hyperelliptic integral - определение. Что такое hyperelliptic integral
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Что (кто) такое hyperelliptic integral - определение

TRADITIONAL NAME FOR AN EVERYWHERE-REGULAR (OR HOLOMORPHIC) DIFFERENTIAL 1-FORM
Differential of the second kind; Differential of the third kind; Hyperelliptic integral; Differentials of the first kind; Abelian differential; Abelian Differential; Holomorphic differential; Hyper-elliptic integral; Hyper-elliptic integrals; Integral of the first kind; Integral of the second kind

Henstock–Kurzweil integral         
GENERALIZATION OF THE RIEMANN INTEGRAL
Henstock-Kurzweil Integral; Perron integral; Gauge integral; Henstock integral; Denjoy Integral; Henstock-Kurzweil-Stieltjes integral; Perron Integral; Henstock-Kurzweil-Stieltjes Integral; Generalized Riemann integral; Denjoy-Perron integral; Henstock-Kurzweil integral; H-K integral
In mathematics, the Henstock–Kurzweil integral or generalized Riemann integral or gauge integral – also known as the (narrow) Denjoy integral (pronounced ), Luzin integral or Perron integral, but not to be confused with the more general wide Denjoy integral – is one of a number of inequivalent definitions of the integral of a function. It is a generalization of the Riemann integral, and in some situations is more general than the Lebesgue integral.
Pettis integral         
Weak integral; Gelfand-Pettis integral; Gelfand–Pettis integral; Gelfand integral; Dunford integral
In mathematics, the Pettis integral or Gelfand–Pettis integral, named after Israel M. Gelfand and Billy James Pettis, extends the definition of the Lebesgue integral to vector-valued functions on a measure space, by exploiting duality.
Improper integral         
  • The improper integral<br/><math>\int_{0}^{\infty} \frac{dx}{(x+1)\sqrt{x}} = \pi</math><br/> has unbounded intervals for both domain and range.
  • The improper integral<br/><math>\int_{-1}^{1} \frac{dx}{\sqrt[3]{x^2}} = 6</math><br/> converges, since both left and right limits exist, though the integrand is unbounded near an interior point.
  • An improper Riemann integral of the second kind. The integral may fail to exist because of a [[vertical asymptote]] in the function.
LIMIT OF A DEFINITE INTEGRAL WITH AS ONE OR BOTH LIMITS APPROACH INFINITY OR VALUES AT WHICH THE INTEGRAND IS UNDEFINED
Improper Riemann integral; Improper integrals; Improper Integrals; Proper integral
In mathematical analysis, an improper integral is the limit of a definite integral as an endpoint of the interval(s) of integration approaches either a specified real number or positive or negative infinity; or in some instances as both endpoints approach limits. Such an integral is often written symbolically just like a standard definite integral, in some cases with infinity as a limit of integration.

Википедия

Differential of the first kind

In mathematics, differential of the first kind is a traditional term used in the theories of Riemann surfaces (more generally, complex manifolds) and algebraic curves (more generally, algebraic varieties), for everywhere-regular differential 1-forms. Given a complex manifold M, a differential of the first kind ω is therefore the same thing as a 1-form that is everywhere holomorphic; on an algebraic variety V that is non-singular it would be a global section of the coherent sheaf Ω1 of Kähler differentials. In either case the definition has its origins in the theory of abelian integrals.

The dimension of the space of differentials of the first kind, by means of this identification, is the Hodge number

h1,0.

The differentials of the first kind, when integrated along paths, give rise to integrals that generalise the elliptic integrals to all curves over the complex numbers. They include for example the hyperelliptic integrals of type

x k d x Q ( x ) {\displaystyle \int {\frac {x^{k}\,dx}{\sqrt {Q(x)}}}}

where Q is a square-free polynomial of any given degree > 4. The allowable power k has to be determined by analysis of the possible pole at the point at infinity on the corresponding hyperelliptic curve. When this is done, one finds that the condition is

kg − 1,

or in other words, k at most 1 for degree of Q 5 or 6, at most 2 for degree 7 or 8, and so on (as g = [(1+ deg Q)/2]).

Quite generally, as this example illustrates, for a compact Riemann surface or algebraic curve, the Hodge number is the genus g. For the case of algebraic surfaces, this is the quantity known classically as the irregularity q. It is also, in general, the dimension of the Albanese variety, which takes the place of the Jacobian variety.