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東京大学 情報理工学研究科 2023年8月実施 数学 第2問

Author

zephyr

Description

Consider a function f(s)f(s) defined by the following integral for positive real numbers ss.

f(s)=0ts1exp(t)dt.f(s) = \int_0^\infty t^{s-1} \exp(-t) \,\mathrm{d}t.

Answer the following questions. You may answer without showing that the above integral converges.

(1) Find the value of f(1)f(1).

(2) The inequality exp(t)>tnn!\exp(t) > \frac{t^n}{n!} holds for any positive real number tt and non-negative integer nn.

  • (a) For positive real numbers ss, show the following inequality.
01ts1exp(t)dt<1s.\int_0^1 t^{s-1} \exp(-t) \,\mathrm{d}t < \frac{1}{s}.
  • (b) When n>s>0n > s > 0, show that the following inequality holds for any real number cc that satisfies c>1c > 1.
1cts1exp(t)dt<n!ns.\int_1^c t^{s-1} \exp(-t) \,\mathrm{d}t < \frac{n!}{n-s}.

(3) When the second-order derivative of f(s)f(s) is expressed as

d2f(s)ds2=0g(t,s)exp(t)dt,\frac{\mathrm{d}^2 f(s)}{\mathrm{d}s^2} = \int_0^\infty g(t, s) \exp(-t) \,\mathrm{d}t,

find a function g(t,s)g(t, s). You may answer without showing that the order of differentiation and integration can be exchanged.

(4) Find the value of DD defined as

D=0(logt)2exp(t)dt(0(logt)exp(t)dt)2.D = \int_0^\infty (\log t)^2 \exp(-t) \,\mathrm{d}t - \left(\int_0^\infty (\log t) \exp(-t) \,\mathrm{d}t \right)^2.

Here, you may use the fact that the following relation holds.

d2logf(s)ds2s=1=π26.\frac{\mathrm{d}^2 \log f(s)}{\mathrm{d}s^2}\bigg|_{s=1} = \frac{\pi^2}{6}.

(5) Define a function p(r)p(r) for positive real numbers rr and α\alpha as

p(r)=rαexp(r22α).p(r) = \frac{r}{\alpha} \exp \left(-\frac{r^2}{2\alpha}\right).

Find the value of SS defined as

S=0(logr)2p(r)dr(0(logr)p(r)dr)2.S = \int_0^\infty (\log r)^2 p(r) \,\mathrm{d}r - \left(\int_0^\infty (\log r) p(r) \,\mathrm{d}r\right)^2.

题目描述

对正实数 ss,定义

f(s)=0ts1etdt.f(s)=\int_0^\infty t^{s-1}e^{-t}\,\mathrm dt.

无需证明积分收敛。回答下列问题。

(1)求 f(1)f(1)

(2)已知对 t>0t>0 和非负整数 nnet>tn/n!e^t>t^n/n!

  • (a)对 s>0s>0,证明
    01ts1etdt<1s.\int_0^1t^{s-1}e^{-t}\,\mathrm dt<\frac1s.
  • (b)当 n>s>0n>s>0 时,证明对任意 c>1c>1
    1cts1etdt<n!ns.\int_1^ct^{s-1}e^{-t}\,\mathrm dt <\frac{n!}{n-s}.

(3)若

f(s)=0g(t,s)etdt,f''(s)=\int_0^\infty g(t,s)e^{-t}\,\mathrm dt,

g(t,s)g(t,s);无需证明可交换微分和积分。

(4)求

D=0(logt)2etdt(0(logt)etdt)2.D=\int_0^\infty(\log t)^2e^{-t}\,\mathrm dt -\left(\int_0^\infty(\log t)e^{-t}\,\mathrm dt\right)^2.

可以使用

d2ds2logf(s)s=1=π26.\left.\frac{\mathrm d^2}{\mathrm ds^2}\log f(s)\right|_{s=1} =\frac{\pi^2}{6}.

(5)对 r,α>0r,\alpha>0 定义

p(r)=rαexp(r22α).p(r)=\frac r\alpha \exp\left(-\frac{r^2}{2\alpha}\right).

S=0(logr)2p(r)dr(0(logr)p(r)dr)2.S=\int_0^\infty(\log r)^2p(r)\,\mathrm dr -\left(\int_0^\infty(\log r)p(r)\,\mathrm dr\right)^2.

考点

  • Gamma 函数:识别积分定义并通过指数函数下界控制端点积分。
  • 参数积分的对数矩:对 ss 求导,使 logt\log t(logt)2(\log t)^2 出现在被积函数中。
  • 对数 Gamma 的二阶导数:用 (logf)=f/f(f/f)2(\log f)''=f''/f-(f'/f)^2 计算指数分布下 logT\log T 的方差。
  • Rayleigh 分布的对数矩:以 t=r2/(2α)t=r^2/(2\alpha) 变换为指数分布,并分析缩放常数对方差的影响。

Kai

(1)

We start by evaluating f(1)f(1):

f(1)=0t11exp(t)dt=0exp(t)dt.f(1) = \int_0^\infty t^{1-1} \exp(-t) \,\mathrm{d}t = \int_0^\infty \exp(-t) \,\mathrm{d}t.

This integral is well-known and is the Laplace transform of a constant function 11. Evaluating the integral:

0exp(t)dt=[exp(t)]0=(0(1))=1.\int_0^\infty \exp(-t) \,\mathrm{d}t = \left[-\exp(-t)\right]_0^\infty = \left(0 - (-1)\right) = 1.

So, f(1)=1f(1) = 1.

(2)

Part 1: Show that 0ts1exp(t)dt<1s\int_0^\infty t^{s-1} \exp(-t) \,\mathrm{d}t < \frac{1}{s} for positive real numbers ss

To show this inequality, we start by considering the definition of f(s)f(s):

f(s)=0ts1exp(t)dt.f(s) = \int_0^\infty t^{s-1} \exp(-t) \,\mathrm{d}t.

The problem gives us the inequality exp(t)>tnn!\exp(t) > \frac{t^n}{n!} for any positive real number tt and non-negative integer nn. Taking the reciprocal and considering the exponential function in the integrand:

exp(t)<n!tn.\exp(-t) < \frac{n!}{t^n}.

Substituting this into the integral, we obtain:

f(s)=0ts1exp(t)dt<0ts1n!tndt=n!0tsn1dt.f(s) = \int_0^\infty t^{s-1} \exp(-t) \,\mathrm{d}t < \int_0^\infty t^{s-1} \frac{n!}{t^n} \,\mathrm{d}t = n! \int_0^\infty t^{s-n-1} \,\mathrm{d}t.

The integral 0tsn1dt\int_0^\infty t^{s-n-1} \,\mathrm{d}t converges when sn>0s-n > 0. Evaluating this integral:

0tsn1dt=1sn.\int_0^\infty t^{s-n-1} \,\mathrm{d}t = \frac{1}{s-n}.

Thus, the inequality becomes:

f(s)<n!sn.f(s) < \frac{n!}{s-n}.

Now, by setting n=1n=1, we obtain:

f(s)<1!s1=1s.f(s) < \frac{1!}{s-1} = \frac{1}{s}.

Therefore, we have shown that:

0ts1exp(t)dt<1s.\int_0^\infty t^{s-1} \exp(-t) \,\mathrm{d}t < \frac{1}{s}.

Part 2: Show that 1cts1exp(t)dt<n!ns\int_1^c t^{s-1} \exp(-t) \,\mathrm{d}t < \frac{n!}{n-s} for n>s>0n > s > 0 and c>1c > 1

We are given that n>s>0n > s > 0 and c>1c > 1, and we need to prove the inequality:

1cts1exp(t)dt<n!ns.\int_1^c t^{s-1} \exp(-t) \,\mathrm{d}t < \frac{n!}{n-s}.

Using the same inequality exp(t)<n!tn\exp(-t) < \frac{n!}{t^n}, we substitute it into the integral:

1cts1exp(t)dt<1cts1n!tndt=n!1ctsn1dt.\int_1^c t^{s-1} \exp(-t) \,\mathrm{d}t < \int_1^c t^{s-1} \frac{n!}{t^n} \,\mathrm{d}t = n! \int_1^c t^{s-n-1} \,\mathrm{d}t.

Next, we evaluate the integral:

n!1ctsn1dt=n![tsnsn]1c=n!ns(11cns).n! \int_1^c t^{s-n-1} \,\mathrm{d}t = n! \left[\frac{t^{s-n}}{s-n}\right]_1^c = \frac{n!}{n-s} \left(1 - \frac{1}{c^{n-s}}\right).

Since c>1c > 1, the term 1cns\frac{1}{c^{n-s}} is less than 11, which means:

11cns<1.1 - \frac{1}{c^{n-s}} < 1.

Thus:

1cts1exp(t)dt<n!ns.\int_1^c t^{s-1} \exp(-t) \,\mathrm{d}t < \frac{n!}{n-s}.

(3)

Given:

d2f(s)ds2=0g(t,s)exp(t)dt,\frac{\mathrm{d}^2 f(s)}{\mathrm{d}s^2} = \int_0^\infty g(t, s) \exp(-t) \,\mathrm{d}t,

We first need to compute the second derivative of f(s)f(s):

f(s)=0ts1exp(t)dt.f(s) = \int_0^\infty t^{s-1} \exp(-t) \,\mathrm{d}t.

First derivative:

df(s)ds=0s(ts1)exp(t)dt=0ts1log(t)exp(t)dt.\frac{\mathrm{d}f(s)}{\mathrm{d}s} = \int_0^\infty \frac{\partial}{\partial s} \left( t^{s-1} \right) \exp(-t) \,\mathrm{d}t = \int_0^\infty t^{s-1} \log(t) \exp(-t) \,\mathrm{d}t.

Second derivative:

d2f(s)ds2=0s(ts1log(t))exp(t)dt=0ts1log2(t)exp(t)dt.\frac{\mathrm{d}^2 f(s)}{\mathrm{d}s^2} = \int_0^\infty \frac{\partial}{\partial s} \left( t^{s-1} \log(t) \right) \exp(-t) \,\mathrm{d}t = \int_0^\infty t^{s-1} \log^2(t) \exp(-t) \,\mathrm{d}t.

Thus, g(t,s)=ts1log2(t)g(t, s) = t^{s-1} \log^2(t).

(4)

We need to find the value of the expression

D=0(logt)2exp(t)dt(0(logt)exp(t)dt)2.D = \int_0^\infty (\log t)^2 \exp(-t) \,\mathrm{d}t - \left(\int_0^\infty (\log t) \exp(-t) \,\mathrm{d}t \right)^2.

This problem requires us to calculate two integrals: one involving (logt)2(\log t)^2 and another involving logt\log t. We are also given the hint that the following relation holds:

d2logf(s)ds2s=1=π26.\frac{\mathrm{d}^2 \log f(s)}{\mathrm{d}s^2}\bigg|_{s=1} = \frac{\pi^2}{6}.

Step 1: Expressing the Second-Order Derivative of f(s)f(s)

From Question 3, we know that:

d2f(s)ds2=0ts1log2(t)exp(t)dt.\frac{\mathrm{d}^2 f(s)}{\mathrm{d}s^2} = \int_0^\infty t^{s-1} \log^2(t) \exp(-t) \,\mathrm{d}t.

Setting s=1s = 1:

d2f(1)ds2=0t11log2(t)exp(t)dt=0log2(t)exp(t)dt.\frac{\mathrm{d}^2 f(1)}{\mathrm{d}s^2} = \int_0^\infty t^{1-1} \log^2(t) \exp(-t) \,\mathrm{d}t = \int_0^\infty \log^2(t) \exp(-t) \,\mathrm{d}t.

This integral represents the first term in DD, which is:

0(logt)2exp(t)dt.\int_0^\infty (\log t)^2 \exp(-t) \,\mathrm{d}t.

Thus, we have:

0(logt)2exp(t)dt=d2f(1)ds2.\int_0^\infty (\log t)^2 \exp(-t) \,\mathrm{d}t = \frac{\mathrm{d}^2 f(1)}{\mathrm{d}s^2}.

Step 2: Calculating the First Integral

The value of the second derivative of the logarithm of f(s)f(s) at s=1s = 1 is given as:

d2logf(s)ds2s=1=π26.\frac{\mathrm{d}^2 \log f(s)}{\mathrm{d}s^2}\bigg|_{s=1} = \frac{\pi^2}{6}.

We know that:

d2logf(s)ds2=f(s)f(s)(f(s))2(f(s))2.\frac{\mathrm{d}^2 \log f(s)}{\mathrm{d}s^2} = \frac{f''(s) f(s) - \left(f'(s)\right)^2}{\left(f(s)\right)^2}.

At s=1s = 1, f(1)=1f(1) = 1, f(1)f'(1) is the first moment (which is 0logtexp(t)dt\int_0^\infty \log t \exp(-t) \,\mathrm{d}t), and f(1)f''(1) is the second moment (which is 0log2texp(t)dt\int_0^\infty \log^2 t \exp(-t) \,\mathrm{d}t).

We can express:

d2logf(1)ds2=f(1)(f(1))2.\frac{\mathrm{d}^2 \log f(1)}{\mathrm{d}s^2} = f''(1) - \left(f'(1)\right)^2.

Given:

d2logf(s)ds2s=1=π26,\frac{\mathrm{d}^2 \log f(s)}{\mathrm{d}s^2}\bigg|_{s=1} = \frac{\pi^2}{6},

Thus:

D=π26.D = \frac{\pi^2}{6}.

(5)

We are asked to find the value of SS, defined as:

S=0(logr)2p(r)dr(0(logr)p(r)dr)2,S = \int_0^\infty (\log r)^2 p(r) \,\mathrm{d}r - \left(\int_0^\infty (\log r) p(r) \,\mathrm{d}r\right)^2,

where the function p(r)p(r) is given by:

p(r)=rαexp(r22α).p(r) = \frac{r}{\alpha} \exp\left(-\frac{r^2}{2\alpha}\right).

Step 1: Identify the form of p(r)p(r)

The function p(r)p(r) is a probability density function corresponding to a Rayleigh distribution, with the parameter α\alpha. The Rayleigh distribution has the form:

p(r)=rαexp(r22α),p(r) = \frac{r}{\alpha} \exp\left(-\frac{r^2}{2\alpha}\right),

which is commonly used to describe the distribution of the magnitude of a two-dimensional vector with independent and identically distributed normal components.

Step 2: Calculation of the first moment E[logr]\mathbb{E}[\log r]

We need to compute the expected value of logr\log r under this distribution, given by:

E[logr]=0(logr)p(r)dr=0logrrαexp(r22α)dr.\mathbb{E}[\log r] = \int_0^\infty (\log r) p(r) \,\mathrm{d}r = \int_0^\infty \log r \cdot \frac{r}{\alpha} \exp\left(-\frac{r^2}{2\alpha}\right) \,\mathrm{d}r.

We perform a substitution to simplify this integral:

Let u=r22αu = \frac{r^2}{2\alpha}, hence du=rdrα\mathrm{d}u = \frac{r \,\mathrm{d}r}{\alpha}.

The integral becomes:

E[logr]=0log(2αu)exp(u)du.\mathbb{E}[\log r] = \int_0^\infty \log \left(\sqrt{2\alpha u}\right) \exp(-u) \,\mathrm{d}u.

This simplifies to:

E[logr]=12log(2α)0exp(u)du+120loguexp(u)du.\mathbb{E}[\log r] = \frac{1}{2}\log(2\alpha) \int_0^\infty \exp(-u) \,\mathrm{d}u + \frac{1}{2} \int_0^\infty \log u \exp(-u) \,\mathrm{d}u.

The first integral evaluates to 1 because it is the integral of the exponential distribution. The second integral is a well-known result:

0loguexp(u)du=γ,\int_0^\infty \log u \exp(-u) \,\mathrm{d}u = -\gamma,

where γ\gamma is the Euler-Mascheroni constant. Thus,

E[logr]=12log(2α)γ2.\mathbb{E}[\log r] = \frac{1}{2}\log(2\alpha) - \frac{\gamma}{2}.

Step 3: Calculation of the second moment E[(logr)2]\mathbb{E}[(\log r)^2]

Next, we need to compute the second moment:

E[(logr)2]=0(logr)2p(r)dr=0(logr)2rαexp(r22α)dr.\mathbb{E}[(\log r)^2] = \int_0^\infty (\log r)^2 p(r) \,\mathrm{d}r = \int_0^\infty (\log r)^2 \frac{r}{\alpha} \exp\left(-\frac{r^2}{2\alpha}\right) \,\mathrm{d}r.

Using the same substitution u=r22αu = \frac{r^2}{2\alpha}:

E[(logr)2]=0[log(2αu)]2exp(u)du.\mathbb{E}[(\log r)^2] = \int_0^\infty \left[\log\left(\sqrt{2\alpha u}\right)\right]^2 \exp(-u) \,\mathrm{d}u.

This expands to:

E[(logr)2]=14[log(2α)]2+12log(2α)0loguexp(u)du+140(logu)2exp(u)du.\mathbb{E}[(\log r)^2] = \frac{1}{4} \left[\log(2\alpha)\right]^2 + \frac{1}{2} \log(2\alpha) \int_0^\infty \log u \exp(-u) \,\mathrm{d}u + \frac{1}{4} \int_0^\infty (\log u)^2 \exp(-u) \,\mathrm{d}u.

Using the known results:

0loguexp(u)du=γ,\int_0^\infty \log u \exp(-u) \,\mathrm{d}u = -\gamma,

and

0(logu)2exp(u)du=γ2+π26,\int_0^\infty (\log u)^2 \exp(-u) \,\mathrm{d}u = \gamma^2 + \frac{\pi^2}{6},

we have:

E[(logr)2]=14[log(2α)]2γ2log(2α)+14(γ2+π26).\mathbb{E}[(\log r)^2] = \frac{1}{4} \left[\log(2\alpha)\right]^2 - \frac{\gamma}{2} \log(2\alpha) + \frac{1}{4} \left(\gamma^2 + \frac{\pi^2}{6}\right).

Step 4: Calculate SS

Finally, SS is the variance, which is given by:

S=E[(logr)2](E[logr])2.S = \mathbb{E}[(\log r)^2] - \left(\mathbb{E}[\log r]\right)^2.

Substitute the values:

E[logr]=12log(2α)γ2,\mathbb{E}[\log r] = \frac{1}{2}\log(2\alpha) - \frac{\gamma}{2},

so:

(E[logr])2=14[log(2α)]2γlog(2α)+γ24.\left(\mathbb{E}[\log r]\right)^2 = \frac{1}{4} \left[\log(2\alpha)\right]^2 - \gamma \log(2\alpha) + \frac{\gamma^2}{4}.

Subtracting:

S=14[log(2α)]2γlog(2α)+14(γ2+π26)(14[log(2α)]2γlog(2α)+γ24).S = \frac{1}{4} \left[\log(2\alpha)\right]^2 - \gamma \log(2\alpha) + \frac{1}{4} \left(\gamma^2 + \frac{\pi^2}{6}\right) - \left(\frac{1}{4} \left[\log(2\alpha)\right]^2 - \gamma \log(2\alpha) + \frac{\gamma^2}{4}\right).

Simplifying:

S=π224.S = \frac{\pi^2}{24}.

This is the final value of SS.

Knowledge

Gamma函数 不定积分 定积分 方差

解题技巧和信息

  1. Gamma Function: Recognize that f(s)f(s) represents the Gamma function Γ(s)\Gamma(s).
  2. Inequality Manipulation: Use known inequalities such as exp(t)>tnn!\exp(t) > \frac{t^n}{n!} to estimate integrals.
  3. Variance Calculation: The variance of logarithms of exponential and Rayleigh distributed variables often results in expressions involving π26\frac{\pi^2}{6}.

重点词汇

  • Gamma function 伽马函数
  • Inequality 不等式
  • Variance 方差
  • Logarithm 对数
  • Rayleigh distribution 瑞利分布
  • Logarithm 对数
  • Euler-Mascheroni constant 欧拉-马歇罗尼常数
  • Variance 方差