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) f ( s ) defined by the following integral for positive real numbers s s s .
f ( s ) = ∫ 0 ∞ t s − 1 exp ( − t ) d t . f(s) = \int_0^\infty t^{s-1} \exp(-t) \,\mathrm{d}t. f ( s ) = ∫ 0 ∞ t s − 1 exp ( − t ) 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) f ( 1 ) .
(2) The inequality exp ( t ) > t n n ! \exp(t) > \frac{t^n}{n!} exp ( t ) > n ! t n holds for any positive real number t t t and non-negative integer n n n .
(a) For positive real numbers s s s , show the following inequality.
∫ 0 1 t s − 1 exp ( − t ) d t < 1 s . \int_0^1 t^{s-1} \exp(-t) \,\mathrm{d}t < \frac{1}{s}. ∫ 0 1 t s − 1 exp ( − t ) d t < s 1 .
(b) When n > s > 0 n > s > 0 n > s > 0 , show that the following inequality holds for any real number c c c that satisfies c > 1 c > 1 c > 1 .
∫ 1 c t s − 1 exp ( − t ) d t < n ! n − s . \int_1^c t^{s-1} \exp(-t) \,\mathrm{d}t < \frac{n!}{n-s}. ∫ 1 c t s − 1 exp ( − t ) d t < n − s n ! .
(3) When the second-order derivative of f ( s ) f(s) f ( s ) is expressed as
d 2 f ( s ) d s 2 = ∫ 0 ∞ g ( t , s ) exp ( − t ) d t , \frac{\mathrm{d}^2 f(s)}{\mathrm{d}s^2} = \int_0^\infty g(t, s) \exp(-t) \,\mathrm{d}t, d s 2 d 2 f ( s ) = ∫ 0 ∞ g ( t , s ) exp ( − t ) d t ,
find a function g ( t , s ) 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 D D D defined as
D = ∫ 0 ∞ ( log t ) 2 exp ( − t ) d t − ( ∫ 0 ∞ ( log t ) exp ( − t ) d t ) 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. D = ∫ 0 ∞ ( log t ) 2 exp ( − t ) d t − ( ∫ 0 ∞ ( log t ) exp ( − t ) d t ) 2 .
Here, you may use the fact that the following relation holds.
d 2 log f ( s ) d s 2 ∣ s = 1 = π 2 6 . \frac{\mathrm{d}^2 \log f(s)}{\mathrm{d}s^2}\bigg|_{s=1} = \frac{\pi^2}{6}. d s 2 d 2 log f ( s ) s = 1 = 6 π 2 .
(5) Define a function p ( r ) p(r) p ( r ) for positive real numbers r r r and α \alpha α as
p ( r ) = r α exp ( − r 2 2 α ) . p(r) = \frac{r}{\alpha} \exp \left(-\frac{r^2}{2\alpha}\right). p ( r ) = α r exp ( − 2 α r 2 ) .
Find the value of S S S defined as
S = ∫ 0 ∞ ( log r ) 2 p ( r ) d r − ( ∫ 0 ∞ ( log r ) p ( r ) d r ) 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. S = ∫ 0 ∞ ( log r ) 2 p ( r ) d r − ( ∫ 0 ∞ ( log r ) p ( r ) d r ) 2 .
题目描述
对正实数 s s s ,定义
f ( s ) = ∫ 0 ∞ t s − 1 e − t d t . f(s)=\int_0^\infty t^{s-1}e^{-t}\,\mathrm dt. f ( s ) = ∫ 0 ∞ t s − 1 e − t d t .
无需证明积分收敛。回答下列问题。
(1)求 f ( 1 ) f(1) f ( 1 ) 。
(2)已知对 t > 0 t>0 t > 0 和非负整数 n n n ,
e t > t n / n ! e^t>t^n/n! e t > t n / n ! 。
(a)对 s > 0 s>0 s > 0 ,证明
∫ 0 1 t s − 1 e − t d t < 1 s . \int_0^1t^{s-1}e^{-t}\,\mathrm dt<\frac1s. ∫ 0 1 t s − 1 e − t d t < s 1 .
(b)当 n > s > 0 n>s>0 n > s > 0 时,证明对任意 c > 1 c>1 c > 1 ,
∫ 1 c t s − 1 e − t d t < n ! n − s . \int_1^ct^{s-1}e^{-t}\,\mathrm dt
<\frac{n!}{n-s}. ∫ 1 c t s − 1 e − t d t < n − s n ! .
(3)若
f ′ ′ ( s ) = ∫ 0 ∞ g ( t , s ) e − t d t , f''(s)=\int_0^\infty g(t,s)e^{-t}\,\mathrm dt, f ′′ ( s ) = ∫ 0 ∞ g ( t , s ) e − t d t ,
求 g ( t , s ) g(t,s) g ( t , s ) ;无需证明可交换微分和积分。
(4)求
D = ∫ 0 ∞ ( log t ) 2 e − t d t − ( ∫ 0 ∞ ( log t ) e − t d t ) 2 . D=\int_0^\infty(\log t)^2e^{-t}\,\mathrm dt
-\left(\int_0^\infty(\log t)e^{-t}\,\mathrm dt\right)^2. D = ∫ 0 ∞ ( log t ) 2 e − t d t − ( ∫ 0 ∞ ( log t ) e − t d t ) 2 .
可以使用
d 2 d s 2 log f ( s ) ∣ s = 1 = π 2 6 . \left.\frac{\mathrm d^2}{\mathrm ds^2}\log f(s)\right|_{s=1}
=\frac{\pi^2}{6}. d s 2 d 2 log f ( s ) s = 1 = 6 π 2 .
(5)对 r , α > 0 r,\alpha>0 r , α > 0 定义
p ( r ) = r α exp ( − r 2 2 α ) . p(r)=\frac r\alpha
\exp\left(-\frac{r^2}{2\alpha}\right). p ( r ) = α r exp ( − 2 α r 2 ) .
求
S = ∫ 0 ∞ ( log r ) 2 p ( r ) d r − ( ∫ 0 ∞ ( log r ) p ( r ) d r ) 2 . S=\int_0^\infty(\log r)^2p(r)\,\mathrm dr
-\left(\int_0^\infty(\log r)p(r)\,\mathrm dr\right)^2. S = ∫ 0 ∞ ( log r ) 2 p ( r ) d r − ( ∫ 0 ∞ ( log r ) p ( r ) d r ) 2 .
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 s s s 求导,使 log t \log t log t 与
( log t ) 2 (\log t)^2 ( log t ) 2 出现在被积函数中。
对数 Gamma 的二阶导数 :用
( log f ) ′ ′ = f ′ ′ / f − ( f ′ / f ) 2 (\log f)''=f''/f-(f'/f)^2 ( log f ) ′′ = f ′′ / f − ( f ′ / f ) 2 计算指数分布下 log T \log T log T 的方差。
Rayleigh 分布的对数矩 :以
t = r 2 / ( 2 α ) t=r^2/(2\alpha) t = r 2 / ( 2 α ) 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 ) :
f ( 1 ) = ∫ 0 ∞ t 1 − 1 exp ( − t ) d t = ∫ 0 ∞ exp ( − t ) d t . f(1) = \int_0^\infty t^{1-1} \exp(-t) \,\mathrm{d}t = \int_0^\infty \exp(-t) \,\mathrm{d}t. f ( 1 ) = ∫ 0 ∞ t 1 − 1 exp ( − t ) d t = ∫ 0 ∞ exp ( − t ) d t .
This integral is well-known and is the Laplace transform of a constant function 1 1 1 . Evaluating the integral:
∫ 0 ∞ exp ( − t ) d t = [ − 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. ∫ 0 ∞ exp ( − t ) d t = [ − exp ( − t ) ] 0 ∞ = ( 0 − ( − 1 ) ) = 1.
So, f ( 1 ) = 1 f(1) = 1 f ( 1 ) = 1 .
(2)
Part 1: Show that ∫ 0 ∞ t s − 1 exp ( − t ) d t < 1 s \int_0^\infty t^{s-1} \exp(-t) \,\mathrm{d}t < \frac{1}{s} ∫ 0 ∞ t s − 1 exp ( − t ) d t < s 1 for positive real numbers s s s
To show this inequality, we start by considering the definition of f ( s ) f(s) f ( s ) :
f ( s ) = ∫ 0 ∞ t s − 1 exp ( − t ) d t . f(s) = \int_0^\infty t^{s-1} \exp(-t) \,\mathrm{d}t. f ( s ) = ∫ 0 ∞ t s − 1 exp ( − t ) d t .
The problem gives us the inequality exp ( t ) > t n n ! \exp(t) > \frac{t^n}{n!} exp ( t ) > n ! t n for any positive real number t t t and non-negative integer n n n . Taking the reciprocal and considering the exponential function in the integrand:
exp ( − t ) < n ! t n . \exp(-t) < \frac{n!}{t^n}. exp ( − t ) < t n n ! .
Substituting this into the integral, we obtain:
f ( s ) = ∫ 0 ∞ t s − 1 exp ( − t ) d t < ∫ 0 ∞ t s − 1 n ! t n d t = n ! ∫ 0 ∞ t s − n − 1 d t . 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. f ( s ) = ∫ 0 ∞ t s − 1 exp ( − t ) d t < ∫ 0 ∞ t s − 1 t n n ! d t = n ! ∫ 0 ∞ t s − n − 1 d t .
The integral ∫ 0 ∞ t s − n − 1 d t \int_0^\infty t^{s-n-1} \,\mathrm{d}t ∫ 0 ∞ t s − n − 1 d t converges when s − n > 0 s-n > 0 s − n > 0 . Evaluating this integral:
∫ 0 ∞ t s − n − 1 d t = 1 s − n . \int_0^\infty t^{s-n-1} \,\mathrm{d}t = \frac{1}{s-n}. ∫ 0 ∞ t s − n − 1 d t = s − n 1 .
Thus, the inequality becomes:
f ( s ) < n ! s − n . f(s) < \frac{n!}{s-n}. f ( s ) < s − n n ! .
Now, by setting n = 1 n=1 n = 1 , we obtain:
f ( s ) < 1 ! s − 1 = 1 s . f(s) < \frac{1!}{s-1} = \frac{1}{s}. f ( s ) < s − 1 1 ! = s 1 .
Therefore, we have shown that:
∫ 0 ∞ t s − 1 exp ( − t ) d t < 1 s . \int_0^\infty t^{s-1} \exp(-t) \,\mathrm{d}t < \frac{1}{s}. ∫ 0 ∞ t s − 1 exp ( − t ) d t < s 1 .
Part 2: Show that ∫ 1 c t s − 1 exp ( − t ) d t < n ! n − s \int_1^c t^{s-1} \exp(-t) \,\mathrm{d}t < \frac{n!}{n-s} ∫ 1 c t s − 1 exp ( − t ) d t < n − s n ! for n > s > 0 n > s > 0 n > s > 0 and c > 1 c > 1 c > 1
We are given that n > s > 0 n > s > 0 n > s > 0 and c > 1 c > 1 c > 1 , and we need to prove the inequality:
∫ 1 c t s − 1 exp ( − t ) d t < n ! n − s . \int_1^c t^{s-1} \exp(-t) \,\mathrm{d}t < \frac{n!}{n-s}. ∫ 1 c t s − 1 exp ( − t ) d t < n − s n ! .
Using the same inequality exp ( − t ) < n ! t n \exp(-t) < \frac{n!}{t^n} exp ( − t ) < t n n ! , we substitute it into the integral:
∫ 1 c t s − 1 exp ( − t ) d t < ∫ 1 c t s − 1 n ! t n d t = n ! ∫ 1 c t s − n − 1 d t . \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. ∫ 1 c t s − 1 exp ( − t ) d t < ∫ 1 c t s − 1 t n n ! d t = n ! ∫ 1 c t s − n − 1 d t .
Next, we evaluate the integral:
n ! ∫ 1 c t s − n − 1 d t = n ! [ t s − n s − n ] 1 c = n ! n − s ( 1 − 1 c n − 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). n ! ∫ 1 c t s − n − 1 d t = n ! [ s − n t s − n ] 1 c = n − s n ! ( 1 − c n − s 1 ) .
Since c > 1 c > 1 c > 1 , the term 1 c n − s \frac{1}{c^{n-s}} c n − s 1 is less than 1 1 1 , which means:
1 − 1 c n − s < 1. 1 - \frac{1}{c^{n-s}} < 1. 1 − c n − s 1 < 1.
Thus:
∫ 1 c t s − 1 exp ( − t ) d t < n ! n − s . \int_1^c t^{s-1} \exp(-t) \,\mathrm{d}t < \frac{n!}{n-s}. ∫ 1 c t s − 1 exp ( − t ) d t < n − s n ! .
(3)
Given:
d 2 f ( s ) d s 2 = ∫ 0 ∞ g ( t , s ) exp ( − t ) d t , \frac{\mathrm{d}^2 f(s)}{\mathrm{d}s^2} = \int_0^\infty g(t, s) \exp(-t) \,\mathrm{d}t, d s 2 d 2 f ( s ) = ∫ 0 ∞ g ( t , s ) exp ( − t ) d t ,
We first need to compute the second derivative of f ( s ) f(s) f ( s ) :
f ( s ) = ∫ 0 ∞ t s − 1 exp ( − t ) d t . f(s) = \int_0^\infty t^{s-1} \exp(-t) \,\mathrm{d}t. f ( s ) = ∫ 0 ∞ t s − 1 exp ( − t ) d t .
First derivative:
d f ( s ) d s = ∫ 0 ∞ ∂ ∂ s ( t s − 1 ) exp ( − t ) d t = ∫ 0 ∞ t s − 1 log ( t ) exp ( − t ) d t . \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. d s d f ( s ) = ∫ 0 ∞ ∂ s ∂ ( t s − 1 ) exp ( − t ) d t = ∫ 0 ∞ t s − 1 log ( t ) exp ( − t ) d t .
Second derivative:
d 2 f ( s ) d s 2 = ∫ 0 ∞ ∂ ∂ s ( t s − 1 log ( t ) ) exp ( − t ) d t = ∫ 0 ∞ t s − 1 log 2 ( t ) exp ( − t ) d t . \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. d s 2 d 2 f ( s ) = ∫ 0 ∞ ∂ s ∂ ( t s − 1 log ( t ) ) exp ( − t ) d t = ∫ 0 ∞ t s − 1 log 2 ( t ) exp ( − t ) d t .
Thus, g ( t , s ) = t s − 1 log 2 ( t ) g(t, s) = t^{s-1} \log^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 ) 2 exp ( − t ) d t − ( ∫ 0 ∞ ( log t ) exp ( − t ) d t ) 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. D = ∫ 0 ∞ ( log t ) 2 exp ( − t ) d t − ( ∫ 0 ∞ ( log t ) exp ( − t ) d t ) 2 .
This problem requires us to calculate two integrals: one involving ( log t ) 2 (\log t)^2 ( log t ) 2 and another involving log t \log t log t . We are also given the hint that the following relation holds:
d 2 log f ( s ) d s 2 ∣ s = 1 = π 2 6 . \frac{\mathrm{d}^2 \log f(s)}{\mathrm{d}s^2}\bigg|_{s=1} = \frac{\pi^2}{6}. d s 2 d 2 log f ( s ) s = 1 = 6 π 2 .
Step 1: Expressing the Second-Order Derivative of f ( s ) f(s) f ( s )
From Question 3 , we know that:
d 2 f ( s ) d s 2 = ∫ 0 ∞ t s − 1 log 2 ( t ) exp ( − t ) d t . \frac{\mathrm{d}^2 f(s)}{\mathrm{d}s^2} = \int_0^\infty t^{s-1} \log^2(t) \exp(-t) \,\mathrm{d}t. d s 2 d 2 f ( s ) = ∫ 0 ∞ t s − 1 log 2 ( t ) exp ( − t ) d t .
Setting s = 1 s = 1 s = 1 :
d 2 f ( 1 ) d s 2 = ∫ 0 ∞ t 1 − 1 log 2 ( t ) exp ( − t ) d t = ∫ 0 ∞ log 2 ( t ) exp ( − t ) d t . \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. d s 2 d 2 f ( 1 ) = ∫ 0 ∞ t 1 − 1 log 2 ( t ) exp ( − t ) d t = ∫ 0 ∞ log 2 ( t ) exp ( − t ) d t .
This integral represents the first term in D D D , which is:
∫ 0 ∞ ( log t ) 2 exp ( − t ) d t . \int_0^\infty (\log t)^2 \exp(-t) \,\mathrm{d}t. ∫ 0 ∞ ( log t ) 2 exp ( − t ) d t .
Thus, we have:
∫ 0 ∞ ( log t ) 2 exp ( − t ) d t = d 2 f ( 1 ) d s 2 . \int_0^\infty (\log t)^2 \exp(-t) \,\mathrm{d}t = \frac{\mathrm{d}^2 f(1)}{\mathrm{d}s^2}. ∫ 0 ∞ ( log t ) 2 exp ( − t ) d t = d s 2 d 2 f ( 1 ) .
Step 2: Calculating the First Integral
The value of the second derivative of the logarithm of f ( s ) f(s) f ( s ) at s = 1 s = 1 s = 1 is given as:
d 2 log f ( s ) d s 2 ∣ s = 1 = π 2 6 . \frac{\mathrm{d}^2 \log f(s)}{\mathrm{d}s^2}\bigg|_{s=1} = \frac{\pi^2}{6}. d s 2 d 2 log f ( s ) s = 1 = 6 π 2 .
We know that:
d 2 log f ( s ) d s 2 = 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}. d s 2 d 2 log f ( s ) = ( f ( s ) ) 2 f ′′ ( s ) f ( s ) − ( f ′ ( s ) ) 2 .
At s = 1 s = 1 s = 1 , f ( 1 ) = 1 f(1) = 1 f ( 1 ) = 1 , f ′ ( 1 ) f'(1) f ′ ( 1 ) is the first moment (which is ∫ 0 ∞ log t exp ( − t ) d t \int_0^\infty \log t \exp(-t) \,\mathrm{d}t ∫ 0 ∞ log t exp ( − t ) d t ), and f ′ ′ ( 1 ) f''(1) f ′′ ( 1 ) is the second moment (which is ∫ 0 ∞ log 2 t exp ( − t ) d t \int_0^\infty \log^2 t \exp(-t) \,\mathrm{d}t ∫ 0 ∞ log 2 t exp ( − t ) d t ).
We can express:
d 2 log f ( 1 ) d s 2 = f ′ ′ ( 1 ) − ( f ′ ( 1 ) ) 2 . \frac{\mathrm{d}^2 \log f(1)}{\mathrm{d}s^2} = f''(1) - \left(f'(1)\right)^2. d s 2 d 2 log f ( 1 ) = f ′′ ( 1 ) − ( f ′ ( 1 ) ) 2 .
Given:
d 2 log f ( s ) d s 2 ∣ s = 1 = π 2 6 , \frac{\mathrm{d}^2 \log f(s)}{\mathrm{d}s^2}\bigg|_{s=1} = \frac{\pi^2}{6}, d s 2 d 2 log f ( s ) s = 1 = 6 π 2 ,
Thus:
D = π 2 6 . D = \frac{\pi^2}{6}. D = 6 π 2 .
(5)
We are asked to find the value of S S S , defined as:
S = ∫ 0 ∞ ( log r ) 2 p ( r ) d r − ( ∫ 0 ∞ ( log r ) p ( r ) d r ) 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, S = ∫ 0 ∞ ( log r ) 2 p ( r ) d r − ( ∫ 0 ∞ ( log r ) p ( r ) d r ) 2 ,
where the function p ( r ) p(r) p ( r ) is given by:
p ( r ) = r α exp ( − r 2 2 α ) . p(r) = \frac{r}{\alpha} \exp\left(-\frac{r^2}{2\alpha}\right). p ( r ) = α r exp ( − 2 α r 2 ) .
The function p ( r ) p(r) p ( r ) is a probability density function corresponding to a Rayleigh distribution, with the parameter α \alpha α . The Rayleigh distribution has the form:
p ( r ) = r α exp ( − r 2 2 α ) , p(r) = \frac{r}{\alpha} \exp\left(-\frac{r^2}{2\alpha}\right), p ( r ) = α r exp ( − 2 α r 2 ) ,
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 [ log r ] \mathbb{E}[\log r] E [ log r ]
We need to compute the expected value of log r \log r log r under this distribution, given by:
E [ log r ] = ∫ 0 ∞ ( log r ) p ( r ) d r = ∫ 0 ∞ log r ⋅ r α exp ( − r 2 2 α ) d r . \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. E [ log r ] = ∫ 0 ∞ ( log r ) p ( r ) d r = ∫ 0 ∞ log r ⋅ α r exp ( − 2 α r 2 ) d r .
We perform a substitution to simplify this integral:
Let u = r 2 2 α u = \frac{r^2}{2\alpha} u = 2 α r 2 , hence d u = r d r α \mathrm{d}u = \frac{r \,\mathrm{d}r}{\alpha} d u = α r d r .
The integral becomes:
E [ log r ] = ∫ 0 ∞ log ( 2 α u ) exp ( − u ) d u . \mathbb{E}[\log r] = \int_0^\infty \log \left(\sqrt{2\alpha u}\right) \exp(-u) \,\mathrm{d}u. E [ log r ] = ∫ 0 ∞ log ( 2 αu ) exp ( − u ) d u .
This simplifies to:
E [ log r ] = 1 2 log ( 2 α ) ∫ 0 ∞ exp ( − u ) d u + 1 2 ∫ 0 ∞ log u exp ( − u ) d u . \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. E [ log r ] = 2 1 log ( 2 α ) ∫ 0 ∞ exp ( − u ) d u + 2 1 ∫ 0 ∞ log u exp ( − u ) 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 u exp ( − u ) d u = − γ , \int_0^\infty \log u \exp(-u) \,\mathrm{d}u = -\gamma, ∫ 0 ∞ log u exp ( − u ) d u = − γ ,
where γ \gamma γ is the Euler-Mascheroni constant. Thus,
E [ log r ] = 1 2 log ( 2 α ) − γ 2 . \mathbb{E}[\log r] = \frac{1}{2}\log(2\alpha) - \frac{\gamma}{2}. E [ log r ] = 2 1 log ( 2 α ) − 2 γ .
Step 3: Calculation of the second moment E [ ( log r ) 2 ] \mathbb{E}[(\log r)^2] E [( log r ) 2 ]
Next, we need to compute the second moment:
E [ ( log r ) 2 ] = ∫ 0 ∞ ( log r ) 2 p ( r ) d r = ∫ 0 ∞ ( log r ) 2 r α exp ( − r 2 2 α ) d r . \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. E [( log r ) 2 ] = ∫ 0 ∞ ( log r ) 2 p ( r ) d r = ∫ 0 ∞ ( log r ) 2 α r exp ( − 2 α r 2 ) d r .
Using the same substitution u = r 2 2 α u = \frac{r^2}{2\alpha} u = 2 α r 2 :
E [ ( log r ) 2 ] = ∫ 0 ∞ [ log ( 2 α u ) ] 2 exp ( − u ) d u . \mathbb{E}[(\log r)^2] = \int_0^\infty \left[\log\left(\sqrt{2\alpha u}\right)\right]^2 \exp(-u) \,\mathrm{d}u. E [( log r ) 2 ] = ∫ 0 ∞ [ log ( 2 αu ) ] 2 exp ( − u ) d u .
This expands to:
E [ ( log r ) 2 ] = 1 4 [ log ( 2 α ) ] 2 + 1 2 log ( 2 α ) ∫ 0 ∞ log u exp ( − u ) d u + 1 4 ∫ 0 ∞ ( log u ) 2 exp ( − u ) d u . \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. E [( log r ) 2 ] = 4 1 [ log ( 2 α ) ] 2 + 2 1 log ( 2 α ) ∫ 0 ∞ log u exp ( − u ) d u + 4 1 ∫ 0 ∞ ( log u ) 2 exp ( − u ) d u .
Using the known results:
∫ 0 ∞ log u exp ( − u ) d u = − γ , \int_0^\infty \log u \exp(-u) \,\mathrm{d}u = -\gamma, ∫ 0 ∞ log u exp ( − u ) d u = − γ ,
and
∫ 0 ∞ ( log u ) 2 exp ( − u ) d u = γ 2 + π 2 6 , \int_0^\infty (\log u)^2 \exp(-u) \,\mathrm{d}u = \gamma^2 + \frac{\pi^2}{6}, ∫ 0 ∞ ( log u ) 2 exp ( − u ) d u = γ 2 + 6 π 2 ,
we have:
E [ ( log r ) 2 ] = 1 4 [ log ( 2 α ) ] 2 − γ 2 log ( 2 α ) + 1 4 ( γ 2 + π 2 6 ) . \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). E [( log r ) 2 ] = 4 1 [ log ( 2 α ) ] 2 − 2 γ log ( 2 α ) + 4 1 ( γ 2 + 6 π 2 ) .
Step 4: Calculate S S S
Finally, S S S 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. S = E [( log r ) 2 ] − ( E [ log r ] ) 2 .
Substitute the values:
E [ log r ] = 1 2 log ( 2 α ) − γ 2 , \mathbb{E}[\log r] = \frac{1}{2}\log(2\alpha) - \frac{\gamma}{2}, E [ log r ] = 2 1 log ( 2 α ) − 2 γ ,
so:
( E [ log r ] ) 2 = 1 4 [ log ( 2 α ) ] 2 − γ log ( 2 α ) + γ 2 4 . \left(\mathbb{E}[\log r]\right)^2 = \frac{1}{4} \left[\log(2\alpha)\right]^2 - \gamma \log(2\alpha) + \frac{\gamma^2}{4}. ( E [ log r ] ) 2 = 4 1 [ log ( 2 α ) ] 2 − γ log ( 2 α ) + 4 γ 2 .
Subtracting:
S = 1 4 [ log ( 2 α ) ] 2 − γ log ( 2 α ) + 1 4 ( γ 2 + π 2 6 ) − ( 1 4 [ log ( 2 α ) ] 2 − γ log ( 2 α ) + γ 2 4 ) . 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). S = 4 1 [ log ( 2 α ) ] 2 − γ log ( 2 α ) + 4 1 ( γ 2 + 6 π 2 ) − ( 4 1 [ log ( 2 α ) ] 2 − γ log ( 2 α ) + 4 γ 2 ) .
Simplifying:
S = π 2 24 . S = \frac{\pi^2}{24}. S = 24 π 2 .
This is the final value of S S S .
Knowledge
Gamma函数 不定积分 定积分 方差
解题技巧和信息
Gamma Function : Recognize that f ( s ) f(s) f ( s ) represents the Gamma function Γ ( s ) \Gamma(s) Γ ( s ) .
Inequality Manipulation : Use known inequalities such as exp ( t ) > t n n ! \exp(t) > \frac{t^n}{n!} exp ( t ) > n ! t n to estimate integrals.
Variance Calculation : The variance of logarithms of exponential and Rayleigh distributed variables often results in expressions involving π 2 6 \frac{\pi^2}{6} 6 π 2 .
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