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<article article-type="research-article" dtd-version="2.3" xml:lang="EN" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">
<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Phys.</journal-id>
<journal-title>Frontiers in Physics</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Phys.</abbrev-journal-title>
<issn pub-type="epub">2296-424X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">731405</article-id>
<article-id pub-id-type="doi">10.3389/fphy.2021.731405</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Physics</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>A Cost-Efficient RGB Laser-Based Visible Light Communication System by Incorporating Hybrid Wavelength and Polarization Division Multiplexing Schemes</article-title>
<alt-title alt-title-type="left-running-head">Xiang-Peng</alt-title>
<alt-title alt-title-type="right-running-head">A Cost-Efficient RGB Laser-Based VLC System</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Xiang-Peng</surname>
<given-names>CAI</given-names>
</name>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1386795/overview"/>
</contrib>
</contrib-group>
<aff>Navigation college, Quanzhou Normal University, Quanzhou, <addr-line>Fujian</addr-line>, <country>China</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>
<bold>Edited by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/983271/overview">Santosh Kumar</ext-link>, Liaocheng University, China</p>
</fn>
<fn fn-type="edited-by">
<p>
<bold>Reviewed by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1389233/overview">Muhammad Saadi</ext-link>, University of Central Punjab, Pakistan</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1389237/overview">Jawad Raza</ext-link>, National College of Business Administration and Economics, Pakistan</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: CAI Xiang-Peng, <email>cxp263263@163.com</email>
</corresp>
<fn fn-type="other">
<p>This article was submitted to Optics and Photonics, a section of the journal Frontiers in Physics</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>26</day>
<month>08</month>
<year>2021</year>
</pub-date>
<pub-date pub-type="collection">
<year>2021</year>
</pub-date>
<volume>9</volume>
<elocation-id>731405</elocation-id>
<history>
<date date-type="received">
<day>27</day>
<month>06</month>
<year>2021</year>
</date>
<date date-type="accepted">
<day>05</day>
<month>07</month>
<year>2021</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2021 Xiang-Peng.</copyright-statement>
<copyright-year>2021</copyright-year>
<copyright-holder>Xiang-Peng</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these&#x20;terms.</p>
</license>
</permissions>
<abstract>
<p>Visible light communication (VLC) has been proven a promising technology to counter the limitations of radio frequency (RF) communication technology such as high interference and high latency issues. VLC offers high bandwidth as well as immunity to interference from other electromagnetic spectrums. Due to these features, VLC can be an excellent solution for biomedical and healthcare applications for transmission of body sensor signals and other crucial patient information. In this work, a highly efficient VLC system is designed to transmit six channels, with each one carrying 10&#xa0;Gbps of data, over a 500&#xa0;m optical fiber link and a 200&#xa0;cm VLC link. To make the VLC system cost effective, simple and efficient on-off keying (OOK) (non-return to zero) is used as the encoding scheme. Moreover, to further enhance the capacity and bandwidth of the proposed VLC system, hybrid wavelength division multiplexing (WDM) and polarization division multiplexing (PDM) schemes are incorporated by using red, green, and blue lasers. The reported results show the successful transmission of all channels (6 &#xd7; 10&#xa0;Gbps) over 500&#xa0;m optical fiber and 200&#xa0;cm of VLC&#x20;link.</p>
</abstract>
<kwd-group>
<kwd>visible light communication</kwd>
<kwd>wavelengh-division multiplexing (WDM)</kwd>
<kwd>polarization division multiplexing (PDM)</kwd>
<kwd>on off keying</kwd>
<kwd>biomedical application</kwd>
</kwd-group>
</article-meta>
</front>
<body>
<sec id="s1">
<title>Introduction</title>
<p>Incessant demand of higher data rates and multifold user support in existing networks has forced researchers to look beyond radio frequencies (RF), which are bandwidth-limited, toward optical wireless systems (OWC) that offer nearly unlimited bandwidth (&#x3e;400&#xa0;THz) via mounting an infrared and ultraviolet region of the electromagnetic spectrum [<xref ref-type="bibr" rid="B1">1</xref>]. Among different employed OWC systems, the visible light communication (VLC) system stands out as an apt future solution for terrestrial communication due to its ubiquitous influence and as light-emitting diodes (LEDs) are readily engaged in innumerable commercial applications ranging from lighting systems to multimedia display units in offices as well as homes, vehicles, and mobile phones. The VLC system offers innumerable features that consist of energy-efficient operation, higher data rates, zero RF or electromagnetic interference, and a physical layer of data security [<xref ref-type="bibr" rid="B2">2</xref>, <xref ref-type="bibr" rid="B3">3</xref>]. Even with so many advantages, LEDs have a limited data rate due to strong internal polarization fields in common c-plane LEDs and hence are not considered suitable for higher speeds (in the gigabit range) [<xref ref-type="bibr" rid="B4">4</xref>&#x2013;<xref ref-type="bibr" rid="B6">6</xref>]. Newly developed micro-LEDs offer a higher data rate in the order of 3&#xa0;Gbps, but due to low illumination levels their use as light sources is not appropriate [<xref ref-type="bibr" rid="B7">7</xref>, <xref ref-type="bibr" rid="B8">8</xref>]. On the other hand, laser diodes (LDs) have a high modulation bandwidth and high output power that allow them to be better candidates for proposing an optimum solution in a high-speed and long-reach VLC system [<xref ref-type="bibr" rid="B9">9</xref>]. Hu et&#x20;al. displayed a VLC link with the link range of 300&#xa0;m by using a 650-<italic>nm</italic> laser diode and data rate of 10&#xa0;Mbps [<xref ref-type="bibr" rid="B10">10</xref>]. Another group of researchers reported construction of a WDM-VLC system over a link range of 10&#xa0;m using red and green lasers with a 500&#xa0;Mbps data rate [<xref ref-type="bibr" rid="B11">11</xref>]. Another work reported using a 450-nm laser diode and QAM-OFDM-based VLC over a range of 5&#xa0;m for a data rate of 9&#xa0;Gbps [<xref ref-type="bibr" rid="B12">12</xref>]. Wei et&#x20;al. [<xref ref-type="bibr" rid="B13">13</xref>] demonstrated a RGB laser diode-based VLC system over a bidirectional 1&#xa0;m. Yeh et&#x20;al. [<xref ref-type="bibr" rid="B14">14</xref>] demonstrated a 1,250&#xa0;Mbps VLC system using a yellow phosphorous LD over a range of 1&#xa0;m. Advanced modulation formats such as OFDM or QAM used with VLC systems are proved to be better in terms of high data rate but with increased cost and complexity of the system. In order to keep the system at minimal cost, on-off keying (OOK) is proved to be efficient in terms of low complexity and cost effectiveness. In 2016, researchers demonstrated a 2-m VLC link with a data rate of 266&#xa0;Kbps using OOK [<xref ref-type="bibr" rid="B15">15</xref>]. In 2017, Lu et&#x20;al. reported a GaN-based VLC system employing NRZ-OOK with a 600&#xa0;Mbps data rate over a transmission range of 0.6&#xa0;m [<xref ref-type="bibr" rid="B16">16</xref>]. For harnessing VLC with indoor white lightning, a new type of red, green, and blue (RGB) LDs are employed. In 2011, researchers reported highly bright white light generated from LDs by mixing red, green blue, and yellow light components [<xref ref-type="bibr" rid="B17">17</xref>]. To enhance data rate, researchers have employed various multiplexing techniques namely wavelength division multiplexing (WDM), multiple input multiple output (MIMO), and polarization division multiplexing (PDM). In 2015 [<xref ref-type="bibr" rid="B18">18</xref>], Tsonev et&#x20;al. proposed a 100&#xa0;Gbps system using an RGB LD-based WDM-VLC system by using 36 parallel data streams. Chi et&#x20;al. [<xref ref-type="bibr" rid="B19">19</xref>] in 2016 proposed and demonstrated an RGB LED-based VLC system with a PS-Manchester and WDM scheme with a data rate of 3.35&#xa0;Gbps and a 1&#xa0;m indoor transmission range. Another study in 2017 [<xref ref-type="bibr" rid="B20">20</xref>] proposed a WDM-based VLC system over a 1&#xa0;m span with a data rate of 4.05&#xa0;Gbps. Recently in 2020 [<xref ref-type="bibr" rid="B21">21</xref>], Messa et&#x20;al. experimentally demonstrated detection of a WDM-VLC signal via a single photodiode with the use of MIMO signal processing. These studies conclude that implementation of RGB-LD-based WDM-VLC can significantly enhance system performance. For further enhancement of the capacity of the proposed system, another multiplexing technique is proposed such as the PDM technique. In 2015 [<xref ref-type="bibr" rid="B22">22</xref>], Kwoon et&#x20;al. experimentally demonstrated enhancement of data rate up to 2.04&#xa0;Gbps by employing the PDM scheme in the VLC system. Hsu et&#x20;al. in 2018 [<xref ref-type="bibr" rid="B23">23</xref>] demonstrated an OFDM-PDM based VLC system with a data rate of 1.4&#xa0;Gbps. Recently in 2020 [<xref ref-type="bibr" rid="B24">24</xref>], authors have demonstrated the transmission of 1.2&#xa0;Gbps and 1.12&#xa0;Gbps of data over a 3 and 4&#xa0;m free space link by using dual polarized green and blue LED-based light streams. On the other hand, hybrid multiplexing schemes are used by many researchers to increase the bandwidth and capacity of optical communication systems [<xref ref-type="bibr" rid="B25">25</xref>&#x2013;<xref ref-type="bibr" rid="B35">35</xref>]. In this work, the OOK modulation technique is used for realization of a low-cost VLC system. Further to increase the capacity of the system, hybrid WDM and PDM multiplexing schemes are proposed using RGB LDs. The remainder of this paper is described as follows: <italic>Hybrid WDM-PDM-VLC Modeling</italic> shows the modeling of the proposed WDM-PDM VLC system, <italic>Results and Discussion</italic> represents the results and discussion, and <italic>Conclusion</italic> shows the overall conclusion of this&#x20;work.</p>
</sec>
<sec id="s2">
<title>Hybrid Wavelength Division Multiplexing-Polarization Division Multiplexing-Visible Light Communication Modeling</title>
<p>The schematic diagram of the proposed 6&#x20;&#xd7; 10&#xa0;Gbps hybrid WDM-PDM-based VLC system, modelled in OptiSystem software, is shown <xref ref-type="fig" rid="F1">Figure&#x20;1</xref>.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Transmission of six channels over a VLC link using hybrid WDM and PDM schemes.</p>
</caption>
<graphic xlink:href="fphy-09-731405-g001.tif"/>
</fig>
<p>As shown in <xref ref-type="fig" rid="F1">Figure&#x20;1</xref>, six channels are transmitted by using hybrid WDM and PDM schemes. A red laser (650&#xa0;nm), green laser (530&#xa0;nm), and blue laser (450&#xa0;nm) are used for the WDM scheme whereas X polarization with a 0<sup>0</sup> phase shift in azimuthal and Y polarization with a 90<sup>0</sup> phase shift in azimuthal are used for the PDM scheme. Each channel generates a pseudo random bit stream of 10&#xa0;Gbps which is encoded using the NRZ modulation format and then the signal is fed to the directly modulated (DM) laser. To ensure the laser diode (LD) operates above threshold, a direct current (D.C.) bias is fed into it. The output of the first three channels are combined together and subjected to a 0<sup>0</sup> azimuthal phase (X polarization) whereas the output of the remaining three channels are combined and fed to the 90<sup>0</sup> phase shift in azimuthal (Y polarization). <xref ref-type="fig" rid="F2">Figure&#x20;2</xref> represents the measured optical spectrum of three channels for each state (X and Y polarizations).</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>Measured optical spectrum, <bold>(A)</bold> X polarization channels, <bold>(B)</bold> Y polarization channels.</p>
</caption>
<graphic xlink:href="fphy-09-731405-g002.tif"/>
</fig>
<p>These outputs from each polarization state are combined and transmitted over 500&#xa0;m optical fiber and diffuser. For the modeling of the diffuse link, the transmitter source is assumed as a Lambertian disk which is irradiating a detector surface located at an axial distance <italic>h</italic> from the source. The Lambertian order which is based on transmitter half angle can be expressed mathematically as follows [<xref ref-type="bibr" rid="B36">36</xref>]:<disp-formula id="e1">
<mml:math id="m1">
<mml:mrow>
<mml:mi>m</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mi>log</mml:mi>
<mml:mo>&#x2061;</mml:mo>
<mml:mn>2</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:mi>l</mml:mi>
<mml:mi>o</mml:mi>
<mml:mi>g</mml:mi>
<mml:mrow>
<mml:mo>[</mml:mo>
<mml:mrow>
<mml:mi>cos</mml:mi>
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:mi>T</mml:mi>
<mml:mi>r</mml:mi>
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<mml:mi>h</mml:mi>
<mml:mi>a</mml:mi>
<mml:mi>l</mml:mi>
<mml:mi>f</mml:mi>
<mml:mo>&#xa0;</mml:mo>
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</mml:mrow>
<mml:mo>]</mml:mo>
</mml:mrow>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:math>
<label>(1)</label>
</disp-formula>whereas optical concentrator gain can be mathematically expressed as:<disp-formula id="e2">
<mml:math id="m2">
<mml:mrow>
<mml:mi>G</mml:mi>
<mml:mi>a</mml:mi>
<mml:mi>i</mml:mi>
<mml:mi>n</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:msup>
<mml:mi>I</mml:mi>
<mml:mn>2</mml:mn>
</mml:msup>
</mml:mrow>
<mml:mrow>
<mml:mi>sin</mml:mi>
<mml:msup>
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:mi>C</mml:mi>
<mml:mi>R</mml:mi>
<mml:mo>)</mml:mo>
</mml:mrow>
<mml:mn>2</mml:mn>
</mml:msup>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:math>
<label>(2)</label>
</disp-formula>where <italic>I</italic> is defined as the internal refractive index of the lens and <italic>CR</italic> is defined as the field of&#x20;view.</p>
<p>At the receiver side, a polarization splitter is used to de-multiplex the polarized signal for each state (X and Y polarizations). For each receiving channel, an avalanche photo diode (APD) is used to detect the light from the diffuser. The down-sampling frequency of APD is set to corresponding wavelengths transmitted at the transmitter side. The output of APD is amplified by using a <italic>trans</italic>-impedance amplifier followed by the low pass filter (LPF). At the output of LPF, bit error rate BER) is measured by using a bit error tester. The received signal at the receiver is expressed as [<xref ref-type="bibr" rid="B37">37</xref>, <xref ref-type="bibr" rid="B38">38</xref>]:<disp-formula id="e3">
<mml:math id="m3">
<mml:mrow>
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<mml:mrow>
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</mml:mrow>
</mml:mrow>
</mml:math>
<label>(3)</label>
</disp-formula>where <italic>y(t)</italic> represents the received signal, <italic>x(t)</italic> represents the transmitted signal, <italic>h(t)</italic> represents the impulse response of the transmitted signal, and <italic>n(t)</italic> represents the additive noise which is composed of shot noise, thermal noise, and dark current noise. However, in this work, background noise is assumed to be negligible. The other modeling parameters considered for the proposed WDM-PDM-VLC link are mentioned in <xref ref-type="table" rid="T1">Table&#x20;1</xref>.</p>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Modeling parameters for the proposed WDM-PDM-VLC&#x20;link.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Component</th>
<th align="center">Parameters</th>
<th align="center">Value</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td rowspan="4" align="left">Laser diode</td>
<td align="center">Wavelengths</td>
<td align="center">650&#xa0;nm, 530&#xa0;nm, and 450&#xa0;nm</td>
</tr>
<tr>
<td align="center">Extension ratio</td>
<td align="center">10&#xa0;dB</td>
</tr>
<tr>
<td align="center">Power</td>
<td align="center">0&#xa0;dB</td>
</tr>
<tr>
<td align="center">Linewidth</td>
<td align="center">10&#xa0;MHz</td>
</tr>
<tr>
<td align="left">DC bias generator</td>
<td align="center">Amplitude</td>
<td align="center">1 a.u</td>
</tr>
<tr>
<td rowspan="7" align="left">Diffuse link</td>
<td align="center">Transmitter half angle</td>
<td align="center">60 deg</td>
</tr>
<tr>
<td align="center">Irradiance half angle</td>
<td align="center">0 deg</td>
</tr>
<tr>
<td align="center">Incidence half angle</td>
<td align="center">0 deg</td>
</tr>
<tr>
<td align="center">Detection surface area</td>
<td align="center">1&#xa0;cm<sup>2</sup>
</td>
</tr>
<tr>
<td align="center">Optical concentration factor</td>
<td align="center">1 deg</td>
</tr>
<tr>
<td align="center">Index concentration factor</td>
<td align="center">1.5</td>
</tr>
<tr>
<td align="center">Propagation delay</td>
<td align="center">0&#xa0;ps/m</td>
</tr>
<tr>
<td rowspan="5" align="left">Avalanche photo diode</td>
<td align="center">Gain`</td>
<td align="center">3</td>
</tr>
<tr>
<td align="center">Responsivity</td>
<td align="center">1A/W</td>
</tr>
<tr>
<td align="center">Ionization ration</td>
<td align="center">0.9</td>
</tr>
<tr>
<td align="center">Dark current</td>
<td align="center">10&#xa0;nA</td>
</tr>
<tr>
<td align="center">Thermal noise</td>
<td align="center">100e-024&#xa0;W/Hz</td>
</tr>
<tr>
<td rowspan="3" align="left">TIA</td>
<td align="center">Voltage gain</td>
<td align="center">600&#xa0;&#x2126;</td>
</tr>
<tr>
<td align="center">Input capacitance</td>
<td align="center">3&#xa0;pF</td>
</tr>
<tr>
<td align="center">Feedback resistance</td>
<td align="center">0.01e&#x2b;009</td>
</tr>
<tr>
<td rowspan="3" align="left">Simulation window</td>
<td align="center">Sequence length</td>
<td align="center">1,024</td>
</tr>
<tr>
<td align="center">Samples per bit</td>
<td align="center">64</td>
</tr>
<tr>
<td align="center">No. of samples</td>
<td align="center">65,536</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec sec-type="results|discussion" id="s3">
<title>Results and Discussion</title>
<p>This section comprises the results from the modeling of the proposed WDM-PDM-VLC link. BER is used to evaluate the performance of the proposed WDM-PDM-VLC link. <xref ref-type="fig" rid="F3">Figure&#x20;3</xref> shows the computed BER for all the channels with respect to diffuse link range. It shows that channel 1 which is transmitted over 640&#xa0;nm with X polarization and channel 4 which is transmitted over 650&#xa0;nm with Y polarization achieved a BER of less than <inline-formula id="inf1">
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<mml:mn>3</mml:mn>
</mml:mrow>
</mml:msup>
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</inline-formula> at a diffuse link range of 200&#xa0;cm. For channel 1 and channel 4, the BER is measured as <inline-formula id="inf2">
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</inline-formula> at the diffuse link range of 140&#xa0;cm. As the diffuse link ranges increase further, BER also increases for both channels. Similarly, channel 2 (transmitted over 530&#xa0;nm with X polarization) and channel 5 (transmitted over 530&#xa0;nm with Y polarization) have also achieved a BER less than<inline-formula id="inf3">
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</mml:math>
</inline-formula>.</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>Measured BER for each polarization channel, <bold>(A)</bold> channels 1 and 4, <bold>(B)</bold> channels 2 and 5, and <bold>(C)</bold> channels 3 and 6.</p>
</caption>
<graphic xlink:href="fphy-09-731405-g003.tif"/>
</fig>
<p>Channels 2 and 4 have also measured a BER of <inline-formula id="inf4">
<mml:math id="m7">
<mml:mrow>
<mml:msup>
<mml:mrow>
<mml:mn>10</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>8</mml:mn>
</mml:mrow>
</mml:msup>
</mml:mrow>
</mml:math>
</inline-formula> at the diffuse link range of 140&#xa0;cm. The values of BER for channel 3 which is transmitted over 430&#xa0;nm with X polarization and channel 6 which is transmitted over 430&#xa0;nm with Y polarization are also measured as less than<inline-formula id="inf5">
<mml:math id="m8">
<mml:mrow>
<mml:mo>&#xa0;</mml:mo>
<mml:msup>
<mml:mrow>
<mml:mn>10</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>3</mml:mn>
</mml:mrow>
</mml:msup>
</mml:mrow>
</mml:math>
</inline-formula>. This satisfies the acceptable BER threshold of<inline-formula id="inf6">
<mml:math id="m9">
<mml:mrow>
<mml:mo>&#xa0;</mml:mo>
<mml:mo>&#x2248;</mml:mo>
<mml:msup>
<mml:mrow>
<mml:mn>10</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>3</mml:mn>
</mml:mrow>
</mml:msup>
</mml:mrow>
</mml:math>
</inline-formula> as per FCC limits. The measured eye diagrams for all the channels at the diffuse link range of 200&#xa0;cm are shown in <xref ref-type="fig" rid="F4">Figure&#x20;4</xref>. It shows that eye diagrams are open enough to receive the 10&#xa0;Gbps of data over a diffuse link up to 200&#xa0;cm with an acceptable&#x20;BER.</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>Computed eye diagrams for all channels at the diffuse link of 200&#xa0;cm.</p>
</caption>
<graphic xlink:href="fphy-09-731405-g004.tif"/>
</fig>
</sec>
<sec sec-type="conclusion" id="s4">
<title>Conclusion</title>
<p>In this work, six channels each carrying 10&#xa0;Gbps of NRZ-encoded data are transmitted over a 500&#xa0;m optical fiber and diffuse link range up to 200&#xa0;cm by incorporating WDM and PDM schemes. RGB lasers are used for the WDM scheme whereas X and Y polarization states are used for the PDM scheme. For X polarization, an azimuthal phase shift of 0<sup>0</sup> is used whereas for Y polarization, a azimuthal phase shift of 90<sup>0</sup> is used. The performance of the proposed WDM-PDM-VLC link is evaluated in terms of BER and eye diagrams. The reported results show the successful transmission of all channels over a 500&#xa0;m optical fiber link and 200&#xa0;cm diffuse link with an acceptable BER <inline-formula id="inf7">
<mml:math id="m10">
<mml:mrow>
<mml:mo>&#x2248;</mml:mo>
<mml:msup>
<mml:mrow>
<mml:mn>10</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>3</mml:mn>
</mml:mrow>
</mml:msup>
</mml:mrow>
</mml:math>
</inline-formula>. This work can be extended by considering real-time test beds to transmit high-speed data over a VLC&#x20;link.</p>
</sec>
</body>
<back>
<sec id="s5">
<title>Data Availability Statement</title>
<p>The raw data supporting the conclusion of this article will be made available by the authors, without undue reservation.</p>
</sec>
<sec id="s6">
<title>Author Contributions</title>
<p>CX-P has conceived of the presented idea, designed the model and performed the computations and wrote the original&#x20;draft.</p>
</sec>
<sec id="s7">
<title>Funding</title>
<p>This work is supported by Education and Scientific research project of middle and young teachers in Fujian (JAT200541).</p>
</sec>
<sec sec-type="COI-statement" id="s8">
<title>Conflict of Interest</title>
<p>The author declares that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<sec sec-type="disclaimer" id="s9">
<title>Publisher&#x2019;s Note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
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