How does one get this idea [for the proof of Sylvester’s Theorem]? The answer is: I don’t know! It is like asking: How did Michelangelo do this?

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How does one get this idea [for the proof of Sylvester’s Theorem]? The answer is: I don’t know! It is like asking: How did Michelangelo do this?

In linear algebra, an

eigenvectorof a linear transformation is a non-zero vector

that only changes by a scalar factor (itseigenvalue) when that linear transformation is

applied to it.

Now* for the sake of simplicity* lets assume that Energy* as a linear transformation, and when it acts on some position (x1,x2) gives you the energy at that point (e0).

(x1,x2) – Eigenvector, e0 – Eigenvalue.

This e0 that you get is a physical measurable quantity and you do not want this value to be complex. Why ? Complex energies are not a thing of the real world.

And the reason why Hermitian matrices are important in Physics is because if a Matrix is hermitian, then it has real eigenvalues.

Thanks for asking!

* It need not be Energy, it could be any physically measurable quantity. We have just taken energy as an example here.

** A Hermitian matrix (or self-adjoint matrix) is a complex square matrix that is equal to its own conjugate transpose ( A = A ^{†} )

[1] Why on earth is matrix multiplication NOT commutative ? – An Intuition

## On the transpose of a matrix

In this post, I would just like to highlight the fact an image can be represented in a matrix form and matrix transformations such as transpose, shearing, scaling, etc, from an image processing point of view are purely physical !

Check out this article from the klein project if this post interested you.

Have a great day!

And for the sake of completion, I would like to also add this compilation to the post:

In this post, I would just like to highlight the fact an image can be represented in a matrix form and matrix transformations such as transpose, shearing, scaling, etc, from an image processing point of view are purely physical !

Check out this article from the klein project if this post interested you.

Have a great day!

Hey! I’ve used the** Serge Lang **book** **in undegrad school, which has, I think, pretty much everything one needs to get a solid basis in linear algebra. It seems fitting to me for both mathematicians and physicists. I liked it because, while keeping things clear and forward, it has a ton of definitions, plus a lot of interesting appendices. Also it’s not a massive book in terms of volume, which I always appreciate. The thing is, it’s rigorous but kind of basic, you know, the stuff you need to get the state space in quantum mechanics, or matrix calculus, but as far as I remember it lacks a proper introduction to groups and group theory. For that, the **Cornwell** is the best stuff around if you’re a physicist**. ** Have not studied on any Russian authors to be honest, so I wouldn’t know about that, sorry. I only know the Kolmogorov book for Functional Analysis, but nothing on linear algebra.

Basis vectors are best thought of in the context of roads.

Imagine you are in a city – X which has only roads that are perpendicular to one another.

You can reach any part of the city but the only constraint is that you

need to move along these perpendicular roads to get there.

Now lets say you go to another city-Y which has a different structure of roads.

In this case as well you can get from one part of the city to any other,

but you have to travel these ‘Sheared cubic’ pathways to get there.

Just like these roads determine how you move about in the city,

Basis

Vectors encode information on how you move about on a plane.

What do I

mean by that ?

**The basis vector of City-X is given as:**

This to be read as – “ If you would like to move in City-X you

can only do so by taking 1 step in the x-direction or 1 step in the

y-direction ”

**The basis vector of City-Y is given as:**

This to be read as – “ If you would like to move in City-Y you can

only do so by taking 1 step in the x-direction or 1 step along the

diagonal OB ”

By

having the knowledge about the Basis Vectors of any city, you can travel

to any destination by merely scaling these basis vectors.

As an

example, lets say need to get to the point (3,2), then in City-X, you

would take 2 steps in the x-direction and 3 steps in the y-direction

And similarly in City-Y, you would take 1 step along the x -direction and 2 steps along the diagonal OB.

Destination Arrived 😀