Suppose $\mathbb{H}$ is a Hilbert space over the reals. Fix two vectors $\alpha$ and $\beta$ in $\mathbb{H}$. I came across a problem that reduces to the following: What are the possible units vector $h$ such that $\langle \alpha , h \rangle \langle \beta,h \rangle= \langle \alpha, \beta \rangle$ ? I could get the set of possible $h$ in the case that $\alpha=\beta$ and in the case that $\alpha$ and $\beta$ are orthogonal. Any idea with the more general formulation ?
Solving an equation in a Hilbert space
89 Views Asked by Bumbble Comm https://math.techqa.club/user/bumbble-comm/detail AtThere are 2 best solutions below
On
To start, let's just acknowledge a special case: if $\alpha \perp \beta$, then the equation becomes $\langle \alpha, h \rangle \langle \beta, h \rangle = 0$. The set of unit vectors $h$ that satisfy this are the perpendicular vectors to at least one of $\alpha$ or $\beta$. So, we will assume $\alpha \not\perp \beta$. Note that this implies $\alpha \neq 0$ and $\beta \neq 0$, and that $\Bbb{H}$ is non-trivial.
Consider also the case where $\Bbb{H}$ is one-dimensional. It's not difficult to see that both unit vectors will work in this case, as $\alpha = ah$ and $\beta = bh$ for some $a, b \in \Bbb{R}$. So, let us assume the space has at least two dimensions.
The equation is equivalent to \begin{align*} \langle \alpha - \langle \alpha, h \rangle h, \beta \rangle = 0 &\iff \alpha - \langle \alpha, h \rangle h \perp \beta \\ &\iff P_{\{h\}^\perp}(\alpha) \perp \beta. \end{align*}
Note that, for any unit vector $h$, $\{h\}^\perp$ is a hyperplane through the origin, and every hyperplane corresponds to precisely two normal unit vectors $\pm h$. Also note that $\langle \alpha, h \rangle \langle \beta, h \rangle = \langle \alpha, \beta \rangle$ if and only if $\langle \alpha, -h \rangle \langle \beta, -h \rangle = \langle \alpha, \beta \rangle$. So, we can solve our problem by looking for hyperplanes $H$ through the origin in $\Bbb{H}$ where $P_H(\alpha) \perp \beta$, and find our solutions $h$ by taking the positive and negative unit normals of our solutions $H$.
Further, we can find all such hyperplanes by finding all the possible projections one can make of $\alpha$ onto a hyperplane. If $p$ is the projection of $\alpha$ onto hyperplane $H$ (through the origin) then we note that, if $p = \alpha$, then our condition $p \perp \beta$ would simplify to $\alpha \perp \beta$, which we assume not to be the case.
Thus, under our assumptions, $p \neq \alpha$, hence $p - \alpha$ is a normal direction to $H$. We obtain precisely two solutions to our original equation from $p$: $$h = \pm \frac{p - \alpha}{\|p - \alpha\|}.$$
Thus, we are interested in finding the complete set of possible projections of $\alpha$ onto a hyperplane through the origin. Let this set be $\mathcal{P}$. Using the above equation, the solution set to the original equation is parameterised by $\mathcal{P} \cap \{\beta\}^\perp$.
Let $\mathcal{P}'$ be the set of projections of $\alpha$ onto a line through the origin. I claim that $\mathcal{P} = \mathcal{P}'$.
Note that $0 \in \mathcal{P}$, as $\{\alpha\}^\perp$ is a hyperplane (recall $\alpha \neq 0$) onto which $\alpha$ projects to $0$. Any line in $\{\alpha\}^\perp$ (and one will exist, as $\Bbb{H}$ has dimension at least $2$) will also project $\alpha$ onto $0$, hence $0 \in \mathcal{P}'$.
If $x \in \mathcal{P} \setminus \{0\}$, then $L = \operatorname{span}\{x\}$ is a line onto which $\alpha$ projects onto $x$, hence $x \in \mathcal{P}'$. Conversely, if $x \in \mathcal{P}' \setminus \{0\}$, then $\{\alpha - x\}^\perp$ is a hyperplane onto which $\alpha$ projects onto $x$, so $x \in \mathcal{P}$. Thus, $\mathcal{P} = \mathcal{P}'$ as claimed. That is, $\mathcal{P}$ is the set of projections both onto hyperplanes, and onto lines, through the origin.
Let $$C := S_{\Bbb{H}}\left[\frac{\alpha}{2}; \frac{\|\alpha\|}{2}\right] = \left\{x \in \Bbb{H} : \left\|x - \frac{\alpha}{2}\right\| = \frac{\|\alpha\|}{2}\right\}.$$ I claim that $C = \mathcal{P}$. Note that: \begin{align*} \left\|x - \frac{\alpha}{2}\right\| = \frac{\|\alpha\|}{2} &\iff \left\|x - \frac{\alpha}{2}\right\|^2 = \frac{\|\alpha\|^2}{4} \\ &\iff \|x\|^2 - \langle x, \alpha \rangle + \frac{\|\alpha\|^2}{4} = \frac{\|\alpha\|^2}{4} \\ &\iff \|x\|^2 = \langle x, \alpha \rangle. \end{align*}
Suppose that $x \in C$. We know that $0 \in \mathcal{P}$ and $0 \in C$, so assume $x \neq 0$. Let $L = \operatorname{span} \{x\}$. Then, $$P_L(\alpha) = \frac{\langle \alpha, x \rangle}{\|x\|^2} x = x.$$ That is, $x \in \mathcal{P}' = \mathcal{P}$.
Conversely, suppose $x$ is the projection of $\alpha$ onto a line $L$ through the origin. Either $x = 0$, which lies in $C$, or $x \neq 0$. If $x \neq 0$, then $L = \operatorname{span}\{x\}$. In this case, we have $$x = P_L(\alpha) = \frac{\langle \alpha, x \rangle}{\|x\|^2} x,$$ and since $x \neq 0$, this implies $$\frac{\langle \alpha, x \rangle}{\|x\|^2} = 1 \implies x \in C.$$ Thus $\mathcal{P} = C$, as claimed. This gives us our family of solutions: $$h = \pm\frac{p - \alpha}{\|p - \alpha\|}, \qquad \text{where } p \in S_{\Bbb{H}}\left[\frac{\alpha}{2}; \frac{\|\alpha\|}{2}\right] \cap \{\beta\}^\perp,$$ where $\alpha \not\perp \beta$, and $$h \in (\{\alpha\}^\perp \cup \{\beta\}^\perp) \cap S_{\Bbb{H}}[0; 1]$$ when $\alpha \perp \beta$.
Some notes about this answer
I have checked this answer a few times, and it seems to be correct. However, I find it interesting that the solution is not obviously symmetric in $\alpha$ and $\beta$, even though the original equation clearly is. This gives me some pause; maybe the solution has some kind of error or hidden assumption that I'm missing?
I did some investigation in two dimensions, using Desmos, and it seems to validate the solution. I saw that the solution set is the same if you exchange $\alpha$ and $\beta$, and I visually saw the importance separating out the $\alpha \perp \beta$ case.
Unfortunately, two dimensions is not really sufficient to visualise the problem; I really need three dimensions for the picture to be truly convincing (the sphere intersected with a hyperplane is just two points in $\Bbb{R}^2$, and I would need to see a full circle at least). That said, I do stand by my solution, since the proof seems to be correct. It just would be nice to see an independent proof that this solution set is indeed symmetric.
WLOG we may assume that $\|\alpha\|=\|\beta\|=1$ and $\langle \alpha,\beta\rangle\ge 0.$ Then $\langle \alpha,\beta\rangle=\cos\theta$ for some $0\le \theta\le {\pi\over 2}.$ Let $V={\rm span}(\alpha,\beta).$ Any $h\in\mathcal{H}$ can be decomposed as $h=v+w,$ where $v\in V$ and $w\perp V.$ It suffices to find all possible $h\in V$ satisfying the condition. Then the general solution can be obtained by adding arbitrary elements in $V^\perp.$ We will skip the easy case when $\alpha=\beta.$ Otherwise the space $V$ is two dimensional if $\alpha\neq \beta.$ Let $h=x\alpha+y\beta.$ The condition is equivalent to $$(x+y\cos\theta ) (y+x\cos\theta )=\cos\theta$$ or equivalently to $$ xy(1+\cos^2\theta)=(1-x^2-y^2)\cos\theta$$ Thus we obtain a quadratic equation in two variables. For $\cos\theta =0$ we get $xy=0.$