802 karma · joined September 16, 2013
Both covariance matrices and Hessians are more naturally thought of as tensors, not matrices (and therefore not linear transformations). That is, they take in two vectors as input and produce a single real number as output.
As for graph adjacency matrix, this can actually be thought of as a linear transformation on the vector space where the basis vectors correspond to nodes in the graph. Linear combinations of these basis vectors correspond to probability distributions over the graph (if properly normalized).
2D images... Yes, these cannot really be interpreted as linear transformations. But I'd say these aren't really matrices in the mathematical sense.
Much of what makes linear algebra interesting and powerful comes from more advanced topics, especially eigenvalues. This power comes when we are not looking at a single matrix in isolation, but when we repeatedly apply a matrix. For instance, consider the equation x_t = A^t x_0. It turns out we can rewrite this an equation by diagonalizing A -- i.e., A = P^{-1} Sigma P, where Sigma is diagonal; most, but not all, matrices can be written in this form. We call s_i the "eigenvalues" of A.
Then, the equation simplifies to x_t = P^{-1} Sigma^t P x_0, or equivalently (P x_t) = Sigma^t (P x_0). This equation is dramatically simpler, since Sigma is diagonal, so if Sigma = diag(s_1, ..., s_n), then Sigma^t = diag(s_1^t, ..., s_n^t). In other words, this transformation "disentangles" the different components of A into ones that act independently. Here, the transformation x -> P x is what is called a "change of basis".
These repeated matrix applications are common in physics, where they represent how a dynamical system evolves over time. The main difference is that in physics, the system evolves continuously, but similar transformations can be applied to solve these problems.
df/dx = f
The solutions are e^x + const; requiring f(0) = 1 gives you the choice const = 0.
Another way to define it is as the infinite series
e^x = \sum_{i=0}^inf x^i/i!
It is pretty easy to show this definition is equivalent to the previous one. A third way is as
lim_{n -> inf} (1 + x/n)^n
This definition comes from the intuition that e^x represents the limit of continually compounding interest. As before, it is pretty easy to show that it is equivalent to the previous two.
In any case, all these definitions extend directly to complex values of x. The fact that
e^{ix} = cos(x) + i sin(x)
holds (and hence Euler's identity holds) is a consequence of a more natural definition, not the typical definition.
https://en.wikipedia.org/wiki/Taylor_series#Analytic_functio...
Nevertheless, it is actually true that all complex differentiable functions satisfy this property, which is miraculous.
In other words, I think both the possibility that we are nearing a complete understanding of the rules and the possibility that we are nowhere close are both quite plausible.
Having said that, your intuition that photons should have gravitational influence makes sense, since according to special relativity, mass and energy are equivalent. Since total energy (mass + energy) is conserved, the gravitational influence of the photon should equal that of the electron-positron pair (assuming they are all located at the same position). I think the article is agreeing with this point of view.
As far as I know, the definition 1a is unrelated and specifically meant to describe sequence relations, usually for positions of power. For example, "Trump succeeded Obama as president" means Trump became president after Obama. Related words are "succession" (e.g., "succession of the throne" refers to the process of transferring power in a monarchy), "successor" (e.g., the successor function in mathematics takes an integer n and returns n+1), and "precede" (the antonym of "succeed").
To get complex values, we can consider the Gaussian integers [1] mod 2. Then, we have (1 + i) (1 + i) = (1 + i + i - 1) = 0 + 2 i = 0. So these integers are a ring where there are nonzero elements that multiply to 0.
[1] https://en.m.wikipedia.org/wiki/Conservation_law#Exact_laws
The main point of thermodynamic time is to describe the idea that time appears to be moving forward. According to fundamental physics, as far as we can tell, time is symmetric (with a few caveats). So going forward in time should look similar to going backwards in time, just like going to the left in deep space is the same as going to the right. But the fact that we are in a pocket of high entropy means that time has an apparent direction.
As far as I can tell, LIDAR makes a lot of prediction tasks much easier (since you have both images and LIDAR point clouds), and is also a backup for obstacle detection to ensure that your self-driving car doesn't crash.
While currently more academic, it also has tremendous promise in healthcare diagnostic tasks [5,6]. It has also been used in economics applications such as measuring the global impact of fishing [7] and in poverty prediction in third world countries [8].
[1] http://citeseerx.ist.psu.edu/viewdoc/download?doi=10.1.1.26....
[2] https://www.infoworld.com/article/2907877/how-paypal-reduces...
[3] https://en.wikipedia.org/wiki/Naive_Bayes_spam_filtering
[4] https://en.wikipedia.org/wiki/Netflix_Prize
[5] https://jamanetwork.com/journals/jama/fullarticle/2588763
[6] https://www.nature.com/articles/nature21056
https://mathoverflow.net/questions/114034/learning-path-for-...
Edit: Here is another overview that seems good:
Of course, things are not so clear cut. Your financial situation can also be a consequence of discrimination, e.g., if you were denied a job or unfairly arrested. At the end of the day, some human has to sit down and decide what is OK and what is not. Personally, I believe the goal of research on algorithmic fairness should be to give the people who will ultimately make these decisions (e.g., judges, politicians, etc.) the tools to understand both broadly, the kinds of things that can go wrong when using algorithms, and also to understand what might have gone wrong in a specific situation.
y_i = A_ij x_j.
If I understand correctly, the paper points out that an algorithm for computing derivatives based on this notation is faster for taking higher-order derivatives compared to using TensorFlow.
Mathematically, tensors are more complicated objects. Basically, they are what you get when you take higher-order derivatives of a function. In particular, the first-order derivative of a function f: R^n -> R^m at a point x \in R^n is the best linear function A_x \in R^{m X n} that approximates the original function, i.e.,
f(x + dx) ~= f(x) + A_x dx.
A linear function is represented by a matrix, so a first-order derivative is a matrix. If I take the second-order derivative, I get a more complicated object B_x, which represents the quadratic term in the Taylor expansion:
f(x + dx) ~= f(x) + A_x dx + B_x(dx, dx)
where B_x(a, b) is a linear function (or more precisely, a "multilinear" function) of two vectors a, b (which are the same in the above formula). That is, whereas A_x is a (linear) function R^n -> R^m, B_x is a (multilinear) function R^n X R^n -> R^m. This mathematical object B_x is an example of a tensor. In R^n and R^m, tensors are pretty boring, but they become more interesting when dealing with functions on manifolds.