(2017年10月AMM征解题)求证
∏j≥1e−1/j(1+1j+12j2)=eπ/2+e−π/2πeγ.
记
xn=n∏k=1(1+1k+12k2)=n∏k=1(2k+1)2+1(2k)2,
则
2n∏k=1(1+1k2)xn=2n∏k=1k2+1k2n∏k=1(2k+1)2+1(2k)2=(12+1)(22+1)(42+1)⋯[(2n)2+1]1232⋯(2n−1)2[(2n+1)2+1]=2n∏k=1(1+14k2)⋅[(2n)!!(2n−1)!!]214n2+4n+2,
由Wallis公式可知
limn→∞[(2n)!!(2n−1)!!]212n+1=π2.
由sinhx的无穷乘积
sinh(πx)πx=∞∏k=1(1+x2k2)
可知
∞∏k=1(1+1k2)=eπ−e−π2π,∞∏k=1(1+14k2)=eπ/2−e−π/2π,
而调和数列
Hn=n∑k=11k=lnn+γ+o(1),
故
limn→∞nn∏k=1e−1/k=e−γ.
因此所求积分为
eπ−e−π2πeγ×π2×eπ/2−e−π/2π=eπ/2+e−π/2πeγ.
事实上,我们还有
cosh(πx)=∞∏n=1(1+4x2(2n−1)2),sinh(πx)πx=∞∏n=1(1+x2n2),cos(πx)=∞∏n=1(1−4x2(2n−1)2),sin(πx)πx=∞∏n=1(1−x2n2),
另外
√2sin(x+14π)=∞∏n=0(1+(−1)nx2n+1),√x+1sin(√x+12π)=∞∏n=0(1−x4n2−1),−√x−1csch(π2)sin(√x−12π)=∞∏n=0(1−x4n2+1),−√−x−1csch(π√a)sin(√−x−1√aπ)=∞∏n=0(1+xan2+1),e−γxΓ(1+x)=∞∏n=11+x/nex/n,
对于求和,我们有
∞∑n=11n2−x2=12x2−π2xcot(πx),|x|<∞∞∑n=11(n2−x2)2=−12x4−π24x2csc2(πx)+π4x3cot(πx),|x|<∞∞∑n=11(2n−1)2−x2=π4xtan(π2x),|x|<∞∞∑n=11[(2n−1)2−x2]2=π216x2sec(π2x)−π8x3tan(π2x),|x|<∞∞∑n=11n2+x2=π2xcoth(πx)−12x2,|x|<∞∞∑n=11(2n−1)2+x2=π4xtanh(π2x),|x|<∞
其中sinhx=ex−e−x2,coshx=ex+e−x2,cschx=2ex−e−x,tanhx=ex−e−xex+e−x,cothx=ex+e−xex−e−x.
The Weierstrass factorization theorem. Sometimes called the Weierstrass product/factor theorem.
Let f be an entire function, and let {an} be the non-zero zeros of ƒ repeated according to multiplicity; suppose also that ƒ′′ has a zero at z=0 of order m≥0 (a zero of order m=0 at z=0 means f(0)≠0.
Then there exists an entire function g and a sequence of integers {pn} such that
f(z)=zmeg(z)∞∏n=1Epn(zan).
====Examples of factorization====
sinπz=πz∏n≠0(1−zn)ez/n=πz∞∏n=1(1−(zn)2)cosπz=∏q∈Z,qodd(1−2zq)e2z/q=∞∏n=0⎛⎝1−(zn+12)2⎞⎠
The cosine identity can be seen as special case of
1Γ(s−z)Γ(s+z)=1Γ(s)2∞∏n=0(1−(zn+s)2)
for s=12.
Mittag-Leffler's theorem.
== Pole expansions of meromorphic functions ==
Here are some examples of pole expansions of meromorphic functions:
1sin(z)=∑n∈Z(−1)nz−nπ=1z+2z∞∑n=1(−1)n1z2−(nπ)2,cot(z)≡cos(z)sin(z)=∑n∈Z1z−nπ=1z+2z∞∑k=11z2−(kπ)2,1sin2(z)=∑n∈Z1(z−nπ)2,1zsin(z)=1z2+∑n≠0(−1)nπn(z−πn)=1z2+∞∑n=1(−1)nnπ2zz2−(nπ)2.
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