DA
All
Articles
Dictionary
Quotes
Map

Wikiwand ❤️ Wikipedia

PrivacyTerms

Fouriertransformation

From Wikipedia, the free encyclopedia

Frekvensrummet
Matematikken bag FouriertransformationenAlternative definitionerDiskret FouriertransformationTabel over vigtige FouriertransformationerFunktionelle sammenhængeKvadratisk-integrable funktionerFordelingerTo-dimensionelle funktionerFormler for generelle n-dimensionelle funktionerKilder/referencerSe ogsåHenvisning

Fouriertransformation også kaldet Fourierafbildning er en matematisk funktion der bruges inden for blandt andet signalbehandling. En Fouriertransformation benyttes til at omregne mellem et tidsdomæne (tidssignal) til et frekvensdomæne (superposition af frekvenser).

For eksempel kan man med Fouriertransformation "måle" hvilke rene toner, der indgår i en digital indspilning af en stump musik. Man kan betragte en Fouriertransformation som en måde at nedbryde en funktion, så alle dens frekvenskomponenter bliver adskilt i et frekvensspektrum. Omvendt vil en invers-Fouriertransformation af et spektrum ideelt set resultere i funktionen selv. Man kan sammenligne det med at tage en akkord (funktionen) og adskille den i de enkelte toner (frekvenser), som den indeholder.

Fouriertransformationen er en uendelig linearkombination af sinus og cosinus funktioner, omskrevet til komplekse funktioner. Den er opkaldt efter den franske matematiker Joseph Fourier. Fourierrækker er et nært beslægtet område.

Fouriertransformation af et kontinuert-tidssignal x ( t ) {\displaystyle x(t)} {\displaystyle x(t)} er givet ved følgende integral:

X ( ω ) = ∫ − ∞ ∞ x ( t ) e − i ω t d t {\displaystyle X(\omega )=\int _{-\infty }^{\infty }x(t)\,e^{-i\omega t}\,dt} {\displaystyle X(\omega )=\int _{-\infty }^{\infty }x(t)\,e^{-i\omega t}\,dt}.

Her er ω {\displaystyle \omega } {\displaystyle \omega } vinkelfrekvensen, e {\displaystyle e} {\displaystyle e} er grundtallet for den naturlige logaritme og i {\displaystyle i} {\displaystyle i} er den imaginære enhed. Denne operation betegnes også som Fourieranalyse. Tilsvarende kan den inverse Fouriertransformation defineres som:

x ( t ) = 1 2 π ∫ − ∞ ∞ X ( ω ) e i ω t d ω {\displaystyle x(t)={\frac {1}{2\pi }}\int _{-\infty }^{\infty }X(\omega )\,e^{i\omega t}\,d\omega } {\displaystyle x(t)={\frac {1}{2\pi }}\int _{-\infty }^{\infty }X(\omega )\,e^{i\omega t}\,d\omega }

Den inverse operation betegnes også som Fouriersyntese. I mange sammenhænge er x ( t ) {\displaystyle x(t)} {\displaystyle x(t)} en reel funktion, mens X ( ω ) {\displaystyle X(\omega )} {\displaystyle X(\omega )} ofte bliver til en kompleks funktion.

Bruger man den cykliske frekvens ν = ω / 2 π {\displaystyle \nu =\omega /2\pi } {\displaystyle \nu =\omega /2\pi } i stedet for vinkelfrekvensen ω {\displaystyle \omega } {\displaystyle \omega } får man Fourierintegralerne til at blive:

X ( ν ) = ∫ − ∞ ∞ x ( t ) e − i 2 π ν t d t {\displaystyle X(\nu )=\int _{-\infty }^{\infty }x(t)\,e^{-i2\pi \nu t}\,dt} {\displaystyle X(\nu )=\int _{-\infty }^{\infty }x(t)\,e^{-i2\pi \nu t}\,dt}
x ( t ) = ∫ − ∞ ∞ X ( ν ) e i 2 π ν t d ν {\displaystyle x(t)=\int _{-\infty }^{\infty }X(\nu )\,e^{i2\pi \nu t}\,d\nu } {\displaystyle x(t)=\int _{-\infty }^{\infty }X(\nu )\,e^{i2\pi \nu t}\,d\nu }

Med Eulers formel kan man omskrive Fourierintegralerne så de bliver udtrykt med sinus og cosinus funktionerne:

X ( ω ) = ∫ − ∞ ∞ x ( t ) e − i ω t d t = ∫ − ∞ ∞ x ( t ) ( cos ⁡ ( ω t ) − i sin ⁡ ( ω t ) ) d t = ∫ − ∞ ∞ x ( t ) cos ⁡ ( ω t ) d t − i ∫ − ∞ ∞ x ( t ) sin ⁡ ( ω t ) d t {\displaystyle {\begin{aligned}X(\omega )&=\int _{-\infty }^{\infty }x(t)\,e^{-i\omega t}\,dt\\&=\int _{-\infty }^{\infty }x(t)\,(\cos(\omega t)-i\sin(\omega t))\,dt\\&=\int _{-\infty }^{\infty }x(t)\,\cos(\omega t)\,dt-i\int _{-\infty }^{\infty }x(t)\,\sin(\omega t)\,dt\\\end{aligned}}\,} {\displaystyle {\begin{aligned}X(\omega )&=\int _{-\infty }^{\infty }x(t)\,e^{-i\omega t}\,dt\\&=\int _{-\infty }^{\infty }x(t)\,(\cos(\omega t)-i\sin(\omega t))\,dt\\&=\int _{-\infty }^{\infty }x(t)\,\cos(\omega t)\,dt-i\int _{-\infty }^{\infty }x(t)\,\sin(\omega t)\,dt\\\end{aligned}}\,}

Alternative definitioner

Fouriertransformationen og dens inverse transformation kan også defineres på andre måder:

X ( ω ) = a ∫ − ∞ ∞ x ( t ) e − i ω t d t {\displaystyle X(\omega )=a\int _{-\infty }^{\infty }x(t)\,e^{-i\omega t}\,dt} {\displaystyle X(\omega )=a\int _{-\infty }^{\infty }x(t)\,e^{-i\omega t}\,dt}.
x ( t ) = b ∫ − ∞ ∞ X ( ω ) e i ω t d ω {\displaystyle x(t)=b\int _{-\infty }^{\infty }X(\omega )\,e^{i\omega t}\,d\omega } {\displaystyle x(t)=b\int _{-\infty }^{\infty }X(\omega )\,e^{i\omega t}\,d\omega }

Her skal det gælde at a b = 1 / ( 2 π ) {\displaystyle ab=1/(2\pi )} {\displaystyle ab=1/(2\pi )}. Indenfor visse områder bruger man følgende normalisering: a = b = 1 / 2 π {\displaystyle a=b=1/{\sqrt {2\pi }}} {\displaystyle a=b=1/{\sqrt {2\pi }}}.

Diskret Fouriertransformation

Hvis tiden t {\displaystyle t} {\displaystyle t} og (vinkel)frekvensen ω {\displaystyle \omega } {\displaystyle \omega } bliver diskretiseret og er endelige taler man om diskret Fouriertransformation (DFT). DFT udføres sædvanligvis med en hurtig algoritme kaldet FFT efter engelsk fast Fourier transform. Den diskrete Fouriertransformation kan defineres som:

X [ k ] = ∑ n = 0 N − 1 x [ n ] e − i 2 π k n / N , k = 0 , 1 , … , N − 1 {\displaystyle X[k]=\sum _{n=0}^{N-1}x[n]\,e^{-i2\pi kn/N},\quad k=0,1,\ldots ,N-1} {\displaystyle X[k]=\sum _{n=0}^{N-1}x[n]\,e^{-i2\pi kn/N},\quad k=0,1,\ldots ,N-1}

Den tilsvarende inverse diskrete Fouriertransformation defineres da som

x [ n ] = 1 N ∑ k = 0 N − 1 X [ k ] e i 2 π k n / N , n = 0 , 1 , … , N − 1. {\displaystyle x[n]={\frac {1}{N}}\sum _{k=0}^{N-1}X[k]\,e^{i2\pi kn/N},\quad n=0,1,\ldots ,N-1.} {\displaystyle x[n]={\frac {1}{N}}\sum _{k=0}^{N-1}X[k]\,e^{i2\pi kn/N},\quad n=0,1,\ldots ,N-1.}

De følgende tabeller viser nogle closed-form Fouriertransformationer. For funktioner f(x), g(x) og h(x) vises deres Fouriertransformationer ved henholdsvis f ^ {\displaystyle {\hat {f}}} {\displaystyle {\hat {f}}}, g ^ {\displaystyle {\hat {g}}} {\displaystyle {\hat {g}}} og h ^ {\displaystyle {\hat {h}}} {\displaystyle {\hat {h}}}. Kun de tre mest almindelige Fouriertransformationskonventioner er inkluderet.

Det kan være nyttigt at bemærke at 105 giver en sammenhæng mellem en Fouriertransformation af en funktion og den oprindelige funktion, hvilket kan ses ved sammenhængen mellem Fouriertransformation og dens inverse.

Funktionelle sammenhænge

Fouriertransformationer i denne tabel kan findes i Erdélyi1954[1] eller Kammler2000[2].

Flere oplysninger , ...
FunktionFouriertransformation
unitær, ordinær frekvens		Fouriertransformation
unitær, angulær frekvens		Fouriertransformation
ikke-unitær, angulær frekvens		Bemærkninger
f ( x ) {\displaystyle \displaystyle f(x)\,} {\displaystyle \displaystyle f(x)\,} f ^ ( ξ ) = {\displaystyle \displaystyle {\hat {f}}(\xi )=} {\displaystyle \displaystyle {\hat {f}}(\xi )=}

∫ − ∞ ∞ f ( x ) e − 2 π i x ξ d x {\displaystyle \displaystyle \int _{-\infty }^{\infty }f(x)e^{-2\pi ix\xi }\,dx} {\displaystyle \displaystyle \int _{-\infty }^{\infty }f(x)e^{-2\pi ix\xi }\,dx}

 f ^ ( ω ) = {\displaystyle \displaystyle {\hat {f}}(\omega )=} {\displaystyle \displaystyle {\hat {f}}(\omega )=}

1 2 π ∫ − ∞ ∞ f ( x ) e − i ω x d x {\displaystyle \displaystyle {\frac {1}{\sqrt {2\pi }}}\int _{-\infty }^{\infty }f(x)e^{-i\omega x}\,dx} {\displaystyle \displaystyle {\frac {1}{\sqrt {2\pi }}}\int _{-\infty }^{\infty }f(x)e^{-i\omega x}\,dx}

 f ^ ( ν ) = {\displaystyle \displaystyle {\hat {f}}(\nu )=} {\displaystyle \displaystyle {\hat {f}}(\nu )=}

∫ − ∞ ∞ f ( x ) e − i ν x d x {\displaystyle \displaystyle \int _{-\infty }^{\infty }f(x)e^{-i\nu x}\,dx} {\displaystyle \displaystyle \int _{-\infty }^{\infty }f(x)e^{-i\nu x}\,dx}

 Definition
101 a ⋅ f ( x ) + b ⋅ g ( x ) {\displaystyle \displaystyle a\cdot f(x)+b\cdot g(x)\,} {\displaystyle \displaystyle a\cdot f(x)+b\cdot g(x)\,} a ⋅ f ^ ( ξ ) + b ⋅ g ^ ( ξ ) {\displaystyle \displaystyle a\cdot {\hat {f}}(\xi )+b\cdot {\hat {g}}(\xi )\,} {\displaystyle \displaystyle a\cdot {\hat {f}}(\xi )+b\cdot {\hat {g}}(\xi )\,} a ⋅ f ^ ( ω ) + b ⋅ g ^ ( ω ) {\displaystyle \displaystyle a\cdot {\hat {f}}(\omega )+b\cdot {\hat {g}}(\omega )\,} {\displaystyle \displaystyle a\cdot {\hat {f}}(\omega )+b\cdot {\hat {g}}(\omega )\,} a ⋅ f ^ ( ν ) + b ⋅ g ^ ( ν ) {\displaystyle \displaystyle a\cdot {\hat {f}}(\nu )+b\cdot {\hat {g}}(\nu )\,} {\displaystyle \displaystyle a\cdot {\hat {f}}(\nu )+b\cdot {\hat {g}}(\nu )\,} Linaritet
102 f ( x − a ) {\displaystyle \displaystyle f(x-a)\,} {\displaystyle \displaystyle f(x-a)\,} e − 2 π i a ξ f ^ ( ξ ) {\displaystyle \displaystyle e^{-2\pi ia\xi }{\hat {f}}(\xi )\,} {\displaystyle \displaystyle e^{-2\pi ia\xi }{\hat {f}}(\xi )\,} e − i a ω f ^ ( ω ) {\displaystyle \displaystyle e^{-ia\omega }{\hat {f}}(\omega )\,} {\displaystyle \displaystyle e^{-ia\omega }{\hat {f}}(\omega )\,} e − i a ν f ^ ( ν ) {\displaystyle \displaystyle e^{-ia\nu }{\hat {f}}(\nu )\,} {\displaystyle \displaystyle e^{-ia\nu }{\hat {f}}(\nu )\,} Parallelforskydning i tidsdomænet
103 f ( x ) e i a x {\displaystyle \displaystyle f(x)e^{iax}\,} {\displaystyle \displaystyle f(x)e^{iax}\,} f ^ ( ξ − a 2 π ) {\displaystyle \displaystyle {\hat {f}}\left(\xi -{\frac {a}{2\pi }}\right)\,} {\displaystyle \displaystyle {\hat {f}}\left(\xi -{\frac {a}{2\pi }}\right)\,} f ^ ( ω − a ) {\displaystyle \displaystyle {\hat {f}}(\omega -a)\,} {\displaystyle \displaystyle {\hat {f}}(\omega -a)\,} f ^ ( ν − a ) {\displaystyle \displaystyle {\hat {f}}(\nu -a)\,} {\displaystyle \displaystyle {\hat {f}}(\nu -a)\,} Parallelforskydning i frekvensdomænet, duale af 102
104 f ( a x ) {\displaystyle \displaystyle f(ax)\,} {\displaystyle \displaystyle f(ax)\,} 1 | a | f ^ ( ξ a ) {\displaystyle \displaystyle {\frac {1}{|a|}}{\hat {f}}\left({\frac {\xi }{a}}\right)\,} {\displaystyle \displaystyle {\frac {1}{|a|}}{\hat {f}}\left({\frac {\xi }{a}}\right)\,} 1 | a | f ^ ( ω a ) {\displaystyle \displaystyle {\frac {1}{|a|}}{\hat {f}}\left({\frac {\omega }{a}}\right)\,} {\displaystyle \displaystyle {\frac {1}{|a|}}{\hat {f}}\left({\frac {\omega }{a}}\right)\,} 1 | a | f ^ ( ν a ) {\displaystyle \displaystyle {\frac {1}{|a|}}{\hat {f}}\left({\frac {\nu }{a}}\right)\,} {\displaystyle \displaystyle {\frac {1}{|a|}}{\hat {f}}\left({\frac {\nu }{a}}\right)\,} Skalering i tidsdomænet. Hvis | a | {\displaystyle \displaystyle |a|\,} {\displaystyle \displaystyle |a|\,} er stor, så er f ( a x ) {\displaystyle \displaystyle f(ax)\,} {\displaystyle \displaystyle f(ax)\,} koncentreret omkring 0 og 1 | a | f ^ ( ω a ) {\displaystyle \displaystyle {\frac {1}{|a|}}{\hat {f}}\left({\frac {\omega }{a}}\right)\,} {\displaystyle \displaystyle {\frac {1}{|a|}}{\hat {f}}\left({\frac {\omega }{a}}\right)\,} spredes ud - og trykkes mod ordinataksen.
105 f ^ ( x ) {\displaystyle \displaystyle {\hat {f}}(x)\,} {\displaystyle \displaystyle {\hat {f}}(x)\,} f ( − ξ ) {\displaystyle \displaystyle f(-\xi )\,} {\displaystyle \displaystyle f(-\xi )\,} f ( − ω ) {\displaystyle \displaystyle f(-\omega )\,} {\displaystyle \displaystyle f(-\omega )\,} 2 π f ( − ν ) {\displaystyle \displaystyle 2\pi f(-\nu )\,} {\displaystyle \displaystyle 2\pi f(-\nu )\,} Dualitet.
106 d n f ( x ) d x n {\displaystyle \displaystyle {\frac {d^{n}f(x)}{dx^{n}}}\,} {\displaystyle \displaystyle {\frac {d^{n}f(x)}{dx^{n}}}\,} ( 2 π i ξ ) n f ^ ( ξ ) {\displaystyle \displaystyle (2\pi i\xi )^{n}{\hat {f}}(\xi )\,} {\displaystyle \displaystyle (2\pi i\xi )^{n}{\hat {f}}(\xi )\,} ( i ω ) n f ^ ( ω ) {\displaystyle \displaystyle (i\omega )^{n}{\hat {f}}(\omega )\,} {\displaystyle \displaystyle (i\omega )^{n}{\hat {f}}(\omega )\,} ( i ν ) n f ^ ( ν ) {\displaystyle \displaystyle (i\nu )^{n}{\hat {f}}(\nu )\,} {\displaystyle \displaystyle (i\nu )^{n}{\hat {f}}(\nu )\,}
107 x n f ( x ) {\displaystyle \displaystyle x^{n}f(x)\,} {\displaystyle \displaystyle x^{n}f(x)\,} ( i 2 π ) n d n f ^ ( ξ ) d ξ n {\displaystyle \displaystyle \left({\frac {i}{2\pi }}\right)^{n}{\frac {d^{n}{\hat {f}}(\xi )}{d\xi ^{n}}}\,} {\displaystyle \displaystyle \left({\frac {i}{2\pi }}\right)^{n}{\frac {d^{n}{\hat {f}}(\xi )}{d\xi ^{n}}}\,} i n d n f ^ ( ω ) d ω n {\displaystyle \displaystyle i^{n}{\frac {d^{n}{\hat {f}}(\omega )}{d\omega ^{n}}}} {\displaystyle \displaystyle i^{n}{\frac {d^{n}{\hat {f}}(\omega )}{d\omega ^{n}}}} i n d n f ^ ( ν ) d ν n {\displaystyle \displaystyle i^{n}{\frac {d^{n}{\hat {f}}(\nu )}{d\nu ^{n}}}} {\displaystyle \displaystyle i^{n}{\frac {d^{n}{\hat {f}}(\nu )}{d\nu ^{n}}}} Dette er den duale af 106
108 ( f ∗ g ) ( x ) {\displaystyle \displaystyle (f*g)(x)\,} {\displaystyle \displaystyle (f*g)(x)\,} f ^ ( ξ ) g ^ ( ξ ) {\displaystyle \displaystyle {\hat {f}}(\xi ){\hat {g}}(\xi )\,} {\displaystyle \displaystyle {\hat {f}}(\xi ){\hat {g}}(\xi )\,} 2 π f ^ ( ω ) g ^ ( ω ) {\displaystyle \displaystyle {\sqrt {2\pi }}{\hat {f}}(\omega ){\hat {g}}(\omega )\,} {\displaystyle \displaystyle {\sqrt {2\pi }}{\hat {f}}(\omega ){\hat {g}}(\omega )\,} f ^ ( ν ) g ^ ( ν ) {\displaystyle \displaystyle {\hat {f}}(\nu ){\hat {g}}(\nu )\,} {\displaystyle \displaystyle {\hat {f}}(\nu ){\hat {g}}(\nu )\,}
109 f ( x ) g ( x ) {\displaystyle \displaystyle f(x)g(x)\,} {\displaystyle \displaystyle f(x)g(x)\,} ( f ^ ∗ g ^ ) ( ξ ) {\displaystyle \displaystyle ({\hat {f}}*{\hat {g}})(\xi )\,} {\displaystyle \displaystyle ({\hat {f}}*{\hat {g}})(\xi )\,} ( f ^ ∗ g ^ ) ( ω ) 2 π {\displaystyle \displaystyle ({\hat {f}}*{\hat {g}})(\omega ) \over {\sqrt {2\pi }}\,} {\displaystyle \displaystyle ({\hat {f}}*{\hat {g}})(\omega ) \over {\sqrt {2\pi }}\,} 1 2 π ( f ^ ∗ g ^ ) ( ν ) {\displaystyle \displaystyle {\frac {1}{2\pi }}({\hat {f}}*{\hat {g}})(\nu )\,} {\displaystyle \displaystyle {\frac {1}{2\pi }}({\hat {f}}*{\hat {g}})(\nu )\,} Dette er den duale af 108
110 For f ( x ) {\displaystyle \displaystyle f(x)\,} {\displaystyle \displaystyle f(x)\,} rent reelle funktioner f ^ ( − ξ ) = f ^ ( ξ ) ¯ {\displaystyle \displaystyle {\hat {f}}(-\xi )={\overline {{\hat {f}}(\xi )}}\,} {\displaystyle \displaystyle {\hat {f}}(-\xi )={\overline {{\hat {f}}(\xi )}}\,} f ^ ( − ω ) = f ^ ( ω ) ¯ {\displaystyle \displaystyle {\hat {f}}(-\omega )={\overline {{\hat {f}}(\omega )}}\,} {\displaystyle \displaystyle {\hat {f}}(-\omega )={\overline {{\hat {f}}(\omega )}}\,} f ^ ( − ν ) = f ^ ( ν ) ¯ {\displaystyle \displaystyle {\hat {f}}(-\nu )={\overline {{\hat {f}}(\nu )}}\,} {\displaystyle \displaystyle {\hat {f}}(-\nu )={\overline {{\hat {f}}(\nu )}}\,} Hermitisk symmetri.
111 For f ( x ) {\displaystyle \displaystyle f(x)\,} {\displaystyle \displaystyle f(x)\,} med rent reelle lige funktioner f ^ ( ω ) {\displaystyle \displaystyle {\hat {f}}(\omega )} {\displaystyle \displaystyle {\hat {f}}(\omega )}, f ^ ( ξ ) {\displaystyle \displaystyle {\hat {f}}(\xi )} {\displaystyle \displaystyle {\hat {f}}(\xi )} og f ^ ( ν ) {\displaystyle \displaystyle {\hat {f}}(\nu )\,} {\displaystyle \displaystyle {\hat {f}}(\nu )\,} er rent reelle lige funktioner.
112 For f ( x ) {\displaystyle \displaystyle f(x)\,} {\displaystyle \displaystyle f(x)\,} med rent reelle ulige funktioner f ^ ( ω ) {\displaystyle \displaystyle {\hat {f}}(\omega )} {\displaystyle \displaystyle {\hat {f}}(\omega )}, f ^ ( ξ ) {\displaystyle \displaystyle {\hat {f}}(\xi )} {\displaystyle \displaystyle {\hat {f}}(\xi )} og f ^ ( ν ) {\displaystyle \displaystyle {\hat {f}}(\nu )} {\displaystyle \displaystyle {\hat {f}}(\nu )} er rene imaginære ulige funktioner.
113 f ( x ) ¯ {\displaystyle \displaystyle {\overline {f(x)}}} {\displaystyle \displaystyle {\overline {f(x)}}} f ^ ( − ξ ) ¯ {\displaystyle \displaystyle {\overline {{\hat {f}}(-\xi )}}} {\displaystyle \displaystyle {\overline {{\hat {f}}(-\xi )}}} f ^ ( − ω ) ¯ {\displaystyle \displaystyle {\overline {{\hat {f}}(-\omega )}}} {\displaystyle \displaystyle {\overline {{\hat {f}}(-\omega )}}} f ^ ( − ν ) ¯ {\displaystyle \displaystyle {\overline {{\hat {f}}(-\nu )}}} {\displaystyle \displaystyle {\overline {{\hat {f}}(-\nu )}}}Kompleks konjugation, generalisering af 110
114 f ( x ) cos ⁡ ( a x ) {\displaystyle \displaystyle f(x)\cos(ax)} {\displaystyle \displaystyle f(x)\cos(ax)} f ^ ( ξ − a 2 π ) + f ^ ( ξ + a 2 π ) 2 {\displaystyle \displaystyle {\frac {\displaystyle {\hat {f}}\left(\xi -{\frac {a}{2\pi }}\right)+{\hat {f}}\left(\xi +{\frac {a}{2\pi }}\right)}{2}}} {\displaystyle \displaystyle {\frac {\displaystyle {\hat {f}}\left(\xi -{\frac {a}{2\pi }}\right)+{\hat {f}}\left(\xi +{\frac {a}{2\pi }}\right)}{2}}} f ^ ( ω − a ) + f ^ ( ω + a ) 2 {\displaystyle \displaystyle {\frac {{\hat {f}}(\omega -a)+{\hat {f}}(\omega +a)}{2}}\,} {\displaystyle \displaystyle {\frac {{\hat {f}}(\omega -a)+{\hat {f}}(\omega +a)}{2}}\,} f ^ ( ν − a ) + f ^ ( ν + a ) 2 {\displaystyle \displaystyle {\frac {{\hat {f}}(\nu -a)+{\hat {f}}(\nu +a)}{2}}} {\displaystyle \displaystyle {\frac {{\hat {f}}(\nu -a)+{\hat {f}}(\nu +a)}{2}}}
115 f ( x ) sin ⁡ ( a x ) {\displaystyle \displaystyle f(x)\sin(ax)} {\displaystyle \displaystyle f(x)\sin(ax)} f ^ ( ξ − a 2 π ) − f ^ ( ξ + a 2 π ) 2 i {\displaystyle \displaystyle {\frac {\displaystyle {\hat {f}}\left(\xi -{\frac {a}{2\pi }}\right)-{\hat {f}}\left(\xi +{\frac {a}{2\pi }}\right)}{2i}}} {\displaystyle \displaystyle {\frac {\displaystyle {\hat {f}}\left(\xi -{\frac {a}{2\pi }}\right)-{\hat {f}}\left(\xi +{\frac {a}{2\pi }}\right)}{2i}}} f ^ ( ω − a ) − f ^ ( ω + a ) 2 i {\displaystyle \displaystyle {\frac {{\hat {f}}(\omega -a)-{\hat {f}}(\omega +a)}{2i}}} {\displaystyle \displaystyle {\frac {{\hat {f}}(\omega -a)-{\hat {f}}(\omega +a)}{2i}}} f ^ ( ν − a ) − f ^ ( ν + a ) 2 i {\displaystyle \displaystyle {\frac {{\hat {f}}(\nu -a)-{\hat {f}}(\nu +a)}{2i}}} {\displaystyle \displaystyle {\frac {{\hat {f}}(\nu -a)-{\hat {f}}(\nu +a)}{2i}}}
Luk

Kvadratisk-integrable funktioner

Fouriertransformationer i denne tabel kan findes i CampbellFoster1948[3], Erdélyi1954[1] eller appendiks af Kammler2000[2].

Flere oplysninger , ...
FunktionFouriertransformation
unitær, ordinær frekvens		Fouriertransformation
unitær, angulær frekvens		Fouriertransformation
ikke-unitær, angulær frekvens		Bemærkninger
f ( x ) {\displaystyle \displaystyle f(x)} {\displaystyle \displaystyle f(x)} f ^ ( ξ ) = {\displaystyle \displaystyle {\hat {f}}(\xi )=} {\displaystyle \displaystyle {\hat {f}}(\xi )=}

∫ − ∞ ∞ f ( x ) e − 2 π i x ξ d x {\displaystyle \displaystyle \int _{-\infty }^{\infty }f(x)e^{-2\pi ix\xi }\,dx} {\displaystyle \displaystyle \int _{-\infty }^{\infty }f(x)e^{-2\pi ix\xi }\,dx}

 f ^ ( ω ) = {\displaystyle \displaystyle {\hat {f}}(\omega )=} {\displaystyle \displaystyle {\hat {f}}(\omega )=}

1 2 π ∫ − ∞ ∞ f ( x ) e − i ω x d x {\displaystyle \displaystyle {\frac {1}{\sqrt {2\pi }}}\int _{-\infty }^{\infty }f(x)e^{-i\omega x}\,dx} {\displaystyle \displaystyle {\frac {1}{\sqrt {2\pi }}}\int _{-\infty }^{\infty }f(x)e^{-i\omega x}\,dx}

 f ^ ( ν ) = {\displaystyle \displaystyle {\hat {f}}(\nu )=} {\displaystyle \displaystyle {\hat {f}}(\nu )=}

∫ − ∞ ∞ f ( x ) e − i ν x d x {\displaystyle \displaystyle \int _{-\infty }^{\infty }f(x)e^{-i\nu x}\,dx} {\displaystyle \displaystyle \int _{-\infty }^{\infty }f(x)e^{-i\nu x}\,dx}
201 rect ⁡ ( a x ) {\displaystyle \displaystyle \operatorname {rect} (ax)\,} {\displaystyle \displaystyle \operatorname {rect} (ax)\,} 1 | a | ⋅ sinc ⁡ ( ξ a ) {\displaystyle \displaystyle {\frac {1}{|a|}}\cdot \operatorname {sinc} \left({\frac {\xi }{a}}\right)} {\displaystyle \displaystyle {\frac {1}{|a|}}\cdot \operatorname {sinc} \left({\frac {\xi }{a}}\right)} 1 2 π a 2 ⋅ sinc ⁡ ( ω 2 π a ) {\displaystyle \displaystyle {\frac {1}{\sqrt {2\pi a^{2}}}}\cdot \operatorname {sinc} \left({\frac {\omega }{2\pi a}}\right)} {\displaystyle \displaystyle {\frac {1}{\sqrt {2\pi a^{2}}}}\cdot \operatorname {sinc} \left({\frac {\omega }{2\pi a}}\right)} 1 | a | ⋅ sinc ⁡ ( ν 2 π a ) {\displaystyle \displaystyle {\frac {1}{|a|}}\cdot \operatorname {sinc} \left({\frac {\nu }{2\pi a}}\right)} {\displaystyle \displaystyle {\frac {1}{|a|}}\cdot \operatorname {sinc} \left({\frac {\nu }{2\pi a}}\right)}
202 sinc ⁡ ( a x ) {\displaystyle \displaystyle \operatorname {sinc} (ax)\,} {\displaystyle \displaystyle \operatorname {sinc} (ax)\,} 1 | a | ⋅ rect ⁡ ( ξ a ) {\displaystyle \displaystyle {\frac {1}{|a|}}\cdot \operatorname {rect} \left({\frac {\xi }{a}}\right)\,} {\displaystyle \displaystyle {\frac {1}{|a|}}\cdot \operatorname {rect} \left({\frac {\xi }{a}}\right)\,} 1 2 π a 2 ⋅ rect ⁡ ( ω 2 π a ) {\displaystyle \displaystyle {\frac {1}{\sqrt {2\pi a^{2}}}}\cdot \operatorname {rect} \left({\frac {\omega }{2\pi a}}\right)} {\displaystyle \displaystyle {\frac {1}{\sqrt {2\pi a^{2}}}}\cdot \operatorname {rect} \left({\frac {\omega }{2\pi a}}\right)} 1 | a | ⋅ rect ⁡ ( ν 2 π a ) {\displaystyle \displaystyle {\frac {1}{|a|}}\cdot \operatorname {rect} \left({\frac {\nu }{2\pi a}}\right)} {\displaystyle \displaystyle {\frac {1}{|a|}}\cdot \operatorname {rect} \left({\frac {\nu }{2\pi a}}\right)} Duale af regel 201.
203 sinc 2 ⁡ ( a x ) {\displaystyle \displaystyle \operatorname {sinc} ^{2}(ax)} {\displaystyle \displaystyle \operatorname {sinc} ^{2}(ax)} 1 | a | ⋅ tri ⁡ ( ξ a ) {\displaystyle \displaystyle {\frac {1}{|a|}}\cdot \operatorname {tri} \left({\frac {\xi }{a}}\right)} {\displaystyle \displaystyle {\frac {1}{|a|}}\cdot \operatorname {tri} \left({\frac {\xi }{a}}\right)} 1 2 π a 2 ⋅ tri ⁡ ( ω 2 π a ) {\displaystyle \displaystyle {\frac {1}{\sqrt {2\pi a^{2}}}}\cdot \operatorname {tri} \left({\frac {\omega }{2\pi a}}\right)} {\displaystyle \displaystyle {\frac {1}{\sqrt {2\pi a^{2}}}}\cdot \operatorname {tri} \left({\frac {\omega }{2\pi a}}\right)} 1 | a | ⋅ tri ⁡ ( ν 2 π a ) {\displaystyle \displaystyle {\frac {1}{|a|}}\cdot \operatorname {tri} \left({\frac {\nu }{2\pi a}}\right)} {\displaystyle \displaystyle {\frac {1}{|a|}}\cdot \operatorname {tri} \left({\frac {\nu }{2\pi a}}\right)}
204 tri ⁡ ( a x ) {\displaystyle \displaystyle \operatorname {tri} (ax)} {\displaystyle \displaystyle \operatorname {tri} (ax)} 1 | a | ⋅ sinc 2 ⁡ ( ξ a ) {\displaystyle \displaystyle {\frac {1}{|a|}}\cdot \operatorname {sinc} ^{2}\left({\frac {\xi }{a}}\right)\,} {\displaystyle \displaystyle {\frac {1}{|a|}}\cdot \operatorname {sinc} ^{2}\left({\frac {\xi }{a}}\right)\,} 1 2 π a 2 ⋅ sinc 2 ⁡ ( ω 2 π a ) {\displaystyle \displaystyle {\frac {1}{\sqrt {2\pi a^{2}}}}\cdot \operatorname {sinc} ^{2}\left({\frac {\omega }{2\pi a}}\right)} {\displaystyle \displaystyle {\frac {1}{\sqrt {2\pi a^{2}}}}\cdot \operatorname {sinc} ^{2}\left({\frac {\omega }{2\pi a}}\right)} 1 | a | ⋅ sinc 2 ⁡ ( ν 2 π a ) {\displaystyle \displaystyle {\frac {1}{|a|}}\cdot \operatorname {sinc} ^{2}\left({\frac {\nu }{2\pi a}}\right)} {\displaystyle \displaystyle {\frac {1}{|a|}}\cdot \operatorname {sinc} ^{2}\left({\frac {\nu }{2\pi a}}\right)} Duale af regel 203.
205 e − a x u ( x ) {\displaystyle \displaystyle e^{-ax}u(x)\,} {\displaystyle \displaystyle e^{-ax}u(x)\,} 1 a + 2 π i ξ {\displaystyle \displaystyle {\frac {1}{a+2\pi i\xi }}} {\displaystyle \displaystyle {\frac {1}{a+2\pi i\xi }}} 1 2 π ( a + i ω ) {\displaystyle \displaystyle {\frac {1}{{\sqrt {2\pi }}(a+i\omega )}}} {\displaystyle \displaystyle {\frac {1}{{\sqrt {2\pi }}(a+i\omega )}}} 1 a + i ν {\displaystyle \displaystyle {\frac {1}{a+i\nu }}} {\displaystyle \displaystyle {\frac {1}{a+i\nu }}}
206 e − α x 2 {\displaystyle \displaystyle e^{-\alpha x^{2}}\,} {\displaystyle \displaystyle e^{-\alpha x^{2}}\,} π α ⋅ e − ( π ξ ) 2 α {\displaystyle \displaystyle {\sqrt {\frac {\pi }{\alpha }}}\cdot e^{-{\frac {(\pi \xi )^{2}}{\alpha }}}} {\displaystyle \displaystyle {\sqrt {\frac {\pi }{\alpha }}}\cdot e^{-{\frac {(\pi \xi )^{2}}{\alpha }}}} 1 2 α ⋅ e − ω 2 4 α {\displaystyle \displaystyle {\frac {1}{\sqrt {2\alpha }}}\cdot e^{-{\frac {\omega ^{2}}{4\alpha }}}} {\displaystyle \displaystyle {\frac {1}{\sqrt {2\alpha }}}\cdot e^{-{\frac {\omega ^{2}}{4\alpha }}}} π α ⋅ e − ν 2 4 α {\displaystyle \displaystyle {\sqrt {\frac {\pi }{\alpha }}}\cdot e^{-{\frac {\nu ^{2}}{4\alpha }}}} {\displaystyle \displaystyle {\sqrt {\frac {\pi }{\alpha }}}\cdot e^{-{\frac {\nu ^{2}}{4\alpha }}}}
207 e − a | x | {\displaystyle \displaystyle \operatorname {e} ^{-a|x|}\,} {\displaystyle \displaystyle \operatorname {e} ^{-a|x|}\,} 2 a a 2 + 4 π 2 ξ 2 {\displaystyle \displaystyle {\frac {2a}{a^{2}+4\pi ^{2}\xi ^{2}}}} {\displaystyle \displaystyle {\frac {2a}{a^{2}+4\pi ^{2}\xi ^{2}}}} 2 π ⋅ a a 2 + ω 2 {\displaystyle \displaystyle {\sqrt {\frac {2}{\pi }}}\cdot {\frac {a}{a^{2}+\omega ^{2}}}} {\displaystyle \displaystyle {\sqrt {\frac {2}{\pi }}}\cdot {\frac {a}{a^{2}+\omega ^{2}}}} 2 a a 2 + ν 2 {\displaystyle \displaystyle {\frac {2a}{a^{2}+\nu ^{2}}}} {\displaystyle \displaystyle {\frac {2a}{a^{2}+\nu ^{2}}}}
208 sech ⁡ ( a x ) {\displaystyle \displaystyle \operatorname {sech} (ax)\,} {\displaystyle \displaystyle \operatorname {sech} (ax)\,} π a sech ⁡ ( π 2 a ξ ) {\displaystyle \displaystyle {\frac {\pi }{a}}\operatorname {sech} \left({\frac {\pi ^{2}}{a}}\xi \right)} {\displaystyle \displaystyle {\frac {\pi }{a}}\operatorname {sech} \left({\frac {\pi ^{2}}{a}}\xi \right)} 1 a π 2 sech ⁡ ( π 2 a ω ) {\displaystyle \displaystyle {\frac {1}{a}}{\sqrt {\frac {\pi }{2}}}\operatorname {sech} \left({\frac {\pi }{2a}}\omega \right)} {\displaystyle \displaystyle {\frac {1}{a}}{\sqrt {\frac {\pi }{2}}}\operatorname {sech} \left({\frac {\pi }{2a}}\omega \right)} π a sech ⁡ ( π 2 a ν ) {\displaystyle \displaystyle {\frac {\pi }{a}}\operatorname {sech} \left({\frac {\pi }{2a}}\nu \right)} {\displaystyle \displaystyle {\frac {\pi }{a}}\operatorname {sech} \left({\frac {\pi }{2a}}\nu \right)}
209 e − a 2 x 2 2 H n ( a x ) {\displaystyle \displaystyle e^{-{\frac {a^{2}x^{2}}{2}}}H_{n}(ax)\,} {\displaystyle \displaystyle e^{-{\frac {a^{2}x^{2}}{2}}}H_{n}(ax)\,} 2 π ( − i ) n a {\displaystyle \displaystyle {\frac {{\sqrt {2\pi }}(-i)^{n}}{a}}} {\displaystyle \displaystyle {\frac {{\sqrt {2\pi }}(-i)^{n}}{a}}}

  ⋅ e − 2 π 2 ξ 2 a 2 H n ( 2 π ξ a ) {\displaystyle \cdot e^{-{\frac {2\pi ^{2}\xi ^{2}}{a^{2}}}}H_{n}\left({\frac {2\pi \xi }{a}}\right)} {\displaystyle \cdot e^{-{\frac {2\pi ^{2}\xi ^{2}}{a^{2}}}}H_{n}\left({\frac {2\pi \xi }{a}}\right)}

 ( − i ) n a {\displaystyle \displaystyle {\frac {(-i)^{n}}{a}}} {\displaystyle \displaystyle {\frac {(-i)^{n}}{a}}}

  ⋅ e − ω 2 2 a 2 H n ( ω a ) {\displaystyle \cdot e^{-{\frac {\omega ^{2}}{2a^{2}}}}H_{n}\left({\frac {\omega }{a}}\right)} {\displaystyle \cdot e^{-{\frac {\omega ^{2}}{2a^{2}}}}H_{n}\left({\frac {\omega }{a}}\right)}

 ( − i ) n 2 π a {\displaystyle \displaystyle {\frac {(-i)^{n}{\sqrt {2\pi }}}{a}}} {\displaystyle \displaystyle {\frac {(-i)^{n}{\sqrt {2\pi }}}{a}}}

  ⋅ e − ν 2 2 a 2 H n ( ν a ) {\displaystyle \cdot e^{-{\frac {\nu ^{2}}{2a^{2}}}}H_{n}\left({\frac {\nu }{a}}\right)} {\displaystyle \cdot e^{-{\frac {\nu ^{2}}{2a^{2}}}}H_{n}\left({\frac {\nu }{a}}\right)}
Luk

Fordelinger

Fouriertransformationer i denne tabel kan findes i Erdélyi1954[1] eller appendiks i Kammler2000[2].

Flere oplysninger , ...
FunktionFouriertransformation
unitær, ordinær frekvens		Fouriertransformation
unitær, angulær frekvens		Fouriertransformation
ikke-unitær, angulær frekvens		Bemærkninger
f ( x ) {\displaystyle \displaystyle f(x)} {\displaystyle \displaystyle f(x)} f ^ ( ξ ) = {\displaystyle \displaystyle {\hat {f}}(\xi )=} {\displaystyle \displaystyle {\hat {f}}(\xi )=}

∫ − ∞ ∞ f ( x ) e − 2 π i x ξ d x {\displaystyle \displaystyle \int _{-\infty }^{\infty }f(x)e^{-2\pi ix\xi }\,dx} {\displaystyle \displaystyle \int _{-\infty }^{\infty }f(x)e^{-2\pi ix\xi }\,dx}

 f ^ ( ω ) = {\displaystyle \displaystyle {\hat {f}}(\omega )=} {\displaystyle \displaystyle {\hat {f}}(\omega )=}

1 2 π ∫ − ∞ ∞ f ( x ) e − i ω x d x {\displaystyle \displaystyle {\frac {1}{\sqrt {2\pi }}}\int _{-\infty }^{\infty }f(x)e^{-i\omega x}\,dx} {\displaystyle \displaystyle {\frac {1}{\sqrt {2\pi }}}\int _{-\infty }^{\infty }f(x)e^{-i\omega x}\,dx}

 f ^ ( ν ) = {\displaystyle \displaystyle {\hat {f}}(\nu )=} {\displaystyle \displaystyle {\hat {f}}(\nu )=}

∫ − ∞ ∞ f ( x ) e − i ν x d x {\displaystyle \displaystyle \int _{-\infty }^{\infty }f(x)e^{-i\nu x}\,dx} {\displaystyle \displaystyle \int _{-\infty }^{\infty }f(x)e^{-i\nu x}\,dx}
301 1 {\displaystyle \displaystyle 1} {\displaystyle \displaystyle 1} δ ( ξ ) {\displaystyle \displaystyle \delta (\xi )} {\displaystyle \displaystyle \delta (\xi )} 2 π ⋅ δ ( ω ) {\displaystyle \displaystyle {\sqrt {2\pi }}\cdot \delta (\omega )} {\displaystyle \displaystyle {\sqrt {2\pi }}\cdot \delta (\omega )} 2 π δ ( ν ) {\displaystyle \displaystyle 2\pi \delta (\nu )} {\displaystyle \displaystyle 2\pi \delta (\nu )} Fordelingen δ(ξ) henviser til Diracs deltafunktion.
302 δ ( x ) {\displaystyle \displaystyle \delta (x)\,} {\displaystyle \displaystyle \delta (x)\,} 1 {\displaystyle \displaystyle 1} {\displaystyle \displaystyle 1} 1 2 π {\displaystyle \displaystyle {\frac {1}{\sqrt {2\pi }}}\,} {\displaystyle \displaystyle {\frac {1}{\sqrt {2\pi }}}\,} 1 {\displaystyle \displaystyle 1} {\displaystyle \displaystyle 1} Duale af regel 301.
303 e i a x {\displaystyle \displaystyle e^{iax}} {\displaystyle \displaystyle e^{iax}} δ ( ξ − a 2 π ) {\displaystyle \displaystyle \delta \left(\xi -{\frac {a}{2\pi }}\right)} {\displaystyle \displaystyle \delta \left(\xi -{\frac {a}{2\pi }}\right)} 2 π ⋅ δ ( ω − a ) {\displaystyle \displaystyle {\sqrt {2\pi }}\cdot \delta (\omega -a)} {\displaystyle \displaystyle {\sqrt {2\pi }}\cdot \delta (\omega -a)} 2 π δ ( ν − a ) {\displaystyle \displaystyle 2\pi \delta (\nu -a)} {\displaystyle \displaystyle 2\pi \delta (\nu -a)} Dette følger af 103 og 301.
304 cos ⁡ ( a x ) {\displaystyle \displaystyle \cos(ax)} {\displaystyle \displaystyle \cos(ax)} δ ( ξ − a 2 π ) + δ ( ξ + a 2 π ) 2 {\displaystyle \displaystyle {\frac {\displaystyle \delta \left(\xi -{\frac {a}{2\pi }}\right)+\delta \left(\xi +{\frac {a}{2\pi }}\right)}{2}}} {\displaystyle \displaystyle {\frac {\displaystyle \delta \left(\xi -{\frac {a}{2\pi }}\right)+\delta \left(\xi +{\frac {a}{2\pi }}\right)}{2}}} 2 π ⋅ δ ( ω − a ) + δ ( ω + a ) 2 {\displaystyle \displaystyle {\sqrt {2\pi }}\cdot {\frac {\delta (\omega -a)+\delta (\omega +a)}{2}}\,} {\displaystyle \displaystyle {\sqrt {2\pi }}\cdot {\frac {\delta (\omega -a)+\delta (\omega +a)}{2}}\,} π ( δ ( ν − a ) + δ ( ν + a ) ) {\displaystyle \displaystyle \pi \left(\delta (\nu -a)+\delta (\nu +a)\right)} {\displaystyle \displaystyle \pi \left(\delta (\nu -a)+\delta (\nu +a)\right)}
305 sin ⁡ ( a x ) {\displaystyle \displaystyle \sin(ax)} {\displaystyle \displaystyle \sin(ax)} δ ( ξ − a 2 π ) − δ ( ξ + a 2 π ) 2 i {\displaystyle \displaystyle {\frac {\displaystyle \delta \left(\xi -{\frac {a}{2\pi }}\right)-\delta \left(\xi +{\frac {a}{2\pi }}\right)}{2i}}} {\displaystyle \displaystyle {\frac {\displaystyle \delta \left(\xi -{\frac {a}{2\pi }}\right)-\delta \left(\xi +{\frac {a}{2\pi }}\right)}{2i}}} 2 π ⋅ δ ( ω − a ) − δ ( ω + a ) 2 i {\displaystyle \displaystyle {\sqrt {2\pi }}\cdot {\frac {\delta (\omega -a)-\delta (\omega +a)}{2i}}} {\displaystyle \displaystyle {\sqrt {2\pi }}\cdot {\frac {\delta (\omega -a)-\delta (\omega +a)}{2i}}} − i π ( δ ( ν − a ) − δ ( ν + a ) ) {\displaystyle \displaystyle -i\pi \left(\delta (\nu -a)-\delta (\nu +a)\right)} {\displaystyle \displaystyle -i\pi \left(\delta (\nu -a)-\delta (\nu +a)\right)}
306 cos ⁡ ( a x 2 ) {\displaystyle \displaystyle \cos(ax^{2})} {\displaystyle \displaystyle \cos(ax^{2})} π a cos ⁡ ( π 2 ξ 2 a − π 4 ) {\displaystyle \displaystyle {\sqrt {\frac {\pi }{a}}}\cos \left({\frac {\pi ^{2}\xi ^{2}}{a}}-{\frac {\pi }{4}}\right)} {\displaystyle \displaystyle {\sqrt {\frac {\pi }{a}}}\cos \left({\frac {\pi ^{2}\xi ^{2}}{a}}-{\frac {\pi }{4}}\right)} 1 2 a cos ⁡ ( ω 2 4 a − π 4 ) {\displaystyle \displaystyle {\frac {1}{\sqrt {2a}}}\cos \left({\frac {\omega ^{2}}{4a}}-{\frac {\pi }{4}}\right)} {\displaystyle \displaystyle {\frac {1}{\sqrt {2a}}}\cos \left({\frac {\omega ^{2}}{4a}}-{\frac {\pi }{4}}\right)} π a cos ⁡ ( π 2 ν 2 a − π 4 ) {\displaystyle \displaystyle {\sqrt {\frac {\pi }{a}}}\cos \left({\frac {\pi ^{2}\nu ^{2}}{a}}-{\frac {\pi }{4}}\right)} {\displaystyle \displaystyle {\sqrt {\frac {\pi }{a}}}\cos \left({\frac {\pi ^{2}\nu ^{2}}{a}}-{\frac {\pi }{4}}\right)}
307 sin ⁡ ( a x 2 ) {\displaystyle \displaystyle \sin(ax^{2})\,} {\displaystyle \displaystyle \sin(ax^{2})\,} − π a sin ⁡ ( π 2 ξ 2 a − π 4 ) {\displaystyle \displaystyle -{\sqrt {\frac {\pi }{a}}}\sin \left({\frac {\pi ^{2}\xi ^{2}}{a}}-{\frac {\pi }{4}}\right)} {\displaystyle \displaystyle -{\sqrt {\frac {\pi }{a}}}\sin \left({\frac {\pi ^{2}\xi ^{2}}{a}}-{\frac {\pi }{4}}\right)} − 1 2 a sin ⁡ ( ω 2 4 a − π 4 ) {\displaystyle \displaystyle {\frac {-1}{\sqrt {2a}}}\sin \left({\frac {\omega ^{2}}{4a}}-{\frac {\pi }{4}}\right)} {\displaystyle \displaystyle {\frac {-1}{\sqrt {2a}}}\sin \left({\frac {\omega ^{2}}{4a}}-{\frac {\pi }{4}}\right)} − π a sin ⁡ ( π 2 ν 2 a − π 4 ) {\displaystyle \displaystyle -{\sqrt {\frac {\pi }{a}}}\sin \left({\frac {\pi ^{2}\nu ^{2}}{a}}-{\frac {\pi }{4}}\right)} {\displaystyle \displaystyle -{\sqrt {\frac {\pi }{a}}}\sin \left({\frac {\pi ^{2}\nu ^{2}}{a}}-{\frac {\pi }{4}}\right)}
308 x n {\displaystyle \displaystyle x^{n}\,} {\displaystyle \displaystyle x^{n}\,} ( i 2 π ) n δ ( n ) ( ξ ) {\displaystyle \displaystyle \left({\frac {i}{2\pi }}\right)^{n}\delta ^{(n)}(\xi )\,} {\displaystyle \displaystyle \left({\frac {i}{2\pi }}\right)^{n}\delta ^{(n)}(\xi )\,} i n 2 π δ ( n ) ( ω ) {\displaystyle \displaystyle i^{n}{\sqrt {2\pi }}\delta ^{(n)}(\omega )\,} {\displaystyle \displaystyle i^{n}{\sqrt {2\pi }}\delta ^{(n)}(\omega )\,} 2 π i n δ ( n ) ( ν ) {\displaystyle \displaystyle 2\pi i^{n}\delta ^{(n)}(\nu )\,} {\displaystyle \displaystyle 2\pi i^{n}\delta ^{(n)}(\nu )\,}
309 1 x {\displaystyle \displaystyle {\frac {1}{x}}} {\displaystyle \displaystyle {\frac {1}{x}}} − i π sgn ⁡ ( ξ ) {\displaystyle \displaystyle -i\pi \operatorname {sgn}(\xi )} {\displaystyle \displaystyle -i\pi \operatorname {sgn}(\xi )} − i π 2 sgn ⁡ ( ω ) {\displaystyle \displaystyle -i{\sqrt {\frac {\pi }{2}}}\operatorname {sgn}(\omega )} {\displaystyle \displaystyle -i{\sqrt {\frac {\pi }{2}}}\operatorname {sgn}(\omega )} − i π sgn ⁡ ( ν ) {\displaystyle \displaystyle -i\pi \operatorname {sgn}(\nu )} {\displaystyle \displaystyle -i\pi \operatorname {sgn}(\nu )}
310 1 x n := {\displaystyle \displaystyle {\frac {1}{x^{n}}}:=} {\displaystyle \displaystyle {\frac {1}{x^{n}}}:=}

( − 1 ) n − 1 ( n − 1 ) ! d n d x n log ⁡ | x | {\displaystyle \displaystyle {\frac {(-1)^{n-1}}{(n-1)!}}{\frac {d^{n}}{dx^{n}}}\log |x|} {\displaystyle \displaystyle {\frac {(-1)^{n-1}}{(n-1)!}}{\frac {d^{n}}{dx^{n}}}\log |x|}

 − i π ( − 2 π i ξ ) n − 1 ( n − 1 ) ! sgn ⁡ ( ξ ) {\displaystyle \displaystyle -i\pi {\frac {(-2\pi i\xi )^{n-1}}{(n-1)!}}\operatorname {sgn}(\xi )} {\displaystyle \displaystyle -i\pi {\frac {(-2\pi i\xi )^{n-1}}{(n-1)!}}\operatorname {sgn}(\xi )} − i π 2 ⋅ ( − i ω ) n − 1 ( n − 1 ) ! sgn ⁡ ( ω ) {\displaystyle \displaystyle -i{\sqrt {\frac {\pi }{2}}}\cdot {\frac {(-i\omega )^{n-1}}{(n-1)!}}\operatorname {sgn}(\omega )} {\displaystyle \displaystyle -i{\sqrt {\frac {\pi }{2}}}\cdot {\frac {(-i\omega )^{n-1}}{(n-1)!}}\operatorname {sgn}(\omega )} − i π ( − i ν ) n − 1 ( n − 1 ) ! sgn ⁡ ( ν ) {\displaystyle \displaystyle -i\pi {\frac {(-i\nu )^{n-1}}{(n-1)!}}\operatorname {sgn}(\nu )} {\displaystyle \displaystyle -i\pi {\frac {(-i\nu )^{n-1}}{(n-1)!}}\operatorname {sgn}(\nu )}
311 | x | α {\displaystyle \displaystyle |x|^{\alpha }\,} {\displaystyle \displaystyle |x|^{\alpha }\,} − 2 sin ⁡ ( π α / 2 ) Γ ( α + 1 ) | 2 π ξ | α + 1 {\displaystyle \displaystyle -2{\frac {\sin(\pi \alpha /2)\Gamma (\alpha +1)}{|2\pi \xi |^{\alpha +1}}}} {\displaystyle \displaystyle -2{\frac {\sin(\pi \alpha /2)\Gamma (\alpha +1)}{|2\pi \xi |^{\alpha +1}}}} − 2 2 π sin ⁡ ( π α / 2 ) Γ ( α + 1 ) | ω | α + 1 {\displaystyle \displaystyle {\frac {-2}{\sqrt {2\pi }}}{\frac {\sin(\pi \alpha /2)\Gamma (\alpha +1)}{|\omega |^{\alpha +1}}}} {\displaystyle \displaystyle {\frac {-2}{\sqrt {2\pi }}}{\frac {\sin(\pi \alpha /2)\Gamma (\alpha +1)}{|\omega |^{\alpha +1}}}} − 2 sin ⁡ ( π α / 2 ) Γ ( α + 1 ) | ν | α + 1 {\displaystyle \displaystyle -2{\frac {\sin(\pi \alpha /2)\Gamma (\alpha +1)}{|\nu |^{\alpha +1}}}} {\displaystyle \displaystyle -2{\frac {\sin(\pi \alpha /2)\Gamma (\alpha +1)}{|\nu |^{\alpha +1}}}}
1 | x | {\displaystyle {\frac {1}{\sqrt {|x|}}}\,} {\displaystyle {\frac {1}{\sqrt {|x|}}}\,} 1 | ξ | {\displaystyle {\frac {1}{\sqrt {|\xi |}}}} {\displaystyle {\frac {1}{\sqrt {|\xi |}}}} 1 | ω | {\displaystyle {\frac {1}{\sqrt {|\omega |}}}} {\displaystyle {\frac {1}{\sqrt {|\omega |}}}} 2 π | ν | {\displaystyle {\frac {\sqrt {2\pi }}{\sqrt {|\nu |}}}} {\displaystyle {\frac {\sqrt {2\pi }}{\sqrt {|\nu |}}}} Specielt tilfælde af 311.
312 sgn ⁡ ( x ) {\displaystyle \displaystyle \operatorname {sgn}(x)} {\displaystyle \displaystyle \operatorname {sgn}(x)} 1 i π ξ {\displaystyle \displaystyle {\frac {1}{i\pi \xi }}} {\displaystyle \displaystyle {\frac {1}{i\pi \xi }}} 2 π 1 i ω {\displaystyle \displaystyle {\sqrt {\frac {2}{\pi }}}{\frac {1}{i\omega }}} {\displaystyle \displaystyle {\sqrt {\frac {2}{\pi }}}{\frac {1}{i\omega }}} 2 i ν {\displaystyle \displaystyle {\frac {2}{i\nu }}} {\displaystyle \displaystyle {\frac {2}{i\nu }}} Den duale af regel 309.
313 u ( x ) {\displaystyle \displaystyle u(x)} {\displaystyle \displaystyle u(x)} 1 2 ( 1 i π ξ + δ ( ξ ) ) {\displaystyle \displaystyle {\frac {1}{2}}\left({\frac {1}{i\pi \xi }}+\delta (\xi )\right)} {\displaystyle \displaystyle {\frac {1}{2}}\left({\frac {1}{i\pi \xi }}+\delta (\xi )\right)} π 2 ( 1 i π ω + δ ( ω ) ) {\displaystyle \displaystyle {\sqrt {\frac {\pi }{2}}}\left({\frac {1}{i\pi \omega }}+\delta (\omega )\right)} {\displaystyle \displaystyle {\sqrt {\frac {\pi }{2}}}\left({\frac {1}{i\pi \omega }}+\delta (\omega )\right)} π ( 1 i π ν + δ ( ν ) ) {\displaystyle \displaystyle \pi \left({\frac {1}{i\pi \nu }}+\delta (\nu )\right)} {\displaystyle \displaystyle \pi \left({\frac {1}{i\pi \nu }}+\delta (\nu )\right)}
314 ∑ n = − ∞ ∞ δ ( x − n T ) {\displaystyle \displaystyle \sum _{n=-\infty }^{\infty }\delta (x-nT)} {\displaystyle \displaystyle \sum _{n=-\infty }^{\infty }\delta (x-nT)} 1 T ∑ k = − ∞ ∞ δ ( ξ − k T ) {\displaystyle \displaystyle {\frac {1}{T}}\sum _{k=-\infty }^{\infty }\delta \left(\xi -{\frac {k}{T}}\right)} {\displaystyle \displaystyle {\frac {1}{T}}\sum _{k=-\infty }^{\infty }\delta \left(\xi -{\frac {k}{T}}\right)} 2 π T ∑ k = − ∞ ∞ δ ( ω − 2 π k T ) {\displaystyle \displaystyle {\frac {\sqrt {2\pi }}{T}}\sum _{k=-\infty }^{\infty }\delta \left(\omega -{\frac {2\pi k}{T}}\right)} {\displaystyle \displaystyle {\frac {\sqrt {2\pi }}{T}}\sum _{k=-\infty }^{\infty }\delta \left(\omega -{\frac {2\pi k}{T}}\right)} 2 π T ∑ k = − ∞ ∞ δ ( ν − 2 π k T ) {\displaystyle \displaystyle {\frac {2\pi }{T}}\sum _{k=-\infty }^{\infty }\delta \left(\nu -{\frac {2\pi k}{T}}\right)} {\displaystyle \displaystyle {\frac {2\pi }{T}}\sum _{k=-\infty }^{\infty }\delta \left(\nu -{\frac {2\pi k}{T}}\right)}
315 J 0 ( x ) {\displaystyle \displaystyle J_{0}(x)} {\displaystyle \displaystyle J_{0}(x)} 2 rect ⁡ ( π ξ ) 1 − 4 π 2 ξ 2 {\displaystyle \displaystyle {\frac {2\,\operatorname {rect} (\pi \xi )}{\sqrt {1-4\pi ^{2}\xi ^{2}}}}} {\displaystyle \displaystyle {\frac {2\,\operatorname {rect} (\pi \xi )}{\sqrt {1-4\pi ^{2}\xi ^{2}}}}} 2 π ⋅ rect ⁡ ( ω 2 ) 1 − ω 2 {\displaystyle \displaystyle {\sqrt {\frac {2}{\pi }}}\cdot {\frac {\operatorname {rect} \left(\displaystyle {\frac {\omega }{2}}\right)}{\sqrt {1-\omega ^{2}}}}} {\displaystyle \displaystyle {\sqrt {\frac {2}{\pi }}}\cdot {\frac {\operatorname {rect} \left(\displaystyle {\frac {\omega }{2}}\right)}{\sqrt {1-\omega ^{2}}}}} 2 rect ⁡ ( ν 2 ) 1 − ν 2 {\displaystyle \displaystyle {\frac {2\,\operatorname {rect} \left(\displaystyle {\frac {\nu }{2}}\right)}{\sqrt {1-\nu ^{2}}}}} {\displaystyle \displaystyle {\frac {2\,\operatorname {rect} \left(\displaystyle {\frac {\nu }{2}}\right)}{\sqrt {1-\nu ^{2}}}}}
316 J n ( x ) {\displaystyle \displaystyle J_{n}(x)} {\displaystyle \displaystyle J_{n}(x)} 2 ( − i ) n T n ( 2 π ξ ) rect ⁡ ( π ξ ) 1 − 4 π 2 ξ 2 {\displaystyle \displaystyle {\frac {2(-i)^{n}T_{n}(2\pi \xi )\operatorname {rect} (\pi \xi )}{\sqrt {1-4\pi ^{2}\xi ^{2}}}}} {\displaystyle \displaystyle {\frac {2(-i)^{n}T_{n}(2\pi \xi )\operatorname {rect} (\pi \xi )}{\sqrt {1-4\pi ^{2}\xi ^{2}}}}} 2 π ( − i ) n T n ( ω ) rect ⁡ ( ω 2 ) 1 − ω 2 {\displaystyle \displaystyle {\sqrt {\frac {2}{\pi }}}{\frac {(-i)^{n}T_{n}(\omega )\operatorname {rect} \left(\displaystyle {\frac {\omega }{2}}\right)}{\sqrt {1-\omega ^{2}}}}} {\displaystyle \displaystyle {\sqrt {\frac {2}{\pi }}}{\frac {(-i)^{n}T_{n}(\omega )\operatorname {rect} \left(\displaystyle {\frac {\omega }{2}}\right)}{\sqrt {1-\omega ^{2}}}}} 2 ( − i ) n T n ( ν ) rect ⁡ ( ν 2 ) 1 − ν 2 {\displaystyle \displaystyle {\frac {2(-i)^{n}T_{n}(\nu )\operatorname {rect} \left(\displaystyle {\frac {\nu }{2}}\right)}{\sqrt {1-\nu ^{2}}}}} {\displaystyle \displaystyle {\frac {2(-i)^{n}T_{n}(\nu )\operatorname {rect} \left(\displaystyle {\frac {\nu }{2}}\right)}{\sqrt {1-\nu ^{2}}}}} Dette er en generalisering af 315.
317 log ⁡ | x | {\displaystyle \displaystyle \log \left|x\right|} {\displaystyle \displaystyle \log \left|x\right|} − 1 2 1 | ξ | − γ δ ( ξ ) {\displaystyle \displaystyle -{\frac {1}{2}}{\frac {1}{\left|\xi \right|}}-\gamma \delta \left(\xi \right)} {\displaystyle \displaystyle -{\frac {1}{2}}{\frac {1}{\left|\xi \right|}}-\gamma \delta \left(\xi \right)} − π / 2 | ω | − 2 π γ δ ( ω ) {\displaystyle \displaystyle -{\frac {\sqrt {\pi /2}}{\left|\omega \right|}}-{\sqrt {2\pi }}\gamma \delta \left(\omega \right)} {\displaystyle \displaystyle -{\frac {\sqrt {\pi /2}}{\left|\omega \right|}}-{\sqrt {2\pi }}\gamma \delta \left(\omega \right)} − π | ν | − 2 π γ δ ( ν ) {\displaystyle \displaystyle -{\frac {\pi }{\left|\nu \right|}}-2\pi \gamma \delta \left(\nu \right)} {\displaystyle \displaystyle -{\frac {\pi }{\left|\nu \right|}}-2\pi \gamma \delta \left(\nu \right)} γ {\displaystyle \gamma } {\displaystyle \gamma } er Euler–Mascheroni konstant.
318 ( ∓ i x ) − α {\displaystyle \displaystyle \left(\mp ix\right)^{-\alpha }} {\displaystyle \displaystyle \left(\mp ix\right)^{-\alpha }} ( 2 π ) α Γ ( α ) u ( ± ξ ) ( ± ξ ) α − 1 {\displaystyle \displaystyle {\frac {\left(2\pi \right)^{\alpha }}{\Gamma \left(\alpha \right)}}u\left(\pm \xi \right)\left(\pm \xi \right)^{\alpha -1}} {\displaystyle \displaystyle {\frac {\left(2\pi \right)^{\alpha }}{\Gamma \left(\alpha \right)}}u\left(\pm \xi \right)\left(\pm \xi \right)^{\alpha -1}} 2 π Γ ( α ) u ( ± ω ) ( ± ω ) α − 1 {\displaystyle \displaystyle {\frac {\sqrt {2\pi }}{\Gamma \left(\alpha \right)}}u\left(\pm \omega \right)\left(\pm \omega \right)^{\alpha -1}} {\displaystyle \displaystyle {\frac {\sqrt {2\pi }}{\Gamma \left(\alpha \right)}}u\left(\pm \omega \right)\left(\pm \omega \right)^{\alpha -1}} 2 π Γ ( α ) u ( ± ν ) ( ± ν ) α − 1 {\displaystyle \displaystyle {\frac {2\pi }{\Gamma \left(\alpha \right)}}u\left(\pm \nu \right)\left(\pm \nu \right)^{\alpha -1}} {\displaystyle \displaystyle {\frac {2\pi }{\Gamma \left(\alpha \right)}}u\left(\pm \nu \right)\left(\pm \nu \right)^{\alpha -1}}
Luk

To-dimensionelle funktioner

Flere oplysninger , ...
FunktionFouriertransformation
unitær, ordinær frekvens		Fouriertransformation
unitær, angulær frekvens		Fouriertransformation
ikke-unitær, angulær frekvens
400 f ( x , y ) {\displaystyle \displaystyle f(x,y)} {\displaystyle \displaystyle f(x,y)} f ^ ( ξ x , ξ y ) = {\displaystyle \displaystyle {\hat {f}}(\xi _{x},\xi _{y})=} {\displaystyle \displaystyle {\hat {f}}(\xi _{x},\xi _{y})=}

∬ f ( x , y ) e − 2 π i ( ξ x x + ξ y y ) d x d y {\displaystyle \displaystyle \iint f(x,y)e^{-2\pi i(\xi _{x}x+\xi _{y}y)}\,dx\,dy} {\displaystyle \displaystyle \iint f(x,y)e^{-2\pi i(\xi _{x}x+\xi _{y}y)}\,dx\,dy}

 f ^ ( ω x , ω y ) = {\displaystyle \displaystyle {\hat {f}}(\omega _{x},\omega _{y})=} {\displaystyle \displaystyle {\hat {f}}(\omega _{x},\omega _{y})=}

1 2 π ∬ f ( x , y ) e − i ( ω x x + ω y y ) d x d y {\displaystyle \displaystyle {\frac {1}{2\pi }}\iint f(x,y)e^{-i(\omega _{x}x+\omega _{y}y)}\,dx\,dy} {\displaystyle \displaystyle {\frac {1}{2\pi }}\iint f(x,y)e^{-i(\omega _{x}x+\omega _{y}y)}\,dx\,dy}

 f ^ ( ν x , ν y ) = {\displaystyle \displaystyle {\hat {f}}(\nu _{x},\nu _{y})=} {\displaystyle \displaystyle {\hat {f}}(\nu _{x},\nu _{y})=}

∬ f ( x , y ) e − i ( ν x x + ν y y ) d x d y {\displaystyle \displaystyle \iint f(x,y)e^{-i(\nu _{x}x+\nu _{y}y)}\,dx\,dy} {\displaystyle \displaystyle \iint f(x,y)e^{-i(\nu _{x}x+\nu _{y}y)}\,dx\,dy}

401 e − π ( a 2 x 2 + b 2 y 2 ) {\displaystyle \displaystyle e^{-\pi \left(a^{2}x^{2}+b^{2}y^{2}\right)}} {\displaystyle \displaystyle e^{-\pi \left(a^{2}x^{2}+b^{2}y^{2}\right)}} 1 | a b | e − π ( ξ x 2 / a 2 + ξ y 2 / b 2 ) {\displaystyle \displaystyle {\frac {1}{|ab|}}e^{-\pi \left(\xi _{x}^{2}/a^{2}+\xi _{y}^{2}/b^{2}\right)}} {\displaystyle \displaystyle {\frac {1}{|ab|}}e^{-\pi \left(\xi _{x}^{2}/a^{2}+\xi _{y}^{2}/b^{2}\right)}} 1 2 π ⋅ | a b | e − ( ω x 2 / a 2 + ω y 2 / b 2 ) 4 π {\displaystyle \displaystyle {\frac {1}{2\pi \cdot |ab|}}e^{\frac {-\left(\omega _{x}^{2}/a^{2}+\omega _{y}^{2}/b^{2}\right)}{4\pi }}} {\displaystyle \displaystyle {\frac {1}{2\pi \cdot |ab|}}e^{\frac {-\left(\omega _{x}^{2}/a^{2}+\omega _{y}^{2}/b^{2}\right)}{4\pi }}} 1 | a b | e − ( ν x 2 / a 2 + ν y 2 / b 2 ) 4 π {\displaystyle \displaystyle {\frac {1}{|ab|}}e^{\frac {-\left(\nu _{x}^{2}/a^{2}+\nu _{y}^{2}/b^{2}\right)}{4\pi }}} {\displaystyle \displaystyle {\frac {1}{|ab|}}e^{\frac {-\left(\nu _{x}^{2}/a^{2}+\nu _{y}^{2}/b^{2}\right)}{4\pi }}}
402 c i r c ( x 2 + y 2 ) {\displaystyle \displaystyle \mathrm {circ} ({\sqrt {x^{2}+y^{2}}})} {\displaystyle \displaystyle \mathrm {circ} ({\sqrt {x^{2}+y^{2}}})} J 1 ( 2 π ξ x 2 + ξ y 2 ) ξ x 2 + ξ y 2 {\displaystyle \displaystyle {\frac {J_{1}\left(2\pi {\sqrt {\xi _{x}^{2}+\xi _{y}^{2}}}\right)}{\sqrt {\xi _{x}^{2}+\xi _{y}^{2}}}}} {\displaystyle \displaystyle {\frac {J_{1}\left(2\pi {\sqrt {\xi _{x}^{2}+\xi _{y}^{2}}}\right)}{\sqrt {\xi _{x}^{2}+\xi _{y}^{2}}}}} J 1 ( ω x 2 + ω y 2 ) ω x 2 + ω y 2 {\displaystyle \displaystyle {\frac {J_{1}\left({\sqrt {\omega _{x}^{2}+\omega _{y}^{2}}}\right)}{\sqrt {\omega _{x}^{2}+\omega _{y}^{2}}}}} {\displaystyle \displaystyle {\frac {J_{1}\left({\sqrt {\omega _{x}^{2}+\omega _{y}^{2}}}\right)}{\sqrt {\omega _{x}^{2}+\omega _{y}^{2}}}}} 2 π J 1 ( ν x 2 + ν y 2 ) ν x 2 + ν y 2 {\displaystyle \displaystyle {\frac {2\pi J_{1}\left({\sqrt {\nu _{x}^{2}+\nu _{y}^{2}}}\right)}{\sqrt {\nu _{x}^{2}+\nu _{y}^{2}}}}} {\displaystyle \displaystyle {\frac {2\pi J_{1}\left({\sqrt {\nu _{x}^{2}+\nu _{y}^{2}}}\right)}{\sqrt {\nu _{x}^{2}+\nu _{y}^{2}}}}}
Luk

Formler for generelle n-dimensionelle funktioner

Flere oplysninger , ...
FunktionFouriertransformation
unitær, ordinær frekvens		Fouriertransformation
unitær, angulær frekvens		Fouriertransformation
ikke-unitær, angulær frekvens
500 f ( x ) {\displaystyle \displaystyle f(\mathbf {x} )\,} {\displaystyle \displaystyle f(\mathbf {x} )\,} f ^ ( ξ ) = {\displaystyle \displaystyle {\hat {f}}({\boldsymbol {\xi }})=} {\displaystyle \displaystyle {\hat {f}}({\boldsymbol {\xi }})=}

∫ R n f ( x ) e − 2 π i x ⋅ ξ d n x {\displaystyle \displaystyle \int _{\mathbf {R} ^{n}}f(\mathbf {x} )e^{-2\pi i\mathbf {x} \cdot {\boldsymbol {\xi }}}\,d^{n}\mathbf {x} } {\displaystyle \displaystyle \int _{\mathbf {R} ^{n}}f(\mathbf {x} )e^{-2\pi i\mathbf {x} \cdot {\boldsymbol {\xi }}}\,d^{n}\mathbf {x} }

 f ^ ( ω ) = {\displaystyle \displaystyle {\hat {f}}({\boldsymbol {\omega }})=} {\displaystyle \displaystyle {\hat {f}}({\boldsymbol {\omega }})=}

1 ( 2 π ) n / 2 ∫ R n f ( x ) e − i ω ⋅ x d n x {\displaystyle \displaystyle {\frac {1}{{(2\pi )}^{n/2}}}\int _{\mathbf {R} ^{n}}f(\mathbf {x} )e^{-i{\boldsymbol {\omega }}\cdot \mathbf {x} }\,d^{n}\mathbf {x} } {\displaystyle \displaystyle {\frac {1}{{(2\pi )}^{n/2}}}\int _{\mathbf {R} ^{n}}f(\mathbf {x} )e^{-i{\boldsymbol {\omega }}\cdot \mathbf {x} }\,d^{n}\mathbf {x} }

 f ^ ( ν ) = {\displaystyle \displaystyle {\hat {f}}({\boldsymbol {\nu }})=} {\displaystyle \displaystyle {\hat {f}}({\boldsymbol {\nu }})=}

∫ R n f ( x ) e − i x ⋅ ν d n x {\displaystyle \displaystyle \int _{\mathbf {R} ^{n}}f(\mathbf {x} )e^{-i\mathbf {x} \cdot {\boldsymbol {\nu }}}\,d^{n}\mathbf {x} } {\displaystyle \displaystyle \int _{\mathbf {R} ^{n}}f(\mathbf {x} )e^{-i\mathbf {x} \cdot {\boldsymbol {\nu }}}\,d^{n}\mathbf {x} }

501 χ [ 0 , 1 ] ( | x | ) ( 1 − | x | 2 ) δ {\displaystyle \displaystyle \chi _{[0,1]}(|\mathbf {x} |)(1-|\mathbf {x} |^{2})^{\delta }} {\displaystyle \displaystyle \chi _{[0,1]}(|\mathbf {x} |)(1-|\mathbf {x} |^{2})^{\delta }} π − δ Γ ( δ + 1 ) | ξ | − n / 2 − δ {\displaystyle \displaystyle \pi ^{-\delta }\Gamma (\delta +1)|{\boldsymbol {\xi }}|^{-n/2-\delta }} {\displaystyle \displaystyle \pi ^{-\delta }\Gamma (\delta +1)|{\boldsymbol {\xi }}|^{-n/2-\delta }}
× J n / 2 + δ ( 2 π | ξ | ) {\displaystyle \displaystyle \times J_{n/2+\delta }(2\pi |{\boldsymbol {\xi }}|)} {\displaystyle \displaystyle \times J_{n/2+\delta }(2\pi |{\boldsymbol {\xi }}|)}		 2 − δ Γ ( δ + 1 ) | ω | − n / 2 − δ {\displaystyle \displaystyle 2^{-\delta }\Gamma (\delta +1)\left|{\boldsymbol {\omega }}\right|^{-n/2-\delta }} {\displaystyle \displaystyle 2^{-\delta }\Gamma (\delta +1)\left|{\boldsymbol {\omega }}\right|^{-n/2-\delta }}
× J n / 2 + δ ( | ω | ) {\displaystyle \displaystyle \times J_{n/2+\delta }(|{\boldsymbol {\omega }}|)} {\displaystyle \displaystyle \times J_{n/2+\delta }(|{\boldsymbol {\omega }}|)}		 π − δ Γ ( δ + 1 ) | ν 2 π | − n / 2 − δ {\displaystyle \displaystyle \pi ^{-\delta }\Gamma (\delta +1)\left|{\frac {\boldsymbol {\nu }}{2\pi }}\right|^{-n/2-\delta }} {\displaystyle \displaystyle \pi ^{-\delta }\Gamma (\delta +1)\left|{\frac {\boldsymbol {\nu }}{2\pi }}\right|^{-n/2-\delta }}
× J n / 2 + δ ( | ν | ) {\displaystyle \displaystyle \times J_{n/2+\delta }(|{\boldsymbol {\nu }}|)} {\displaystyle \displaystyle \times J_{n/2+\delta }(|{\boldsymbol {\nu }}|)}
502 | x | − α , 0 < Re ⁡ α < n . {\displaystyle \displaystyle |\mathbf {x} |^{-\alpha },\quad 0<\operatorname {Re} \alpha <n.} {\displaystyle \displaystyle |\mathbf {x} |^{-\alpha },\quad 0<\operatorname {Re} \alpha <n.} c n − α , n ( 2 π ) α − n | ξ | − ( n − α ) {\displaystyle \displaystyle c_{n-\alpha ,n}(2\pi )^{\alpha -n}|{\boldsymbol {\xi }}|^{-(n-\alpha )}} {\displaystyle \displaystyle c_{n-\alpha ,n}(2\pi )^{\alpha -n}|{\boldsymbol {\xi }}|^{-(n-\alpha )}} c n − α , n ( 2 π ) − n / 2 | ω | − ( n − α ) {\displaystyle \displaystyle c_{n-\alpha ,n}(2\pi )^{-n/2}|{\boldsymbol {\omega }}|^{-(n-\alpha )}} {\displaystyle \displaystyle c_{n-\alpha ,n}(2\pi )^{-n/2}|{\boldsymbol {\omega }}|^{-(n-\alpha )}} c n − α , n | ν | − ( n − α ) {\displaystyle \displaystyle c_{n-\alpha ,n}|{\boldsymbol {\nu }}|^{-(n-\alpha )}} {\displaystyle \displaystyle c_{n-\alpha ,n}|{\boldsymbol {\nu }}|^{-(n-\alpha )}}
503 1 ‖ σ ‖ ( 2 π ) n / 2 e − 1 2 x T σ − T σ − 1 x {\displaystyle \displaystyle {\frac {1}{\left\|{\boldsymbol {\sigma }}\right\|\left(2\pi \right)^{n/2}}}e^{-{\frac {1}{2}}\mathbf {x} ^{\mathrm {T} }{\boldsymbol {\sigma }}^{-\mathrm {T} }{\boldsymbol {\sigma }}^{-1}\mathbf {x} }} {\displaystyle \displaystyle {\frac {1}{\left\|{\boldsymbol {\sigma }}\right\|\left(2\pi \right)^{n/2}}}e^{-{\frac {1}{2}}\mathbf {x} ^{\mathrm {T} }{\boldsymbol {\sigma }}^{-\mathrm {T} }{\boldsymbol {\sigma }}^{-1}\mathbf {x} }} e − 1 2 ν T σ σ T ν {\displaystyle \displaystyle e^{-{\frac {1}{2}}{\boldsymbol {\nu }}^{\mathrm {T} }{\boldsymbol {\sigma }}{\boldsymbol {\sigma }}^{\mathrm {T} }{\boldsymbol {\nu }}}} {\displaystyle \displaystyle e^{-{\frac {1}{2}}{\boldsymbol {\nu }}^{\mathrm {T} }{\boldsymbol {\sigma }}{\boldsymbol {\sigma }}^{\mathrm {T} }{\boldsymbol {\nu }}}}
504 e − 2 π α | x | {\displaystyle \displaystyle e^{-2\pi \alpha |\mathbf {x} |}} {\displaystyle \displaystyle e^{-2\pi \alpha |\mathbf {x} |}} c n α ( α 2 + | ξ | 2 ) ( n + 1 ) / 2 {\displaystyle c_{n}{\frac {\alpha }{(\alpha ^{2}+|\xi |^{2})^{(n+1)/2}}}} {\displaystyle c_{n}{\frac {\alpha }{(\alpha ^{2}+|\xi |^{2})^{(n+1)/2}}}}
Luk


  1. [1]
    Erdélyi, Arthur, ed. (1954), Tables of Integral Transforms 1, New Your: McGraw-Hill
  2. [2]
    [Kammler, David (2000), A First Course in Fourier Analysis, Prentice Hall,] ISBN 0-13-578782-3
  3. [3]
    Campbell, George; Foster, Ronald (1948), Fourier Integrals for Practical Applications, New York: D. Van Nostrand Company, Inc..
  • Diskret cosinustransformation (DCT)
  • Fast Fourier Transform (FFT)
  • Wavelet-transformation (WT)
  • Diskret wavelet-transformation (DWT)
  • Fast wavelet-transformation (FWT)
  • Hilbertrum
  • Mogens Oddershede Larsen, Fourieranalyse Arkiveret 21. oktober 2007 hos Wayback Machine, 2. udgave, 2007.
Edit in WikipediaRevision historyRead in Wikipedia

Wikiwand in your browser!

Seamless Wikipedia browsing. On steroids.

Every time you click a link to Wikipedia, Wiktionary or Wikiquote in your browser's search results, it will show the modern Wikiwand interface.

Wikiwand extension is a five stars, simple, with minimum permission required to keep your browsing private, safe and transparent.

Chrome
Wikiwand for Chrome
Edge
Wikiwand for Edge
Firefox
Wikiwand for Firefox

Matematikken bag Fouriertransformationen

Tabel over vigtige Fouriertransformationer

Kilder/referencer

Se også

Henvisning