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&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Short description|Pairs of sequences}}&lt;br /&gt;
: &amp;#039;&amp;#039;For complementary sequences in biology, see [[complementarity (molecular biology)]]. For integer sequences with complementary sets of members see [[Lambek–Moser theorem]].&amp;#039;&amp;#039;&lt;br /&gt;
In applied mathematics, &amp;#039;&amp;#039;&amp;#039;complementary sequences&amp;#039;&amp;#039;&amp;#039; (&amp;#039;&amp;#039;&amp;#039;CS&amp;#039;&amp;#039;&amp;#039;) are pairs of [[sequence]]s with the useful property that their out-of-phase aperiodic [[autocorrelation]] coefficients sum to zero. Binary complementary sequences were first introduced by [[Marcel J. E. Golay]] in 1949. In 1961–1962 Golay gave several methods for constructing sequences of length 2&amp;lt;sup&amp;gt;&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;/sup&amp;gt; and gave examples of complementary sequences of lengths 10 and 26.  In 1974 R. J. Turyn gave a method for constructing sequences of length &amp;#039;&amp;#039;mn&amp;#039;&amp;#039; from sequences of lengths &amp;#039;&amp;#039;m&amp;#039;&amp;#039; and &amp;#039;&amp;#039;n&amp;#039;&amp;#039; which allows the construction of sequences of any length of the form 2&amp;lt;sup&amp;gt;&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;/sup&amp;gt;10&amp;lt;sup&amp;gt;&amp;#039;&amp;#039;K&amp;#039;&amp;#039;&amp;lt;/sup&amp;gt;26&amp;lt;sup&amp;gt;&amp;#039;&amp;#039;M&amp;#039;&amp;#039;&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Later the theory of complementary sequences was generalized by other authors to polyphase complementary sequences, multilevel complementary sequences, and arbitrary complex complementary sequences. &amp;#039;&amp;#039;&amp;#039;Complementary sets&amp;#039;&amp;#039;&amp;#039; have also been considered; these can contain more than two sequences.&lt;br /&gt;
&lt;br /&gt;
== Definition ==&lt;br /&gt;
&lt;br /&gt;
Let (&amp;#039;&amp;#039;a&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;, &amp;#039;&amp;#039;a&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, ..., &amp;#039;&amp;#039;a&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;amp;nbsp;&amp;amp;minus;&amp;amp;nbsp;1&amp;lt;/sub&amp;gt;) and (&amp;#039;&amp;#039;b&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;, &amp;#039;&amp;#039;b&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, ..., &amp;#039;&amp;#039;b&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;amp;nbsp;&amp;amp;minus;&amp;amp;nbsp;1&amp;lt;/sub&amp;gt;) be a pair of bipolar sequences, meaning that &amp;#039;&amp;#039;a&amp;#039;&amp;#039;(&amp;#039;&amp;#039;k&amp;#039;&amp;#039;) and &amp;#039;&amp;#039;b&amp;#039;&amp;#039;(&amp;#039;&amp;#039;k&amp;#039;&amp;#039;) have values +1 or &amp;amp;minus;1. Let the aperiodic [[autocorrelation function]] of the sequence &amp;#039;&amp;#039;&amp;#039;x&amp;#039;&amp;#039;&amp;#039; be defined by&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;R_x(k)=\sum_{j=0}^{N-k-1} x_jx_{j+k}.\,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Then the pair of sequences &amp;#039;&amp;#039;a&amp;#039;&amp;#039; and &amp;#039;&amp;#039;b&amp;#039;&amp;#039; is complementary if:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;R_a(k) + R_b(k) = 2N,\, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
for &amp;#039;&amp;#039;k&amp;#039;&amp;#039; = 0, and &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;R_a(k) + R_b(k) = 0,\, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
for &amp;#039;&amp;#039;k&amp;#039;&amp;#039; = 1, ..., &amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;amp;nbsp;&amp;amp;minus;&amp;amp;nbsp;1.&lt;br /&gt;
&lt;br /&gt;
Or using [[Kronecker delta]] we can write:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;R_a(k) + R_b(k) = 2N\delta(k),\, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
So we can say that the sum of autocorrelation functions of complementary sequences is a delta function, which is an ideal autocorrelation for many applications like [[radar]] [[pulse compression]] and [[spread spectrum]] [[telecommunications]].&lt;br /&gt;
&lt;br /&gt;
== Examples ==&lt;br /&gt;
&lt;br /&gt;
* As the simplest example we have sequences of length 2: (+1,&amp;amp;nbsp;+1) and (+1,&amp;amp;nbsp;&amp;amp;minus;1). Their autocorrelation functions are (2,&amp;amp;nbsp;1) and (2,&amp;amp;nbsp;&amp;amp;minus;1), which add up to (4,&amp;amp;nbsp;0).&lt;br /&gt;
* As the next example (sequences of length 4), we have (+1,&amp;amp;nbsp;+1,&amp;amp;nbsp;+1,&amp;amp;nbsp;&amp;amp;minus;1) and (+1,&amp;amp;nbsp;+1,&amp;amp;nbsp;&amp;amp;minus;1,&amp;amp;nbsp;+1). Their autocorrelation functions are (4,&amp;amp;nbsp;1,&amp;amp;nbsp;0,&amp;amp;nbsp;&amp;amp;minus;1) and (4,&amp;amp;nbsp;&amp;amp;minus;1,&amp;amp;nbsp;0,&amp;amp;nbsp;1), which add up to (8,&amp;amp;nbsp;0,&amp;amp;nbsp;0,&amp;amp;nbsp;0).&lt;br /&gt;
* One example of length 8 is (+1,&amp;amp;nbsp;+1,&amp;amp;nbsp;+1,&amp;amp;nbsp;&amp;amp;minus;1,&amp;amp;nbsp;+1,&amp;amp;nbsp;+1,&amp;amp;nbsp;&amp;amp;minus;1,&amp;amp;nbsp;+1) and (+1,&amp;amp;nbsp;+1,&amp;amp;nbsp;+1,&amp;amp;nbsp;&amp;amp;minus;1,&amp;amp;nbsp;&amp;amp;minus;1,&amp;amp;nbsp;&amp;amp;minus;1,&amp;amp;nbsp;+1,&amp;amp;nbsp;&amp;amp;minus;1). Their autocorrelation functions are (8,&amp;amp;nbsp;&amp;amp;minus;1,&amp;amp;nbsp;0,&amp;amp;nbsp;3,&amp;amp;nbsp;0,&amp;amp;nbsp;1,&amp;amp;nbsp;0,&amp;amp;nbsp;1) and (8,&amp;amp;nbsp;1,&amp;amp;nbsp;0,&amp;amp;nbsp;&amp;amp;minus;3,&amp;amp;nbsp;0,&amp;amp;nbsp;&amp;amp;minus;1,&amp;amp;nbsp;0,&amp;amp;nbsp;&amp;amp;minus;1).&lt;br /&gt;
* An example of length 10 given by Golay is (+1,&amp;amp;nbsp;+1,&amp;amp;nbsp;&amp;amp;minus;1,&amp;amp;nbsp;+1,&amp;amp;nbsp;&amp;amp;minus;1,&amp;amp;nbsp;+1,&amp;amp;nbsp;&amp;amp;minus;1,&amp;amp;nbsp;&amp;amp;minus;1,&amp;amp;nbsp;+1,&amp;amp;nbsp;+1) and (+1,&amp;amp;nbsp;+1,&amp;amp;nbsp;&amp;amp;minus;1,&amp;amp;nbsp;+1,&amp;amp;nbsp;+1,&amp;amp;nbsp;+1,&amp;amp;nbsp;+1,&amp;amp;nbsp;+1,&amp;amp;nbsp;&amp;amp;minus;1,&amp;amp;nbsp;&amp;amp;minus;1). Their autocorrelation functions are (10,&amp;amp;nbsp;&amp;amp;minus;3,&amp;amp;nbsp;0,&amp;amp;nbsp;&amp;amp;minus;1,&amp;amp;nbsp;0,&amp;amp;nbsp;1,&amp;amp;minus;2,&amp;amp;nbsp;&amp;amp;minus;1,&amp;amp;nbsp;2,&amp;amp;nbsp;1) and (10,&amp;amp;nbsp;3,&amp;amp;nbsp;0,&amp;amp;nbsp;1,&amp;amp;nbsp;0,&amp;amp;nbsp;&amp;amp;minus;1,&amp;amp;nbsp;2,&amp;amp;nbsp;1,&amp;amp;nbsp;&amp;amp;minus;2,&amp;amp;nbsp;&amp;amp;minus;1).&lt;br /&gt;
&lt;br /&gt;
== Properties of complementary pairs of sequences ==&lt;br /&gt;
&lt;br /&gt;
* Complementary [[sequences]] have complementary spectra. As the autocorrelation function and the power spectra form a Fourier pair, complementary sequences also have complementary spectra. But as the Fourier transform of a delta function is a constant, we can write&lt;br /&gt;
&lt;br /&gt;
:: &amp;lt;math&amp;gt;S_a + S_b = C_S,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
: where &amp;#039;&amp;#039;C&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;S&amp;#039;&amp;#039;&amp;lt;/sub&amp;gt; is a constant.&lt;br /&gt;
&lt;br /&gt;
: &amp;#039;&amp;#039;S&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;a&amp;#039;&amp;#039;&amp;lt;/sub&amp;gt; and &amp;#039;&amp;#039;S&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;b&amp;#039;&amp;#039;&amp;lt;/sub&amp;gt; are defined as a squared magnitude of the [[Fourier transform]] of the sequences. The Fourier transform can be a direct DFT of the sequences, it can be a DFT of zero padded sequences or it can be a continuous Fourier transform of the sequences which is equivalent to the [[Z transform]] for {{math|1=&amp;#039;&amp;#039;Z&amp;#039;&amp;#039; = &amp;#039;&amp;#039;e&amp;#039;&amp;#039;&amp;lt;sup&amp;gt;&amp;#039;&amp;#039;j&amp;#039;&amp;#039;ω&amp;lt;/sup&amp;gt;}}.&lt;br /&gt;
&lt;br /&gt;
* CS spectra is upper bounded. As &amp;#039;&amp;#039;S&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;a&amp;#039;&amp;#039;&amp;lt;/sub&amp;gt; and &amp;#039;&amp;#039;S&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;b&amp;#039;&amp;#039;&amp;lt;/sub&amp;gt; are non-negative values we can write&lt;br /&gt;
&lt;br /&gt;
:: &amp;lt;math&amp;gt;S_a = C_S - S_b &amp;lt; C_S,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
: also&lt;br /&gt;
&lt;br /&gt;
:: &amp;lt;math&amp;gt;S_b &amp;lt; C_S.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* If either of the sequences of the CS pair is inverted (multiplied by −1) they remain complementary. More generally if any of the sequences is multiplied by &amp;#039;&amp;#039;e&amp;#039;&amp;#039;&amp;lt;sup&amp;gt;&amp;#039;&amp;#039;j&amp;#039;&amp;#039;φ&amp;lt;/sup&amp;gt; they remain complementary;&lt;br /&gt;
* If either of the sequences is reversed they remain complementary;&lt;br /&gt;
* If either of the sequences is delayed they remain complementary;&lt;br /&gt;
* If the sequences are interchanged they remain complementary;&lt;br /&gt;
* If both sequences are multiplied by the same constant (real or complex) they remain complementary;&lt;br /&gt;
* If alternating bits of both sequences are inverted they remain complementary. In general for arbitrary complex sequences if both sequences are multiplied by &amp;#039;&amp;#039;e&amp;#039;&amp;#039;&amp;lt;sup&amp;gt;&amp;#039;&amp;#039;j&amp;#039;&amp;#039;&amp;amp;pi;&amp;#039;&amp;#039;kn&amp;#039;&amp;#039;/&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;/sup&amp;gt; (where &amp;#039;&amp;#039;k&amp;#039;&amp;#039; is a constant and &amp;#039;&amp;#039;n&amp;#039;&amp;#039; is the time index) they remain complementary;&lt;br /&gt;
* A new pair of complementary sequences can be formed as [&amp;#039;&amp;#039;a&amp;#039;&amp;#039; &amp;#039;&amp;#039;b&amp;#039;&amp;#039;] and [&amp;#039;&amp;#039;a&amp;#039;&amp;#039;&amp;amp;nbsp;−&amp;#039;&amp;#039;b&amp;#039;&amp;#039;] where [..] denotes concatenation and &amp;#039;&amp;#039;a&amp;#039;&amp;#039; and &amp;#039;&amp;#039;b&amp;#039;&amp;#039; are a pair of CS;&lt;br /&gt;
* A new pair of sequences can be formed as {&amp;#039;&amp;#039;a&amp;#039;&amp;#039; &amp;#039;&amp;#039;b&amp;#039;&amp;#039;} and {&amp;#039;&amp;#039;a&amp;#039;&amp;#039;&amp;amp;nbsp;−&amp;#039;&amp;#039;b&amp;#039;&amp;#039;} where {..} denotes [[Interleave sequence|interleaving]] of sequences.&lt;br /&gt;
* A new pair of sequences can be formed as &amp;#039;&amp;#039;a&amp;#039;&amp;#039;&amp;amp;nbsp;+&amp;amp;nbsp;&amp;#039;&amp;#039;b&amp;#039;&amp;#039; and &amp;#039;&amp;#039;a&amp;#039;&amp;#039;&amp;amp;nbsp;−&amp;amp;nbsp;&amp;#039;&amp;#039;b&amp;#039;&amp;#039;.&lt;br /&gt;
&lt;br /&gt;
==Golay pair==&lt;br /&gt;
A complementary pair &amp;#039;&amp;#039;a&amp;#039;&amp;#039;, &amp;#039;&amp;#039;b&amp;#039;&amp;#039; may be encoded as polynomials &amp;#039;&amp;#039;A&amp;#039;&amp;#039;(&amp;#039;&amp;#039;z&amp;#039;&amp;#039;) = &amp;#039;&amp;#039;a&amp;#039;&amp;#039;(0) + &amp;#039;&amp;#039;a&amp;#039;&amp;#039;(1)&amp;#039;&amp;#039;z&amp;#039;&amp;#039; + ... + &amp;#039;&amp;#039;a&amp;#039;&amp;#039;(&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;amp;nbsp;&amp;amp;minus;&amp;amp;nbsp;1)&amp;#039;&amp;#039;z&amp;#039;&amp;#039;&amp;lt;sup&amp;gt;&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;amp;minus;1&amp;lt;/sup&amp;gt; and similarly for &amp;#039;&amp;#039;B&amp;#039;&amp;#039;(&amp;#039;&amp;#039;z&amp;#039;&amp;#039;).  The complementarity property of the sequences is equivalent to the condition&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\vert A(z) \vert^2 + \vert B(z) \vert^2 = 2N \, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
for all &amp;#039;&amp;#039;z&amp;#039;&amp;#039; on the unit circle, that is, |&amp;#039;&amp;#039;z&amp;#039;&amp;#039;|&amp;amp;nbsp;=&amp;amp;nbsp;1.  If so, &amp;#039;&amp;#039;A&amp;#039;&amp;#039; and &amp;#039;&amp;#039;B&amp;#039;&amp;#039; form a &amp;#039;&amp;#039;&amp;#039;Golay pair&amp;#039;&amp;#039;&amp;#039; of polynomials.  Examples include the [[Shapiro polynomials]], which give rise to complementary sequences of length a [[power of two]].&lt;br /&gt;
&lt;br /&gt;
== Applications of complementary sequences ==&lt;br /&gt;
&lt;br /&gt;
* Multislit spectrometry&lt;br /&gt;
* Ultrasound measurements&lt;br /&gt;
* Acoustic measurements&lt;br /&gt;
* [[radar]] [[pulse compression]]&lt;br /&gt;
* [[Wi-Fi]] networks, &lt;br /&gt;
* [[3G]] [[CDMA]] wireless networks&lt;br /&gt;
* [[OFDM]] communication systems&lt;br /&gt;
* Train wheel detection systems&amp;lt;ref&amp;gt;&lt;br /&gt;
Donato, P.G.; Ureña, J.; Mazo, M.; Alvarez, F.&lt;br /&gt;
&amp;quot;Train wheel detection without electronic equipment near the rail line&amp;quot;.&lt;br /&gt;
2004.&lt;br /&gt;
{{doi | 10.1109/IVS.2004.1336500 }}&lt;br /&gt;
&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;&lt;br /&gt;
J.J. Garcia; A. Hernandez; J. Ureña; J.C. Garcia; M. Mazo; J.L. Lazaro; M.C. Perez; F. Alvarez.&lt;br /&gt;
[http://geintra-uah.org/system/files/private/IV04_I.pdf &amp;quot;Low cost obstacle detection for smart railway infrastructures&amp;quot;].&lt;br /&gt;
2004.&lt;br /&gt;
&amp;lt;/ref&amp;gt;&lt;br /&gt;
* Non-destructive tests (NDT)&lt;br /&gt;
* Communications&lt;br /&gt;
* [[coded aperture]] masks are designed using a 2-dimensional generalization of complementary sequences.&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
* [[Binary Golay code]] ([[Error-correcting code]])&lt;br /&gt;
* [[Gold code|Gold sequences]]&lt;br /&gt;
* [[Kasami code|Kasami sequences]]&lt;br /&gt;
* [[Polyphase sequence]]&lt;br /&gt;
* [[Pseudorandom binary sequence]]s (also called [[maximum length sequence]]s or M-sequences)&lt;br /&gt;
* [[Ternary Golay code]] ([[Error-correcting code]])&lt;br /&gt;
* [[Hadamard code|Walsh-Hadamard sequences]]&lt;br /&gt;
* [[Zadoff–Chu sequence]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
{{Reflist}}&lt;br /&gt;
{{refbegin}}&lt;br /&gt;
*{{cite journal |first=Marcel J.E. |last=Golay |authorlink=Marcel J. E. Golay |title=Multislit spectroscopy |journal=J. Opt. Soc. Am. |volume=39 |issue=6 |pages=437–444 |year=1949 |doi=10.1364/JOSA.39.000437 |pmid=18152021 }}&lt;br /&gt;
*{{cite journal |first=Marcel J.E. |last=Golay |title=Complementary series |journal=IRE Trans. Inf. Theory |volume=7 |issue=2 |pages=82–87 |date=April 1961 |doi=10.1109/TIT.1961.1057620  }}&lt;br /&gt;
*{{cite journal |first=Marcel J.E. |last=Golay |title=Note on &amp;quot;Complementary series&amp;quot; |journal=[[Proc. IRE]] |volume=50 |pages=84 |year=1962 |doi=10.1109/JRPROC.1962.288278 }}&lt;br /&gt;
*{{cite journal |first=R.J. |last=Turyn |title=Hadamard matrices, Baumert-Hall units, four-symbol sequences, pulse compression, and surface wave encodings |journal=J. Comb. Theory A |volume=16 |pages=313–333 |year=1974 |doi=10.1016/0097-3165(74)90056-9 |issue=3 |doi-access=free }}&lt;br /&gt;
*{{cite book |authorlink=Peter Borwein |first=Peter |last=Borwein |title=Computational Excursions in Analysis and Number Theory |url=https://books.google.com/books?id=A_ITwN13J6YC&amp;amp;pg=PA110 |year=2002 |publisher=Springer |isbn=978-0-387-95444-8 |pages=110–9}}&lt;br /&gt;
*{{cite journal |first1=P.G. |last1=Donato |first2=J. |last2=Ureña |first3=M. |last3=Mazo |first4=C. |last4=De Marziani |first5=A. |last5=Ochoa |title=Design and signal processing of a magnetic sensor array for train wheel detection |journal=Sensors and Actuators A: Physical |volume=132 |pages=516–525 |year=2006 |doi=10.1016/j.sna.2006.02.043 |issue=2 |bibcode=2006SeAcA.132..516D }}&lt;br /&gt;
{{refend}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Sequences and series]]&lt;br /&gt;
[[Category:Signal processing]]&lt;br /&gt;
[[Category:Pseudorandom number generators]]&lt;/div&gt;</summary>
		<author><name>imported&gt;Citation bot</name></author>
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