I think I can explain this. I'm not sure how well, I'll do but I can try.
For "nice" objects, we all have an intuition about how many dimensions the object is, which is roughly how many variables it takes to specify a given location on the object. For example, on a line embedded in your standard Cartesian two dimensions, say y=3x+2, you can just tell someone the x coordinate and they know exactly where they are. This works in general, so typical 3 dimensional space needs 3 coordinates. Etc. Similar, a circle (even though it lives in 2 dimensions) just needs 1 variable to tell someone where you are on it because you can take an angle from the center.
However, lots of objects turn out to have a notion of dimension that doesn't quite match up this way. This is roughly what people mean when they call something a "fractal" (although some people use fractal more to mean a thing deifned by a recursive procedure. Defining it precisely is tough.) Now, to talk about objects that are fractals, like say the Koch snowflake https://en.wikipedia.org/wiki/Koch_snowflake we want a notion of dimension that makes sense for them. Ideally, for a given object we want a notion of "dimension" which gives the correct value of dimension when we apply it to an object that is a traditional object with a known dimension, like a line, or sphere or ball. The Minkowski dimension is one such approach. It is easiest to explain in 2 dimensions, but the same basic idea looks in any number of dimensions. Roughly speaking, you take the object you want, and you pick some tiny number epsilon, and then you make a grid on the plane of little boxes each which are epsilon by epsilon, and then you ask how many tiny boxes does it take to cover the object? Then, you take that number and divide it by log (epsilon), and then you let epsilon go to zero. This essentially measures how pointy thick the object is. If the object is thick this will just be two. If it is just a few isolated points (even infinitely many but not a lot) this will be zero. It isn't obvious that this is the right thing to count but turns out to work pretty well. You then generalize this to any number of dimensions for your space your object lives in by using boxes of the corresponding dimension number. So, for a fractal which lives on the real line, you use intervals of length epsilon, in 3 dimensions you use cubes of side length epsilon and so on.
Now, the Minkowski dimension is not the only notion of dimension we have that works this way. There's a related idea called the Hausdorff dimension which is defined in a more complicated fashion but turns out to often be easier to calculate. For example, it is not too hard to show that the Hausdorff dimension of the Koch snowflake is (ln 4)/(ln 3) which is about 1.26. (This reflects the intuition one might have that the Koch snowflake is much closer to being a thing made of lines than it is to being a thing with normal area). Now, it turns out that the Minkowski is always at least as large as the Hausdorff dimension, and they are equal in many situations. But there are some annoyingly simple situations where they are not. For example, if you take the interval of points between 0 and 1 and just take the rational points, then it has has Hausdorff dimension zero and Minkowski dimension one, which is about as far as you could want. Sometimes we'll calculate Haussdorff dimension for an object but really care about the Minkowski dimension, where finding that takes more work.
In the case of Hong Wang's work. She and Zahl proved that if you had what is called a Kakeya set in 3 dimensions (where you want a set that can fit a needle in every direction but you don't care about rotating it around, you just want a needle to fit at any orientation you choose), is that the Haussdorf dimension of the set, and the Minkowski dimension have to be equal and in fact equal to 3. But note that this isn't obvious in part because one doesn't have the rotation requirement here.
Does that help/make sense?