Harmonic Analysis

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Harmonic analysis
For the process of determining the structure of a piece of these requirements in terms of the Fourier transform of
music, see Harmony.
f. The Paley–Wiener theorem is an example of this. The
Harmonic analysis is a branch of mathematics con- Paley–Wiener theorem immediately implies that if f is
a nonzero distribution of compact support (these include
Light Harmonics
functions of compact support), then its Fourier transform
is never compactly supported. This is a very elementary
form of an uncertainty principle in a harmonic analysis
setting. See also: Convergence of Fourier series.
650nm − Red

607nm − Orange
578nm − Yellow
520nm − Green
487nm − Blue

475nm − Indigo

Fourier series can be conveniently studied in the context
of Hilbert spaces, which provides a connection between
harmonic analysis and functional analysis.

405nm − Violet
325nm − UV

Har monics of red light in relation to other colors
λ/14 −
λ/8 −
λ/4 −

1 Applied harmonic analysis

λ/3 −
λ/2.67 −
λ/2.5 −
λ/2 −

White light (all colors interfer ing with each other)

The harmonics of color. The harmonic-analysis chart shows
how the different wavelengths interact with red light. At a difference of λ/2 (wavelength/2), red is perfectly in sync with its
second-generation harmonic in the ultraviolet. All other wavelengths in the visual spectrum have less than a λ/2 difference
between them, forming harmonic oscillations in the combined
waves. At λ/14, the oscillations will cycle every fourteenth wave,
while at λ/8 they will cycle every eighth. The oscillations are
most rapid at λ/4, cycling every fourth wave, while at λ/3 they
cycle every seventh wave, and at λ/2.5 they cycle every thirteenth.
The lower section shows how the λ/4 harmonic interacts in visible
light (green and red), as photographed in an optical flat.

Bass guitar time signal of open string A note (55 Hz).

cerned with the representation of functions or signals as
the superposition of basic waves, and the study of and
generalization of the notions of Fourier series and Fourier
transforms (i.e. an extended form of Fourier analysis).
In the past two centuries, it has become a vast subject
with applications in areas as diverse as signal processing,
quantum mechanics, tidal analysis and neuroscience.
The term "harmonics" originated as the ancient Greek
word, “harmonikos,” meaning “skilled in music.”[1] In
physical eigenvalue problems it began to mean waves
whose frequencies are integer multiples of one another, as
are the frequencies of the harmonics of music notes, but
the term has been generalized beyond its original meaning.

Fourier transform of bass guitar time signal of open string A
note (55 Hz), computed with https://sourceforge.net/projects/
amoreaccuratefouriertransform/ .

Many applications of harmonic analysis in science and
engineering begin with the idea or hypothesis that a phenomenon or signal is composed of a sum of individual oscillatory components. Ocean tides and vibrating strings
are common and simple examples. The theoretical approach is often to try to describe the system by a differential equation or system of equations to predict the essential features, including the amplitude, frequency, and

The classical Fourier transform on Rn is still an area of
ongoing research, particularly concerning Fourier transformation on more general objects such as tempered distributions. For instance, if we impose some requirements on a distribution f, we can attempt to translate
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5

REFERENCES

phases of the oscillatory components. The specific equations depend on the field, but theories generally try to select equations that represent major principles that are applicable.

If the group is neither abelian nor compact, no general satisfactory theory is currently known. (“Satisfactory” means at least as strong as the Plancherel theorem.) However, many specific cases have been analyzed,
The experimental approach is usually to acquire data for example SLn. In this case, representations in infinite
that accurately quantifies the phenomenon. For exam- dimensions play a crucial role.
ple, in a study of tides, the experimentalist would acquire
samples of water depth as a function of time at closely
enough spaced intervals to see each oscillation and over 3 Other branches
a long enough duration that multiple oscillatory periods
are likely included. In a study on vibrating strings, it is
• Study of the eigenvalues and eigenvectors of the
common for the experimentalist to acquire a sound waveLaplacian on domains, manifolds, and (to a lesser
form sampled at a rate at least twice that of the highest
extent) graphs is also considered a branch of harfrequency expected and for a duration many times the pemonic analysis. See e.g., hearing the shape of a
riod of the lowest frequency expected.
drum.
For example, the top signal at the right is a sound waveform of a bass guitar playing an open string corresponding
to an A note with fundamental frequency or 55 Hz. The
waveform appears oscillatory, but it is more complex than
a simple sine wave, indicating the presence of additional
waves. The different wave components contributing to
the sound can be revealed by applying a mathematical
analysis technique known as the Fourier transform, which
is shown in the lower figure. Note that there is a prominent peak at 55 Hz, but that there are other peaks at 110
Hz, 165 Hz, and at other frequencies corresponding to integer multiples of 55 Hz. In this case, 55 Hz is identified
as the fundamental frequency of the string vibration, and
the integer multiples are known as harmonics.

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Abstract harmonic analysis

One of the most modern branches of harmonic analysis,
having its roots in the mid-twentieth century, is analysis
on topological groups. The core motivating ideas are the
various Fourier transforms, which can be generalized to a
transform of functions defined on Hausdorff locally compact topological groups.
The theory for abelian locally compact groups is called
Pontryagin duality.
Harmonic analysis studies the properties of that duality
and Fourier transform, and attempts to extend those features to different settings, for instance to the case of nonabelian Lie groups.
For general non-abelian locally compact groups, harmonic analysis is closely related to the theory of unitary group representations. For compact groups, the
Peter–Weyl theorem explains how one may get harmonics by choosing one irreducible representation out of each
equivalence class of representations. This choice of harmonics enjoys some of the useful properties of the classical Fourier transform in terms of carrying convolutions
to pointwise products, or otherwise showing a certain understanding of the underlying group structure. See also:
Non-commutative harmonic analysis.

• Harmonic analysis on Euclidean spaces deals with
properties of the Fourier transform on Rn that have
no analog on general groups. For example, the fact
that the Fourier transform is rotation invariant. Decomposing the Fourier transform into its radial and
spherical components leads to topics such as Bessel
functions and spherical harmonics.
• Harmonic analysis on tube domains is concerned
with generalizing properties of Hardy spaces to
higher dimensions.

4 See also
• Harmonic (mathematics)
• Spectral density estimation

5 References
[1] http://www.etymonline.com/index.php?term=harmonic

• Elias Stein and Guido Weiss, Introduction to Fourier
Analysis on Euclidean Spaces, Princeton University
Press, 1971. ISBN 0-691-08078-X
• Elias Stein with Timothy S. Murphy, Harmonic
Analysis: Real-Variable Methods, Orthogonality,
and Oscillatory Integrals, Princeton University
Press, 1993.
• Elias Stein, Topics in Harmonic Analysis Related to
the Littlewood-Paley Theory, Princeton University
Press, 1970.
• Yitzhak Katznelson, An introduction to harmonic
analysis, Third edition. Cambridge University
Press, 2004. ISBN 0-521-83829-0; 0-521-543592

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• Terence Tao, Fourier Transform. (Introduces the
decomposition of functions into odd + even parts as
a harmonic decomposition over ℤ₂.)
• Yurii I. Lyubich. Introduction to the Theory of
Banach Representations of Groups. Translated
from the 1985 Russian-language edition (Kharkov,
Ukraine). Birkhäuser Verlag. 1988.

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6 TEXT AND IMAGE SOURCES, CONTRIBUTORS, AND LICENSES

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Text and image sources, contributors, and licenses

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• Harmonic analysis Source: https://en.wikipedia.org/wiki/Harmonic_analysis?oldid=702632299 Contributors: AxelBoldt, Zundark,
ChangChienFu, Michael Hardy, Gabbe, Looxix~enwiki, Stevan White, Stevenj, Rob Hooft, Revolver, Charles Matthews, Dysprosia,
Hyacinth, Samsara, Robbot, Sverdrup, Giftlite, BenFrantzDale, CSTAR, D6, Gadykozma, Gauge, DanP, Bobo192, La goutte de pluie,
Drf5n, Msh210, Linas, Guardian of Light, BD2412, FlaBot, Jeff02, Krishnavedala, Sunev, YurikBot, RobotE, Gaius Cornelius, Wiki
alf, Tong~enwiki, Dhollm, Crasshopper, Levnir, Kompik, Reyk, Banus, SmackBot, Saihtam, Chrislewis.au, Chlewbot, Mhym, Radagast83, LaMenta3, Zero sharp, Prof.Maque, Basawala, Tawkerbot4, Thijs!bot, Thenub314, VoABot II, David Eppstein, R'n'B, Maurice
Carbonaro, Vanished user 39948282, JohnBlackburne, Random3f, Digby Tantrum, Seraphita~enwiki, Addbot, Fgnievinski, Topology Expert, CarsracBot, Zaereth, Omnipaedista, Kiefer.Wolfowitz, EmausBot, KHamsun, Slawekb, Mmqte, Boashash, MerlIwBot, Solomon7968,
Brad7777, Declaration1776, Lemnaminor, Erru il 1988, Sheliazhenko, Niki Goss, KasparBot, Fourier1789, Headabot and Anonymous:
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Images

• File:Bass_Guitar_Time_Signal_of_open_string_A_note_(55_Hz).png Source: https://upload.wikimedia.org/wikipedia/commons/a/
a6/Bass_Guitar_Time_Signal_of_open_string_A_note_%2855_Hz%29.png License: CC BY-SA 4.0 Contributors: Own work Original
artist: Fourier1789
• File:Fourier_Transform_of_bass_guitar_time_signal.png Source: https://upload.wikimedia.org/wikipedia/commons/0/08/Fourier_
Transform_of_bass_guitar_time_signal.png License: CC BY-SA 4.0 Contributors: Own work Original artist: Fourier1789
• File:Light_wave_harmonic_diagram.svg Source:
https://upload.wikimedia.org/wikipedia/commons/7/71/Light_wave_harmonic_
diagram.svg License: CC BY-SA 3.0 Contributors: Own work Original artist: Rubber Duck (☮ • ✍)

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Content license

• Creative Commons Attribution-Share Alike 3.0

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