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31: 6.4 Analytic Continuation
Analytic continuation of the principal value of E 1 ( z ) yields a multi-valued function with branch points at z = 0 and z = . … Unless indicated otherwise, in the rest of this chapter and elsewhere in the DLMF the functions E 1 ( z ) , Ci ( z ) , Chi ( z ) , f ( z ) , and g ( z ) assume their principal values, that is, the branches that are real on the positive real axis and two-valued on the negative real axis. …
32: 4.7 Derivatives and Differential Equations
4.7.1 d d z ln z = 1 z ,
4.7.3 d n d z n ln z = ( 1 ) n 1 ( n 1 ) ! z n ,
4.7.9 d d z a z = a z ln a , a 0 .
When a z is a general power, ln a is replaced by the branch of Ln a used in constructing a z . …
33: 6.8 Inequalities
6.8.1 1 2 ln ( 1 + 2 x ) < e x E 1 ( x ) < ln ( 1 + 1 x ) ,
34: 25.8 Sums
25.8.4 k = 1 ( 1 ) k k ( ζ ( n k ) 1 ) = ln ( j = 0 n 1 Γ ( 2 e ( 2 j + 1 ) π i / n ) ) , n = 2 , 3 , 4 , .
25.8.7 k = 2 ζ ( k ) k z k = γ z + ln Γ ( 1 z ) , | z | < 1 .
25.8.8 k = 1 ζ ( 2 k ) k z 2 k = ln ( π z sin ( π z ) ) , | z | < 1 .
25.8.9 k = 1 ζ ( 2 k ) ( 2 k + 1 ) 2 2 k = 1 2 1 2 ln 2 .
35: 25.12 Polylogarithms
Other notations and names for Li 2 ( z ) include S 2 ( z ) (Kölbig et al. (1970)), Spence function Sp ( z ) (’t Hooft and Veltman (1979)), and L 2 ( z ) (Maximon (2003)). In the complex plane Li 2 ( z ) has a branch point at z = 1 . The principal branch has a cut along the interval [ 1 , ) and agrees with (25.12.1) when | z | 1 ; see also §4.2(i). The remainder of the equations in this subsection apply to principal branches. …
25.12.6 Li 2 ( x ) + Li 2 ( 1 x ) = 1 6 π 2 ( ln x ) ln ( 1 x ) , 0 < x < 1 .
36: 4.26 Integrals
The results in §§4.26(ii) and 4.26(iv) can be extended to the complex plane by using continuous branches and avoiding singularities. …
4.26.3 tan x d x = ln ( cos x ) , 1 2 π < x < 1 2 π .
4.26.16 arctan x d x = x arctan x 1 2 ln ( 1 + x 2 ) , < x < ,
37: 9.16 Physical Applications
Airy functions are applied in many branches of both classical and quantum physics. … The KdV equation and solitons have applications in many branches of physics, including plasma physics lattice dynamics, and quantum mechanics. …
38: 10.31 Power Series
10.31.1 K n ( z ) = 1 2 ( 1 2 z ) n k = 0 n 1 ( n k 1 ) ! k ! ( 1 4 z 2 ) k + ( 1 ) n + 1 ln ( 1 2 z ) I n ( z ) + ( 1 ) n 1 2 ( 1 2 z ) n k = 0 ( ψ ( k + 1 ) + ψ ( n + k + 1 ) ) ( 1 4 z 2 ) k k ! ( n + k ) ! ,
10.31.2 K 0 ( z ) = ( ln ( 1 2 z ) + γ ) I 0 ( z ) + 1 4 z 2 ( 1 ! ) 2 + ( 1 + 1 2 ) ( 1 4 z 2 ) 2 ( 2 ! ) 2 + ( 1 + 1 2 + 1 3 ) ( 1 4 z 2 ) 3 ( 3 ! ) 2 + .
39: 16.2 Definition and Analytic Properties
The branch obtained by introducing a cut from 1 to + on the real axis, that is, the branch in the sector | ph ( 1 z ) | π , is the principal branch (or principal value) of F q q + 1 ( 𝐚 ; 𝐛 ; z ) ; compare §4.2(i). Elsewhere the generalized hypergeometric function is a multivalued function that is analytic except for possible branch points at z = 0 , 1 , and . Unless indicated otherwise it is assumed that in the DLMF generalized hypergeometric functions assume their principal values. … When p q + 1 and z is fixed and not a branch point, any branch of 𝐅 q p ( 𝐚 ; 𝐛 ; z ) is an entire function of each of the parameters a 1 , , a p , b 1 , , b q .
40: 19.27 Asymptotic Approximations and Expansions
19.27.2 R F ( x , y , z ) = 1 2 z ( ln 8 z a + g ) ( 1 + O ( a z ) ) , a / z 0 .
19.27.4 R G ( x , y , z ) = z 2 ( 1 + O ( a z ln z a ) ) , a / z 0 .
19.27.6 R G ( 0 , y , z ) = z 2 + y 8 z ( ln ( 16 z y ) 1 ) ( 1 + O ( y z ) ) , y / z 0 .
19.27.7 R D ( x , y , z ) = 3 2 z 3 / 2 ( ln ( 8 z a + g ) 2 ) ( 1 + O ( a z ) ) , a / z 0 .
19.27.9 R D ( x , y , z ) = 3 x z ( y + z ) ( 1 + O ( b x ln x b ) ) , b / x 0 .