
 
range investigated is in between 400 nm and 100 
m, 
which covers a wide range of TN-RN distances for 
water medium as reported in (Mahfuz et al., 2010b). 
Finally, the effects of data rate on BER are shown in 
Fig. 7 such that BER increases as f increases. This is 
also due to the ISI caused by the temporal spreading 
of the channel when the input symbol changes at a 
higher rate. When f  increases the symbol duration 
decreases and as a result the receiver cannot cope up 
with the input signal to decode the transmitted bits 
correctly, and in addition, suffers from the ISI. The 
effects of ISI become more severe when f  increases 
further giving rise to BER of ~6% at f=0.01 bits per 
second (bps) to ~7% at f=1 bps when r  and  N  are 
kept fixed at 800 nm and 10 samples per symbol 
respectively. 
 
1 2 4  8  10
10
-2
10
-1
10
0
No. of samples per bit (N)
BER
 
Figure 5: Effects of number of samples per symbol (N) on 
BER when r=800 nm and f=0.01 bps. 
400 nm 1 um 10 um 100 um
10
-2
10
-1
10
0
r (nm)
BER
 
Figure 6: Effects of communication range on BER when 
N=10, f=0.01 bps. 
0.01 0.02 0.05 0.1 0.5 1
10
-1.19
10
-1.16
10
-1.13
f (bps)
BER
 
Figure 7: Effects of transmission data rate on BER when 
r=800 nm and N=10. 
4 CONCLUSIONS 
In this paper we have developed and evaluated the 
performance of sampling-based optimum receiver 
architecture of CEMC system. The proposed receiver 
model should be valid for any type of input signal 
transmission with any modulation format, e.g. pulse 
amplitude modulation (PAM) transmission, and can 
also be extended to detect signals with multilevel (M-
ary) amplitude modulation in CEMC system. 
Bionanomachines existing in the nature can sense the 
concentration of molecules at their receptors, which 
may help implement sampling-based receivers 
through engineering of bionanomachines. Finally, the 
results presented in this paper will surely help a 
molecular communication engineer to evaluate the 
performance of a CEMC system in greater details.    
REFERENCES 
Akyildiz, I. F., Brunetti, F. and Blazquez, C., 2008. 
"Nanonetworks: A New Communication Paradigm", 
Computer Networks Journal (Elsevier), vol. 52, pp. 
2260-2279.  
Atakan, B. and Akan, O. B., 2010. "Deterministic capacity 
of information flow in molecular nanonetworks", 
Nano Communication Networks, vol. 1, no. 1, pp. 31-
42.  
Berg, H. C., 1993. Random Walks in Biology, Princeton 
University Press, NJ, USA. .  
Bossert, W. H. and Wilson, E. O., 1963. "The analysis of 
olfactory communication among animals", Journal of 
theoretical biology, vol. 5, no. 3, pp. 443-469.  
Haykin, S., 2000. Communication Systems, 4th edn, John 
Wiley & Sons.  
Kay, S. M., 1993. Fundamentals of statistical signal 
processing, Vol. 2 Detection Theory, Englewood 
Cliffs, NJ: PTR Prentice-Hall. 
Mahfuz, M. U., Makrakis, D. and Mouftah, H. T. 2010a, 
"Characterization of Molecular Communication 
Channel for Nanoscale Networks", Proc. 
BIOSIGNALS-2010, pp. 327, Spain, 20-23 January.  
Mahfuz, M. U., Makrakis, D. and Mouftah, H. T. 2010b, 
"On the characterization of binary concentration-
encoded molecular communication in nanonetworks", 
Nano Communication Networks, vol. 1, no. 4, pp. 289-
300.  
Moore, M.-., Suda, T. and Oiwa, K., 2009. "Molecular 
Communication: Modeling Noise Effects on 
Information Rate", NanoBioscience, IEEE 
Transactions on, vol. 8, no. 2, pp. 169-180.  
Nakano, T., Moore, M. J., Fang Wei, Vasilakos, A. V. and 
Jianwei Shuai 2012. "Molecular Communication and 
Networking: Opportunities and Challenges", 
NanoBioscience, IEEE Transactions on, vol. 11, no. 2, 
pp. 135-148. 
 
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