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31: 26.6 Other Lattice Path Numbers
§26.6 Other Lattice Path Numbers
Delannoy Number D ( m , n )
Motzkin Number M ( n )
Narayana Number N ( n , k )
Schröder Number r ( n )
32: 29.2 Differential Equations
29.2.9 d 2 w d η 2 + ( g ν ( ν + 1 ) ( η ) ) w = 0 ,
29.2.11 ζ = ( η ; g 2 , g 3 ) = ( η ) ,
33: 20.7 Identities
20.7.15 A A ( τ ) = 1 / θ 4 ( 0 | 2 τ ) ,
20.7.16 θ 1 ( 2 z | 2 τ ) = A θ 1 ( z | τ ) θ 2 ( z | τ ) ,
§20.7(viii) Transformations of Lattice Parameter
20.7.28 θ 3 ( z | τ + 1 ) = θ 4 ( z | τ ) ,
20.7.29 θ 4 ( z | τ + 1 ) = θ 3 ( z | τ ) .
34: 20.10 Integrals
§20.10(i) Mellin Transforms with respect to the Lattice Parameter
§20.10(ii) Laplace Transforms with respect to the Lattice Parameter
35: 20.1 Special Notation
m , n integers.
τ ( ) the lattice parameter, τ > 0 .
q ( ) the nome, q = e i π τ , 0 < | q | < 1 . Since τ is not a single-valued function of q , it is assumed that τ is known, even when q is specified. Most applications concern the rectangular case τ = 0 , τ > 0 , so that 0 < q < 1 and τ and q are uniquely related.
36: 26.9 Integer Partitions: Restricted Number and Part Size
It follows that p k ( n ) also equals the number of partitions of n into parts that are less than or equal to k . … It is also equal to the number of lattice paths from ( 0 , 0 ) to ( m , k ) that have exactly n vertices ( h , j ) , 1 h m , 1 j k , above and to the left of the lattice path. …
Figure 26.9.2: The partition 5 + 5 + 3 + 2 represented as a lattice path.
37: 20.5 Infinite Products and Related Results
20.5.5 θ 1 ( z | τ ) = θ 1 ( 0 | τ ) sin z n = 1 sin ( n π τ + z ) sin ( n π τ z ) sin 2 ( n π τ ) ,
20.5.6 θ 2 ( z | τ ) = θ 2 ( 0 | τ ) cos z n = 1 cos ( n π τ + z ) cos ( n π τ z ) cos 2 ( n π τ ) ,
20.5.7 θ 3 ( z | τ ) = θ 3 ( 0 | τ ) n = 1 cos ( ( n 1 2 ) π τ + z ) cos ( ( n 1 2 ) π τ z ) cos 2 ( ( n 1 2 ) π τ ) ,
20.5.8 θ 4 ( z | τ ) = θ 4 ( 0 | τ ) n = 1 sin ( ( n 1 2 ) π τ + z ) sin ( ( n 1 2 ) π τ z ) sin 2 ( ( n 1 2 ) π τ ) .
20.5.9 θ 3 ( π z | τ ) = n = p 2 n q n 2 = n = 1 ( 1 q 2 n ) ( 1 + q 2 n 1 p 2 ) ( 1 + q 2 n 1 p 2 ) ,
38: 21.3 Symmetry and Quasi-Periodicity
The set of points 𝐦 1 + 𝛀 𝐦 2 form a g -dimensional lattice, the period lattice of the Riemann theta function. …
39: 26.4 Lattice Paths: Multinomial Coefficients and Set Partitions
§26.4 Lattice Paths: Multinomial Coefficients and Set Partitions
§26.4(i) Definitions
It is also the number of k -dimensional lattice paths from ( 0 , 0 , , 0 ) to ( n 1 , n 2 , , n k ) . …
40: 20.9 Relations to Other Functions
20.9.1 k = θ 2 2 ( 0 | τ ) / θ 3 2 ( 0 | τ )