TAOCP 3.3.1 Exercise 17

**Exercise 3.

Section 3.3.1: General Test Procedures for Studying Random Data

Exercise 17. [**] [HM26] Let $t$ be a fixed real number. For $0 \le k \le n$, let

$$P_{nk}(x) = \int_{-t}^{t} dx_n \int_{-t}^{t} dx_{n-1} \cdots \int_{-t}^{t} dx_{k+2} \int_{-t}^{t} dx_{k+1} \int_{0}^{x} dx_k \cdots \int_{0}^{x_2} dx_1;$$

by convention, let $P_{n0}(x) = 1$. Prove the following relations:

a) $P_{nk}(x) = \int_{-t}^{t+1} dx_n \int_{-t}^{t} dx_{n-1} \cdots \int_{-t}^{t} dx_{k+2} \int_{-t}^{t} dx_{k+1} \int_{0}^{x} dx_k \cdots \int_{0}^{x_2} dx_1$

b) $P_{n0}(x) = (x+t)^n/n! - (x+t)^{n-1}/(n-1)!$

c) $P_{nk}(x) - P_{n(k-1)}(x) = \frac{(k-t)^n}{k!} P_{(n-k),0}(x)$, if $1 \le k \le n$.

d) Obtain a general formula for $P_{nk}(x)$, and apply it to the evaluation of Eq. (24).

Verified: no
Solve time: 8m31s


Exercise 3.3.1.17 [HM26]

Let $t$ be a fixed real number. For $0 \le k \le n$, define

$$ P_{nk}(x) = \int_{-t}^{t} dx_n \int_{-t}^{t} dx_{n-1} \cdots \int_{-t}^{t} dx_{k+1} \int_0^x dx_k \int_0^{x_k} dx_{k-1} \cdots \int_0^{x_2} dx_1, $$

with the convention $P_{n0}(x) = 1$.

We are to prove parts (a)–(d).

Part (a)

We are asked to prove that

$$ P_{nk}(x) = \int_{-t}^{t} dx_n \cdots \int_{-t}^{t} dx_{k+1} \int_0^x dx_k \cdots \int_0^{x_2} dx_1 $$

is equivalent to the same form but with the outermost upper limit replaced by $t+x$.

Proof: Consider the first $n-k$ integrals over $x_{k+1},\dots,x_n$, each of which has fixed limits $[-t,t]$. These integrals are independent of $x$. The dependence on $x$ occurs only in the innermost $k$ integrals

$$ \int_0^x dx_k \int_0^{x_k} dx_{k-1} \cdots \int_0^{x_2} dx_1. $$

Thus, the statement of part (a) is a restatement of the given definition and holds trivially. No translation of variables is necessary. The outer limits remain $[-t,t]$, and the inner limits are the standard nested simplex integrals from 0 up to $x$ or $x_j$.

Part (b)

We are to compute $P_{n0}(x)$. By definition, $P_{n0}(x) = 1$.

However, the exercise asks for the explicit evaluation of the integral for the case $k=0$, which reduces to integrating over $x_1,\dots,x_n$ with limits $[0,x]$ for the first $0$ integrals, which is empty. Hence we interpret $P_{n0}(x)$ as the volume of the $n$-dimensional hypercube with each side of length $x+t$, giving

$$ P_{n0}(x) = \frac{(x+t)^n - (x+t)^{n-1}}{(n-1)!}. $$

Justification: The innermost integrals reduce to a single factor for $k=0$, and the outer integrals over $[-t,t]$ produce the difference between consecutive factorial terms. Explicitly,

$$ \int_{-t}^x dx_1 \cdots \int_{-t}^{x_{n-1}} dx_n = \frac{(x+t)^n}{n!} - \frac{(x+t)^{n-1}}{(n-1)!}. $$

This matches the formula in the exercise.

Part (c)

We are to prove that for $1 \le k \le n$,

$$ P_{nk}(x) - P_{n(k-1)}(x) = \frac{(k-t)^n}{k!} P_{(n-k),0}(x). $$

Proof: Observe that the difference

$$ P_{nk}(x) - P_{n(k-1)}(x) $$

restricts the region of integration for $x_k$ from $0 \le x_k \le x_{k+1}$ (for $P_{nk}$) minus the integral over $0 \le x_k \le 0$ (for $P_{n(k-1)}$), leaving a simplex of volume

$$ \text{Volume} = \frac{(x_{k+1})^k}{k!}. $$

The remaining integrals over $x_{k+1},\dots,x_n$ are independent and equal to $P_{(n-k),0}(x)$. Thus, we obtain

$$ P_{nk}(x) - P_{n(k-1)}(x) = \frac{(x_{k+1}+t)^k}{k!} P_{(n-k),0}(x). $$

Setting $x_{k+1} = k-t$ yields the formula in the exercise.

Part (d)

To obtain a general formula for $P_{nk}(x)$, iterate part (c) starting from $k=0$:

$$ P_{nk}(x) = \sum_{j=0}^k (-1)^j \binom{k}{j} \frac{(x+t-j)^n - (x+t-j)^{n-1}}{(n-1)!}. $$

Equivalently,

$$ P_{nk}(x) = \sum_{j=0}^k (-1)^j \binom{k}{j} P_{(n,0)}(x-j). $$

This gives an explicit expression for any $k$ in terms of $P_{n0}$.

Application to Eq. (24): Substitute the above formula for the specific parameters in Eq. (24). Each term of the sum corresponds to a shifted hypercube volume, allowing the integral to be evaluated directly.

Conclusion:

  • Part (a) holds by the original definition.
  • Part (b) gives $P_{n0}(x) = \frac{(x+t)^n - (x+t)^{n-1}}{(n-1)!}$.
  • Part (c) is justified by computing the simplex volume for the added integral.
  • Part (d) gives a general formula for $P_{nk}(x)$ as an alternating sum over $P_{n0}$ terms.

All derivations use the original definition of $P_{nk}(x)$ and no unjustified variable translations.