Hurwitz determinant: Difference between revisions

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In [[mathematical analysis]], the '''Dirichlet kernel''' is the collection of functions
 
:<math>D_n(x)=\sum_{k=-n}^n
e^{ikx}=1+2\sum_{k=1}^n\cos(kx)=\frac{\sin\left(\left(n +1/2\right) x \right)}{\sin(x/2)}.</math>
 
It is named after [[Peter Gustav Lejeune Dirichlet]].
 
The importance of the Dirichlet kernel comes from its relation to [[Fourier series]]. The [[convolution]] of ''D<sub>n</sub>''(''x'') with any function ''f'' of period 2π is the ''n''th-degree Fourier series approximation to ''f'', i.e., we have
 
:<math>(D_n*f)(x)=\frac{1}{2\pi}\int_{-\pi}^\pi f(y)D_n(x-y)\,dy=\sum_{k=-n}^n \hat{f}(k)e^{ikx},</math>
 
where
 
:<math>\hat{f}(k)=\frac{1}{2\pi}\int_{-\pi}^\pi f(x)e^{-ikx}\,dx</math>
 
is the ''k''th Fourier coefficient of ''f''. This implies that in order to study convergence of Fourier series it is enough to study properties of the Dirichlet kernel. Of particular importance is the fact that the [[Lp space|''L''<sup>1</sup>]] norm of ''D<sub>n</sub>'' diverges to infinity as ''n'' → ∞. One can estimate that
 
:<math>\| D_n \| _{L^1} \approx \log n</math>
 
where <math>\approx</math> denotes "is of the order." This lack of uniform integrability is behind many divergence phenomena for the Fourier series. For example, together with the [[uniform boundedness principle]], it can be used to show that the Fourier series of a [[continuous function]] may fail to converge pointwise, in rather dramatic fashion. See [[convergence of Fourier series]] for further details.
 
[[File:Dirichlet.png|thumb|400px|Plot of the first few Dirichlet kernels]]
 
==Relation to the delta function==
<!--I am not sure this is useful here.
 
To understand the definition, one can see that it is 2&pi; times the ''n''th-degree Fourier series approximation to a "function" with period 2&pi; given by
 
:<math>\delta_p(x)=\sum_{k=-\infty}^\infty\delta(x-2\pi k)</math>
where &delta;-->
 
Take the [[periodic function|periodic]] [[Dirac delta function]], which is not really a function, in the sense of mapping one set into another, but is rather a "[[generalized function]]", also called a "distribution", and multiply by 2π. We get the [[identity element]] for convolution on functions of period 2π. In other words, we have
 
:<math>f*(2\pi \delta)=f \,</math>
 
for every function ''f'' of period 2π. The Fourier series representation of this "function" is
 
:<math>2\pi \delta(x)\sim\sum_{k=-\infty}^\infty e^{ikx}=\left(1 +2\sum_{k=1}^\infty\cos(kx)\right).</math>
 
Therefore the Dirichlet kernel, which is just the sequence of partial sums of this series, can be thought of as an ''[[approximate identity]]''. Abstractly speaking it is not however an approximate identity of ''positive'' elements (hence the failures mentioned above).
 
==Proof of the trigonometric identity==
 
The [[trigonometric identity]]
 
:<math>\sum_{k=-n}^n e^{ikx}
=\frac{\sin((n+1/2)x)}{\sin(x/2)}</math>
 
displayed at the top of this article may be established as follows. First recall that the sum of a finite [[geometric series]] is
 
:<math>\sum_{k=0}^n a r^k=a\frac{1-r^{n+1}}{1-r}.</math>
 
In particular, we have
 
:<math>\sum_{k=-n}^n r^k=r^{-n}\cdot\frac{1-r^{2n+1}}{1-r}.</math>
 
Multiply both the numerator and the denominator by ''r''<sup>&minus;1/2</sup>, getting
 
:<math>\frac{r^{-n-1/2}}{r^{-1/2}}\cdot\frac{1-r^{2n+1}}{1-r} =\frac{r^{-n-1/2}-r^{n+1/2}}{r^{-1/2}-r^{1/2}}.</math>
 
In the case ''r'' = ''e''<sup>''ix''</sup> we have
 
:<math>\sum_{k=-n}^n e^{ikx}=\frac{e^{-(n+1/2)ix}-e^{(n+1/2)ix}}{e^{-ix/2}-e^{ix/2}} =\frac{-2i\sin((n+1/2)x)}{-2i\sin(x/2)} = \frac{\sin((n+1/2)x)}{\sin(x/2)}</math>
 
as required.
 
===Alternative proof of the trigonometric identity===
 
Start with the series
 
:<math>f(x) = 1/2 + \sum_{k=1}^n\cos(kx).</math>
 
Multiply both sides of the above by
 
:<math>2\sin(x/2)\!</math>
 
and use the trigonometric identity
 
:<math>\cos(a)\sin(b) = (\sin(a + b) - \sin(a - b))/2\!</math>
 
to reduce the r.h.s. to
 
:<math>\sin((n + 1/2)x).\!</math>
 
== Variant of identity ==
If the sum is only over positive integers (which may arise when computing a DFT that is not centered), then using similar techniques we can show the following identity:
:<math>\sum_{k=0}^n e^{ikx}
=e^{ixn/2}\frac{\sin((n/2+1/2)x)}{\sin(x/2)}</math>
 
==References==
* Andrew M. Bruckner, Judith B. Bruckner, Brian S. Thomson: ''Real Analysis''. ClassicalRealAnalysis.com 1996, ISBN 0-13-458886-X, S.620 ([http://books.google.de/books?id=1WY6u0C_jEsC vollständige Online-Version (Google Books)])
* {{springer|title=Dirichlet kernel|id=p/d032880}}
* [http://planetmath.org/encyclopedia/DirichletKernel.html Dirichlet-Kernel at [[PlanetMath]]]
 
[[Category:Mathematical analysis]]
[[Category:Fourier series]]
[[Category:Approximation theory]]
[[Category:Articles containing proofs]]

Latest revision as of 14:24, 5 May 2014

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