Visible Light Communication based on Chaos Encryption Scheme
HUDA KADHIM RUMUH, IBRAHIM ABDULLAH MARDAS
College of Engineering, Electrical Engineering,
Babylon University,
Babylon,
IRAQ
Abstract: -To accommodate extremely high levels of data traffic, today's communications networks are
undergoing several different technical transformations. In addition to the already present video and voice
services, newly created technologies and applications, such as internet services, interactive gaming, and
telemedicine, are adding to the already tremendous amounts of traffic and vulnerability generated. The
semiconductor laser chaos generation is now being utilized to improve data security and protect data from theft
during its transmission from the transmitter to receivers a means of concealing multi-level data signals to
address these concerns regarding data security. The incoming signals are concealed before the optical chaotic
signal's transmission via the optical fiber medium by our suggested method, which makes use of the double
delay feedback technique to create the optical chaotic signal. The additive chaos masking system is utilized to
execute the mixing of incoming signals with chaos. This method demonstrates several valuable qualities,
including simplicity and the ease with which a message may be recovered. To explore the propagation concerns
that are related to secure signal transmission, chaotic data, which is a combination of incoming signals and
random noise, is transmitted via the medium of optical fiber. To properly regulate the linear impairments of
optical fiber, which is required for the efficient transmission of a secure signal, the plan is put into action for
long-haul communication to facilitate the long-distance transfer of data. Adjustments are made to the
parameters on both the transmitting and receiving ends to achieve synchronization between the two processes.
This is done in such a way that the received signal may be restored to its original state by subtracting the
broadcast signal from the same chaos on the receiving side. Obtaining Q-factors allows the method to be
evaluated for a variety of optical fiber cable lengths, during which the Q-factors serve to evaluate the quality of
the signal that is received.
Key-Words: - Semiconductor laser, chaotic signal, double delay, Mach-Zehnder Modulator(MZM),
optoelectronic feedback, opt electric oscillator.
Received: April 22, 2023. Revised: February 15, 2024. Accepted: March 15, 2023. Published: May 27, 2024.
1 Introduction
This study presents the method for secured
communication in Optisystem software by making
use of a chaotic laser. Spread spectrum signals are
used in chaotic communication; these signals make
use of a vast bandwidth and have a low power
spectrum density. [1], to supply the security data
signal, the chaotic masked signal is utilized. Using
chaotic modulation, the message is first encrypted
when it is sent from the sender to the receiver, and
then it is decrypted when it is received, [2]. As
comparative metrics, the Q factor and the BER are
employed, [3]. The Q-factor is the minimum optical
signal-to-noise ratio required to achieve a specific
bit error rate. Optical fiber cable is currently the
suggested choice for data transfer, with less noise
interference, and a longer transmission range
because of its high bandwidth. Furthermore, because
chaos-based optical communication systems have
better security features than traditional cryptography
techniques, they offer improved security, [4].
The physical layer of the Open System
Interconnection (OSI) architecture has advantages in
terms of easier installation, streamlined key
management, and flexibility for digital signal
processing, [5]. There are two types of chaos-based
communication in the physical layer: data
encryption in the electrical domain using techniques
like exclusive OR scrambling, optical key
distribution, chaotic laser communication, and
optical steganography, and data encryption in the
optical domain using fractional Fourier transform
and piecewise chaotic permutation, [6].
In the case of encryption using the electrical
domain, the finite precision of the computer restricts
the high unpredictability of chaotic sequences, [7].
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Optical chaos for secure communication may be
further subdivided into two forms, depending on the
transmission channel. These two categories
comprise wireless communication technologies
including free space optics (FSO) and optical
wireless communications (OWC) as well as optical
fiber communication, [8], [9]. One of the types is
communication through optical fiber. There are
three different ways to hide messages inside the
chaos of an optical communication system: Additive
chaos masking (ACM), also known as chaos
modulation (CM), or chaos shift keying (CSK),
[10]. [ACM] stands for additive chaos masking;
CSK stands for chaos shift keying; and CM is for
chaos modulation. These three distinct strategies
each have their own set of advantages and
disadvantages; nevertheless, in the model that we
have presented, we have decided to use ACM
because of its ease of use, its ability to easily
recover messages, and its implementation in
Optisystem software version 14.0, [11]. In Figure 1,
which depicts our suggested security
implementation via the ACM method, as you can
see, both the transmitting and receiving sides are
equipped with two chaotic systems that are rather
comparable to one another. The first data signal,
represented by d(t), is covered up by the chaotic
signal, denoted by c(t), which is produced at the
transmitting end using the double delay feedback
method. This is done to form a secure signal,
denoted by s(t), which is then sent through the
optical fiber channel. We take advantage of a
technique known as direct modulation, in which the
semiconductor laser and a current source are
connected, to produce optical chaos through a
chaotic laser, [12]. To generate chaos with the
characteristics that are wanted, the settings of the
current source and the semiconductor laser are
altered. This signal (s(t)) serves as noise for
potential intruders and conceals the original data
(d(t)) in its transmissions, [13]. The signal, denoted
by s(t), is then sent across the channel and is
followed by the subtraction of another chaotic
signal, denoted by c(t), which is analogous to s(t)
but is instead produced by a second chaotic
semiconductor laser that is positioned at the
receiving end. Because all of the parameters of the
second chaotic laser are maintained in the same
manner as the parameters of the transmitting laser,
the subtraction formula may be utilized to
successfully extract the initial data (d(t)), [14]. The
two chaotic lasers need to have identical properties,
but synchronization between them is also an
essential goal to work toward. It just takes a very
slight misalignment between these lasers for this
plan to be rendered completely ineffective.
Fig. 1: A layering of additive chaos as a mask.
2 Related Work
Over the past few years, numerous researches have
been carried out to develop communication systems
for securing data. These studies have explored
various approaches and techniques to enhance
security with a low error rate. In this section, we will
discuss some notable works that have contributed to
the field.
In 2018, [15], research suggests that semi-
conductor lasers are used to emulate chaotic lasers
to reliably convey messages. To solve data security
problems, semi-conductor laser chaos creation is
being used to hide multi-level data signals. Dual
binary modulation offers higher spectral efficiency
than NRZ, RZ, and other modulation methods and
optimizes bandwidth to increase channel capacity.
Thus, it is crucial to encrypt communication
delivery. The chaotic laser processed safe dual
binary signal transmission in the optical
communication network. Synchronize to get eye
diagrams and quality. Simulation analysis was done
with Optisystem 15.0. Using a chaotic laser, the
optical communication network's transmitter and
reception were synchronized. Before
synchronization, the dual binary modulated signal is
sent across SMF fibers of various lengths and DCF
fibers to reduce dispersion. After 70 km, the received
signal's Qfactor declined to 4.64 from 25.47 at 10
km fiber length.
In 2019, [16], authors used optics in a remote
health monitoring system to protect EEG signals
over an optical fiber link. They use a semiconductor
laser source to create optical chaos to hide an EEG
signal before transmitting it across an optical wire.
This happens before signal transmission. The 14-
channel Emotive headgear collects EEG data, which
are analyzed and rescaled for the experimental
context (Optisystem). The additive chaos masking
approach, which boasts fast message retrieval and
simplicity, is used to combine EEG signals with
chaos to achieve the desired effect. For different
optical fiber cable lengths, Q-factors can be used to
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evaluate signal quality. They found that the received
signal's Qfactor dropped to 5.72 from 66.67 at 5 km
fiber length after 120 km.
In 2021, [17], they successfully implemented
security. Their research report focuses on the
implementation of a Radio-over-Fiber (RoF)
network in the context of 5G front haul. The three
most widely used approaches are CSK, CM, and
CMS. CMS is the most cost-effective and user-
friendly option. The initial phase of the study
confirms the security of the RoF signal by
employing optical time domain and spectrum graphs
with the use of optical time domain visualizers and
analyzers. In the second portion of the paper, laser
power and fiber lengths are varied to evaluate
system performance. The absence and presence of
linear impairments are used to measure system
performance.
Results demonstrate that the system functions
well up to 15 km of fiber length with 10 Gbps data
throughput and security features. By boosting laser
power to 20 dBm, BER decreases considerably.
However, linear impairment control is essential for
optimal RoF signal quality.
In 2023, [18], they demonstrated Optisystem
7.0's chaos-based secure fiber-optic communication
system. Standard single-mode fiber transmits a 10
Gb/s externally modulated signal across 100
kilometers. Changing semiconductor laser rate
parameters generates a chaotic optical signal that
hides modulated data. Chaos diminishes the
efficiency of the system and limits the transmission
range to 70 kilometers. Signal dispersion is
mitigated via a chirped Fiber-Bragg grating with an
erbium-doped fiber amplifier, which increases
transmission distance to 104 km (80%). Data was
retrieved at the receiver with a maximum Q-factor
of 4.2 and a minimum bit error rate of.
In 2023, [19], an optical chaotic system was
created and tested using OptiSystem software to
evaluate its performance under different weather
situations. The system is a secure hybrid
combination of free space and fiber optic (FSO/FO)
technology. The chaotic signal conceals the message
within this highly secure communication
mechanism. This security solution is potentially
superior to encryption techniques. By incorporating
the chaotic signal into the message, the link distance
is decreased by 100 kilometers regardless of
weather conditions. Under all circumstances, the use
of dual Free-Space Optical (FSO) channels
enhances the link distance by a significant margin of
37-40%.
3 Proposed Methodology
In our plane, we make use of chaos masking to
accomplish both high data rate and security at the
same time. To provide a more chaotic pattern of
activity, the created chaos has a pulsing quality.
Fig. 2: The plan that we have developed is to
introduce chaos to the incoming signals
In Figure 2 the input signal is fed and pre-
processed into an MZM rectifier our suggested plan
for the security of the communication system
through optical chaos. The MZM rectifier modulates
the input signal using the light beam produced by
the CW laser. To transmit the signal with less
attenuation loss, the CW laser's frequency is set to
500THz. To enable the modulation of the input
signal with the laser light, the extinction ratio of the
MZM—defined as the ratio of two levels of optical
power to the digital signal produced by the laser—
was set at 50:50. The chaotic semiconductor laser's
optical output was then provided to the MZM,
where it was combined with this waveform. The
semiconductor laser's operating frequency was
maintained at approximately 500THz, allowing the
two waveforms—the light produced by the input
waveform modulated by the CW laser and the chaos
produced by the semiconductor laser—to be
properly mixed. Over a single-mode fiber, the
optical adder output is sent after the input signal has
been made safe in the optical field, [14]. On the
receiving side, a signal was removed from a
comparable chaos that was produced using double
delay feedback techniques before the optical
receiver or signal was detected by the photodiode.
The first location where the signal was detected was
the optical receiver, whose function was to
transform the signal from the visual field to the
electric field. A low-pass filter was then employed
to further lessen the impact of noise and recover the
input signal, [20].
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4 Generating Chaotic Signal
Generating Chaotic signals by using a double delay
feedback system:
Optical detection, encrypted communication, and a
variety of other applications make regular use of
chaotic lasers for a variety of reasons, including
their cacophonous chaos, exceptional anti-jamming
capabilities, and other advantages. Within the scope
of this study is an investigation of the chaotic laser's
efficiency at a cheap cost. It has been seen how well
a semiconductor laser functions with double delayed
feedback in the course of an experimental study
conducted with the OPtiSystem simulator. The
characteristics of this laser have also been
established. Initially, the Mach-Zehnder modulator
(MZM) was constructed by sending the chaotic laser
output back into the system. The system
incorporates a second time delay in addition to the
adjustment of the dynamic gain coefficient. We
study the enhanced chaotic system's feedback
duration and intensity under various input bias
current, frequency, and modulation beak current
circumstances. The optoelectronic oscillator's
(OEO) chaotic laser output is more complex and
exhibits lower delay characteristics, according to
the bifurcation diagram. These revelations were
made, [21].
Fig. 3: Schematic for an OEO chaotic system with
double delay feedback, [22]
Figure 3 depicts the chaotic system with a
double feedback strategy. Figure 3, PD is a
photodetector with a specific effect amplifier; LD is
a continuous light laser; The MZM modulator is
driven by a frequency (RF) driver; OC1 and OC2
are couplers; OC2 Light divides the MZM output
into two; and finally, the RF and PD driver leads to
the MZM optoelectronic reflection feedback. From
the EDFA to the MZM optical feedback, the laser
output is chaotic and has the power of Pout thanks
to the MZM, [22].
Equation (1) represents the output property of
the nonlinear device MZM of the OEO chaotic
system with double delay feedback:
  [󰇛󰇜


] (1)
where VRF stands for the RF half-wave voltage,
VDC for the bias half-wave voltage, and V (t) for
the load on the MZM modulation voltage. The input
optical power is shown by pin.
The development and simulation of an optical
chaos-producing circuit with double delay feedback
is accomplished with the help of the OptiSystem 16
software. Additionally, OptiSystem may be
understood as a software package for optical
communication devices. This software package
gives users the ability to develop, test, and simulate
optical links in the transmission layer of
sophisticated optical networks. Figure 4 depicts the
simulated circuit architecture of the proposed
method, which makes use of built-in components
and adheres to the appropriate standards. A MZM,
amplifier, and photodetector (PD) are the
components that make up this device. The MZM
may be characterized as a device that is employed
for the determination of the relative phase shifting
between two collimated beams from a coherent
source of the light either by altering the length of
one of the arms or by inserting a sample in one of
the beams' pathways. This can be accomplished in
one of two ways: either by changing the length of
one of the arms or by placing the sample in the path
of one of the beams. MZM comes with two input
ports as well as two output ports. Two couplers are
utilized in the construction of a basic MZM. One
coupler is located at the input and functions as a
splitter, while the second coupler is located at the
output and performs the duty of a combiner, [22].
Fig. 4: The simulated diagram of a chaotic system
(sub-system)
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Light is shown to be coupled into two
interferometer arms by an input coupler in Figure 4,
and then recombined at an output-by-output coupler.
The coupler produces two beams of light, each of
which is equally strong, but only one of these is
amplified by EDFA. After that, it is linked with the
static fixed power laser that is generated by the
continuous laser, and it is then entered into the
MZM for a second time to carry out non-linear
modulation and make chaotic lasers. The second one
goes from the feedback arm (MZM) into the
photodetector (PD) to transform an optical signal
into an electrical signal. The photodetector is
connected to the amplifier, which is subsequently
coupled to the MZM feedback arm. Because the
length of the optical channel along each of the two
arms is different from one another, the phase shift
that occurs as a result of the delay is a function of
the wavelength of the input signal. Studies have
been conducted to investigate the effects of MZM
bias voltage on the chaotic behavior of OEFB. The
output of the optoelectronic oscillator is sent back to
the MZM over a delayed optical channel. This
causes the gain coefficient of the original OEO to be
dynamically altered, and it also adds an extra time
delay to the system, which causes it to produce a
more complicated and chaotic laser signal. The
aforementioned features help construct a chaotic
secure communication system that offers a better
level of protection. The variation in the bias current
and modulation peak current leads to the complexity
chaotic to change. Table 1 shows the input
parameters for generating the chaotic signal. With
the decrease in the value of bias current, clear
variation in the amplitude of pulses can be observed
that is mean, chaotic behavior increased and the
opposite happens with modulation peak current.
Table 1. Semiconductor laser Parameter of Chaotic
Signal
parameter
value
Frequency
190 THz
Power
10 dBm
Bias current
70 mA
Modulation beak current
40 mA
Threshold current
33.45723 mA
Threshold power
0.01516 mW
Frequency of current source
5 GHz
Amplitude
1 a.u
Phase
90 Deg
5 Result and Discussion
Simulations are performed with varying the length
of the channel, the data rate of the system, and the
power of the laser to perform an evaluation of the
proposed setup. Since the NRZ pulse format is more
efficient than the RZ format, we have chosen to use
it. Figure 5 presents the encoded message that was
received at a rate of 10 gigabits per second without
any noise.
Fig. 5: Input encoded message
A continuous wave laser with an operating
frequency of 500THz and a laser strength of 10
dBm is what is utilized here. In Figure 6, you can
see the chaos that was created by the chaotic laser
diode. The chaos that is produced in this method is
exceedingly unpredictable and has amplitudes that
are completely random. The disarray seen in Figure
6 may be utilized to conceal the information
displayed in Figure 5.
Fig. 6: Generated chaos
In the subsequent stage of our simulation model,
optical adders are utilized to conceal the incoming
signal within the produced chaos. Following the
chaotic masking strategy allows for the mixing of
both signals to take place within the optical domain.
The intensity of the chaotic laser is adjusted to 10
dBm so that it may produce pulses with greater
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amplitudes in comparison to the level of the
message's amplitude. In addition to this, it is capable
of fully encrypting the message while operating at
500 THz. Figure 7 illustrates a time domain signal
that the invaders are unable to comprehend in any
way. A person who does not have the appropriate
information and understanding of the created
chaotic signal is unable to recognize the original
message signal that was transmitted from the
transmitting end, as seen in Figure 7. This can be
seen quite clearly in Figure 8. This ensured that our
signal would not be intercepted by unauthorized
parties and offered an adequate level of protection
against potential invaders.
Fig. 7: Input message embedded in chaos
Analysing the signal in the frequency domain is
another method that may be utilized to do an effect
analysis of adding a security feature to an input
message. To accomplish this goal, an optical
spectrum analyzer is utilized. The change in the
optical spectrum is seen in Figure 8 both before
adding and after the subtraction of chaos to the
signal. To reiterate, the intruder is unable to
decipher the real information in the frequency
domain.
At the receiving end, the chaotic signal that was
found to have been contaminated with the official
signal was removed from the similar chaos that had
been generated by the second semiconductor laser.
The signal was picked up by the photodiode, which
then transformed it into a signal that was analogous
to the signal that was initially coming in. To further
purify the signal that was received, a low-pass filter
was used. The unaltered and deciphered versions of
the incoming signals are shown in Figure 8(a) and
Figure (b), respectively. We determined the signal's
Q-factor by measuring it (Figure 9) in preparation
for long-distance transmission. We found that when
the fiber lengths increased, the Q-factor dropped by
a significant amount.
(a) : Before the addition of chaos, the optical
spectrum of the input signal.
(b): After the addition of chaos, the optical spectrum
of the input signal
Fig. 8(a) and (b): Before and after the addition of
chaos, the optical spectrum of the input signal
Fig. 9: The relationship between the Q factor and
channel length
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The next step involves calculating the bit error
rate (BER) of the system against various lengths of
optical fiber. Controlling the effects of dispersion
and attenuation is required in order to carry out
simulations. The results are displayed in Figure 10,
which demonstrates that the system functions well
up to a channel length of 4 km. After that, an
exponential increase in bit error rate is detected,
which suggests that it is feasible to recover the
signal that was originally broadcast, although with
errors. Since the suggested system is optimized for
10 Gbps, it can function satisfactorily up to a fiber
length of 4 km because of this. An increase in the
data rate will cause the channel lengths to be
reduced to their lower limitations.
Fig. 10: Evaluation of performance (which is based
on BER vs. length)
Table 2. RESULT of the simulation of Proposed
double delay feedback with data rate (10Gbps)
Channel Length
Q factor
100 m
19.7411
200 m
19.595
500 m
10.4998
1000 m
10.52
2000 m
10.503
4000 m
10.5034
The results of a comparison of the bit error rate
and the Q-factor for various fiber lengths are
presented in Table 2. After researching the bit error
rate as well as the Q factor for fibers of varying
lengths, the researchers concluded that the bit error
rate was growing with the rising fiber lengths. On
the other hand, the Q-factor decreased when the
length of the fiber was increased. This nonlinear
degradation, such as an amplifier and fiber non-
linearity, is to blame for the dramatic fall in Q-factor
that occurs with an increase in fiber length. Noise in
the transmission channel, interference, distortion,
issues with bit synchronization, and attenuation are
all potential factors that might impact the bit error
rate.
6 Conclusion
We suggested a method for the safe transmission of
input signals that makes use of light that is visible to
the human eye. The procedure of double delay
feedback was employed to generate chaos, wherein
the parameters were adjusted to get the desired
bandwidth and amplitude. Subsequently, this
disorder was integrated with incoming signals that
had been altered by continuous-wave (CW) laser
light before transmission through a single-mode
optical fiber. The investigation and testing focused
on the characteristics of chaos that obscure the
incoming signal, to facilitate long-distance
communication. The different lengths were
deliberately selected with this objective in mind.
Analyzed in both the frequency and temporal
domains, the installation of security measures in the
input signal was verified. An optical subtractor was
employed to distinguish the incoming signals from
the noise. Based on our inquiry and comparison
with previous research, the QFactor of the received
signal decreased to 10.5034 when the channel length
was 4 kilometers, whereas it was 19.7411 when the
channel length was 100 meters. These findings
demonstrate favorable outcomes in comparison to
prior research and the utilization of visible light
technology. This technology is commonly employed
in short-range underwater communications, the
Internet, healthcare facilities, and various other
applications.
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WSEAS TRANSACTIONS on ELECTRONICS
DOI: 10.37394/232017.2024.15.7
Huda Kadhim Rumuh, Ibrahim Abdullah Mardas
E-ISSN: 2415-1513
61
Volume 15, 2024
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Contribution of Individual Authors to the
Creation of a Scientific Article (Ghostwriting
Policy)
- Huda Kadhim has implemented the simulation in
optisystem.
- Ibrahim Abdullah has supervised on the paper.
Sources of Funding for Research Presented in a
Scientific Article or Scientific Article Itself
No funding was received for conducting this study.
Conflict of Interest
The authors have no conflicts of interest to declare.
Creative Commons Attribution License 4.0
(Attribution 4.0 International, CC BY 4.0)
This article is published under the terms of the
Creative Commons Attribution License 4.0
https://creativecommons.org/licenses/by/4.0/deed.en
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WSEAS TRANSACTIONS on ELECTRONICS
DOI: 10.37394/232017.2024.15.7
Huda Kadhim Rumuh, Ibrahim Abdullah Mardas
E-ISSN: 2415-1513
62
Volume 15, 2024