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Welch bounds

From Wikipedia, the free encyclopedia

Inmathematics,Welch bounds are a family ofinequalities pertinent to the problem of evenly spreading a set of unitvectors in avector space. The bounds are important tools in the design and analysis of certain methods intelecommunication engineering, particularly incoding theory. The bounds were originally published in a 1974 paper byL. R. Welch.[1]

Mathematical statement

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If{x1,,xm}{\displaystyle \{x_{1},\ldots ,x_{m}\}} are unit vectors inCn{\displaystyle \mathbb {C} ^{n}}, definecmax=maxij|xi,xj|{\displaystyle c_{\max }=\max _{i\neq j}|\langle x_{i},x_{j}\rangle |}, where,{\displaystyle \langle \cdot ,\cdot \rangle } is the usualinner product onCn{\displaystyle \mathbb {C} ^{n}}. Then the following inequalities hold fork=1,2,{\displaystyle k=1,2,\dots }:(cmax)2k1m1[m(n+k1k)1].{\displaystyle (c_{\max })^{2k}\geq {\frac {1}{m-1}}\left[{\frac {m}{\binom {n+k-1}{k}}}-1\right].}Welch bounds are also sometimes stated in terms of the averaged squared overlap between the set of vectors. In this case, one has the inequality[2][3][4]1m2i,j=1m|xi,xj|2k1(n+k1k).{\displaystyle {\frac {1}{m^{2}}}\sum _{i,j=1}^{m}|\langle x_{i},x_{j}\rangle |^{2k}\geq {\frac {1}{\binom {n+k-1}{k}}}.}

Applicability

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Ifmn{\displaystyle m\leq n}, then the vectors{xi}{\displaystyle \{x_{i}\}} can form anorthonormal set inCn{\displaystyle \mathbb {C} ^{n}}. In this case,cmax=0{\displaystyle c_{\max }=0} and the bounds are vacuous. Consequently, interpretation of the bounds is only meaningful ifm>n{\displaystyle m>n}. This will be assumed throughout the remainder of this article.

Proof fork = 1

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The "first Welch bound," corresponding tok=1{\displaystyle k=1}, is by far the most commonly used in applications. Its proof proceeds in two steps, each of which depends on a more basic mathematical inequality. The first step invokes theCauchy–Schwarz inequality and begins by considering them×m{\displaystyle m\times m}Gram matrixG{\displaystyle G} of the vectors{xi}{\displaystyle \{x_{i}\}}; i.e.,

G=[x1,x1x1,xmxm,x1xm,xm]{\displaystyle G=\left[{\begin{array}{ccc}\langle x_{1},x_{1}\rangle &\cdots &\langle x_{1},x_{m}\rangle \\\vdots &\ddots &\vdots \\\langle x_{m},x_{1}\rangle &\cdots &\langle x_{m},x_{m}\rangle \end{array}}\right]}

Thetrace ofG{\displaystyle G} is equal to the sum of its eigenvalues. Because therank ofG{\displaystyle G} is at mostn{\displaystyle n}, and it is apositive semidefinite matrix,G{\displaystyle G} has at mostn{\displaystyle n} positiveeigenvalues with its remaining eigenvalues all equal to zero. Writing the non-zero eigenvalues ofG{\displaystyle G} asλ1,,λr{\displaystyle \lambda _{1},\ldots ,\lambda _{r}} withrn{\displaystyle r\leq n} and applying the Cauchy-Schwarz inequality to the inner product of anr{\displaystyle r}-vector of ones with a vector whose components are these eigenvalues yields

(TrG)2=(i=1rλi)2ri=1rλi2ni=1mλi2{\displaystyle (\mathrm {Tr} \;G)^{2}=\left(\sum _{i=1}^{r}\lambda _{i}\right)^{2}\leq r\sum _{i=1}^{r}\lambda _{i}^{2}\leq n\sum _{i=1}^{m}\lambda _{i}^{2}}

The square of theFrobenius norm (Hilbert–Schmidt norm) ofG{\displaystyle G} satisfies

||G||2=i=1mj=1m|xi,xj|2=i=1mλi2{\displaystyle ||G||^{2}=\sum _{i=1}^{m}\sum _{j=1}^{m}|\langle x_{i},x_{j}\rangle |^{2}=\sum _{i=1}^{m}\lambda _{i}^{2}}

Taking this together with the preceding inequality gives

i=1mj=1m|xi,xj|2(TrG)2n{\displaystyle \sum _{i=1}^{m}\sum _{j=1}^{m}|\langle x_{i},x_{j}\rangle |^{2}\geq {\frac {(\mathrm {Tr} \;G)^{2}}{n}}}

Because eachxi{\displaystyle x_{i}} has unit length, the elements on the main diagonal ofG{\displaystyle G} are ones, and hence its trace isTrG=m{\displaystyle \mathrm {Tr} \;G=m}. So,

i=1mj=1m|xi,xj|2=m+ij|xi,xj|2m2n{\displaystyle \sum _{i=1}^{m}\sum _{j=1}^{m}|\langle x_{i},x_{j}\rangle |^{2}=m+\sum _{i\neq j}|\langle x_{i},x_{j}\rangle |^{2}\geq {\frac {m^{2}}{n}}}

or

ij|xi,xj|2m(mn)n{\displaystyle \sum _{i\neq j}|\langle x_{i},x_{j}\rangle |^{2}\geq {\frac {m(m-n)}{n}}}

The second part of the proof uses an inequality encompassing the simple observation that the average of a set of non-negative numbers can be no greater than the largest number in the set. In mathematical notation, ifa0{\displaystyle a_{\ell }\geq 0} for=1,,L{\displaystyle \ell =1,\ldots ,L}, then

1L=1Lamaxa{\displaystyle {\frac {1}{L}}\sum _{\ell =1}^{L}a_{\ell }\leq \max a_{\ell }}

The previous expression hasm(m1){\displaystyle m(m-1)} non-negative terms in the sum, the largest of which iscmax2{\displaystyle c_{\max }^{2}}. So,

(cmax)21m(m1)ij|xi,xj|2mnn(m1){\displaystyle (c_{\max })^{2}\geq {\frac {1}{m(m-1)}}\sum _{i\neq j}|\langle x_{i},x_{j}\rangle |^{2}\geq {\frac {m-n}{n(m-1)}}}

or

(cmax)2mnn(m1){\displaystyle (c_{\max })^{2}\geq {\frac {m-n}{n(m-1)}}}

which is precisely the inequality given by Welch in the case thatk=1{\displaystyle k=1}.

Achieving the Welch bounds

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In certain telecommunications applications, it is desirable to construct sets of vectors that meet the Welch bounds with equality. Several techniques have been introduced to obtain so-calledWelch Bound Equality (WBE) sets of vectors for thek=1{\displaystyle k=1} bound.

The proof given above shows that two separate mathematical inequalities are incorporated into the Welch bound whenk=1{\displaystyle k=1}. The Cauchy–Schwarz inequality is met with equality when the two vectors involved are collinear. In the way it is used in the above proof, this occurs when all the non-zero eigenvalues of the Gram matrixG{\displaystyle G} are equal, which happens precisely when the vectors{x1,,xm}{\displaystyle \{x_{1},\ldots ,x_{m}\}} constitute atight frame forCn{\displaystyle \mathbb {C} ^{n}}.

The other inequality in the proof is satisfied with equality if and only if|xi,xj|{\displaystyle |\langle x_{i},x_{j}\rangle |} is the same for every choice ofij{\displaystyle i\neq j}. In this case, the vectors areequiangular. So this Welch bound is met with equality if and only if the set of vectors{xi}{\displaystyle \{x_{i}\}} is an equiangular tight frame inCn{\displaystyle \mathbb {C} ^{n}}.

Similarly, the Welch bounds stated in terms of average squared overlap, are saturated for allkt{\displaystyle k\leq t} if and only if the set of vectors is at{\displaystyle t}-design in the complex projective spaceCPn1{\displaystyle \mathbb {CP} ^{n-1}}.[4]


See also

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References

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  1. ^Welch, L. (1974-05-01)."Lower bounds on the maximum cross correlation of signals (Corresp.)".IEEE Transactions on Information Theory.20 (3):397–399.doi:10.1109/TIT.1974.1055219.ISSN 1557-9654.
  2. ^Klappenecker, Andreas; Roetteler, Martin (2005-02-11). "Mutually Unbiased Bases are Complex Projective 2-Designs".arXiv:quant-ph/0502031.{{cite journal}}:Cite journal requires|journal= (help)
  3. ^Belovs, Aleksandrs; Smotrovs, Juris (2008-07-22). "A Criterion for Attaining the Welch Bounds with Applications for Mutually Unbiased Bases".arXiv:0802.0855.{{cite journal}}:Cite journal requires|journal= (help)
  4. ^abDatta, Somantika; Howard, Stephen; Cochran, Douglas (2012-05-29). "Geometry of the Welch Bounds".arXiv:0909.0206.{{cite journal}}:Cite journal requires|journal= (help)
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