Let $A$ be a tall matrix that is not rank-deficient and has normalized columns. That is $A$ is $m\times n$, $m<n$ and rank$(A)=m$, and $||a_i||_2=1$ for all columns $a_i$.
Define $$\delta_v(A):=\max_i \ \frac{|\langle a_i,v\rangle|^2}{||v||_2^2}.$$
Let $$\delta(A):=\inf_v\ \ \delta_v(A).$$
This is called the "decay factor" in some places. Is there a natural way to compute this? For an orthogonal matrix it is clear that $\delta$ is $1/n$. I tried to incorporate SVD and relate $\delta$ to the minimum singular value, but didn't get anywhere.
Alternatively, the problem may be stated as finding the infimum of $\frac{||A^tv||_\infty^2}{||v||_2^2}$, which is related to the problem of finding the smallest eigenvalue of $AA^t$. So might there be a way to find $\delta$ by studying $AA^t$?
EDIT: In plain English, the question is: given a set of $n>m$ unit vectors that span $\mathbb{R}^m$, how can one find the vector $v$ having the property that the angle between it and the "closest" unit vector (closest in angle) is as large as possible. Essentially, how can one find the vector farthest away from all of the other vectors.
The Question: $$\inf_{ ||v||_2 = 1}||v^\top A||_{\infty}$$
The solution to this has a similar flavor as the simplex algorithm. The simplex algorithm deals with a convex region in n-dimensional space defined by the hyperplanes given from the inequalities of the original problem. This question deals with the infimum of the infinity norm. Just as the best solution to the simplex is one of the vertices of the convex region (called the simplex), the solution here is a vertex of a hyper-cube. The difference here is that the hypercube varies, depending on the vector for which the infinity norm the box represents.
Insert here image of vector in 2-d with box around it representing the max value of the vector's elements, with the box having smallest size when the vector rotates so that the box's corner and the vector meet.
My Answer:
Overview: To get within 90 degrees in every dimension of the desired vertex, start with the vector found through use of the SVD. The minimum singular value's vector is that vector. From there "follow" the surfaces and edges of the bounding box (hyper-cube) until the vertex is reached. The end result is a row $r$ with the following properties: $r$ has $m$ distinct elements of equal magnitude each with a value of $||r||_{\infty}$. That is, those $m$ values are the maximal value in $r$.
Box Rotation To obtain a row with values equal in desired indices, use the basic operation I call a box rotation.
$$\pmatrix{\gamma & \sigma \\ -\sigma & \gamma}\pmatrix{a & b \\ c & d} = \pmatrix{\star & \star \\ z_0 & z_0 \\} \tag{1}$$ $$\pmatrix{\gamma & \sigma \\ -\sigma & \gamma}\pmatrix{a & b \\ c & d} = \pmatrix{\star & \star \\ z_0 & -z_0 \\} \tag{2}$$ (1) requires solving $$-\sigma a + \gamma c= -\sigma b + \gamma d = z_0$$ which simply gives $$ \frac{\sigma}{\gamma} = \frac{d-c}{b-a} $$
(2) requires solving $$-\sigma a + \gamma c= \sigma b - \gamma d = z_0$$ which simply gives $$ \frac{\sigma}{\gamma} = \frac{d+c}{b+a} $$
From here the idea is to keep a set of equal and maximal values that are ever diminishing until all the rows are exhausted. If $m$ maximal values in the row are achieved, then the row represents the corner of a hyper-cube, thus is the smallest possible in the infinity norm.
Here is a "silent description" of how to use the box rotation to find the edge of the hypercube described by the first three elements being equal in magnitude:
\begin{align} \pmatrix{\star & \star & \star \\ \star & \star & \star \\\star & \star & \star\\} \overset{\text{QR}}{\rightarrow} \pmatrix{\star & \star & \star \\ 0 & \star & \star \\ 0 & 0 & \star\\} \overset{\text{box-1}}{\rightarrow} \pmatrix{\star & \star & \star \\ a & a & \star \\ 0 & 0 & \star\\} \overset{\text{box-2}}{\rightarrow} \pmatrix{\star & \star & \star \\ \star & \star & \star \\ b & b & b \\}\\ \end{align}