPOXY COATING 2. FOR SOLDER BUMP COMPOSITION, SEE "SOLDER INFORMATION" IN THE PACKAGING SECTION OF THE NATIONAL SEMICONDUCTOR WEB (www.national.com). 3. RECOMMEND NON-SOLDER MASK DEFINED LANDING PAD. 4. PIN A1 IS ESTABLISHED BY LOWER LEFT CORNER WITH RESPECT TO TEXT ORIENTATION. 5. XXX IN DRAWING NUMBER REPRESENTS PACKAGE SIZE VARIATION WHERE X1 IS PACKAGE WIDTH, X2 IS PACKAGE LENGTH AND X3 IS PACKAGE HEIGHT. REFERENCE JEDEC REGISTRATION MO-211, VARIATION DD. 8-Bump micro SMD NS Package Number TLA08AAA X1 = 1.514 0.030 mm X2 = 1.514 0.030 mm X3 = 0.600 0.075 mm National does not assume any responsibility for use of any circuitry described, no circuit patent licenses are implied and National reserves the right at any time without notice to change said circuitry and specifications. For the most current product information visit us at www.national.com. LIFE SUPPORT POLICY NATIONAL'S PRODUCTS ARE NOT AUTHORIZED FOR USE AS CRITICAL COMPONENTS IN LIFE SUPPORT DEVICES OR SYSTEMS WITHOUT THE EXPRESS WRITTEN APPROVAL OF THE PRESIDENT AND GENERAL COUNSEL OF NATIONAL SEMICONDUCTOR CORPORATION. As used herein: 1. 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National Semiconductor Americas Customer Support Center Email: new.feedback@nsc.com Tel: 1-800-272-9959 www.national.com National Semiconductor Europe Customer Support Center Fax: +49 (0) 180-530 85 86 Email: europe.support@nsc.com Deutsch Tel: +49 (0) 69 9508 6208 English Tel: +44 (0) 870 24 0 2171 Francais Tel: +33 (0) 1 41 91 8790 National Semiconductor Asia Pacific Customer Support Center Email: ap.support@nsc.com National Semiconductor Japan Customer Support Center Fax: 81-3-5639-7507 Email: jpn.feedback@nsc.com Tel: 81-3-5639-7560 LMV232 Dual-Channel Integrated Mean Square Power Detector for CDMA & WCDMA Physical Dimensions