Note the
current test configuration includes octoScope's MPE, which implements IEEE 802.11n/ac Model B.
The problem is that usually a propagation model shall simulate antennas plus propagation medium, which means the interface of the propagaion model is usually a (physical) RF connection (=conducted input/output)
But by picking up the DUT RF singals "wireless" via probe antennas, effectively a second model is put in series to the Octobox propagation model, which increases the (unhealthy) correlation between the MIMO pathes.
Means: DUT antenna 1 will couple to all 3 probe antennas, DUT antenna 2 will couple to all 3 probe antennas and so on,...while in a conducted setup this additional "mix-up" of the signals doesn't happen.
The air loss inside the test box can not only be seen as simple attenuator, but as a combination of attenuators and signal combiners.
The signal combining property will add additional correlation to the spatial streams which, depending on how strong the combining effect is, will more or less hurt the MIMO decoding, such that the link will more or less earlier switch from 3 stream to 2 stream and finally to single stream transmission.
(In my simplified audio metaphor:if left and right channel of a stereo signal are connected via a resistor (in extreme case 0-Ohms ) then the stereo effect is reduced, in worst case both channels carry the same "mono" signal and less information can be transferred accordingly)
As i wrote in my start posting: i experimented quite a bit with a similar setup, and by adjusting the DUT position in the box, it's easy to create cases, where full troughput isn't possible at all, because of the additional mixup and attenuation differences in the pathes (too much correlation). Then you move the probe antennas just by some degrees or some inches in the positon and suddenly ("digitally") the throughput is back to full rate, but still can be close to the "cliff" where little changes like increasing the attenuation immediately result in switching back to operate with lower number of spatial streams.
Therefore it's important to make the correlation (=signal combining inside the box) as small as possible = giving the probe antennas as much spacing as possible.
http://www.microwavejournal.com/articles/10835-mimo-ota-device-testing-with-anechoic-chambers
Each chamber is equipped with a number (usually 4, 8 or 16) of cross-polarized antenna pairs, all of which are fed signals via the channel emulator. Figure 2 illustrates the distribution of power across 8 probes of 6 multipath delays. Each probe has a vertical (top) and horizontal (bottom) element.
http://www.hindawi.com/journals/ijap/2012/615954.fig.001.jpg
As those systems are very costly, I have also been experimenting with another method, where the DUT is placed in the anechoic Box and (tiny) position variable probe antennas are located close as possible to the individual DUT antennas (fixed with adhesive tape on the housing)
This allows lowest possible correlation because of operating in the near field of the DUT antennas.
By observing the RF power on each probe antenna, it's possible to estimate the coupling loss as absolute value and also to make it equal for all streams by fine tuning the probe position.
If you have no power meter, a simple diode rectifier head connected to an oscilloscope will at least allow relative measurements within a 15 dB range.
This method is close to testing conducted, but has the advantage that it's not required to open the DUT and also any platform noise leaking into the DUT antennas is still fully taken into account.
Off course it's extra work to do this "probe-calibration" once for each product, but on the other side you save all the rotations and repetitions and the level accuracy will be much better than with the actual method.
What this method does not cover are the differences in antenna propagation properties.
However in such small chambers it's not possible at all to judge MIMO propagation properties, so in my eyes it's not a big disadvantage.
bonsai