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		<title>Quantum t-design</title>
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		<summary type="html">&lt;p&gt;216.58.117.253: I fixed a typo, removing index k from the state Psi&lt;/p&gt;
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&lt;div&gt;In [[combinatorics]], a &#039;&#039;&#039;Davenport–Schinzel sequence&#039;&#039;&#039; is a [[sequence]] of symbols in which the number of times any two symbols may appear in alternation is limited. The maximum possible length of a Davenport–Schinzel sequence is bounded by the number of its distinct symbols multiplied by a small but nonconstant factor that depends on the number of alternations that are allowed. Davenport–Schinzel sequences were first defined in 1965 by [[Harold Davenport]] and [[Andrzej Schinzel]] to analyze [[linear differential equation]]s. Following {{harvtxt|Atallah|1985}} these sequences and their length bounds have also become a standard tool in [[discrete geometry]] and in the analysis of [[Computational geometry|geometric algorithms]].&amp;lt;ref&amp;gt;{{harvtxt|Sharir|Agarwal|1995}}, pp. x and 2.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Definition==&lt;br /&gt;
A finite sequence &#039;&#039;U&#039;&#039; = &#039;&#039;u&#039;&#039;&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, &#039;&#039;u&#039;&#039;&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, &#039;&#039;u&#039;&#039;&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, is said to be a Davenport–Schinzel sequence of order &#039;&#039;s&#039;&#039; if it satisfies the following two properties:&lt;br /&gt;
#No two consecutive values in the sequence are equal to each other.&lt;br /&gt;
#If &#039;&#039;x&#039;&#039; and &#039;&#039;y&#039;&#039; are two distinct values occurring in the sequence, then the sequence does not contain a subsequence ... &#039;&#039;x&#039;&#039;, ... &#039;&#039;y&#039;&#039;, ..., &#039;&#039;x&#039;&#039;, ..., &#039;&#039;y&#039;&#039;, ... consisting of &#039;&#039;s&#039;&#039;&amp;amp;nbsp;+&amp;amp;nbsp;2 values alternating between &#039;&#039;x&#039;&#039; and &#039;&#039;y&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
For instance, the sequence&lt;br /&gt;
:1, 2, 1, 3, 1, 3, 2, 4, 5, 4, 5, 2, 3&lt;br /&gt;
is a Davenport–Schinzel sequence of order 3: it contains alternating subsequences of length four, such as ...1, ... 2, ... 1, ... 2, ... (which appears in four different ways as a subsequence of the whole sequence) but it does not contain any alternating subsequences of length five.&lt;br /&gt;
&lt;br /&gt;
If a Davenport–Schinzel sequence of order &#039;&#039;s&#039;&#039; includes &#039;&#039;n&#039;&#039; distinct values, it is called an (&#039;&#039;n&#039;&#039;,&#039;&#039;s&#039;&#039;) Davenport–Schinzel sequence, or a &#039;&#039;DS&#039;&#039;(&#039;&#039;n&#039;&#039;,&#039;&#039;s&#039;&#039;)-sequence.&amp;lt;ref&amp;gt;See {{harvtxt|Sharir|Agarwal|1995}}, p. 1, for this notation.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Length bounds==&lt;br /&gt;
The complexity of &#039;&#039;DS&#039;&#039;(&#039;&#039;n&#039;&#039;,&#039;&#039;s&#039;&#039;)-sequence has been analyzed [[asymptotics|asymptotically]] in the limit as &#039;&#039;n&#039;&#039; goes to infinity, with the assumption that &#039;&#039;s&#039;&#039; is a fixed constant, and nearly tight bounds are known for all &#039;&#039;s&#039;&#039;. Let λ&amp;lt;sub&amp;gt;&#039;&#039;s&#039;&#039;&amp;lt;/sub&amp;gt;(&#039;&#039;n&#039;&#039;) denote the length of the longest &#039;&#039;DS&#039;&#039;(&#039;&#039;n&#039;&#039;,&#039;&#039;s&#039;&#039;)-sequence. The best bounds known on λ&amp;lt;sub&amp;gt;&#039;&#039;s&#039;&#039;&amp;lt;/sub&amp;gt; involve the [[Ackermann function#Inverse|inverse Ackermann function]]&lt;br /&gt;
:&amp;amp;alpha;(&#039;&#039;n&#039;&#039;) = min { &#039;&#039;m&#039;&#039; | A(&#039;&#039;m&#039;&#039;,&#039;&#039;m&#039;&#039;) ≥ &#039;&#039;n&#039;&#039; },&lt;br /&gt;
where &#039;&#039;A&#039;&#039; is the Ackermann function. Due to the very rapid growth of the Ackermann function, its inverse α grows very slowly, and is at most four for problems of any practical size.&amp;lt;ref&amp;gt;{{harvtxt|Sharir|Agarwal|1995}}, p.14.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Using [[big O notation|big O and big &amp;amp;Theta; notation]], the following bounds are known:&lt;br /&gt;
*λ&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;(&#039;&#039;n&#039;&#039;)&amp;amp;nbsp;=&amp;amp;nbsp;&#039;&#039;n&#039;&#039;.&amp;lt;ref name=&amp;quot;DS12&amp;quot;&amp;gt;{{harvtxt|Sharir|Agarwal|1995}}, p.6.&amp;lt;/ref&amp;gt;&lt;br /&gt;
*λ&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(&#039;&#039;n&#039;&#039;)&amp;amp;nbsp;=&amp;amp;nbsp;2&#039;&#039;n&#039;&#039;&amp;amp;nbsp;&amp;amp;minus;&amp;amp;nbsp;1.&amp;lt;ref name=&amp;quot;DS12&amp;quot; /&amp;gt;&lt;br /&gt;
*&amp;lt;math&amp;gt;2n\alpha(n)-O(n)\le\lambda_3(n)\le2n\alpha(n)+O(n\sqrt{\alpha(n)})&amp;lt;/math&amp;gt;.&amp;lt;ref&amp;gt;{{harvtxt|Sharir|Agarwal|1995}}, Chapter 2, pp. 12–42; {{harvtxt|Hart|Sharir|1986}}; {{harvtxt|Wiernik|Sharir|1988}}; {{harvtxt|Komjáth|1988}}; {{harvtxt|Klazar|1999}}; {{harvtxt|Nivasch|2009}}.&amp;lt;/ref&amp;gt; This complexity bound can be realized to within a constant factor by line segments: there exist arrangements of &#039;&#039;n&#039;&#039; line segments in the plane whose lower envelopes have complexity Ω(&#039;&#039;n&#039;&#039;&amp;amp;nbsp;α(&#039;&#039;n&#039;&#039;)).&amp;lt;ref&amp;gt;{{harvtxt|Sharir|Agarwal|1995}}, Chapter 4, pp. 86–114; {{harvtxt|Wiernik|Sharir|1988}}.&amp;lt;/ref&amp;gt;&lt;br /&gt;
*For even values of &#039;&#039;s&#039;&#039; ≥ 4,&amp;lt;ref name=&amp;quot;high-order&amp;quot;&amp;gt;{{harvtxt|Sharir|Agarwal|1995}}, Chapter 3, pp. 43–85; {{harvtxt|Agarwal|Sharir|1989}}; {{harvtxt|Nivasch|1999}}.&amp;lt;/ref&amp;gt;&lt;br /&gt;
::&amp;lt;math&amp;gt;\lambda_s(n)=n\cdot 2^{\frac{1}{t!}\alpha(n)^t(1+o(1))}&amp;lt;/math&amp;gt;, where &#039;&#039;t&#039;&#039;&amp;amp;nbsp;=&amp;amp;nbsp;(&#039;&#039;s&#039;&#039;&amp;amp;nbsp;&amp;amp;minus;&amp;amp;nbsp;2)/2.&lt;br /&gt;
*For odd values of &#039;&#039;s&#039;&#039; ≥ 5 the best known upper bound is &amp;lt;ref name=&amp;quot;high-order&amp;quot; /&amp;gt;&lt;br /&gt;
::&amp;lt;math&amp;gt;\lambda_s(n) &amp;lt; n\cdot 2^{\frac{1}{t!}\alpha(n)^t\log\alpha(n)(1+o(1))}&amp;lt;/math&amp;gt;, where &#039;&#039;t&#039;&#039;&amp;amp;nbsp;=&amp;amp;nbsp;(&#039;&#039;s&#039;&#039;&amp;amp;nbsp;&amp;amp;minus;&amp;amp;nbsp;3)/2.&lt;br /&gt;
However, this bound is not known to be tight.&amp;lt;ref name=&amp;quot;high-order&amp;quot; /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The value of λ&amp;lt;sub&amp;gt;&#039;&#039;s&#039;&#039;&amp;lt;/sub&amp;gt;(&#039;&#039;n&#039;&#039;) is also known when &#039;&#039;s&#039;&#039; is variable but &#039;&#039;n&#039;&#039; is a small constant:&amp;lt;ref&amp;gt;{{harvtxt|Roselle|Stanton|1970/71}}.&amp;lt;/ref&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;\lambda_s(2)=s+1\,&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;\lambda_s(3)=3s-2+(s\, \bmod \, 2)&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;\lambda_s(4)=6s-2+(s\, \bmod\, 2).&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Application to lower envelopes==&lt;br /&gt;
[[Image:Line segment lower envelope.svg|thumb|300px|A Davenport–Schinzel sequence formed by the lower envelope of line segments.]]&lt;br /&gt;
The &#039;&#039;lower envelope&#039;&#039; of a set of functions ƒ&amp;lt;sub&amp;gt;&#039;&#039;i&#039;&#039;&amp;lt;/sub&amp;gt;(&#039;&#039;x&#039;&#039;) of a [[real variable]] &#039;&#039;x&#039;&#039; is the function given by their pointwise minimum:&lt;br /&gt;
:&amp;amp;fnof;(&#039;&#039;x&#039;&#039;)&amp;amp;nbsp;=&amp;amp;nbsp;min&amp;lt;sub&amp;gt;&#039;&#039;i&#039;&#039;&amp;lt;/sub&amp;gt;&amp;amp;fnof;&amp;lt;sub&amp;gt;&#039;&#039;i&#039;&#039;&amp;lt;/sub&amp;gt;(&#039;&#039;x&#039;&#039;).&lt;br /&gt;
Suppose that these functions are particularly well behaved: they are all [[continuous function|continuous]], and any two of them are equal on at most &#039;&#039;s&#039;&#039; values. With these assumptions, the real line can be partitioned into finitely many [[interval (mathematics)|intervals]] within which one function has values smaller than all of the other functions. The sequence of these intervals, labeled by the minimizing function within each interval, forms a Davenport–Schinzel sequence of order &#039;&#039;s&#039;&#039;. Thus, any upper bound on the complexity of a Davenport–Schinzel sequence of this order also bounds the number of intervals in this representation of the lower envelope.&lt;br /&gt;
&lt;br /&gt;
In the original application of Davenport and Schinzel, the functions under consideration were a set of different solutions to the same homogeneous [[linear differential equation]] of order &#039;&#039;s&#039;&#039;. Any two distinct solutions can have at most &#039;&#039;s&#039;&#039; values in common, so the lower envelope of a set of &#039;&#039;n&#039;&#039; distinct solutions forms a &#039;&#039;DS&#039;&#039;(&#039;&#039;n&#039;&#039;,&#039;&#039;s&#039;&#039;)-sequence.&lt;br /&gt;
&lt;br /&gt;
The same concept of a lower envelope can also be applied to functions that are only [[piecewise]] continuous or that are defined only over intervals of the real line; however, in this case, the points of discontinuity of the functions and the endpoints of the interval within which each function is defined add to the order of the sequence. For instance, a non-vertical line segment in the plane can be interpreted as the [[graph of a function]] mapping an interval of &#039;&#039;x&#039;&#039; values to their corresponding &#039;&#039;y&#039;&#039; values, and the lower envelope of a collection of line segments forms a Davenport–Schinzel sequence of order three because any two line segments can form an alternating subsequence with length at most four.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
* [[Squarefree word]]&lt;br /&gt;
&lt;br /&gt;
==Notes==&lt;br /&gt;
{{reflist|2}}&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
*{{citation&lt;br /&gt;
 | last1 = Agarwal | first1 = P. K. | author1-link = Pankaj K. Agarwal&lt;br /&gt;
 | last2 = Sharir | first2 = Micha | authorlink2 = Micha Sharir&lt;br /&gt;
 | last3 = Shor | first3 = P. | authorlink3 = Peter Shor&lt;br /&gt;
 | title = Sharp upper and lower bounds on the length of general Davenport–Schinzel sequences&lt;br /&gt;
 | journal = Journal of Combinatorial Theory, Series A&lt;br /&gt;
 | volume = 52 | issue = 2 | year = 1989 | pages = 228–274&lt;br /&gt;
 | mr = 1022320 | doi = 10.1016/0097-3165(89)90032-0}}.&lt;br /&gt;
*{{citation&lt;br /&gt;
 | last = Atallah | first = Mikhail J.&lt;br /&gt;
 | authorlink = Mikhail Atallah&lt;br /&gt;
 | title = Some dynamic computational geometry problems&lt;br /&gt;
 | journal = Computers and Mathematics with Applications&lt;br /&gt;
 | mr = 0822083 | doi = 10.1016/0898-1221(85)90105-1&lt;br /&gt;
 | volume = 11 | pages = 1171–1181 | year = 1985}}.&lt;br /&gt;
*{{citation&lt;br /&gt;
 | last1 = Davenport | first1 = H. | authorlink1 = Harold Davenport&lt;br /&gt;
 | last2 = Schinzel | first2 = Andrzej | authorlink2 = Andrzej Schinzel&lt;br /&gt;
 | title = A combinatorial problem connected with differential equations&lt;br /&gt;
 | journal = American Journal of Mathematics&lt;br /&gt;
 | volume = 87 | year = 1965 | pages = 684–694&lt;br /&gt;
 | mr = 0190010 | doi = 10.2307/2373068&lt;br /&gt;
 | jstor = 2373068&lt;br /&gt;
 | issue = 3&lt;br /&gt;
 | publisher = The Johns Hopkins University Press}}.&lt;br /&gt;
*{{citation&lt;br /&gt;
 | last1 = Hart | first1 = S.&lt;br /&gt;
 | last2 = Sharir | first2 = Micha | authorlink2 = Micha Sharir&lt;br /&gt;
 | title = Nonlinearity of Davenport–Schinzel sequences and of generalized path compression schemes&lt;br /&gt;
 | journal = Combinatorica&lt;br /&gt;
 | volume = 6 | issue = 2 | year = 1986 | pages = 151–177&lt;br /&gt;
 | mr = 0875839 | doi = 10.1007/BF02579170}}.&lt;br /&gt;
*{{citation&lt;br /&gt;
 | last = Klazar | first = M.&lt;br /&gt;
 | contribution = On the maximum lengths of Davenport–Schinzel sequences&lt;br /&gt;
 | pages = 169–178&lt;br /&gt;
 | publisher = American Mathematical Society&lt;br /&gt;
 | series = DIMACS Series in Discrete Mathematics and Theoretical Computer Science&lt;br /&gt;
 | title = Contemporary Trends in Discrete Mathematics&lt;br /&gt;
 | volume = 49&lt;br /&gt;
 | year = 1999}}.&lt;br /&gt;
*{{citation&lt;br /&gt;
 | authorlink = Péter Komjáth&lt;br /&gt;
 | last = Komjáth | first = Péter&lt;br /&gt;
 | title = A simplified construction of nonlinear Davenport–Schinzel sequences&lt;br /&gt;
 | journal = Journal of Combinatorial Theory, Series A&lt;br /&gt;
 | volume = 49 | year = 1988 | issue = 2 | pages = 262–267&lt;br /&gt;
 | mr = 0964387 | doi = 10.1016/0097-3165(88)90055-6}}.&lt;br /&gt;
*{{citation&lt;br /&gt;
 | last1 = Mullin | first1 = R. C.&lt;br /&gt;
 | last2 = Stanton | first2 = R. G.&lt;br /&gt;
 | title = A map-theoretic approach to Davenport-Schinzel sequences.&lt;br /&gt;
 | journal = Pacific Journal of Mathematics&lt;br /&gt;
 | volume = 40 | year = 1972 | pages = 167–172&lt;br /&gt;
 | url = http://projecteuclid.org/getRecord?id=euclid.pjm/1102968831&lt;br /&gt;
 | mr = 0302601 }}.&lt;br /&gt;
*{{citation&lt;br /&gt;
 | last = Nivasch | first = Gabriel&lt;br /&gt;
 | contribution = Improved bounds and new techniques for Davenport–Schinzel sequences and their generalizations&lt;br /&gt;
 | arxiv = 0807.0484 | pages = 1–10&lt;br /&gt;
 | title = Proc. 20th ACM-SIAM Symp. Discrete Algorithms&lt;br /&gt;
 | url = http://www.siam.org/proceedings/soda/2009/SODA09_001_nivaschg.pdf&lt;br /&gt;
 | year = 2009}}.&lt;br /&gt;
*{{citation&lt;br /&gt;
 | last1 = Roselle | first1 = D. P. | author1-link = David Roselle&lt;br /&gt;
 | last2 = Stanton | first2 = R. G.&lt;br /&gt;
 | title = Some properties of Davenport-Schinzel sequences&lt;br /&gt;
 | journal = Acta Arithmetica&lt;br /&gt;
 | volume = 17 | year = 1970/71 | pages = 355–362&lt;br /&gt;
 | mr = 0284414 }}.&lt;br /&gt;
*{{citation&lt;br /&gt;
 | last1 = Sharir | first1 = Micha | authorlink1 = Micha Sharir&lt;br /&gt;
 | last2 = Agarwal | first2 = Pankaj K.&lt;br /&gt;
 | title = Davenport–Schinzel Sequences and Their Geometric Applications&lt;br /&gt;
 | publisher = Cambridge University Press&lt;br /&gt;
 | year = 1995&lt;br /&gt;
 | isbn = 0-521-47025-0}}.&lt;br /&gt;
*{{citation&lt;br /&gt;
 | last1 = Stanton | first1 = R. G.&lt;br /&gt;
 | last2 = Dirksen | first2 = P. H.&lt;br /&gt;
 | title = Davenport-Schinzel sequences.&lt;br /&gt;
 | journal = Ars Combinatoria&lt;br /&gt;
 | volume = 1 | year = 1976 | issue = 1 | pages = 43–51&lt;br /&gt;
 | mr = 0409347 }}.&lt;br /&gt;
*{{citation&lt;br /&gt;
 | last1 = Stanton | first1 = R. G.&lt;br /&gt;
 | last2 = Roselle | first2 = D. P. | author2-link = David Roselle&lt;br /&gt;
 | contribution = A result on Davenport-Schinzel sequences&lt;br /&gt;
 | title = Combinatorial theory and its applications, III (Proc. Colloq., Balatonfüred, 1969)&lt;br /&gt;
 | pages = 1023–1027&lt;br /&gt;
 | publisher = North-Holland | location = Amsterdam | year = 1970&lt;br /&gt;
 | mr = 0304189 }}.&lt;br /&gt;
*{{citation&lt;br /&gt;
 | last1 = Wiernik | first1 = Ady&lt;br /&gt;
 | last2 = Sharir | first2 = Micha | authorlink2 = Micha Sharir&lt;br /&gt;
 | title = Planar realizations of nonlinear Davenport–Schinzel sequences by segments&lt;br /&gt;
 | journal = Discrete &amp;amp;amp; Computational Geometry&lt;br /&gt;
 | volume = 3 | issue = 1 | year = 1988 | pages = 15–47&lt;br /&gt;
 | mr = 0918177 | doi = 10.1007/BF02187894}}.&lt;br /&gt;
&lt;br /&gt;
== External links ==&lt;br /&gt;
* [http://mathworld.wolfram.com/Davenport-SchinzelSequence.html Davenport-Schinzel Sequence], from [[MathWorld]].&lt;br /&gt;
* [http://planning.cs.uiuc.edu/node304.html  Davenport-Schinzel Sequences], a section in the book &#039;&#039;Motion Planning&#039;&#039;, by Steven M. LaValle.&lt;br /&gt;
&lt;br /&gt;
{{DEFAULTSORT:Davenport-Schinzel sequence}}&lt;br /&gt;
[[Category:Sequences and series]]&lt;br /&gt;
[[Category:Combinatorics on words]]&lt;br /&gt;
[[Category:Discrete geometry]]&lt;/div&gt;</summary>
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