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Jacobi

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1: 22.16 Related Functions
§22.16(i) Jacobi’s Amplitude ( am ) Function
§22.16(ii) Jacobi’s Epsilon Function
Integral Representations
§22.16(iii) Jacobi’s Zeta Function
Properties
2: 18.3 Definitions
§18.3 Definitions
The classical OP’s comprise the Jacobi, Laguerre and Hermite polynomials. … This table also includes the following special cases of Jacobi polynomials: ultraspherical, Chebyshev, and Legendre. … For finite power series of the Jacobi, ultraspherical, Laguerre, and Hermite polynomials, see §18.5(iii) (in powers of x 1 for Jacobi polynomials, in powers of x for the other cases). …
Jacobi on Other Intervals
3: 22.8 Addition Theorems
22.8.1 sn ( u + v ) = sn u cn v dn v + sn v cn u dn u 1 k 2 sn 2 u sn 2 v ,
22.8.14 sn ( u + v ) = sn u cn u dn v + sn v cn v dn u cn u cn v + sn u dn u sn v dn v ,
22.8.15 cn ( u + v ) = sn u cn u dn v sn v cn v dn u sn u cn v dn v sn v cn u dn u ,
22.8.17 dn ( u + v ) = sn u cn v dn u sn v cn u dn v sn u cn v dn v sn v cn u dn u ,
22.8.23 | sn z 1 cn z 1 cn z 1 dn z 1 cn z 1 dn z 1 sn z 2 cn z 2 cn z 2 dn z 2 cn z 2 dn z 2 sn z 3 cn z 3 cn z 3 dn z 3 cn z 3 dn z 3 sn z 4 cn z 4 cn z 4 dn z 4 cn z 4 dn z 4 | = 0 .
4: 22.6 Elementary Identities
22.6.2 1 + cs 2 ( z , k ) = k 2 + ds 2 ( z , k ) = ns 2 ( z , k ) ,
22.6.5 sn ( 2 z , k ) = 2 sn ( z , k ) cn ( z , k ) dn ( z , k ) 1 k 2 sn 4 ( z , k ) ,
22.6.8 cd ( 2 z , k ) = cd 2 ( z , k ) k 2 sd 2 ( z , k ) nd 2 ( z , k ) 1 + k 2 k 2 sd 4 ( z , k ) ,
§22.6(iv) Rotation of Argument (Jacobi’s Imaginary Transformation)
Table 22.6.1: Jacobi’s imaginary transformation of Jacobian elliptic functions.
sn ( i z , k ) = i sc ( z , k ) dc ( i z , k ) = dn ( z , k )
5: 22.13 Derivatives and Differential Equations
22.13.1 ( d d z sn ( z , k ) ) 2 = ( 1 sn 2 ( z , k ) ) ( 1 k 2 sn 2 ( z , k ) ) ,
22.13.2 ( d d z cn ( z , k ) ) 2 = ( 1 cn 2 ( z , k ) ) ( k 2 + k 2 cn 2 ( z , k ) ) ,
22.13.3 ( d d z dn ( z , k ) ) 2 = ( 1 dn 2 ( z , k ) ) ( dn 2 ( z , k ) k 2 ) .
22.13.7 ( d d z dc ( z , k ) ) 2 = ( dc 2 ( z , k ) 1 ) ( dc 2 ( z , k ) k 2 ) ,
22.13.10 ( d d z ns ( z , k ) ) 2 = ( ns 2 ( z , k ) k 2 ) ( ns 2 ( z , k ) 1 ) ,
6: 22.21 Tables
§22.21 Tables
Spenceley and Spenceley (1947) tabulates sn ( K x , k ) , cn ( K x , k ) , dn ( K x , k ) , am ( K x , k ) , ( K x , k ) for arcsin k = 1 ( 1 ) 89 and x = 0 ( 1 90 ) 1 to 12D, or 12 decimals of a radian in the case of am ( K x , k ) . … Lawden (1989, pp. 280–284 and 293–297) tabulates sn ( x , k ) , cn ( x , k ) , dn ( x , k ) , ( x , k ) , Z ( x | k ) to 5D for k = 0.1 ( .1 ) 0.9 , x = 0 ( .1 ) X , where X ranges from 1. … Zhang and Jin (1996, p. 678) tabulates sn ( K x , k ) , cn ( K x , k ) , dn ( K x , k ) for k = 1 4 , 1 2 and x = 0 ( .1 ) 4 to 7D. …
7: 22.4 Periods, Poles, and Zeros
For example, the poles of sn ( z , k ) , abbreviated as sn in the following tables, are at z = 2 m K + ( 2 n + 1 ) i K . … Then: (a) In any lattice unit cell p q ( z , k ) has a simple zero at z = p and a simple pole at z = q . (b) The difference between p and the nearest q is a half-period of p q ( z , k ) . This half-period will be plus or minus a member of the triple K , i K , K + i K ; the other two members of this triple are quarter periods of p q ( z , k ) . … For example, sn ( z + K , k ) = cd ( z , k ) . …
8: 20.4 Values at z = 0
20.4.1 θ 1 ( 0 , q ) = θ 2 ( 0 , q ) = θ 3 ( 0 , q ) = θ 4 ( 0 , q ) = 0 ,
Jacobi’s Identity
20.4.6 θ 1 ( 0 , q ) = θ 2 ( 0 , q ) θ 3 ( 0 , q ) θ 4 ( 0 , q ) .
20.4.7 θ 1 ′′ ( 0 , q ) = θ 2 ′′′ ( 0 , q ) = θ 3 ′′′ ( 0 , q ) = θ 4 ′′′ ( 0 , q ) = 0 .
20.4.12 θ 1 ′′′ ( 0 , q ) θ 1 ( 0 , q ) = θ 2 ′′ ( 0 , q ) θ 2 ( 0 , q ) + θ 3 ′′ ( 0 , q ) θ 3 ( 0 , q ) + θ 4 ′′ ( 0 , q ) θ 4 ( 0 , q ) .
9: 20.7 Identities
20.7.6 θ 4 2 ( 0 , q ) θ 1 ( w + z , q ) θ 1 ( w z , q ) = θ 3 2 ( w , q ) θ 2 2 ( z , q ) θ 2 2 ( w , q ) θ 3 2 ( z , q ) ,
20.7.7 θ 4 2 ( 0 , q ) θ 2 ( w + z , q ) θ 2 ( w z , q ) = θ 4 2 ( w , q ) θ 2 2 ( z , q ) θ 1 2 ( w , q ) θ 3 2 ( z , q ) ,
20.7.8 θ 4 2 ( 0 , q ) θ 3 ( w + z , q ) θ 3 ( w z , q ) = θ 4 2 ( w , q ) θ 3 2 ( z , q ) θ 1 2 ( w , q ) θ 2 2 ( z , q ) ,
20.7.9 θ 4 2 ( 0 , q ) θ 4 ( w + z , q ) θ 4 ( w z , q ) = θ 3 2 ( w , q ) θ 3 2 ( z , q ) θ 2 2 ( w , q ) θ 2 2 ( z , q ) .
20.7.10 θ 1 ( 2 z , q ) = 2 θ 1 ( z , q ) θ 2 ( z , q ) θ 3 ( z , q ) θ 4 ( z , q ) θ 2 ( 0 , q ) θ 3 ( 0 , q ) θ 4 ( 0 , q ) .
10: 22.1 Special Notation
The functions treated in this chapter are the three principal Jacobian elliptic functions sn ( z , k ) , cn ( z , k ) , dn ( z , k ) ; the nine subsidiary Jacobian elliptic functions cd ( z , k ) , sd ( z , k ) , nd ( z , k ) , dc ( z , k ) , nc ( z , k ) , sc ( z , k ) , ns ( z , k ) , ds ( z , k ) , cs ( z , k ) ; the amplitude function am ( x , k ) ; Jacobi’s epsilon and zeta functions ( x , k ) and Z ( x | k ) . … The notation sn ( z , k ) , cn ( z , k ) , dn ( z , k ) is due to Gudermann (1838), following Jacobi (1827); that for the subsidiary functions is due to Glaisher (1882). Other notations for sn ( z , k ) are sn ( z | m ) and sn ( z , m ) with m = k 2 ; see Abramowitz and Stegun (1964) and Walker (1996). …