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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, 祭音Myyura

Description​

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

f(s)=∫0∞ts−1exp⁡(−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.
∫01ts−1exp⁡(−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.
∫1cts−1exp⁡(−t) dt<n!n−s.\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=∫0∞g(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∞(log⁡t)2exp⁡(−t) dt−(∫0∞(log⁡t)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.

d2log⁡f(s)ds2∣s=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∞(log⁡r)2p(r) dr−(∫0∞(log⁡r)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)=∫0∞ts−1e−t dt.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 nn, et>tn/n!e^t>t^n/n!。

  • (a)对 s>0s>0,证明

    ∫01ts−1e−t dt<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,

    ∫1cts−1e−t dt<n!n−s.\int_1^ct^{s-1}e^{-t}\,\mathrm dt <\frac{n!}{n-s}.

(3)若

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

求 g(t,s)g(t,s);无需证明可交换微分和积分。

(4)求

D=∫0∞(log⁡t)2e−t dt−(∫0∞(log⁡t)e−t dt)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

d2ds2log⁡f(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).

求

S=∫0∞(log⁡r)2p(r) dr−(∫0∞(log⁡r)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.

Kai​

(1)​

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

f(1)=∫0∞t1−1exp⁡(−t) dt=∫0∞exp⁡(−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:

∫0∞exp⁡(−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 ∫01ts−1exp⁡(−t) dt<1s\int_0^1 t^{s-1} \exp(-t) \,\mathrm{d}t < \frac{1}{s} for positive real numbers ss​

For t>0t>0, e−t<1e^{-t}<1. Hence, since s>0s>0,

∫01ts−1e−t dt<∫01ts−1 dt=1s.\int_0^1 t^{s-1}e^{-t}\,\mathrm{d}t <\int_0^1 t^{s-1}\,\mathrm{d}t =\frac1s.

Part 2: Show that ∫1cts−1exp⁡(−t) dt<n!n−s\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:

∫1cts−1exp⁡(−t) dt<n!n−s.\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:

∫1cts−1exp⁡(−t) dt<∫1cts−1n!tn dt=n!∫1cts−n−1 dt.\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!∫1cts−n−1 dt=n![ts−ns−n]1c=n!n−s(1−1cn−s).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 1cn−s\frac{1}{c^{n-s}} is less than 11, which means:

1−1cn−s<1.1 - \frac{1}{c^{n-s}} < 1.

Thus:

∫1cts−1exp⁡(−t) dt<n!n−s.\int_1^c t^{s-1} \exp(-t) \,\mathrm{d}t < \frac{n!}{n-s}.

(3)​

Given:

d2f(s)ds2=∫0∞g(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)=∫0∞ts−1exp⁡(−t) dt.f(s) = \int_0^\infty t^{s-1} \exp(-t) \,\mathrm{d}t.

First derivative:

df(s)ds=∫0∞∂∂s(ts−1)exp⁡(−t) dt=∫0∞ts−1log⁡(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=∫0∞∂∂s(ts−1log⁡(t))exp⁡(−t) dt=∫0∞ts−1log⁡2(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)=ts−1log⁡2(t)g(t, s) = t^{s-1} \log^2(t).

(4)​

We need to find the value of the expression

D=∫0∞(log⁡t)2exp⁡(−t) dt−(∫0∞(log⁡t)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 (log⁡t)2(\log t)^2 and another involving log⁡t\log t. We are also given the hint that the following relation holds:

d2log⁡f(s)ds2∣s=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=∫0∞ts−1log⁡2(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:

f′′(1)=∫0∞t1−1log⁡2(t)exp⁡(−t) dt=∫0∞log⁡2(t)exp⁡(−t) dt.f''(1) = \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∞(log⁡t)2exp⁡(−t) dt.\int_0^\infty (\log t)^2 \exp(-t) \,\mathrm{d}t.

Thus, we have:

∫0∞(log⁡t)2exp⁡(−t) dt=f′′(1).\int_0^\infty (\log t)^2 \exp(-t) \,\mathrm{d}t = f''(1).

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:

d2log⁡f(s)ds2∣s=1=π26.\frac{\mathrm{d}^2 \log f(s)}{\mathrm{d}s^2}\bigg|_{s=1} = \frac{\pi^2}{6}.

We know that:

d2log⁡f(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 ∫0∞log⁡texp⁡(−t) dt\int_0^\infty \log t \exp(-t) \,\mathrm{d}t), and f′′(1)f''(1) is the second moment (which is ∫0∞log⁡2texp⁡(−t) dt\int_0^\infty \log^2 t \exp(-t) \,\mathrm{d}t).

We can express:

d2log⁡f(s)ds2∣s=1=f′′(1)−(f′(1))2.\left.\frac{\mathrm{d}^2\log f(s)}{\mathrm{d}s^2}\right|_{s=1} = f''(1) - \left(f'(1)\right)^2.

Given:

d2log⁡f(s)ds2∣s=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∞(log⁡r)2p(r) dr−(∫0∞(log⁡r)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).

The substitution u=r2/(2α)u=r^2/(2\alpha) gives p(r) dr=e−u dup(r)\,\mathrm dr=e^{-u}\,\mathrm du and log⁡r=12log⁡u+12log⁡(2α)\log r=\tfrac12\log u+\tfrac12\log(2\alpha). Adding a constant does not change variance, so (4) directly gives S=D/4=π2/24S=D/4=\pi^2/24.

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 zero-mean normal components, each with variance α\alpha.

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

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

E[log⁡r]=∫0∞(log⁡r)p(r) dr=∫0∞log⁡r⋅rαexp⁡(−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=r drα\mathrm{d}u = \frac{r \,\mathrm{d}r}{\alpha}.

The integral becomes:

E[log⁡r]=∫0∞log⁡(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[log⁡r]=12log⁡(2α)∫0∞exp⁡(−u) du+12∫0∞log⁡uexp⁡(−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:

∫0∞log⁡uexp⁡(−u) du=−γ,\int_0^\infty \log u \exp(-u) \,\mathrm{d}u = -\gamma,

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

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

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

Next, we need to compute the second moment:

E[(log⁡r)2]=∫0∞(log⁡r)2p(r) dr=∫0∞(log⁡r)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[(log⁡r)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[(log⁡r)2]=14[log⁡(2α)]2+12log⁡(2α)∫0∞log⁡uexp⁡(−u) du+14∫0∞(log⁡u)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:

∫0∞log⁡uexp⁡(−u) du=−γ,\int_0^\infty \log u \exp(-u) \,\mathrm{d}u = -\gamma,

and

∫0∞(log⁡u)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[(log⁡r)2]=14[log⁡(2α)]2−γ2log⁡(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[(log⁡r)2]−(E[log⁡r])2.S = \mathbb{E}[(\log r)^2] - \left(\mathbb{E}[\log r]\right)^2.

Substitute the values:

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

so:

(E[log⁡r])2=14[log⁡(2α)]2−γ2log⁡(2α)+γ24.\left(\mathbb{E}[\log r]\right)^2 = \frac{1}{4} \left[\log(2\alpha)\right]^2 - \frac{\gamma}{2} \log(2\alpha) + \frac{\gamma^2}{4}.

Subtracting:

S=14[log⁡(2α)]2−γ2log⁡(2α)+14(γ2+π26)−(14[log⁡(2α)]2−γ2log⁡(2α)+γ24).S = \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) - \left(\frac{1}{4} \left[\log(2\alpha)\right]^2 - \frac{\gamma}{2} \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