Page 68 - ITU Journal Future and evolving technologies Volume 2 (2021), Issue 3 – Internet of Bio-Nano Things for health applications
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ITU Journal on Future and Evolving Technologies, Volume 2 (2021), Issue 3




          Two  methods  of  adaptive  threshold  detection  for  OOK   Further,  a  signal  detection  scheme  with  initial  distance
          transmission  were  proposed  in  [118].   The  adaptive   estimation was proposed in [137].  In this scheme,  a pi‑
          threshold calculation was based on determining the aver‑   lot  signal  was  released  before information  transmission
          age distance variation within a symbol interval.  The dis‑   which assisted to estimate the stochastic distance based
          tance was calculated using the diffusion equation (6). The   on maximizing the likelihood of the received signal in the
           irst adaptive detection scheme was based on a compari‑    irst step.  In the second step,  maximum likelihood esti‑
          son of received concentration with the adaptive threshold.   mation was used to  ind the initial distance by maximiz‑
          In this scheme, the adaptive threshold was selected as half   ing the likelihood function based on the PDF of distance.
          of the maximum value of the reconstructed signal during   Authors employed a MAP‑based detection scheme at the
          the interval where the last bit‑1 was detected.  Thus, the   receiver  and  based  on  this,  the  expression  for  optimal
          decision rule to detect the transmitted bit in the jth bit   threshold was obtained. Furthermore, an adaptive detec‑
          interval can be expressed as                         tion scheme for OOK modulation was proposed in [138],
                                                               where  the  decision  threshold  in  the  current  bit‑interval
                        {                                      was selected as the weighted sum of the received signals
                          1 if h j,peak ≥ h ∗,peak /2,
                   ˆ                                   (13)    in the previous two bit‑intervals.  The weights were ob‑
                   b j =
                          0 otherwise,                         tained by minimizing the error rate at the receiver nano‑
                                                               machine.  Also,  a  pre‑coding  scheme  was  presented  to
          where ∗ denotes the index of the last bit‑1 detected, and  combat ISI, where the transmitter scaled the number of
          h j,peak is the peak value of reconstructed signal using av‑  released  molecules  if  two  consecutive  bit‑1  were  trans‑
          erage distance between the transmitter and the receiver  mitted. The probability of error was further minimized to
          in jth bit interval.                                 determine the optimal scaling factor.  The proposed tech‑
                                                               nique outperformed the  ixed threshold technique and the
          The second detection scheme was peak time‑based de‑  one presented in [47] where the received signal in the pre‑
          tection in which the peak time of the current bit‑interval  vious bit‑interval was considered as an adaptive thresh‑
          was compared with 1.6 times the peak time of the recon‑  old.
          structed signal where the last bit‑1 was detected. More‑
          over, ISI mitigation was also performed by subtracting the  Optimal  LLR  based  decision  rule  was  derived  at  the  re‑
          reconstructed signals of previous bit‑intervals from the  ceiver  in  [139].  Based  on  the  derived  optimal  rule,  the
          total received signal in the current bit‑interval. Simula‑  probability of error with respect to the number of trans‑
          tion results demonstrated that these detection schemes  mitted  molecules  and  channel  capacity  with  increasing
          perform well if the coherence time of the channel is large,  external  interference  was  also  evaluated.  A  detection
          however they fail to give satisfactory performance if the  scheme  based  on  slope  values  within  a  symbol  interval
          coherence time is small (i.e., around 1‑bit interval).  was proposed in [140] considering OOK based transmis‑
                                                               sion at the transmitter. In this work, Einsteins’ law of dif‑
          To overcome the limitations of this work, another de‑
                                                               fusion was used to  ind the CIR. Moreover, the detection
          tection scheme was proposed in [136] in which mod‑
                                                               threshold was set to zero as the slope value was positive
          i ied concentration shift keying was used where some
                                                               for bit‑1 and negative for bit‑0.  Cell‑to‑cell communica‑
          molecules for bit‑0 were also transmitted. This could
                                                               tion  based  on  calcium  signaling  was  proposed  in  [141].
          help the receiver to  ind the distance using the diffusion
                                                               In this work, intra‑cellular and intercellular calcium sig‑
          equation even when bit‑0 was transmitted and the adap‑
                                                               naling  was  studied  for  mobile  cells  in  an  environment
          tive threshold was calculated based on the reconstructed
                                                               composed of cytoplasm.  Based on the external diffusion
          signals of previous bit duration unlike [118] where the
                                                               model of calcium,  the transmission of calcium‑based on
          threshold calculation based on the bit duration in which  concentration and waveform was also studied. Moreover,
          the last bit‑1 was transmitted. The detection rule in [136]  the decay of calcium signals in the environment and the
          is given by                                          number of activated cells as a percentage of sender cells
                                                              were analyzed.
                                    f 1,max (j−1,t)−f 0,max (j−1,t)
                1 if max(x r k ,k [j]) ≥              ;
          ˆ b j =                        ln  f 1,max (j−1,t)
                                          f 0,max (j−1,t)
                 0 otherwise.
                                                              The  work  in  [142]  studied  cluster  formation  by  a  set
                                                      (14)     of mobile nano‑machines using the attractant molecules.
                                                               This work considered that the angular movement of nano‑
          where x r k ,k [j] is the ISI mitigated signal in jth bit inter‑
                                                               machines  was  in  the  direction  of  the  maximum  concen‑
          val, r k  is the distance between the transmitter and the re‑   tration  gradient  and  the  concentration  sensed  by  nano‑
          ceiver at kth sample, f 1,max (j −1, t) and f 0,max (j −1, t) are   machines was governed by their sensitivity.  The number
          the peak values of the reconstructed signals for bit‑1 and   and size of clusters were shown to be controlled by the
          bit‑0 respectively in (j − 1)th bit interval. It is shown that   sensitivity  of  nano‑machines  to  the  concentration  of  at‑
          the detection scheme in [136] performs well for a coher‑   tractants. An MMC system for drug delivery was proposed
          ence time of ≈ 2‑bit duration.                       in [143] where drug carriers and diseased cells were con‑
                                                               sidered as transmitters and receivers, respectively.  Using
                                                               the  PDF  of  stochastic  CIR  and  the  reception  probability


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