<?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.2016.68B003</article-id><article-id pub-id-type="publisher-id">OPJ-70292</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>
 
 
  Timing Synchronization Method for Asymmetrically Clipped DC Biased Optical OFDM System
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yong</surname><given-names>Wang</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>College of Information &amp;amp; Communication Engineering, Harbin Engineering University, Harbin, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:</corresp></author-notes><pub-date pub-type="epub"><day>25</day><month>08</month><year>2016</year></pub-date><volume>06</volume><issue>08</issue><fpage>14</fpage><lpage>18</lpage><history><date date-type="received"><day>19</day>	<month>April</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>19</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>
 
 
   
   In a typical intensity-modulated direct-detection optical system, the information is carried on the intensity of the optical signal, and therefore can only be positive. Existing synchronization methods for RF-based OFDM system cannot be used directly in asymmetrically clipped DC biased optical of DM (ADO-OFDM) system. In order to solve the above problem, according to the characteristics of ADO-OFDM signal, the modified training symbol is presented. The simulation results show that the modified synchronization method gives good performance. 
  
 
</p></abstract><kwd-group><kwd>Optical Wireless Communication</kwd><kwd> ADO-OFDM</kwd><kwd> Timing Synchronization</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In recent years, interest in optical wireless communication as a promising complementary technology for radio frequency in short-rang communications has gained new momentum. Optical wireless communication offers attractive features, distinct from those of radio transmission, such as low cost, low power consumption, high security, high data rate, and so on. Besides, along with the continuing development of technology, optical wireless communication has been shown to be a good wireless interconnect technology for high capacity communication networks in the first and last mile. However, a large number of scatter exist in optical wireless communication link, and it will generate multiple scattering on the transmitted beam. The multiple scattering will make the received signal contain direct signal and multipath scattering signal. It is very easy to cause the receiver to generate serious inter-symbol interference. The quality of optical wireless communication is severely influenced. Recently, ACO-OFDM [<xref ref-type="bibr" rid="scirp.70292-ref1">1</xref>] has emerged as an effective solution to deal with the inter-symbol interference caused by multipath transmission. At low data rate, ACO-OFDM is more efficient in terms of optical power but it suffers from spectral inefficiency. In order to improve spectral efficiencies, a new technique called ADO-OFDM was proposed in [<xref ref-type="bibr" rid="scirp.70292-ref2">2</xref>]. This technique consists of transmitting simultaneously ACO-OFDM on the odd subcarriers and DCO-OFDM on the even subcarriers. However, one of the prominent problems of ADO-OFDM is timing synchronization, it restricts the system performance. Therefore, the new synchronization method will be studied to reduce the ADO-OFDM system timing synchronization error.</p></sec><sec id="s2"><title>2. System Model</title><p><xref ref-type="fig" rid="fig1">Figure 1</xref> shows the block diagram of the transmitter part of the ADO-OFDM system [<xref ref-type="bibr" rid="scirp.70292-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.70292-ref3">3</xref>]. The input data will be mapped to a complex vector<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x4.png" xlink:type="simple"/></inline-formula>. In the optical intensity- modulated direct-detection system, the baseband signals must be a real signal, not a complex signal. To obtain such a signal, the complex vector X is constrained to have Hermitian symmetry. X is divided into odd and even components, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x5.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x6.png" xlink:type="simple"/></inline-formula>. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x7.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x8.png" xlink:type="simple"/></inline-formula> are input to separate IFFT blocks to produce <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x9.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x10.png" xlink:type="simple"/></inline-formula> respectively. The signal <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x11.png" xlink:type="simple"/></inline-formula> at the IFFT output in the ACO-OFDM generation block is clipped at zero to produce ACO-OFDM signal,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x12.png" xlink:type="simple"/></inline-formula>. At the output of the IFFT block in the DCO-OFDM signal generation, a DC bias is added to the signal<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x13.png" xlink:type="simple"/></inline-formula> and any remaining negative peaks are clipped to give DCO-OFDM signal,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x14.png" xlink:type="simple"/></inline-formula>. Signal <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x15.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x16.png" xlink:type="simple"/></inline-formula> are added together to give the signal<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x17.png" xlink:type="simple"/></inline-formula>.</p><p><xref ref-type="fig" rid="fig2">Figure 2</xref> shows the receiver part of the ADO-OFDM system. There is a separate path to demodulate the ACO-OFDM symbols and another path to demodulate the DCO-OFDM symbols. The ACO-OFDM demodulation block is the same as that of the conventional ACO-OFDM receiver. However, to recover the symbols transmitted on the even subcarriers, an estimate of the ACO-OFDM signal is first generated. This is achieved by taking the odd subcarriers from Y to obtain<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x18.png" xlink:type="simple"/></inline-formula>. An estimate of the ACO-OFDM signal is calculated from <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x19.png" xlink:type="simple"/></inline-formula> and subtracted from y to recover the DCO-OFDM component.</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> The transmitter of ADO-OFDM system</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70292x20.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> The receiver of ADO-OFDM system</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70292x21.png"/></fig></sec><sec id="s3"><title>3. Timing Synchronization Methods</title><sec id="s3_1"><title>3.1. Schmidl’s Method</title><p>Schmidl’s method [<xref ref-type="bibr" rid="scirp.70292-ref4">4</xref>] uses a symbol which consists of a repeated time domain sequence with the form <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x22.png" xlink:type="simple"/></inline-formula> where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x23.png" xlink:type="simple"/></inline-formula> represents a sequence of length<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x24.png" xlink:type="simple"/></inline-formula>. The Schmidl’s timing estimator finds the starting point of the symbol at the maximum point of the timing metric. The Schmidl’s timing metric is given by</p><disp-formula id="scirp.70292-formula199"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70292x25.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.70292-formula200"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70292x26.png"  xlink:type="simple"/></disp-formula><p>The timing metric has a plateau which leads to some uncertainty as to the start of OFDM symbol. The mean- square error of the Schmidl’s estimator is quite large.</p></sec><sec id="s3_2"><title>3.2. Park’s Method</title><p>To reduce the uncertainty due to timing metric plateau and improve the timing offset eatimation, Park [<xref ref-type="bibr" rid="scirp.70292-ref5">5</xref>] proposed a time domain training symbol with the format<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x27.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x28.png" xlink:type="simple"/></inline-formula> represents PN sequence of length<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x29.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x30.png" xlink:type="simple"/></inline-formula> represents a conjugate of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x31.png" xlink:type="simple"/></inline-formula>. To get impulse-shaped timing metric, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x32.png" xlink:type="simple"/></inline-formula>is designed to be the mirror image of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x33.png" xlink:type="simple"/></inline-formula>. To make use of the property that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x34.png" xlink:type="simple"/></inline-formula> is symmetric with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x35.png" xlink:type="simple"/></inline-formula>, a new timing metric can be written as</p><disp-formula id="scirp.70292-formula201"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70292x36.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.70292-formula202"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70292x37.png"  xlink:type="simple"/></disp-formula></sec><sec id="s3_3"><title>3.3. The Modified Timing Synchronization Method</title><p>Because ADO-OFDM modulates the intensity of the light source, the signals must be real and positive. So time domain training sequences is constituted by real signals. Based on the above reason, a new training symbol is proposed in this paper. The time domain training symbol is defined as below:</p><disp-formula id="scirp.70292-formula203"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70292x38.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x39.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x40.png" xlink:type="simple"/></inline-formula> are a sequence of real values, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x41.png" xlink:type="simple"/></inline-formula>is the mirror image of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x42.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x43.png" xlink:type="simple"/></inline-formula> is the mirror image of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x44.png" xlink:type="simple"/></inline-formula>.The timing metric function is given by</p><disp-formula id="scirp.70292-formula204"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70292x45.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.70292-formula205"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70292x46.png"  xlink:type="simple"/></disp-formula></sec></sec><sec id="s4"><title>4. Simulation Results and Analysis</title><p>Schmidl and Park timing synchronization methods are all used in the RF-based OFDM system, and the training symbols is required to be bipolar and complex. Therefore, these methods cannot directly be applied to ADO-OFDM system. The data form of training symbols must be changed in order to apply the timing synchronization methods to optical wireless communication system. <xref ref-type="fig" rid="fig3">Figure 3</xref> and <xref ref-type="fig" rid="fig4">Figure 4</xref> shows the average timing metric of the adapted methods applied to ADO-OFDM system. Simulation parameters: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x47.png" xlink:type="simple"/></inline-formula>subcarriers, a QPSK constellation on each of the available subcarriers, cyclic prefix length of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x48.png" xlink:type="simple"/></inline-formula>, and 1000 random training symbols.</p><p>The timing metric curve still remains the plateau when the adapted Schmidl timing synchronization method is used. The adapted Park timing synchronization method has two extra peaks at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x49.png" xlink:type="simple"/></inline-formula> because the training symbols are symmetry about the points. Therefore, it can be seen clearly that the adapted Schmidl and Park timing synchronization methods are not ideal for ADO-OFDM system. <xref ref-type="fig" rid="fig5">Figure 5</xref> shows the average timing metrics of the modified timing synchronization method applied to ADO-OFDM system. Comparing with the adapted Park method, new timing synchronization method can effectively eliminates the two extra peaks at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70292x50.png" xlink:type="simple"/></inline-formula>. From the results of simulations, it is obvious that the performance of the modified timing synchronization method is better than other methods.</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> The Schmidl’s timing metric in ADO-OFDM system</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70292x51.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> The Park’s timing metric in ADO-OFDM system</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70292x52.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> The modified timing synchronization metric in ADO-OFDM system</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70292x53.png"/></fig></sec><sec id="s5"><title>5. Conclusion</title><p>The conventional timing synchronization methods for RF-based OFDM system are studied. The timing synchronization methods are adapted and applied to ADO-OFDM system. The analysis shows that these methods do not perform well in ADO-OFDM system. Therefore, a modified training symbol is proposed in this paper. The simulation results show the modified timing synchronization method can obtain higher timing accuracy.</p></sec><sec id="s6"><title>Acknowledgements</title><p>This work was financially supported by the Natural Science Foundation of China (61275082).</p></sec><sec id="s7"><title>Cite this paper</title><p>Yong Wang, (2016) Timing Synchronization Method for Asymmetrically Clipped DC Biased Optical OFDM System. Optics and Photonics Journal,06,14-18. doi: 10.4236/opj.2016.68B003</p></sec></body><back><ref-list><title>References</title><ref id="scirp.70292-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Armstrong, J and Lowery, A.J. (2006) Power Efficient Optical OFDM. Electron. Lett, 42, 370-372.  
http://dx.doi.org/10.1049/el:20063636</mixed-citation></ref><ref id="scirp.70292-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Dissanayake, S.D., Panta, K. and Armstrong, J. (2011) A Novel Technique to Simulta-neously Transmit ACO-OFDM and DCO-OFDM in IM/DD Systems. IEEE GLOBECOM Workshops, 782-786. 
http://dx.doi.org/10.1109/glocomw.2011.6162561</mixed-citation></ref><ref id="scirp.70292-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Dissanayake, S.D. and Armstrong, J.  (2013) Comparison of ACO-OFDM, DCO-OFDM and ADO-OFDM in IM/DD Systems. Journal of Lightwave Technology, 31, 1063-1072. http://dx.doi.org/10.1109/JLT.2013.2241731</mixed-citation></ref><ref id="scirp.70292-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Schmidl, T.M. and Cox, D.C. (1997) Robust Frequency and Timing Synchroniza-tion for OFDM. IEEE Transactions on Communications, 45, 1613-1621. http://dx.doi.org/10.1109/26.650240</mixed-citation></ref><ref id="scirp.70292-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Park, B., Cheon, H., Kang, C. and Hong, D. (2003) A Novel Timing Estimation Method for OFDM Systems. IEEE Communications Letters, 7, 239-241. http://dx.doi.org/10.1109/LCOMM.2003.812181</mixed-citation></ref></ref-list></back></article>