They are for the Ps in weak SQ regime and for separately quantized electron and positron in strong SQ regime.
As shown in the figure, the obtained energy of the coupled electron-positron pair - a positronium - is much smaller than the energy of separately quantized particles.
The fundamental differences between the physical properties of a Ps as well as separately quantized electron and positron in the case of Kane's dispersion law, in contrast to the parabolic case, were revealed.
Finally, Figure 5 represents the comparative dependences of ground-state energies on the QD radius in two QS regimes simultaneously: for Ps in weak SQ regime and for separately quantized electron and positron in strong SQ regime.
We consider two types of quantization: quantized feedback and quantized state.
For the sake of simplicity, the effect of path loss and shadow fading have not been taken into account since they are usually quantized and fed back separately.
Instead, a quantization scheme that does not necessitate the storage of analog values is proposed, where the relay separately quantizes the signals received in the first and second slot and then properly combines the quantized values.
The measurement signal is quantized by a logarithmic quantizer.
The measurement signal is quantized by a static logarithmic quantizer.
That is to say, information is quantized.
