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Dirichlet–Jordan test for Fourier series: fixed minor definition issues regarding "pointwise convergence"
 
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{{distinguish|Dirichlet boundary condition}}
{{redirect-distinguish|Dirichlet conditions|Dirichlet boundary condition}}
In [[mathematics]], the '''Dirichlet–Jordan test''' gives [[sufficient condition]]s for a [[complex numbers|complex-valued]], [[periodic function]] <math>f</math> to be equal to the sum of its [[Fourier series]] at a point of continuity. Moreover, the behavior of the Fourier series at points of discontinuity is determined as well (it is the midpoint of the values of the discontinuity). It is one of many conditions for the [[convergence of Fourier series]].
{{unreferenced|date=December 2014}}
In [[mathematics]], the '''Dirichlet conditions''' are [[sufficient condition]]s for a [[real numbers|real]]-valued, [[periodic function]] ''f''(''x'') to be equal to the sum of its [[Fourier series]] at each point where ''f'' is [[continuous function|continuous]]. Moreover, the behavior of the Fourier series at points of discontinuity is determined as well (it is the midpoint of the values of the discontinuity). These conditions are named after [[Peter Gustav Lejeune Dirichlet]].


The original test was established by [[Peter Gustav Lejeune Dirichlet]] in 1829,<ref>{{citation|author=Dirichlet|year=1829|title=Sur la convergence des series trigonometriques qui servent à represénter une fonction arbitraire entre des limites donnees|journal=J. Reine Angew. Math.|volume= 4|pages=157–169}}</ref> for piecewise [[monotone function]]s (functions with a finite number of sections per period each of which is monotonic). It was extended in the late 19th century by [[Camille Jordan]] to functions of [[bounded variation]] in each period (any function of bounded variation is the difference of two monotonically increasing functions).<ref name="Fourier series and Fourier integrals"/><ref>{{citation|author=C. Jordan|title= Cours d'analyse de l'Ecole Polytechnique, t.2, calcul integral|publisher= Gauthier-Villars, Paris, 1894}}</ref>
The conditions are:
*''f''(''x'') must be [[absolutely integrable]] over a period.
*''f''(''x'') must have a finite number of [[Maxima_and_minima|extrema]] in any given bounded interval, i.e. there must be a finite number of maxima and minima in the interval.
*''f''(''x'') must have a finite number of [[Classification_of_discontinuities|discontinuities]] in any given bounded interval, however the discontinuity cannot be infinite.
*''f''(''x'') must be [[bounded function|bounded]]


==Dirichlet–Jordan test for Fourier series==
The last three conditions are satisfied if ''f'' is a function of [[bounded variation]] over a period.
Let <math>f(x)</math> be complex-valued [[Lebesgue_integral#Complex-valued_functions|integrable]] function on the interval <math>[-\pi,\pi]</math> and the [[Series_(mathematics)#Partial_sum_of_a_series|partial sums]] of its Fourier series <math>S_nf(x)</math>, given by
<math display="block">S_nf(x) = \sum_{k=-n}^nc_k e^{ikx},</math>
with [[Fourier coefficients]] <math>c_k</math> defined as
<math display="block"> c_k = \frac{1}{2\pi} \int_{-\pi}^\pi f(x) e^{-ikx}\, dx.</math>
The Dirichlet-Jordan test states that if <math>f</math> is of [[bounded variation]], then for each <math>x \in [-\pi,\pi]</math> the limit <math>S_nf(x)</math> exists and is equal to{{sfn|Zygmund|Fefferman|2003|p=57}}{{sfn|Lion|1986|pp=281–282}}
<math display="block">\lim_{n \to \infty} S_nf(x) =\lim_{\varepsilon\to 0}\frac{f(x+\varepsilon)+f(x-\varepsilon)}{2}.</math>
Alternatively, Jordan's test states that if <math>f\in L^1</math> is of bounded variation in a neighborhood of <math>x</math>, then the limit of <math>S_nf(x)</math> exists and converges in a similar manner.{{sfn|Edwards|1979|p=156}}


If, in addition, <math>f</math> is continuous at <math>x</math>, then
==Dirichlet's theorem for 1-dimensional Fourier series==
<math display="block">\lim_{n \to \infty} S_nf(x) = f(x).</math>
Moreover, if <math>f</math> is continuous at every point in <math>[-\pi,\pi]</math>, then the convergence is [[uniform convergence|uniform]] rather than just [[pointwise convergence|pointwise]].


The analogous statement holds irrespective of the choice of period of <math>f</math>, or which [[Fourier_series#Synthesis|version of the Fourier series]] is chosen.
We state Dirichlet's theorem assuming ''f'' is a periodic function of period 2π with Fourier series expansion where


== Jordan test for Fourier integrals ==
:<math> a_n = \frac{1}{2\pi} \int_{-\pi}^\pi f(x) e^{-inx}\, dx. </math>
For the [[Fourier transform]] on the real line, there is a version of the test as well.<ref>{{citation|author=[[E. C. Titchmarsh]]|title=Introduction to the theory of Fourier integrals|year=1948|page=13|publisher=Oxford Clarendon Press}}.</ref> Suppose that <math>f(x)</math> is in <math>L^1(-\infty,\infty)</math> and of bounded variation in a neighborhood of the point <math>x</math>. Then
<math display="block">\frac1\pi\lim_{M\to\infty}\int_0^{M}du\int_{-\infty}^\infty f(t)\cos u(x-t)\,dt = \lim_{\varepsilon\to 0}\frac{f(x+\varepsilon)+f(x-\varepsilon)}{2}.</math>
If <math>f</math> is continuous in an open interval, then the integral on the left-hand side converges uniformly in the interval, and the limit on the right-hand side is <math>f(x)</math>.


This version of the test (although not satisfying modern demands for rigor) is historically prior to Dirichlet, being due to [[Joseph Fourier]].<ref name="Fourier series and Fourier integrals">{{citation|author=[[Jaak Peetre]]|title=On Fourier's discovery of Fourier series and Fourier integrals|year=2000|url=https://web.archive.org/web/20221201121132/https://citeseerx.ist.psu.edu/document?repid=rep1&type=pdf&doi=d72e7ff6baf9008d523a192bab2e3400982389d3}}</ref>
The analogous statement holds irrespective of what the period of ''f'' is, or which version of the Fourier expansion is chosen (see [[Fourier series]]).
<br>
:'''Dirichlet's theorem:''' If ''f'' satisfies Dirichlet conditions, then for all ''x'', we have that the series obtained by plugging ''x'' into the Fourier series is convergent, and is given by


== Dirichlet conditions in signal processing ==
::<math> \sum_{n = -\infty}^\infty a_n e^{inx} = \frac{1}{2}(f(x+) + f(x-)), </math>
In [[signal processing]], the test is often retained in the original form due to Dirichlet:<ref name='sands'>{{cite book|last1= Alan V. Oppenheim|last2= Alan S. Willsky|last3= Syed Hamish Nawab|year= 1997|title= Signals & Systems|url= https://books.google.com/books?id=O9ZHSAAACAAJ&q=signals+and+systems|publisher= Prentice Hall| isbn= 9780136511755|page= 198}}</ref>{{sfn|Khare|Butola|Rajora|2023|p=9}}{{sfn|Proakis|Manolakis|1996|p=234}} a piecewise monotone bounded periodic function <math>f</math> (having a finite number of monotonic intervals per period) has a convergent Fourier series whose value at each point is the arithmetic mean of the left and right limits of the function. The condition of piecewise monotonicity stipulates having only finitely many local extrema per period, which implies <math>f</math> is of bounded variation (though the reverse is not true).<ref name="Fourier series and Fourier integrals"/> (Dirichlet required in addition that the function have only finitely many discontinuities, but this constraint is unnecessarily stringent.{{sfn|Lanczos|2016|p=46}}) Any signal that can be physically produced in a laboratory satisfies these conditions.<ref>{{citation|author=B P Lathi|title=Signal processing and linear systems|year=2000|publisher=Oxford}}</ref>


As in the pointwise case of the Jordan test, the condition of boundedness can be relaxed if the function is assumed to be [[absolutely integrable]] (i.e., <math>L^1</math>) over a period, provided it satisfies the other conditions of the test in a neighborhood of the point <math>x</math> where the limit is taken.{{sfn|Lanczos|2016|p=48}}
:where the notation


==See also==
::<math> f(x+) = \lim_{y \to x^+} f(y) </math>
* [[Dini test]]
::<math> f(x-) = \lim_{y \to x^-} f(y) </math>


==Notes==
:denotes the right/left limits of ''f''.
{{Reflist}}

==References==
A function satisfying Dirichlet's conditions must have right and left limits at each point of discontinuity, or else the function would need to oscillate at that point, violating the condition on maxima/minima. Note that at any point where ''f'' is continuous,
* {{cite book | last=Edwards | first=R. E. | title=Fourier Series | publisher=Springer New York | publication-place=New York, NY | volume=64 | date=1979 | isbn=978-1-4612-6210-7 | doi=10.1007/978-1-4612-6208-4}}

* {{cite book | last=Lanczos | first=Cornelius | title=Discourse on Fourier Series | publisher=Society for Industrial and Applied Mathematics | publication-place=Philadelphia, PA | date=2016-09-12 | isbn=978-1-61197-451-5 | doi=10.1137/1.9781611974522 | doi-access=free | url=https://epubs.siam.org/doi/pdf/10.1137/1.9781611974522.fm | access-date=2024-12-15}}
:<math> \frac{1}{2}(f(x+) + f(x-)) = f(x). </math>
* {{cite journal | last=Lion | first=Georges A. | title=A Simple Proof of the Dirichlet-Jordan Convergence Test | journal=The American Mathematical Monthly | volume=93 | issue=4 | date=1986 | issn=0002-9890 | doi=10.1080/00029890.1986.11971805 | pages=281–282}}

* {{cite book | last1=Khare | first1=Kedar | last2=Butola | first2=Mansi | last3=Rajora | first3=Sunaina | title=Fourier Optics and Computational Imaging | publisher=Springer International Publishing | publication-place=Cham | date=2023 | isbn=978-3-031-18352-2 | doi=10.1007/978-3-031-18353-9}}
Thus Dirichlet's theorem says in particular that under the Dirichlet conditions the Fourier series for ''f'' converges and is equal to ''f'' wherever ''f'' is continuous.
* {{cite book|last1=Proakis|first1=John G. |last2=Manolakis|first2=Dimitris G.|author2-link= Dimitris Manolakis |title=Digital Signal Processing: Principles, Algorithms, and Applications|url=https://archive.org/details/digitalsignalpro00proa|url-access=registration|year=1996|publisher=Prentice Hall|isbn=978-0-13-373762-2|edition=3rd}}
* {{cite book | last=Zygmund | first=A. | last2=Fefferman | first2=Robert | title=Trigonometric Series | publisher=Cambridge University Press | date=2003-02-06 | isbn=978-0-521-89053-3 | doi=10.1017/cbo9781316036587}}


==External links==
==External links==
*{{planetmath reference|id=3891|title=Dirichlet conditions}}
*{{planetmath reference|urlname=DirichletConditions|title=Dirichlet conditions}}


[[Category:Fourier series]]
[[Category:Fourier series]]
[[Category:Theorems in analysis]]
[[Category:Theorems in analysis]]
{{DEFAULTSORT:Dirichlet-Jordan test}}

Latest revision as of 08:38, 23 December 2024

In mathematics, the Dirichlet–Jordan test gives sufficient conditions for a complex-valued, periodic function to be equal to the sum of its Fourier series at a point of continuity. Moreover, the behavior of the Fourier series at points of discontinuity is determined as well (it is the midpoint of the values of the discontinuity). It is one of many conditions for the convergence of Fourier series.

The original test was established by Peter Gustav Lejeune Dirichlet in 1829,[1] for piecewise monotone functions (functions with a finite number of sections per period each of which is monotonic). It was extended in the late 19th century by Camille Jordan to functions of bounded variation in each period (any function of bounded variation is the difference of two monotonically increasing functions).[2][3]

Dirichlet–Jordan test for Fourier series

[edit]

Let be complex-valued integrable function on the interval and the partial sums of its Fourier series , given by with Fourier coefficients defined as The Dirichlet-Jordan test states that if is of bounded variation, then for each the limit exists and is equal to[4][5] Alternatively, Jordan's test states that if is of bounded variation in a neighborhood of , then the limit of exists and converges in a similar manner.[6]

If, in addition, is continuous at , then Moreover, if is continuous at every point in , then the convergence is uniform rather than just pointwise.

The analogous statement holds irrespective of the choice of period of , or which version of the Fourier series is chosen.

Jordan test for Fourier integrals

[edit]

For the Fourier transform on the real line, there is a version of the test as well.[7] Suppose that is in and of bounded variation in a neighborhood of the point . Then If is continuous in an open interval, then the integral on the left-hand side converges uniformly in the interval, and the limit on the right-hand side is .

This version of the test (although not satisfying modern demands for rigor) is historically prior to Dirichlet, being due to Joseph Fourier.[2]

Dirichlet conditions in signal processing

[edit]

In signal processing, the test is often retained in the original form due to Dirichlet:[8][9][10] a piecewise monotone bounded periodic function (having a finite number of monotonic intervals per period) has a convergent Fourier series whose value at each point is the arithmetic mean of the left and right limits of the function. The condition of piecewise monotonicity stipulates having only finitely many local extrema per period, which implies is of bounded variation (though the reverse is not true).[2] (Dirichlet required in addition that the function have only finitely many discontinuities, but this constraint is unnecessarily stringent.[11]) Any signal that can be physically produced in a laboratory satisfies these conditions.[12]

As in the pointwise case of the Jordan test, the condition of boundedness can be relaxed if the function is assumed to be absolutely integrable (i.e., ) over a period, provided it satisfies the other conditions of the test in a neighborhood of the point where the limit is taken.[13]

See also

[edit]

Notes

[edit]
  1. ^ Dirichlet (1829), "Sur la convergence des series trigonometriques qui servent à represénter une fonction arbitraire entre des limites donnees", J. Reine Angew. Math., 4: 157–169
  2. ^ a b c Jaak Peetre (2000), On Fourier's discovery of Fourier series and Fourier integrals
  3. ^ C. Jordan, Cours d'analyse de l'Ecole Polytechnique, t.2, calcul integral, Gauthier-Villars, Paris, 1894
  4. ^ Zygmund & Fefferman 2003, p. 57.
  5. ^ Lion 1986, pp. 281–282.
  6. ^ Edwards 1979, p. 156.
  7. ^ E. C. Titchmarsh (1948), Introduction to the theory of Fourier integrals, Oxford Clarendon Press, p. 13.
  8. ^ Alan V. Oppenheim; Alan S. Willsky; Syed Hamish Nawab (1997). Signals & Systems. Prentice Hall. p. 198. ISBN 9780136511755.
  9. ^ Khare, Butola & Rajora 2023, p. 9.
  10. ^ Proakis & Manolakis 1996, p. 234.
  11. ^ Lanczos 2016, p. 46.
  12. ^ B P Lathi (2000), Signal processing and linear systems, Oxford
  13. ^ Lanczos 2016, p. 48.

References

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