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2                                                 Transport aspects


            Figure 9-3 shows the measured symbol constellation and electrical spectra of regenerated LTE signals for
            the transmission before transmission and after transmission with a total optical path loss of 32 dB. From
            the  electrical  spectra,  the  SNR  decreased  due  to  the  optical  loss,  compared  with  that  for  the  optical
            transmission signal. However, it can be seen that all symbol constellations were clearly apparent for all
            modulation formats, even when the total optical path loss was 20 dB.


                                                      QPSK         16QAM          64QAM





                               Transmission signal






                                 Receiver signal


                              Total optical loss: 32dB

                                  40-km SMF
                                  20-dB VOA

                                                                                 G Suppl.55(15)_F9-3


                              Figure 9-3 – Measured symbol constellations and electrical spectra


            The measured EVM as a function of an additional loss after a 40 km-long SMF transmission is shown in
            Figure 9-4. According to "LTE; E-UTRA; BS radio transmission and reception" [b-3GPP TS 36.104], required
            EVMs of LTE transmitted signal at the BS for the modulation formats of QPSK, 16-QAM, and 64-QAM are
            ≤17.5, ≤12.5 and ≤8.0% r.m.s., respectively. From the measured EVMs and the requirements, it can be seen
            that 30 dB optical path loss, corresponding to 64 split, are acceptable, which has a margin of 7 dB for 64-
            QAM. For the modulation format of 64-QAM, the EVM at the optical path loss of 42 dB was degraded so
            much  due  to  small  power,  which  caused  loss  of  synchronization.  In  the  low  additional  loss  region,  the
            degradation of EVM was also observed. This is because nonlinearity of an electrical amplifier in the RoF Rx
            causes signal distortion of the received RoF signal. However, it is expected that these problems should be
            easily overcome by means of a power control of the received RoF signal, which is in general a common
            technique of optical transmission. From the above, it can be concluded that analogue RoF transmission
            over a typical ODN is feasible.























                                      Figure 9-4 – Measured EVMs vs. optical path loss


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