k = 0 ∑ ∞ ∏ j = 0 k ( 2 j + 3 ) k !
If the value of the expression above is of the form a + b π c , where a and c are integers and b is a rational number, then find the value of 1 0 3 ( a 3 + b 3 + c 3 ) .
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The following sum mentioned in the question can be written in the form n = 2 ∑ ∞ ( 2 n ) ! ( n − 2 ) ! 2 n n ! = n = 2 ∑ ∞ Γ ( 2 n + 1 ) ( n − 1 ) Γ ( n + 1 ) Γ ( n ) 2 n we know that ∫ 0 1 t x − 1 ( 1 − t ) y − 1 d t = Γ ( x + y ) Γ ( x ) Γ ( y ) Therefore the sum in terms of the gamma function can be written as n = 2 ∑ ∞ n − 1 2 n ∫ 0 1 t n ( 1 − t ) n − 1 d t on interchanging the sum and integral we get ∫ 0 1 1 − t 1 n = 2 ∑ ∞ n − 1 ( 2 t ( 1 − t ) ) n d t = ∫ 0 1 − ( 2 t ln ( 1 − 2 t ( 1 − t ) ) ) d t since n = 2 ∑ ∞ n − 1 ( 2 t ( 1 − t ) ) n = − 2 t ( 1 − t ) ln ( 1 − 2 t ( 1 − t ) ) by applying Integration by parts , we will get ∫ 0 1 − 2 t ln ( 1 − 2 t ( 1 − t ) ) d t = 2 − 2 π therefore a = 2 , b = − 2 1 and c = 1 i.e 1 0 3 ( 8 − 8 1 + 1 ) = 8 8 7 5
This solution will be heavily based on this paper by Renzo Sprugnoli.
Simplifying the summand gives us
∏ j = 0 k ( 2 k + 3 ) k ! = ( 2 k + 3 ) ! ! k ! = ( 2 k + 3 ) ! 2 k + 1 k ! ( k + 1 ) ! = ( 2 k + 3 ) ( k + 1 ) ( 2 k + 2 k + 1 ) 2 k + 1
After reindexing we get
k = 0 ∑ ∞ ( 2 k + 3 ) ( k + 1 ) ( 2 k + 2 k + 1 ) 2 k + 1 = k = 1 ∑ ∞ ( 2 k + 1 ) ( k ) ( 2 k k ) 2 k = k = 1 ∑ ∞ k ( 2 k k ) 2 k − ( 2 k + 1 ) ( 2 k k ) 2 k + 1
We can further simplify the term on the right to get
k = 1 ∑ ∞ ( 2 k + 1 ) ( 2 k k ) 2 k + 1 = k = 1 ∑ ∞ 2 ( k + 1 ) ( k + 1 ) 2 ( 2 k + 2 k + 1 ) 2 k + 1 = k = 1 ∑ ∞ ( k + 1 ) ( 2 k + 2 k + 1 ) 2 k + 2 = 2 ⎝ ⎜ ⎜ ⎛ k = 1 ∑ ∞ k ( 2 k k ) 2 k − 1 ⎠ ⎟ ⎟ ⎞ k = 1 ∑ ∞ k ( 2 k k ) 2 k − ( 2 k + 1 ) ( 2 k k ) 2 k + 1 = k = 1 ∑ ∞ k ( 2 k k ) 2 k − 2 ⎝ ⎜ ⎜ ⎛ k = 1 ∑ ∞ k ( 2 k k ) 2 k − 1 ⎠ ⎟ ⎟ ⎞ = 2 − k = 1 ∑ ∞ k ( 2 k k ) 2 k
Now, let Z k denote ( 2 k k ) 2 k , and its generating function be Z ( t ) = ∑ k = 0 ∞ Z k t k . We can show that Z k + 1 = ( 2 k + 2 k + 1 ) 2 k + 1 = ( k + 1 ) 2 2 ( k + 1 ) ( 2 k + 1 ) 2 ( 2 k k ) 2 k = 2 k + 1 k + 1 ( 2 k k ) 2 k = 2 k + 1 k + 1 Z k 2 ( k + 1 ) Z k + 1 − Z k + 1 = k Z k + Z k 2 Z ′ ( t ) − t Z ( t ) − Z 0 = t Z ′ ( t ) + Z ( t ) t ( 2 − t ) Z ′ ( t ) − ( 1 + t ) Z ( t ) + 1 = 0
This differential equation can be solved by integrating factor to yield Z ( t ) = 2 − t 2 + ( 2 − t ) 2 3 2 t arcsin 2 t
Now, let W ( t ) = ∑ k = 1 ∞ W k t k = ∑ k = 1 ∞ k ( 2 k k ) 2 k t k . To get W ( t ) from Z ( t ) , we can observe that W k = k Z k . Knowing this, it is simply a matter of reindexing then integrating. We can thus define W ( t ) = ∫ 0 t z Z ( z ) − Z 0 d z = ∫ 0 t z ( 2 − z 2 + ( 2 − z ) 2 3 2 z arcsin 2 z ) − 1 d z = 2 2 − t t arcsin 2 t
Going back to the original sum in question, it is obvious that W ( 1 ) = k = 1 ∑ ∞ k ( 2 k k ) 2 k = 2 2 − 1 1 arcsin 2 1 = 2 arcsin 2 1 = 2 π
Hence ∑ k = 0 ∞ ∏ j = 0 k ( 2 j + 3 ) k ! = 2 − 2 π
Thanks for that interesting paper!!!!
There is a really beautiful approach to solve this problem. Here, I refer to the w a l l i s p r o d u c t for odd powers of sin ( x ) (which you can pretty easily derive using the reduction formula), which is,
∫ 0 2 π sin 2 n + 1 ( x ) d x = ( 1 ) ( 3 ) ( 5 ) … ( 2 n + 1 ) ( 2 n ) n ! ∀ n ∈ N .
Using this, the above sum can be written as ∑ k = 1 ∞ ( 2 k ) ( k ) 1 ∫ 0 2 π sin 2 k + 1 ( x ) d x
Swapping the integral and summation,
∫ 0 2 π sin ( x ) ∑ k = 1 ∞ k ( 2 sin 2 ( x ) ) k d x
If you take 2 sin 2 ( x ) = t , you note that the term k ( 2 sin 2 ( x ) ) k = ∫ t k − 1 d t .
The sum as of now is:
∫ 0 2 π sin ( x ) ∑ k = 1 ∞ ∫ t k − 1 d t d x
Swapping the inner integral and summation,
∫ 0 2 π sin ( x ) ∫ ∑ k = 1 ∞ t k − 1 d t d x
Because 0 < t < 1 ∀ x ∈ R ,
∫ 0 2 π sin ( x ) ∫ 1 / ( 1 − t ) d t d x
After a couple of steps, this integral is:
∫ 0 2 π sin ( x ) ln ∣ 1 + cos 2 ( x ) ∣ d x .
This can be easily solved using u-substitution to give the result 2 − 2 π
Nice approach!!
Let us denote the product P = j = 0 ∏ k ( 2 j + 3 ) = j = 1 ∏ k + 1 ( 2 j + 1 ) = ( 2 k + 3 ) ! ! The latter double factorial can further be expressed in terms of gamma function as ( 2 k + 3 ) ! ! = π 2 k + 2 Γ ( k + 2 5 ) = π 2 k + 2 ( 2 2 k + 4 ( n + 2 ) ! ( 2 k + 4 ) ! π ) and simplifying the latter expression we can get k = 0 ∑ ∞ k ! P − 1 = k = 0 ∑ ∞ ( 2 k + 1 ) ( 2 k + 3 ) ( 2 k ) ! 2 k ( k ! ) 2 = 2 1 k = 0 ∑ ∞ ( 2 k + 1 1 − 2 k + 3 1 ) 2 n ( k 2 k ) − 1 Since 2 ( sin − 1 x ) 2 = k = 1 ∑ ∞ k 2 ( 2 x ) 2 k ( k 2 k ) − 1 we want to get rid of k 2 term in the denominator as first we differentiate the function and we repeate once again and hence on multiplying by x we can get 1 − x 2 2 sin − 1 x 2 x d x d 1 − x 2 sin − 1 x = ( 1 − x 2 ) 1 − x 2 x sin − 1 x + x 2 1 − x 2 = = k = 1 ∑ ∞ k ( 2 k ) 2 k ( k 2 k ) − 1 k = 1 ∑ ∞ ( 2 x ) 2 k ( k 2 k ) − 1 now we integrate with respect to x from 0 to 2 1 we get 2 1 k = 1 ∑ ∞ 2 k + 1 2 k ( k 2 k ) − 1 = 1 − x 2 sin − 1 x − x ∣ 0 2 1 = 2 1 ( 2 π − 1 ) and hence we have k = 0 ∑ ∞ 2 k + 1 2 k ( k 2 k ) − 1 = 2 π similarly we multiply by x 2 and hnece on integrating from to 0 to 2 1 . We get k = 1 ∑ ∞ 2 k + 3 2 k ( k 2 k ) − 1 k = 0 ∑ ∞ 2 k + 3 2 k ( k 2 k ) − 1 = 2 2 ( 4 2 3 π − 6 2 1 3 ) = 2 3 π − 4 and hence k = 0 ∑ ∞ k ! ( j = 0 ∏ k ( 2 j + 3 ) ) − 1 = 2 1 ( 2 π + 4 − 2 3 π ) = 2 − 2 π
I left the working of integral since its not difficult to do. One can now easily derive the following more identities k ≥ 0 ∑ 2 k + 1 2 k ( k 2 k ) − 1 k ≥ 0 ∑ 2 k + 3 2 k ( k 2 k ) − 1 k ≥ 0 ∑ 2 k + 5 2 k ( k 2 k ) − 1 k ≥ 0 ∑ 2 k + 7 2 k ( k 2 k ) − 1 k ≥ 0 ∑ 2 k + 9 2 k ( k 2 k ) − 1 k ≥ 0 ∑ 2 k + 1 1 2 k ( k 2 k ) − 1 = 2 π = 2 3 π − 4 = 6 2 3 π − 9 1 0 4 = 1 0 9 1 π − 7 5 2 1 1 6 = 7 0 1 4 5 1 π − 3 6 7 5 2 3 8 9 1 2 = 1 2 6 5 7 9 7 π − 1 9 8 4 5 2 8 6 3 2 0 4 and soon. We can even solve using beta function.
I'm stupid
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The following identity is due to Lehmer (from a paper in the American Mathematical Monthly, 1985): m ≥ 1 ∑ m ( m 2 m ) ( 2 x ) 2 m = 1 − x 2 2 x sin − 1 x . Take the antiderivative of both sides (use integration by parts on the right, plug in 0 to get the integration constant); then plug in k = m + 1 : m ≥ 1 ∑ m ( 2 m + 1 ) ( 2 m ) ! 2 2 m x 2 m + 1 ( m ! ) 2 m ≥ 1 ∑ ( 2 m + 1 ) ! 2 2 m x 2 m + 1 ( m − 1 ) ! m ! k ≥ 0 ∑ ( 2 k + 3 ) ! 2 2 k + 2 x 2 k + 3 k ! ( k + 1 ) ! k ≥ 0 ∑ ( 2 k + 3 ) ! 2 k + 1 x 2 k + 3 k ! ( 2 ⋅ 4 ⋯ ( 2 k + 2 ) ) k ≥ 0 ∑ 2 k + 1 x 2 k + 3 ∏ j = 0 k ( 2 j + 3 ) k ! = 2 x − 2 ( sin − 1 x ) 1 − x 2 = 2 x − 2 ( sin − 1 x ) 1 − x 2 = 2 x − 2 ( sin − 1 x ) 1 − x 2 = 2 x − 2 ( sin − 1 x ) 1 − x 2 = 2 x − 2 ( sin − 1 x ) 1 − x 2 Now plug in x = 1 / 2 , to get 2 1 k ≥ 0 ∑ ∏ j = 0 k ( 2 j + 3 ) k ! k ≥ 0 ∑ ∏ j = 0 k ( 2 j + 3 ) k ! = 2 2 − 2 2 ( sin − 1 2 1 ) = 2 − 2 ( 4 π ) = 2 − 2 π . So a = 2 , b = − 1 / 2 , c = 1 and the answer is 8 8 7 5 .