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Removing the interstage transmit SAW in WCDMA Feb 1, 2007 12:00 PM By Tajinder Manku Typically, in a WCDMA radio, there is a transmit (Tx) SAW filter between the transceiver Tx output and the power amplifier to reduce the transmit output from increasing the receiver's (Rx) noise figure, as well as to reduce out-of-band spurious and noise emission from the Tx. However, if the Tx SAW filter was eliminated, it would save area on the PCB as well as cost. This article analyzes the trade-offs required for removing the Tx SAW from the transceiver and duplexer sections of the handset.
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The interstage transmitter (Tx) SAW filter between the transceiver's Tx output and the power amplifier has effectively two functions.
If this Tx SAW filter can be eliminated, it would save cost and area on the PCB. This article analyzes the trade-offs involved with removing the Tx SAW filter from the perspective of improving the performance of either the transceiver and/or the duplexer. Item (1) is not a concern for GSM/GPRS/EDGE radios because these standards are half-duplex — i.e., the Rx and Tx are not on at the same time. However, item (2) is an important concern for GSM/GPRS/EDGE. According to the 3GPP specification, Tx noise within the low bands of GSM/GPRS (850 MHz and 900 MHz) cannot exceed -79 dBm over a bandwidth of 100 kHz at an offset of 20 MHz. At +33 dBm output (as per the 3GPP specification) the noise at a 20 MHz offset has to be better than -163 dBc/Hz (i.e., -79 dBm-10log (100 kHz)-33 dBm). This number is achievable for both the transceiver and the power amplifier. Consequently, a Tx SAW is not required for the GSM standard. Both functions 1 and 2 are explored with a SAW and without a SAW for WCDMA, and various trade-offs are discussed. However, the article addresses item (1) in much more detail since item (2) is well understood for GSM. Transmitter to receiver desensitization
Tx to Rx desensitization occurs because the transmit noise in the Rx band leaks into the Rx chain and effectively increases the noise floor of the Rx. This increase in the noise floor increases the overall noise figure of the Rx. If we assume the E
In our initial analysis, we will assume the DAC noise is lower (at least 10 dB lower) than the transceiver and power amplifier noise. Figure 1 illustrates a generalized WCDMA system with an intrastage Tx SAW filter. All the variables within the following analysis are defined within Figure 1. The Rx noise due to the transceiver at the output of the power amplifier, N Therefore, the total in-band Rx noise at the output of the power amplifier, N Given this, the noise at the input of the Rx, N Therefore, the NF at the antenna input with the Tx on is given by the following equation; By using equations (1) to (4), the effective noise figure of the Rx can be derived. In a typical application, the duplexer Tx to Rx isolation is approximately 42 dB, the noise from the PA is typically around -73 dBm, the noise figure of the Rx with the Tx off is typically around 3 dB, and the power and noise output of the transceiver is +4 dBm and -153 dBc/Hz, respectively. If a low-cost Tx SAW is used, one would expect an in-band loss of 1 dB and an out-of-band loss of 30 dB. The in-band loss from the switch and duplexer to the antenna is typically around 2 dB and 3 dB for the Tx and Rx, respectively. Given all this, the gain of the PA would have to be 23 dB to achieve an output power of +24 dBm as per the 3GPP requirement. With all these variables, the noise figure with the Tx on would be NF = 6.4 dB, which meets the spec and has about 2.6 dB of margin. For this particular case, the transmit noise in the Rx band is mainly influenced by the PA noise rather than the transceiver noise. For example, if the transceiver noise increased by 8 dB, NF = 6.5 dB, which is only a 0.1 dB increase. Consequently, with a Tx SAW filter, the affects of the transceiver noise in the Rx band can be effectively ignored. Now, let's assume the SAW is removed from the Tx chain and the transceiver noise is -153 dBc/Hz; see Figure 2. Under this scenario, the NF at the antenna port is 10.9 dB, which fails the NF spec of 9 dB. From the analysis, it becomes apparent that there are only two variables that dramatically influence the amount of Tx to Rx desensitization; (a) the duplex isolation between the Tx and Rx (D The other variable is the transceiver noise in the Rx band. To improve this usually implies increasing the current consumption within the transceiver, which would in turn reduce battery life. In any case, let's assume N In summary, Table 1 depicts the trade offs without the SAW filter. Transmit out-of-band spurious requirements
Table 2 illustrates the closest spurious requirements for four popular WCDMA bands. These numbers can be translated into a noise requirement at the output of the transceiver if no Tx SAW is used; The hardest requirements in terms of noise are bands I and V. These requirements are -145 dBc/Hz at 40 MHz offset and -150 dBc/Hz at 45 MHz offset, respectively. However, not only does the noise have to be below these settings, care has to be taken to make sure the spurious components are below these values. However, for band I, five exceptions are allowed within the band limits of 1805 MHz and 1880 MHz. Conclusion
When an interstage Tx SAW is used, the Rx sensitivity is optimized for best performance. By removing the Tx SAW there becomes a design trade off between duplexer technology, the transmit noise in the Rx band, and the Rx noise figure. If the Tx SAW is removed, the specification requirements of either/both the transceiver and duplexer have to be better. The Tx must be designed to have less noise in the Rx band and less spurious power out-of-band. The duplexer, on the other hand, has to have better isolation characteristics between the Tx and Rx. However, increasing the duplexer requirements may not be the right choice given better duplexer performance may come at a higher cost and more PCB area.
ABOUT THE AUTHOR
Tajinder Manku is chief technology officer and founder of Sirific Wireless Corporation, Richardson, Texas. Prior to Sirific, Manku served as an associate professor at the University of Waterloo in Canada, where he earned his B.S in solid-state physics and a PhD.
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