Gaussian integral
E29365
The Gaussian integral is a fundamental result in mathematics that evaluates the integral of the exponential of a negative quadratic function over the entire real line, yielding a value proportional to the square root of π and underpinning the normal distribution in probability theory.
All labels observed (2)
| Label | Occurrences |
|---|---|
| Gaussian integral canonical | 1 |
| Gaussian integrals | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T228925 — resolving that mention is where its identity was fixed. The disambiguator weighed these candidate entities and picked the highlighted one (or “None”, minting a new entity). This is how homonymy is resolved: the same surface form can point to different entities.
Target entity: Gaussian integral Context triple: [Carl Friedrich Gauss, notableWork, Gaussian integral]
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A.
Feynman path integral
The Feynman path integral is a formulation of quantum mechanics in which a particle’s behavior is described as a sum over all possible paths it can take, each weighted by a phase factor derived from the classical action.
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B.
Feynman–Kac formula
The Feynman–Kac formula is a fundamental result connecting solutions of certain partial differential equations with expectations over stochastic processes, forming a bridge between quantum mechanics, probability theory, and mathematical finance.
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C.
Born–Huang expansion
The Born–Huang expansion is a quantum mechanical method that systematically improves upon the Born–Oppenheimer approximation by including couplings between electronic and nuclear motions in molecular systems.
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D.
Fokker–Planck equation
The Fokker–Planck equation is a partial differential equation that describes the time evolution of the probability density function of a stochastic (random) process, such as Brownian motion.
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E.
Feynman–Hellmann theorem
The Feynman–Hellmann theorem is a result in quantum mechanics that relates the derivative of an energy eigenvalue with respect to a parameter in the Hamiltonian to the expectation value of the corresponding derivative of the Hamiltonian.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Gaussian integral Target entity description: The Gaussian integral is a fundamental result in mathematics that evaluates the integral of the exponential of a negative quadratic function over the entire real line, yielding a value proportional to the square root of π and underpinning the normal distribution in probability theory.
-
A.
Feynman path integral
The Feynman path integral is a formulation of quantum mechanics in which a particle’s behavior is described as a sum over all possible paths it can take, each weighted by a phase factor derived from the classical action.
-
B.
Feynman–Kac formula
The Feynman–Kac formula is a fundamental result connecting solutions of certain partial differential equations with expectations over stochastic processes, forming a bridge between quantum mechanics, probability theory, and mathematical finance.
-
C.
Born–Huang expansion
The Born–Huang expansion is a quantum mechanical method that systematically improves upon the Born–Oppenheimer approximation by including couplings between electronic and nuclear motions in molecular systems.
-
D.
Fokker–Planck equation
The Fokker–Planck equation is a partial differential equation that describes the time evolution of the probability density function of a stochastic (random) process, such as Brownian motion.
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E.
Feynman–Hellmann theorem
The Feynman–Hellmann theorem is a result in quantum mechanics that relates the derivative of an energy eigenvalue with respect to a parameter in the Hamiltonian to the expectation value of the corresponding derivative of the Hamiltonian.
- F. None of above. chosen
Statements (48)
| Predicate | Object |
|---|---|
| instanceOf |
definite integral
ⓘ
mathematical concept ⓘ |
| appearsIn |
Brownian motion theory
ⓘ
central limit theorem proofs ⓘ heat equation solutions ⓘ |
| category |
closed-form integrals
ⓘ
special integrals ⓘ |
| condition | a > 0 in ∫_{−∞}^{∞} e^{−a x^2} dx ⓘ |
| consequence | moments of the normal distribution are finite ⓘ |
| convergenceReason | rapid decay of e^{−x^2} at infinity ⓘ |
| definedAs | ∫_{−∞}^{∞} e^{−x^2} dx ⓘ |
| dimension | one-dimensional case of Gaussian measures ⓘ |
| domainOfIntegration | (−∞, ∞) ⓘ |
| evaluationMethod |
squaring the integral and using polar coordinates
ⓘ
using the Gamma function Γ(1/2) = √π ⓘ |
| field |
mathematical analysis
ⓘ
probability theory ⓘ statistics ⓘ |
| generalization | ∫_{−∞}^{∞} e^{−a x^2} dx = √(π/a) ⓘ |
| historicalAttribution | Carl Friedrich Gauss ⓘ |
| implies | ∫_{0}^{∞} e^{−x^2} dx = √π / 2 ⓘ |
| integrand | e^{−x^2} ⓘ |
| notation | ∫_{−∞}^{∞} e^{−x^2} dx = √π ⓘ |
| property | convergent improper integral ⓘ |
| relatedTo |
Gamma function
ⓘ
Laplace method ⓘ error function ⓘ multidimensional Gaussian integral ⓘ normal distribution ⓘ saddle-point approximation ⓘ standard normal distribution ⓘ |
| requires | a > 0 for convergence in ∫_{−∞}^{∞} e^{−a x^2} dx ⓘ |
| role |
basis for defining Gaussian measure
ⓘ
normalization constant for Gaussian distributions ⓘ |
| symmetryProperty | even integrand ⓘ |
| type |
Lebesgue integration
ⓘ
surface form:
Lebesgue integral
improper Riemann integral ⓘ |
| usedFor |
approximating sums by integrals in asymptotic analysis
ⓘ
computing partition functions of quadratic Hamiltonians ⓘ evaluating Fresnel-type integrals via transformations ⓘ |
| usedIn |
Fourier analysis
ⓘ
derivation of the normal distribution ⓘ error function definition ⓘ path integrals ⓘ probability density normalization ⓘ quantum mechanics ⓘ statistical mechanics ⓘ |
| value | √π ⓘ |
How these facts were elicited
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Subject: Gaussian integral Description of subject: The Gaussian integral is a fundamental result in mathematics that evaluates the integral of the exponential of a negative quadratic function over the entire real line, yielding a value proportional to the square root of π and underpinning the normal distribution in probability theory.
Referenced by (2)
Full triples — surface form annotated when it differs from this entity's canonical label.