<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">OPJ</journal-id><journal-title-group><journal-title>Optics and Photonics Journal</journal-title></journal-title-group><issn pub-type="epub">2160-8881</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/opj.2016.68B025</article-id><article-id pub-id-type="publisher-id">OPJ-70319</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Chemistry&amp;Materials Science</subject><subject> Engineering</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Performance Comparison among ASK, FSK and DPSK in Visible Light Communication
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Chengji</surname><given-names>Yao</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Zengqiao</surname><given-names>Guo</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Gongtao</surname><given-names>Long</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hongming</surname><given-names>Zhang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Tsinghua National Laboratory Science and Technology (TNList), Department of Electronic Engineering, 
Tsinghua University, Beijing, China</addr-line></aff><aff id="aff2"><addr-line>Beijing Smart-Chip Microelectronics Technology Company Ltd., Beijing, China</addr-line></aff><pub-date pub-type="epub"><day>25</day><month>08</month><year>2016</year></pub-date><volume>06</volume><issue>08</issue><fpage>150</fpage><lpage>154</lpage><history><date date-type="received"><day>8</day>	<month>March</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>21</month>	<year>August</year>	</date><date date-type="accepted"><day>25</day>	<month>August</month>	<year>2016</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
   
   We consider the detection of Amplitude-Shift Keying (ASK), Frequency-Shift Keying (FSK) and Differential Phase-Shift Keying (DPSK) in Visible Light Communication (VLC). And their performance is compared according to data rate, transmission distance and incident angle respectively. 
  
 
</p></abstract><kwd-group><kwd>VLC</kwd><kwd> ASK</kwd><kwd> FSK</kwd><kwd> DPSK</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Nowadays, Light-Emitting-Diodes (LEDs) are widely used and they have a lot of advantages [<xref ref-type="bibr" rid="scirp.70319-ref1">1</xref>], such as high energy and high brightness. In addition to lighting, LED can also be used for communication. Visible Light Communication (VLC) can do better than radio wireless communication in confidentiality and it has no electromagnetic radiation so that it can be used in some special situation.</p><p>VLC normally uses the ASK modulation technique, which is simple and widely used. But FSK, DPSK is seldom used in VLC system. As it is almost as simple as ASK, we have done some analyses to FSK and DPSK, as well as compare them to ASK in a line-of-sight (LOS) VLC system, to see whether the performance can be improved when FSK or DPSK is introduced [<xref ref-type="bibr" rid="scirp.70319-ref2">2</xref>].</p><p>In this paper, we look into the VLC system and figure out what influences the signal noise ratio (SNR) and bit rate error (BER) in the first section. Secondly, we do some simulation to show the BER influenced by data rate, transmission distance and incident angle respectively. Finally, the performance of OOK, FSK and DPSK is summed up.</p></sec><sec id="s2"><title>2. System Analysis</title><p>As shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>, a general VLC system includes a transmitter and a receiver. The transmitter consists of modulator, LED driver and LED, and the receiver is composed of photo detector (PD), amplifier, demodulator and decision device.</p><p>The modulator refers to ASK, FSK and DPSK modulator in this paper, and the demodulator is the corres-</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title>System Scheme</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70319x4.png"/></fig><p>ponding one of the modulator. The PD converts the signal from optical power to electrical current. And then it is amplified and converted to voltage signal.</p><p>In a general LOS VLC system as shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>, we define the parameters as follows. The angle of the LED’s half illuminance is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70319x5.png" xlink:type="simple"/></inline-formula>, and the irradiance angle is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70319x6.png" xlink:type="simple"/></inline-formula>, The photodiode’s (PD) light incident angle is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70319x7.png" xlink:type="simple"/></inline-formula>, and the field of view of PD is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70319x8.png" xlink:type="simple"/></inline-formula>. Finally, the distance between the LED and the PD is d.</p><p>The radiation pattern of LED is generally regarded as Lambertian pattern, therefore, the optical intensity at</p><p>angle ϕ is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70319x9.png" xlink:type="simple"/></inline-formula>. Where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70319x10.png" xlink:type="simple"/></inline-formula> is the perpendicular incidence intensity of the LED, m is the order of Lambertian radiation and the relationship between m and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70319x11.png" xlink:type="simple"/></inline-formula> is given by [<xref ref-type="bibr" rid="scirp.70319-ref3">3</xref>]</p><disp-formula id="scirp.70319-formula325"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70319x12.png"  xlink:type="simple"/></disp-formula><p>And then we can calculate the received power. It is given by</p><disp-formula id="scirp.70319-formula326"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70319x13.png"  xlink:type="simple"/></disp-formula><p>In this formula, A is the receiving area of PD, R is the PD sensitivity. And a PD can’t receive any signal if φ is larger than the field of view (FOV) of PD marked as Ψ. So we can see that</p><disp-formula id="scirp.70319-formula327"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70319x14.png"  xlink:type="simple"/></disp-formula><p>In order to decrease the system complexity, we choose to use noncoherent demodulation, the bit error rate (BER) of ASK, FSK and DPSK is given by [<xref ref-type="bibr" rid="scirp.70319-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.70319-ref5">5</xref>]:</p><disp-formula id="scirp.70319-formula328"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70319x15.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70319-formula329"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70319x16.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70319-formula330"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70319x17.png"  xlink:type="simple"/></disp-formula></sec><sec id="s3"><title>3. Simulation Results and Discussion</title><p>Now the performance of ASK, FSK and DPSK is given out according to data rate, transmission distance and incident angle respectively, whose model is the LOS model I mention above. And the bandwidths of these modulations are calculated according to the feature of the modulation. The parameters used in the simulation are shown in <xref ref-type="table" rid="table1">Table 1</xref> [<xref ref-type="bibr" rid="scirp.70319-ref6">6</xref>].</p><p>In ASK modulation, the bandwidth is equal to the data rate Rb, in FSK modulation, the bandwidth is equal to abs (f2 − f1)/2 + Rb, where f1 and f2 are the carrier frequencies of FSK, and in DPSK modulation the bandwidth is also equal to Rb.</p><p>AS shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>, we assume the incident angle is 0 degree, the carrier frequencies of FSK are 1 MHz and 2 MHz, the transmission distance is 100 m, and the data rate ranges from 100 Kbps to 1 Mbps. We can see that DPSK performs best, and ASK is better than FSK when data rate is low, when data rate goes high, FSK can finally exceeds ASK.</p><p>As shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>, the incident angle is set to 0 degree, the carrier frequencies of FSK are 1 MHz and 2 MHz, the transmission distance ranges from 10 m to 200 m. We can see that the BER increase significantly for</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> LOS VLC scheme diagram</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70319x18.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> BER vs. data rate</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70319x19.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Simulation parameter</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Parameter</th><th align="center" valign="middle" >Value</th><th align="center" valign="middle" >Parameter</th><th align="center" valign="middle" >Value</th></tr></thead><tr><td align="center" valign="middle" >Transmitted optical power</td><td align="center" valign="middle" >900 mW</td><td align="center" valign="middle" >Fixed capacitance per unit area</td><td align="center" valign="middle" >112 pF/cm<sup>2 </sup></td></tr><tr><td align="center" valign="middle" >Semi-angle at half power</td><td align="center" valign="middle" >70 degree</td><td align="center" valign="middle" >Open-loop gain</td><td align="center" valign="middle" >10</td></tr><tr><td align="center" valign="middle" >Effective area in PD</td><td align="center" valign="middle" >1 cm<sup>2 </sup></td><td align="center" valign="middle" >Temperature</td><td align="center" valign="middle" >298 K</td></tr><tr><td align="center" valign="middle" >FOV of PD</td><td align="center" valign="middle" >60 degree</td><td align="center" valign="middle" >FET trans-conductance</td><td align="center" valign="middle" >30 mS</td></tr><tr><td align="center" valign="middle" >PD sensitivity</td><td align="center" valign="middle" >0.2 A/W</td><td align="center" valign="middle" >FET noise factor</td><td align="center" valign="middle" >1.5</td></tr><tr><td align="center" valign="middle" >Back ground current</td><td align="center" valign="middle" >0.0051 A</td><td align="center" valign="middle" >I<sub>3 </sub></td><td align="center" valign="middle" >0.0868</td></tr><tr><td align="center" valign="middle" >Noise bandwidth factor</td><td align="center" valign="middle" >0.562</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><p>all the modulation methods. We can derive above result from that the optical power is proportional to the square of the transmission distance. And DPSK is the best, FSK is better than ASK at every point of fixed distance.</p><p>We set the transmission distance to 100 m, the carrier frequencies of FSK are 1 MHz and 2 MHz, the incident angle varies from 0 degree to 60 degree. And we can learn that all of the modulation methods could not demodulate correctly when the angle is larger than 15 degree. Among these three methods, DPSK performs best. (<xref ref-type="fig" rid="fig5">Figure 5</xref>)</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> BER vs. distance</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70319x20.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> BER vs. incident angle</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70319x21.png"/></fig></sec><sec id="s4"><title>4. Conclusion</title><p>In this paper, we have done some analyses to the LOS VLC transmission system and compared the noncoherent detection performance of ASK, FSK and DPSK according to different data rate, transmission distance and incident angle. DPSK always performs best, and FSK can beat ASK when the ratio of data rate to carrier frequencies difference is large.</p></sec><sec id="s5"><title>Acknowledgements</title><p>This work was supported by the SGCC Tech Program (Grant No. SGHAZZ00FCJS1500238).</p></sec><sec id="s6"><title>Cite this paper</title><p>Chengji Yao,Zengqiao Guo,Gongtao Long,Hongming Zhang, (2016) Performance Comparison among ASK, FSK and DPSK in Visible Light Communication. Optics and Photonics Journal,06,150-154. doi: 10.4236/opj.2016.68B025</p></sec></body><back><ref-list><title>References</title><ref id="scirp.70319-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">O’Brien, D.C., Zeng, L., Le-Minh, H., et al. (2008) Visible Light Communications: Challenges and Possibilities. 2008 IEEE 19th International Symposium on Personal, Indoor and Mobile Radio Communications, 1-5.</mixed-citation></ref><ref id="scirp.70319-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Tomasi, W. (1993) Advanced Electronic Communication Systems. Prentice Hall PTR.</mixed-citation></ref><ref id="scirp.70319-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Komine, T. and Nakagawa, M. (2004) Fundamental Analysis for Visible-Light Communication System Using LED Lights. IEEE Transactions on Consumer Electronics, 50, 100-107. http://dx.doi.org/10.1109/TCE.2004.1277847</mixed-citation></ref><ref id="scirp.70319-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Foschini, G.J., Greenstein, L.J. and Vannucci, G. (1988) Noncoherent Detection of Coherent Lightwave Signals Corrupted by Phase Noise. IEEE Transactions on Communications, 36, 306-314. http://dx.doi.org/10.1109/26.1456</mixed-citation></ref><ref id="scirp.70319-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Ziemer, R.E. and Peterson, R.L. (1985) Digital Communications and Spread Spectrum Sys-tems. Macmillan Publishing Company.</mixed-citation></ref><ref id="scirp.70319-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Lou, P., Zhang, H., Zhang, X., et al. (2012) Fundamental Analysis for Indoor Visible Light Positioning System. 2012 1st IEEE International Conference on Communications in China Workshops (ICCC), 59-63.</mixed-citation></ref></ref-list></back></article>