ATS theorem
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In mathematics, the ATS theorem is the theorem on the approximation of a trigonometric sum by a shorter one. The application of the ATS theorem in certain problems of mathematical and theoretical physics can be very helpful.


History of the problem

In some fields of
mathematics Mathematics is a field of study that discovers and organizes methods, Mathematical theory, theories and theorems that are developed and Mathematical proof, proved for the needs of empirical sciences and mathematics itself. There are many ar ...
and
mathematical physics Mathematical physics is the development of mathematics, mathematical methods for application to problems in physics. The ''Journal of Mathematical Physics'' defines the field as "the application of mathematics to problems in physics and the de ...
, sums of the form : S = \sum_ \varphi(k)e^ \qquad (1) are under study. Here \varphi(x) and f(x) are real valued functions of a real argument, and i^2= -1. Such sums appear, for example, in
number theory Number theory is a branch of pure mathematics devoted primarily to the study of the integers and arithmetic functions. Number theorists study prime numbers as well as the properties of mathematical objects constructed from integers (for example ...
in the analysis of the
Riemann zeta function The Riemann zeta function or Euler–Riemann zeta function, denoted by the Greek letter (zeta), is a mathematical function of a complex variable defined as \zeta(s) = \sum_^\infty \frac = \frac + \frac + \frac + \cdots for and its analytic c ...
, in the solution of problems connected with integer points in the domains on plane and in space, in the study of the
Fourier series A Fourier series () is an Series expansion, expansion of a periodic function into a sum of trigonometric functions. The Fourier series is an example of a trigonometric series. By expressing a function as a sum of sines and cosines, many problems ...
, and in the solution of such differential equations as the
wave equation The wave equation is a second-order linear partial differential equation for the description of waves or standing wave fields such as mechanical waves (e.g. water waves, sound waves and seismic waves) or electromagnetic waves (including light ...
, the potential equation, the heat conductivity equation. The problem of approximation of the series (1) by a suitable function was studied already by
Euler Leonhard Euler ( ; ; ; 15 April 170718 September 1783) was a Swiss polymath who was active as a mathematician, physicist, astronomer, logician, geographer, and engineer. He founded the studies of graph theory and topology and made influential ...
and Poisson. We shall define the length of the sum S to be the number b-a (for the integers a and b, this is the number of the summands in S). Under certain conditions on \varphi(x) and f(x) the sum S can be substituted with good accuracy by another sum S_1, : S_1 = \sum_ \Phi(k)e^ , \ \ \ (2) where the length \beta-\alpha is far less than b-a. First relations of the form : S = S_1 + R , \qquad (3) where S , S_1 are the sums (1) and (2) respectively, R is a remainder term, with concrete functions \varphi(x) and f(x), were obtained by
G. H. Hardy Godfrey Harold Hardy (7 February 1877 – 1 December 1947) was an English mathematician, known for his achievements in number theory and mathematical analysis. In biology, he is known for the Hardy–Weinberg principle, a basic principle of pop ...
and J. E. Littlewood, when they deduced approximate functional equation for the Riemann zeta function \zeta(s) and by I. M. Vinogradov, in the study of the amounts of integer points in the domains on plane. In general form the theorem was proved by J. Van der Corput, (on the recent results connected with the Van der Corput theorem one can read at ). In every one of the above-mentioned works, some restrictions on the functions \varphi(x) and f(x) were imposed. With convenient (for applications) restrictions on \varphi(x) and f(x), the theorem was proved by A. A. Karatsuba in (see also,A. A. Karatsuba, M. A. Korolev. The theorem on the approximation of a trigonometric sum by a shorter one. Izv. Ross. Akad. Nauk, Ser. Mat. 71:3, pp. 63—84 (2007).).


Certain notations

''For'' B > 0, B \to +\infty, ''or'' B \to 0, ''the record'' :: 1 \ll \frac \ll 1 : '' means that there are the constants'' C_1 > 0 : ''and'' C_2 > 0, : ''such that'' :: C_1 \leq\frac \leq C_2. ''For a real number'' \alpha, ''the record'' \, \alpha\, ''means that'' :: \, \alpha\, = \min(\,1- \), :''where'' :: \ :''is the fractional part of'' \alpha.


ATS theorem

''Let the real functions'' ''ƒ''(''x'') ''and'' \varphi(x) ''satisfy on the segment'' 'a'', ''b''''the following conditions:'' 1) f'(x) ''and'' \varphi''(x) ''are continuous;'' 2) ''there exist numbers'' H, U ''and'' V ''such that'' :: H > 0, \qquad 1 \ll U \ll V, \qquad 0 < b-a \leq V :''and'' :: \begin \frac \ll f''(x) \ll \frac \ ,& \varphi(x) \ll H ,\\ \\ f(x) \ll \frac \ ,& \varphi'(x) \ll \frac ,\\ \\ f'(x) \ll \frac \ ,& \varphi''(x) \ll \frac . \\ \\ \end ''Then, if we define the numbers'' x_\mu ''from the equation'' : f'(x_\mu) = \mu, ''we have'' : \sum_ \varphi(\mu)e^ = \sum_C(\mu)Z(\mu) + R , ''where'' : R = O \left(\frac + HT_a + HT_b + H\log\left(f'(b)-f'(a)+2\right)\right); : T_j = \begin 0, & \text f'(j) \text; \\ \min\left(\frac, \sqrt\right), & \text \, f'(j)\, \ne 0; \\ \end j = a,b; : C(\mu) = \begin 1, & \text f'(a) < \mu < f'(b) ; \\ \frac,& \text \mu = f'(a)\text\mu = f'(b) ;\\ \end : Z(\mu) = \frac \frac e^ \ . The most simple variant of the formulated theorem is the statement, which is called in the literature the Van der Corput lemma.


Van der Corput lemma

''Let'' f ''be a real differentiable function in the interval'' ]a,b], ''moreover, inside of this interval, its derivative'' f' ''is a monotonic and a sign-preserving function, and for the constant'' \delta ''such that'' 0 < \delta < 1 ''satisfies the inequality'' , f', \leq \delta . ''Then'' : \sum_ e^ = \int_a^be^dx + \theta\left(3 + \frac\right), ''where'' , \theta, \le 1.


Remark

If the parameters a and b are integers, then it is possible to substitute the last relation by the following ones: : \sum_ e^ = \int_a^be^ \, dx + \frac12e^ - \frac12e^ + \theta\frac, where , \theta, \le 1.


Additional sources

On the applications of ATS to the problems of physics see: * * * *


Notes

{{DEFAULTSORT:Ats Theorem Theorems in mathematical analysis