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11: 27.11 Asymptotic Formulas: Partial Sums
27.11.3 n x d ( n ) n = 1 2 ( ln x ) 2 + 2 γ ln x + O ( 1 ) ,
27.11.6 n x ϕ ( n ) = 3 π 2 x 2 + O ( x ln x ) .
27.11.7 n x ϕ ( n ) n = 6 π 2 x + O ( ln x ) .
27.11.8 p x 1 p = ln ln x + A + O ( 1 ln x ) ,
27.11.10 p x ln p p = ln x + O ( 1 ) .
12: 10.15 Derivatives with Respect to Order
§10.15 Derivatives with Respect to Order
For the notations Ci and Si see §6.2(ii). …
13: 19.1 Special Notation
In Abramowitz and Stegun (1964, Chapter 17) the functions (19.1.1) and (19.1.2) are denoted, in order, by K ( α ) , E ( α ) , Π ( n \ α ) , F ( ϕ \ α ) , E ( ϕ \ α ) , and Π ( n ; ϕ \ α ) , where α = arcsin k and n is the α 2 (not related to k ) in (19.1.1) and (19.1.2). …
14: 27.2 Functions
27.2.3 π ( x ) x ln x .
An equivalent form states that the n th prime p n (when the primes are listed in increasing order) is asymptotic to n ln n as n :
27.2.4 p n n ln n .
It is the special case k = 2 of the function d k ( n ) that counts the number of ways of expressing n as the product of k factors, with the order of factors taken into account. …
27.2.14 Λ ( n ) = ln p , n = p a ,
15: 2.5 Mellin Transform Methods
2.5.4 I ( z ) = f ( 1 z ) h ( z ) .
In the half-plane z > max ( 0 , 2 ν ) , the product f ( 1 z ) h ( z ) has a pole of order two at each positive integer, and …
2.5.26 f ( z ) = f 1 ( z ) + f 2 ( z )
(The last order estimate follows from the Riemann–Lebesgue lemma, §1.8(i).) … In the notation of (2.5.18) and (2.5.20), κ = 0 , β s = s + 1 , and c = 0 . …
16: 27.12 Asymptotic Formulas: Primes
27.12.5 | π ( x ) li ( x ) | = O ( x exp ( c ( ln x ) 1 / 2 ) ) , x .
27.12.6 | π ( x ) li ( x ) | = O ( x exp ( d ( ln x ) 3 / 5 ( ln ln x ) 1 / 5 ) ) .
27.12.8 li ( x ) ϕ ( m ) + O ( x exp ( λ ( α ) ( ln x ) 1 / 2 ) ) , m ( ln x ) α , α > 0 ,
17: 1.17 Integral and Series Representations of the Dirac Delta
Formal interchange of the order of integration in the Fourier integral formula ((1.14.1) and (1.14.4)): … Formal interchange of the order of summation and integration in the Fourier summation formula ((1.8.3) and (1.8.4)): …
1.17.25 δ ( cos θ 1 cos θ 2 ) δ ( ϕ 1 ϕ 2 ) = = 0 m = Y , m ( θ 1 , ϕ 1 ) Y , m ( θ 2 , ϕ 2 ) ¯ .
18: 3.4 Differentiation
First-Order
For partial derivatives we use the notation u t , s = u ( x 0 + t h , y 0 + s h ) . …
Second-Order
3.4.28 2 u 0 , 0 = 1 h 2 ( u 1 , 0 + u 0 , 1 + u 1 , 0 + u 0 , 1 4 u 0 , 0 ) + O ( h 2 ) ,
Fourth-Order
19: 18.39 Applications in the Physical Sciences
The nature of, and notations and common vocabulary for, the eigenvalues and eigenfunctions of self-adjoint second order differential operators is overviewed in §1.18. …
20: 30.1 Special Notation
§30.1 Special Notation
(For other notation see Notation for the Special Functions.) … These notations are similar to those used in Arscott (1964b) and Erdélyi et al. (1955). …
Other Notations