Introductory university-level calculus, linear algebra, abstract algebra, probability, statistics, and stochastic processes.
Vector space of functions
Get link
Facebook
X
Pinterest
Email
Other Apps
-
We study the collection of functions \(\mathcal{R}_{2\pi}^2\) (square-integrable functions with period \(2\pi\)) as a vector space. We define the \(L^2\) norm and \(L^2\) inner product on this vector space so that we can investigate the ``geometric'' structure of the space of functions.
Let us show that \(\mathcal{R}_{2\pi}^{2}\), the set of square-integrable functions with period \(2\pi\), is a vector space over \(\mathbb{C}\). First, we need to define addition and scalar multiplication. Let \(f, g\in \mathcal{R}_{2\pi}^2\). We define \(f + g \in \mathcal{R}_{2\pi}^2\) by
\[(f+g)(x) = f(x) + g(x), ~ x \in \mathbb{R}.\tag{eq:add}\]
Note that the ``\(+\)'' on the left-hand side is defined between the two functions \(f\) and \(g\), whereas the ``\(+\)'' on the right-hand side is the addition between two complex numbers \(f(x)\) and \(g(x)\). Next, we define scalar multiplication. Let \(\alpha\in \mathbb{C}\) and \(f \in \mathcal{R}_{2\pi}^2\). We define \(\alpha f\) by
\[(\alpha f)(x) = \alpha f(x).\tag{eq:scale}\]
Note that the product on the left-hand side is between the scalar \(\alpha\) and the function \(f\), whereas the product on the right-hand side is between the two complex numbers \(\alpha\) and \(f(x)\).
Lemma
\(\mathcal{R}_{2\pi}^2\) is a vector space with vector addition (eq:add) and scalar multiplication (eq:scale).
Proof. We show that \(\mathcal{R}_{2\pi}^2\) satisfies all the axioms of the vector space. In the following, \(f, g, h\in\mathcal{R}_{2\pi}^2\) and \(\alpha, \beta \in \mathbb{C}\).
1. \(\mathcal{R}_{2\pi}^2\) is closed under vector addition.
Suppose \(f, g \in \mathcal{R}_{2\pi}^2\). We show \(f + g\in\mathcal{R}_{2\pi}^2\).
By assumption, \(\int_{\pi}^{\pi}|f(x)|^2\,dx < +\infty\) and \(\int_{-\pi}^{\pi}|g(x)|^2\,dx < +\infty\). Thus,
Thus, \(\mathcal{R}_{2\pi}^{2}\) is a vector space over \(\mathbb{C}\). ■
Definition (\(L^2\)-norm, mean-square norm)
Let \(f\) be a function on \((-\pi, \pi)\) that is square-integrable, i.e.,
\[\int_{-\pi}^{\pi}|f(x)|^2dx < +\infty.\]
We define the mean-square norm or \(L^2\) norm \(\|f\|\) by
\[\|f\| = \sqrt{\int_{-\pi}^{\pi}|f(x)|^2dx}.\]
Remark. The \(L\) in \(L^2\) stands for ``Lebesgue.'' suggesting that we should use the Lebesgue integral rather than the Riemann integral. But the term ``\(L^2\)'' is so widespread that we use it, although we only use the Riemann integral. □
Remark. The \(L^2\) inner product corresponds to the scalar (dot) product in a vector space. □
In general, an inner product is defined as follows.
Definition (Inner product (general))
Let \(V\) be a vector space over the field \(K\). An inner product \((\cdot, \cdot): V\times V \to K\) is a map with the following properties for all vectors \(x,y,z\in V\) and all scalars \(\alpha, \beta \in K\):
(Linearity in the first argument) \[(\alpha x + \beta y, z) = \alpha(x,z) + \beta(y,z)\]
(Positive definiteness) If \(x \neq 0\), \[(x,x) > 0.\]
Example. Consider the vector space \(\mathbb{R}^n\). For \(x = (x_1, x_2, \cdots, x_n), y = (y_1, y_2, \cdots, y_n) \in \mathbb{R}^n\), the scalar product is defined as
\[(x,y) = \sum_{i=1}^{n}x_iy_i.\]
For each \(a \in \mathbb{R}\), its ``conjugate'' is the same \(a\): \(\overline{a} = a\). Thus,
Defining the birth process Consider a colony of bacteria that never dies. We study the following process known as the birth process , also known as the Yule process . The colony starts with \(n_0\) cells at time \(t = 0\). Assume that the probability that any individual cell divides in the time interval \((t, t + \delta t)\) is proportional to \(\delta t\) for small \(\delta t\). Further assume that each cell division is independent of others. Let \(\lambda\) be the birth rate. The probability of a cell division for a population of \(n\) cells during \(\delta t\) is \(\lambda n \delta t\). We assume that the probability that two or more births take place in the time interval \(\delta t\) is \(o(\delta t)\). That is, it can be ignored. Consequently, the probability that no cell divides during \(\delta t\) is \(1 - \lambda n \delta t - o(\delta t)\). Note that this process is an example of the Markov chain with states \({n_0}, {n_0 + 1}, {n_0 + 2}...
Joseph Fourier introduced the Fourier series to solve the heat equation in the 1810s. In this post, we show how the Fourier transform arises naturally in a simplified version of the heat equation. Suppose we have the unit circle \(S\) made of a metal wire. Pick an arbitrary point \(A\) on the circle. Any point \(P\) on the circle is identified by the distance \(x\) from \(A\) to \(P\) along the circle in the counter-clockwise direction (i.e., \(x\) is the angle of the section between \(A\) and \(P\) in radian). Let \(u(t,x)\) represent the temperature at position \(x\) and time \(t\). The temperature distribution at \(t = 0\) is given by \(u(0, x) = f(x)\). Assuming no radiation of heat out of the metal wire, \(u(t,x)\) for \(t > 0\) and \(0\leq x \leq 2\pi\) is determined by the following partial differential equation (PDE) called the heat equation : \[\gamma\frac{\partial u}{\partial t} = \kappa\frac{\partial^2 u}{\partial x^2}\] and the initial condition \[u(0,x) = f(x...
Given a sequence \(\{a_n\}\), the expression \[\sum_{n=0}^{\infty}a_n = a_0 + a_1 + a_2 + \cdots\] is called a series (or infinite series ). This expression may or may not have value. At this point, it is purely formal. Note that the order of addition matters : We first add \(a_0\) and \(a_1\), to the result of which we add \(a_2\), to the result of which we add \(a_3\), and so on (Not something like we first add \(a_{101}\) and \(a_{58}\), then add \(a_{333051}\), and so on). We will see, however, that for a special class of series (the positive term series), the order of addition does not matter if the series converges. Example . The sum of a geometric progression \(\{ar^n\}\), that is, \(\sum_{n=0}^{\infty}ar^n\) is called a geometric series . It is understood that \(r^0 = 1\) including the case when \(r = 0\). □ Given a series \(\sum_{n=0}^{\infty}a_n\) and a number \(n\geq 0\), the sum \[\sum_{k=0}^{n}a_k = a_0 + a_1 + \cdots + a_n\] is called the \(n\)-th partial sum . We m...
Comments
Post a Comment