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The fact that the LO operates at a higher frequency that the superheterodyne receiver47 causes larger coupling of the LO to the antenna port and therefore a larger LO reradiation However, the fact that the LO reradiation is in the center of the desired channel may translate into looser specifications imposed by the standard or the FCC If a band-select filter is not used between the antenna and the LNA, and depending on the choice of intermediate frequency, a superheterodyne receiver may have the most severe LO reradiation specifications However, if a band-select filter is utilized, the reradiated LO signal would be significantly attenuated by this filter With a band-select filter, a low IF receiver would probably impose the most stringent requirements on the LO reradiation specifications (since the frequency of the LO is quite high and the limited Q band-select filter cannot attenuate the LO signal).

If two measurements of the average laser frequency are made within a second or so of one another, then it is likely that the two values would be within 3 108 Hz (10 6 f0 ) of one another Over such a short time technical noise does not significantly shift the frequency of the laser However, increasing the time between the two measurements to 100 seconds allows sufficient time for temperature or current perturbations to take effect and can result in the two averages differing by as much as 1010 Hz (10 4 f0 ) as indicated in Figure 825 If optical feedback from a Fabry Perot etalon is used to stabilize the laser, a dramatic improvement in the short-term stability is observed Over longer time scales, however, the stability starts to degrade again because of changes in the etalon length and the spacing between the etalon and laser.

Stabilizing the laser with electronic feedback from an etalon does not produce the same reduction in short-term stability because of the inability of the servo loop to respond quickly enough to correct fast frequency fluctuations However, the servo loop does correct slower (1 s to 1000 s) drifts in frequency, improving the stability when averaged over those time scales Ultimately a stability limit over long time scales will be reached, that corresponds to the stability of the Fabry Perot stabilizing mode itself Since the cavity length of the etalon is also susceptible to environmental perturbations, any drift in it will be passed onto the laser frequency..

For the most part the same remedies can be applied to solving the DCoffset-related issues as well as the LO reradiation issues..

Ruling Distributed Dynamic Worlds, by Peter S. Sapaty ISBN 0-471-65575-9 Copyright # 2005 John Wiley & Sons, Inc.

The return value for a function call is in the EAX register. The jump instructions JL/JG are used in signed comparisons. The jump instructions JB/JA are used in unsigned comparisons.

10

5

Another set of receiver-related impairments are issues related to DC offsets and LO leakage. In some aspects these impairments are related, since the leakage of the LO into the input port of the mixer can cause DC offsets, while this same leakage into the antenna port can cause LO reradiation. Relatively small values of DC offsets can cause corruption of the baseband-modulated signal, while large values of DC offsets can cause the saturation of the following stages. On the other hand, LO leakage back to the antenna would cause reradiation of the LO, which may violate the standard s requirements or FCC requirements. In a direct-conversion receiver, this LO would typically be at the center of the receiver desired band. In a low IF or superheterodyne receiver, the LO would typically fall on an adjacent band or an entirely different band. In either case, these radiations would be governed by the standard or the FCC since they would cause interference with other users. Several ways by which DC offsets or reradiation can be created are shown in Figure 3.1. Coupling through path 1 would cause the LO to leak to the RF port of the mixer and can therefore create a DC offset. Coupling through path 2 is even more problematic than through path 1 since the LO at the RF port of the mixer is now amplified by the gain of the LNA and would therefore create DC offsets with larger amplitudes. A large received interfering signal as shown in path 3 can couple to the LO port and mix with it-