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21: 26.5 Lattice Paths: Catalan Numbers
Table 26.5.1: Catalan numbers.
n C ( n ) n C ( n ) n C ( n )
3 5 10 16796 17 1296 44790
22: 26.10 Integer Partitions: Other Restrictions
Table 26.10.1: Partitions restricted by difference conditions, or equivalently with parts from A j , k .
p ( 𝒟 , n ) p ( 𝒟 2 , n ) p ( 𝒟 2 , T , n ) p ( 𝒟 3 , n )
16 32 17 11 10
17 38 19 12 12
23: 27.2 Functions
Table 27.2.1: Primes.
n p n p n + 10 p n + 20 p n + 30 p n + 40 p n + 50 p n + 60 p n + 70 p n + 80 p n + 90
7 17 59 103 157 211 269 331 389 449 509
Table 27.2.2: Functions related to division.
n ϕ ( n ) d ( n ) σ ( n ) n ϕ ( n ) d ( n ) σ ( n ) n ϕ ( n ) d ( n ) σ ( n ) n ϕ ( n ) d ( n ) σ ( n )
4 2 3 7 17 16 2 18 30 8 8 72 43 42 2 44
24: Bibliography E
  • A. Erdélyi, W. Magnus, F. Oberhettinger, and F. G. Tricomi (1953a) Higher Transcendental Functions. Vol. I. McGraw-Hill Book Company, Inc., New York-Toronto-London.
  • A. Erdélyi, W. Magnus, F. Oberhettinger, and F. G. Tricomi (1953b) Higher Transcendental Functions. Vol. II. McGraw-Hill Book Company, Inc., New York-Toronto-London.
  • F. H. L. Essler, H. Frahm, A. R. Its, and V. E. Korepin (1996) Painlevé transcendent describes quantum correlation function of the X X Z antiferromagnet away from the free-fermion point. J. Phys. A 29 (17), pp. 5619–5626.
  • 25: 4.19 Maclaurin Series and Laurent Series
    4.19.3 tan z = z + z 3 3 + 2 15 z 5 + 17 315 z 7 + + ( 1 ) n 1 2 2 n ( 2 2 n 1 ) B 2 n ( 2 n ) ! z 2 n 1 + , | z | < 1 2 π ,
    26: 17.5 ϕ 0 0 , ϕ 0 1 , ϕ 1 1 Functions
    27: 26.7 Set Partitions: Bell Numbers
    Table 26.7.1: Bell numbers.
    n B ( n ) n B ( n )
    7 877 17 8 28648 69804
    28: 33.19 Power-Series Expansions in r
    29: 13.9 Zeros
    30: 23.22 Methods of Computation
    Then α = 1 2 i , β = 1 , γ = 2 i ; k 2 = ( 7 + 6 i ) / 17 , and k 2 = ( 10 6 i ) / 17 . …