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AD9857/PCB 数据表(PDF) 15 Page - Analog Devices |
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AD9857/PCB 数据表(HTML) 15 Page - Analog Devices |
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15 / 31 page ![]() AD9857 –15– REV. 0 0 0 0.05 0.10 0.15 0.20 0.25 0.01 0.008 0.006 0.004 0.002 –0.002 –0.004 –0.006 –0.008 –0.01 0.2 FREQUENCY Figure 23. Half-Band 1 and 2 Pass Band Detail; Frequency Relative to HB1 Output Sample Rate The usable bandwidth of the filter chain puts a limit on the maximum data rate that can be propagated through the AD9857. A look at the pass band detail of the half-band filter response indicates that in order to maintain an amplitude error of no more than 1 dB, we are restricted to signals having a bandwidth of no more than about 90% of fNYQ. Thus, in order to keep the bandwidth of the data in the flat portion of the filter pass band, the user must oversample the baseband data by at least a factor of two prior to presenting it to the AD9857. Note that without oversampling, the Nyquist bandwidth of the baseband data cor- responds to the fNYQ. Because of this, the upper end of the data bandwidth will suffer 6 dB or more of attenuation due to the frequency response of the half-band filters. Furthermore, if the baseband data applied to the AD9857 has been pulse shaped there is an additional concern. Typically, pulse shaping is applied to the baseband data via a filter having a raised cosine response. In such cases, an α value is used to modify the bandwidth of the data where the value of α is such that 0 < α < 1. A value of 0 causes the data bandwidth to correspond to the Nyquist bandwidth. A value of 1 causes the data bandwidth to be extended to twice the Nyquist bandwidth. Thus, with 2 × oversampling of the baseband data and α = 1, the Nyquist bandwidth of the data will correspond with the I/Q Nyquist bandwidth. As stated earlier, this results in problems near the upper edge of the data bandwidth due to the roll-off attenuation of the half-band filters. The following diagrams illustrate the relationship between α and the bandwidth of raised cosine shaped pulses. The problem area is indicated by the shading in the tail of the pulse with α = 1, which extends into the roll-off region of the half-band filter. The effect of raised cosine filtering on baseband pulse bandwidth, and the relationship to the half-band filter response is shown in Figure 24. fNYQ 2*fNYQ f fIQ fNYQ 2*fNYQ f fNYQ 2*fNYQ f HALF-BAND FILTER RESPONSE 2 OVERSAMPLE RATE = 0 = 0.5 = 1 BANDWIDTH of I or Q DATA Figure 24. Effect of Alpha Programmable (2 –63 ) CIC Interpolating Filter The Programmable Interpolator is implemented as a CIC (Cascaded Integrator-Comb) filter. It is programmable by a 6-bit control word, giving a range of 2 × to 63× interpolation. This interpolator has a low-pass frequency characteristic that is compensated by the Inverse CIC filter. The Programmable Interpolator can be bypassed to yield a 1 × (no interpolation) configuration by setting the bit in the appropri- ate control register, per each profile. Whenever the Programmable Interpolator is bypassed (1 × CIC rate) power to the stage is removed. If the Programmable Interpolator is bypassed, the Inverse CIC filter (see above) is automatically bypassed, since its compensation is not needed in this case. The output of the Programmable Interpolator is the data from the 4 × interpolator upsampled by an additional 2× to 63×, accord- ing to the rate chosen by the user. This results in the input data being upsampled by a factor of 8 × to 252×. |
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