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11: 27.13 Functions
The basic problem is that of expressing a given positive integer n as a sum of integers from some prescribed set S whose members are primes, squares, cubes, or other special integers. … This problem is named after Edward Waring who, in 1770, stated without proof and with limited numerical evidence, that every positive integer n is the sum of four squares, of nine cubes, of nineteen fourth powers, and so on. …
27.13.5 ( ϑ ( x ) ) 2 = 1 + n = 1 r 2 ( n ) x n .
By similar methods Jacobi proved that r 4 ( n ) = 8 σ 1 ( n ) if n is odd, whereas, if n is even, r 4 ( n ) = 24 times the sum of the odd divisors of n . …
12: 26.12 Plane Partitions
where σ 2 ( j ) is the sum of the squares of the divisors of j . …
13: 18.39 Applications in the Physical Sciences
The fact that non- L 2 continuum scattering eigenstates may be expressed in terms or (infinite) sums of L 2 functions allows a reformulation of scattering theory in atomic physics wherein no non- L 2 functions need appear. …
14: 18.18 Sums
In all three cases of Jacobi, Laguerre and Hermite, if f ( x ) is L 2 on the corresponding interval with respect to the corresponding weight function and if a n , b n , d n are given by (18.18.1), (18.18.5), (18.18.7), respectively, then the respective series expansions (18.18.2), (18.18.4), (18.18.6) are valid with the sums converging in L 2 sense. …
15: 27.6 Divisor Sums
27.6.1 d | n λ ( d ) = { 1 , n  is a square , 0 , otherwise .
16: 1.8 Fourier Series
1.8.5 1 π π π | f ( x ) | 2 d x = 1 2 | a 0 | 2 + n = 1 ( | a n | 2 + | b n | 2 ) ,
1.8.6 1 2 π π π | f ( x ) | 2 d x = n = | c n | 2 ,
17: 1.18 Linear Second Order Differential Operators and Eigenfunction Expansions
1.18.64 f ( x ) = 𝝈 c f ^ ( λ ) ϕ λ ( x ) d λ + 𝝈 p f ^ ( λ n ) ϕ λ n ( x ) , f ( x ) C ( X ) L 2 ( X ) .
1.18.65 X | f ( x ) | 2 d x = 𝝈 c | f ^ ( λ ) | 2 d λ + 𝝈 p | f ^ ( λ n ) | 2 , f L 2 ( X ) .
1.18.66 ( z T ) 1 f , f = 𝝈 p | f ^ ( λ n ) | 2 z λ n + 𝝈 c | f ^ ( λ ) | 2 d λ z λ , f L 2 ( X ) , z 𝝈 .
18: 26.18 Counting Techniques
26.18.1 | S ( A 1 A 2 A n ) | = | S | + t = 1 n ( 1 ) t 1 j 1 < j 2 < < j t n | A j 1 A j 2 A j t | .
26.18.2 N + t = 1 n ( 1 ) t 1 j 1 < j 2 < < j t n N p j 1 p j 2 p j t .
With the notation of §26.15, the number of placements of n nonattacking rooks on an n × n chessboard that avoid the squares in a specified subset B is
26.18.3 n ! + t = 1 n ( 1 ) t r t ( B ) ( n t ) ! .
26.18.4 k n + t = 1 n ( 1 ) t ( k t ) ( k t ) n .
19: 28.30 Expansions in Series of Eigenfunctions
Then every continuous 2 π -periodic function f ( x ) whose second derivative is square-integrable over the interval [ 0 , 2 π ] can be expanded in a uniformly and absolutely convergent series
28.30.3 f ( x ) = m = 0 f m w m ( x ) ,
20: 22.11 Fourier and Hyperbolic Series
22.11.13 sn 2 ( z , k ) = 1 k 2 ( 1 E K ) 2 π 2 k 2 K 2 n = 1 n q n 1 q 2 n cos ( 2 n ζ ) .