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ADRF6807ACPZ-R7 数据表(PDF) 24 Page - Analog Devices |
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ADRF6807ACPZ-R7 数据表(HTML) 24 Page - Analog Devices |
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24 / 36 page ![]() ADRF6807 Data Sheet Rev. B | Page 24 of 36 EVM MEASUREMENTS Figure 42 shows the excellent EVM of the ADRF6807 being better than −40 dB over an RF input range of about 40 dB for a 4 QAM modulated signal, at a 5 MHz symbol rate and at a 0 Hz IF. The roll-off, or alpha, of the pulse shaping filter was set to 0.35. The reported RF input power is the power integrated across the bandwidth of EVM is a measure used to quantify the performance of a digital radio transmitter or receiver. A signal received by a receiver has all constellation points at their ideal locations; however, various imperfections in the implementation (such as magnitude imbalance, noise floor, and phase imbalance) cause the actual constellation points to deviate from their ideal locations. BW = (1 + α) × (Symbol Rate) EVM was tested for both power modes: low power mode disabled (LPEN = 0) and low power mode enabled (LPEN = 1). When the low power mode is enabled, the EVM is better at lower RF input signal levels due to less noise while running in the low power mode. In general, a demodulator exhibits three distinct EVM limitations vs. received input signal power. As signal power increases, the distortion components increase. At large signal levels, where the distortion components due to the harmonic nonlinearities in the device are falling in-band, EVM degrades as signal levels increase. At medium signal levels, where the demodulator behaves in a linear manner and the signal is well above any notable noise contributions, the EVM has a tendency to reach an optimal level determined dominantly by either quadrature accuracy and I/Q gain match of the demodulator or the precision of the test equipment. As signal levels decrease, such that the noise is a major contribution, the EVM performance vs. the signal level exhibits a decibel-for-decibel degradation with decreasing signal level. At lower signal levels, where noise proves to be the dominant limitation, the decibel EVM proves to be directly proportional to the SNR. –50 –35 –45 –30 –40 –25 –20 –15 –10 –5 0 RF INPUT POWER (dBm) LPEN = 1 LPEN = 0 –60 –50 –40 –30 –20 –10 0 10 20 The basic test setup for testing the EVM of the ADRF6807 consisted of an Agilent E4438C, which was used as a signal source. The 900 MHz modulated signal was driven single ended into the RFIN SMA connector of the ADRF6807 evaluation board. The IQ baseband outputs were taken differentially into a pair of AD8130 difference amplifiers to convert the differential signals to single ended. The output impedance that the ADRF6807 drove was set to 450 Ω differential. The single-ended I and Q signals were then sampled by an Agilent DSO7104B oscilloscope. The Agilent 89400 VSA software was used to calculate the EVM of the signal. The signal source that was used for the reference input was a Wenzel 100 MHz quarts oscillator set at an amp- tude of 1 V p-p. The reference path was set to a divide-by-four, thus making the PFD frequency 25 MHz. Figure 42. EVM Measurements at 900 MHz 4 QAM, Symbol Rate = 5 MHz, Baseband Frequency = 0 Hz IF |
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