Page 36 - ITU Journal Future and evolving technologies Volume 2 (2021), Issue 7 – Terahertz communications
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ITU Journal on Future and Evolving Technologies, Volume 2 (2021), Issue 7




          non-ideal  communication  symbols  in  the  time  domain,   A  compromise  between  these  two  extremes  allows  for
         which have experienced a nonlinear  phase  shift  due  to   high  bit  rates  with  higher  dispersion  tolerance  when
         GVD  in  the  atmosphere,  resulting  in  ISI  in  the  time   bandwidth and modulation order are properly balanced.
         domain.  At  this  point,  AWGN  is  added to  the  distorted   Note that the remaining combinations of bandwidth and
         symbol  sequence,  which  is  then  demodulated  and   modulation order fare quite poorly: a high bandwidth link
         compared to the original symbol vector to determine the   with  high  order  modulation  can  have  a  very  high  capa‑
         number  of  errors.  This  procedure  is  repeated  until   city  but  suffers  severe  ISI  due  to  simultaneously  high
         enough  iterations  have  run  to  ensure  the  errors  gene‑   dispersion  and  tight  decision  boundaries,  while  a  low
         rated are true to the stochastic distribution of the noise.   band‑width link with low modulation order has greatly
         Averaging the error rates observed on each iteration gives   reduced data capacity, defeating the purpose of terahertz
         the error rate of the link for that particular combination of   commu‑ nications.  An example of the simulation results
         distance,  bandwidth,  modulation  type,  and  atmospheric   that  led  us  to  these  conclusions  is  illustrated  in  Fig.  2,
         properties.                                           which  shows  the  bit‑error  rate  of  a  60  Gb/s  M‑QAM
                                                               communication link for  ive different modulation orders
          This simulation process has the advantage of abstracting   over 0 to 20 km.
          away much of the hardware, focusing on the mathemati‑
          cal, fundamental interactions between the data‑carrying   It  is  important  to  note  that  atmospheric  dispersion  is  a
          symbols  and  the  atmospheric  channel.  Notably,  it  also   cumulative phenomenon, meaning the greater distance a
          defines parameters such as received SNR directly prior to   signal propagates, the more dispersion accumulates and
          demodulation,  so  that  the  results  are  applicable  to  a   affects  that  signal.  It  is  also  important  to  note  that  no
          broad  range  of  physical  systems.  For  a  much  more   noise is added to the signal in Fig. 2, which allows us to
          in‑depth  description  of  the  simulation  process  using  a   con idently state that any change in error rates observed
          slightly  different  mathematical  convention,  readers  are   are  due  to  GVD  increasing  with  distance,  and  the  that
          referred to our previous  work  [26],  which  is  currently   differences  between  the  various  curves  are  due  to
          under  consideration  for  publication  at  the  time  of  this   changes  in  modulation  order  (which  affects  both
          writing.                                             bandwidth  and  symbol  spacing  on  the  constellation
                                                               diagram).  Even  in  the  absence  of  noise,  increasing
                                                               dispersion  over  distance  will  eventually  cause  some
          3.  RESULTS AND DISCUSSION                           communication  symbols  to  be  misinterpreted  by  the
                                                               receiver  for  all  modulation  types,  resulting in a bit error
          A principal result taken from our simulations is that GVD
                                                               rate that rises rapidly from insigni icance to some  inite
          can produce increasing SER in two opposing cases: when
                                                               value,  often  by  several  orders  of  magnitude  in  only  a
          low  bandwidth  and  high  order  modulation  is  employed   kilometer or two.
          and  when  high  bandwidth  and  low  order  modulation
          is  employed.  Moreover,  there  exists  an  optimum  trade‑   The  point  at  which  the  error  rate  jumps  from  insigni i‑
          off between modulation order and bandwidth that mini‑   cance to a  inite value is the uncompensated “dispersion
          mizes SER due to GVD for a particular desired data rate. In   limit” of that link, marked by vertical dashed lines in Fig. 2.
          order to clarify this point, we have chosen to conduct our   Beyond this limit, the error rate of the link cannot be con‑
          simulations such that data rate is held constant, whereas   tinuously  improved  by  increasing  the  SNR,  because  dis‑
          bandwidth  and  modulation  order  are  variable.  Further   persion is the dominant source of errors [26].  For the 60
          justi ication for this approach is offered later in the discus‑   Gb/s link shown in Fig. 2, BPSK has the lowest dispersion
          sion.  To elaborate on our results, the following relation‑   limit, meaning it is most severely affected by atmospheric
          ships between modulation order and GVD were found:   temporal dispersion.  4‑QAM, or QPSK, is next,  followed
                                                               by 256‑QAM, 16‑QAM, and  inally 64‑QAM. In other words,
          For  a  high  bandwidth  link  with  low  modulation  order,   the dispersion limit increases with modulation order for
         achievable  data  rate  is  high,  but  the  link  suffers  a  high   most of the modulation orders simulated, meaning there
         number of symbol errors because of the large frequency‑   is more robust operation as the bandwidth decreases.
         dependent  change  in  refractive  index  across  the  band‑
         width  (high  GVD)  causes  severe  ISI,  large  enough  to   The  results  and  discussion  presented  so  far  may  seem
         push  received  symbols  across  the  broadly‑spaced  deci‑   obvious  and  well‑established.  It  is  well‑known  that  de‑
         sion boundaries used in low‑order modulation types.   creasing the bandwidth of a wireless link operating in a
                                                               frequency‑selective environment will increase the perfor‑
          For a low bandwidth link with high order modulation, the   mance of the link by ” lattening” the fading pro ile of the
         achievable  data  rate  is  equally  high,  but  the  link  still   channel,  thereby  reducing  errors,  ISI,  and  the  comple-
         suffers  a  high  number  of  symbol  errors  due  to   xity  of  signal  processing.  The  atmosphere  is  a  frequency‑
         dispersion.  This  time,  the  errors  are  not  because  of  a   selective channel over the huge bandwidths available to
         large frequency dependency  in  the  narrow  channel,  but   terahertz  communication  links,  so  it  may  not  initially
         because decision boundaries are so tightly spaced on the   seem  surprising  that  as  we  decrease  the  bandwidth  we
         constellation diagram that even the small amount of GVD   also  observe  an  improvement  in  error  rate.  However,
         exhibited  by  the  channel  is  enough  to  push  received   closer  inspection  of  the  data  reveal  additional  and
         symbol values across them, again causing ISI.         unexpected  behaviors  that  are  not  readily  explained


          24                                 © International Telecommunication Union, 2021
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