12.07.2015 Views

System Level Modeling and Optimization of the LTE Downlink

System Level Modeling and Optimization of the LTE Downlink

System Level Modeling and Optimization of the LTE Downlink

SHOW MORE
SHOW LESS
  • No tags were found...

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

3. Physical Layer <strong>Modeling</strong> <strong>and</strong> <strong>LTE</strong> <strong>System</strong> <strong>Level</strong> Simulationcan be ei<strong>the</strong>r a 2D or a 3D pattern. In <strong>the</strong> last case, it combines a horizontal <strong>and</strong>vertical component with an optional mechanical/electrical tilt [79].ˆ L pathloss : A distance-dependent pathloss between <strong>the</strong> transmitter <strong>and</strong> <strong>the</strong> receiver.ˆ L shadow : Shadow fading, which models slow-changing deviations from <strong>the</strong> averagepathloss values that model irregularities such as geographical features. Modeledas a zero-mean space-correlated lognormal distribution.ˆ |h r,t | 2 : Assumed to be a χ 2 distribution with a number <strong>of</strong> degrees <strong>of</strong> freedom N<strong>of</strong> two, as <strong>the</strong> underlying distribution <strong>of</strong> h is assumed to be circular symmetriccomplex normal with an average power <strong>of</strong> one.As <strong>the</strong> macro-scale parameters are scalars applied to all <strong>of</strong> <strong>the</strong> entries <strong>of</strong> <strong>the</strong> MIMOchannel matrix, it can be trivially decomposed into a normalized 3 channel matrix Hmultiplied by <strong>the</strong> factors L pathloss , L shadow , <strong>and</strong> G antenna . Applying <strong>the</strong> link budget<strong>of</strong> Equation (3.10) to Equation (3.9) we can rewrite Equation (3.9), expressing <strong>the</strong>subcarrier post-equalization SINR for layer i asγ i =ζ i P ′ L,0ξ i P ′ L,0 + ψ iσ 2 n +N int ∑m=1θ i,m P ′ L,m, (3.11)where PL,m ′ = P L,m · G antenna,m · L pathloss,m · L shadown,m , <strong>and</strong> <strong>the</strong> index m denotes <strong>the</strong>transmitting eNodeB (m = 0 for <strong>the</strong> target transmitter <strong>and</strong> m = 1, . . . , N int for <strong>the</strong>interferers).Decomposing <strong>the</strong> combined fading experienced over <strong>the</strong> link into a slowly-changingposition-dependent macro-scale component <strong>and</strong> a faster-changing small-scale [80]enables to model <strong>the</strong> fading as two separate <strong>of</strong>fline-computable components: oneposition-dependent <strong>and</strong> one time-dependent.3.1.1.2. On <strong>the</strong> <strong>Modeling</strong> <strong>of</strong> OLSM <strong>and</strong> <strong>the</strong> Block Fading AssumptionOver <strong>the</strong> course <strong>of</strong> this chapter, it has been stressed that block fading is assumed,i.e., unchanging channel conditions for <strong>the</strong> duration <strong>of</strong> a TTI, <strong>and</strong> this assumptionis applied to <strong>the</strong> calculation <strong>of</strong> <strong>the</strong> post-equalization SINR in Section 3.1.1.1.However, it is clearly mentioned in Section 2.2.1.2 that <strong>the</strong> OLSM transmit mode isbased on cyclically applying a set <strong>of</strong> precoders, as well as a shift <strong>of</strong> <strong>the</strong> signal, to eachmodulated symbol during one TTI. Thus, even if a constant channel is considered,<strong>the</strong> effective channel, i.e., <strong>the</strong> combination <strong>of</strong> <strong>the</strong> channel <strong>and</strong> <strong>the</strong> precoder is notconstant during a TTI due to <strong>the</strong> applied CDD <strong>and</strong> cyclical precoding.3 Through <strong>the</strong> course <strong>of</strong> this <strong>the</strong>sis, a normalized channel matrix refers to one in which all <strong>of</strong> itsentries have a mean power <strong>of</strong> one.31

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!