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klkuttler.com
klkuttler.com
The only reason why I am now doing theoretical physics (I was in the dumb group initially and worked my way up largely by myself) is because I read a calculus textbook by accident and got hooked when I was 14. Even when I made it to the top of the pile I still wasn't allowed to do anything more than calculus because the module system means we had to choose as a class whether to do group theory or not.
Apologies for the negative waves.
Paul Halmos "Finite-Dimensional Vector Spaces"
For instance, the way Halmos introduces the determinant of a matrix (or an operator) is the most consistent, elegant and simple way I ever encountered. OTOH, in Kenneth Kuttler's LinAlg books the determinant is pulled out of the thin air like in 1000+ other similar books.
The title is a reference to a somewhat well-known book, Linear Algebra Done Right, which avoids using determinants to develop the theory (resulting in a somewhat novel/cleaner presentation). It's unfortunately not freely available online (published by Springer – I would suspect most university students can get it freely through their library's website, however).
Really, I don't see what you like about Halmos definition of the determinant... I have just read it (page 99 of my copy) and he admits that it is a "somewhat roundabout procedure", just after giving the definition! There's other references that seem much cleaner (e.g. Spivak's calculus on manifolds, using exterior algebra).
Halmos shows (it is almost trivial) that the space of anti-symmetric n-forms Wn over L_n is 1-dimensional. Wn(Ae1,...,Aen) = const*Wn(e1,...,en). This scalar const is called determinant. It has all the properties you would ascribe to Volume like volume spanned by collinear column-vectors is zero. This is a nice bridge to geometry in Ln. Also, in a space of just one page (p.99) he introduces determinant and proves its main properties like det(A*B) = det(A)*det(B) and therefore det(A^-1) = 1/det(A).
( v1 ∧ v2 ∧ ··· ∧ vn ) / ( e1 ∧ e2 ∧ ··· ∧ en )
The signed volume per se is just the n-vector: v1 ∧ v2 ∧ ··· ∧ vn
Generally working with the wedge product is more pleasant and conceptually clearer than working with determinants. Among other things we don't need to make an arbitrary choice of basis or unit n-vector. There's also no reason to limit ourselves to n terms. v1 ∧ v2 is also a reasonable quantity to use, etc.
When you take the basis out, that's the wedge product, which inherently includes the orientation. Conveniently, there is only one degree of freedom for n-vectors in n-dimensional space. When we take the quotient of two n-vectors in n-dimensional space we therefore get a scalar.
Say we live in an n-dimensional vector space V and have an endomorphism f : V -> V. Now, we consider the pullback [1] f* : Λⁿ(V) -> Λⁿ(V) induced by f on the vector space of n-linear alternating forms Λⁿ(V) on V.
This is just an endomorphism on Λⁿ(V). However, Λⁿ(V) is one-dimensional, hence necessarily invariant under f*. This means f* has an eigenvalue (!). This eigenvalue is what we usually call the determinant of f.
This is completely independent of any choice of basis, orientation, or an inner product.
[1] That is, given an element w ∈ Λⁿ(V) and an arbitrary n-tuple v₁, ..., vₙ of vectors from V, we have (f*w)(v₁, ..., vₙ) = w(f(v₁), ..., f(vₙ))
And the "outermorphism" f̱ of your linear transformation, when limited to considering its application to an arbitrary pseudoscalar, returns another pseudoscalar which necessarily has the same orientation, making that a scaling operation.
So what we could say in that case is that f̱(p) / p = d (some scalar, the "determinant" of f), where p is any pseudoscalar p = v1 ∧ v2 ∧ ··· ∧ vn.
This turns out to be about the same as what I wrote a few comments upthread. We are just dealing with
f̱( v1 ∧ v2 ∧ ··· ∧ vn ) / ( v1 ∧ v2 ∧ ··· ∧ vn ) = d
= ( f(v1) ∧ f(v2) ∧ ··· ∧ f(vn) ) / ( v1 ∧ v2 ∧ ··· ∧ vn )
instead of ( v1 ∧ v2 ∧ ··· ∧ vn ) / ( e1 ∧ e2 ∧ ··· ∧ en ) = d
And now we are talking about a property of a linear transformation instead of a property of a collection of n vectors.
In many practical situations, an oriented quantity like v1 ∧ v2 ∧ ··· ∧ vn is more useful than a scalar ratio d though.
And strictly speaking, determinant is not volume because the former is dimensionless. It is the scaling factor of the volume when a geometric entity is transformed by a linear map.
How do you define "length" and "area"? I guess that if you don't have already a very firm grasp of these basic concepts, then there's no business for you (yet) in studying determinants. Much later, once you master thoroughly lengths, areas, volumes and hypervolumes; and also linear algebra and determinants (however they are defined), then you can embark in the elegant definitions using exterior algebra and the like. Notice that Halmos itself says that his treatment is appropriate for a *second* course in linear algebra, preparing the field for the later study of infinite-dimensional spaces.
> And strictly speaking, determinant is not volume because the former is dimensionless.
This really depends on the context. If you are working on euclidean space, you already have "units" and the determinant makes sense in itself, as the volume spanned by sets of vectors.
*A* determinate function (not the) is simply a skew symmetric n-linear map into the underlying field.
Done. Now we get the volume interpretation when it’s appropriate, the wedge product interpretation, and the generalization to finitely generated projective modules (if a determinate function exists, there are additional conditions needed for the existence.)
Go to John Baez's awesome list "How to Learn Math and Physics":
https://math.ucr.edu/home/baez/books.html
And then to Library Genesis.
Do you really care about the format being PDF or is it about the books being FREE? I'd like to make common queries like yours easier. LearnAwesome is open-source, so of course you're free to contribute: https://github.com/learn-awesome/learn
To paraphrase a typical rant: “Making knowledge free and accessible is useless unless a libre format is used like Markdown.” Lol
The PDF beef is funnier in that people usually don’t know why they are morally opposed to PDF, it usually boils down to not liking Adobe Acrobat a decade ago, not accepting that page format preservation is a thing, or some beef with zooming or something. End of the day, it seeks to be digital paper.
End of the day, it’s an open standard with multiple implementations. Just by virtue of the US Federal Courts using it for millions of documents it will be usable for the foreseeable future, well beyond our lifetimes. (And there are many similar or even bigger examples)
Kenneth Kuttler's books doesn't seem to be there though.
http://www.theassayer.org/cgi-bin/asbrowsesubject.cgi?class=...
The notes are utter dogshit because there's no culture of publishing them online for the public.
Kibble's classical mechanics book is deep, easy to read and cheap, I'd start there. Most physics books past a certain level end up with an increasingly hand-wavy derivation of the Euler-lagrange equations in some context
Two hard copies since I moved countries, one on kindle and one on Apple Books.
Great book :D
[1] http://www.damtp.cam.ac.uk/user/tong/dynamics.html [2] http://www.lightandmatter.com
The typesetting is also a crime against humanity - they should be done similarly to the Feynman lectures, so typed up in LaTeX rather than whatever they are now
So I sort of agree, but take the two Oxford books on QFT and Statistical physics - they pack in enormous amounts of detail in a 3 or 4 hundred pages. There's room to spare if the book is the right shape.
Concepts in thermal physics
Not at the same level as L&L but they are absolute masterpieces in pedagogy and the formula should be extended to a 800page tome to cover more material. It's the way MTW should be written...
The first few chapters are precisely about the extraction of concrete conserved quantities from symmetries. A sufficiently "russian" reader will be able to see immediately the general case from these very complete examples. Noether's theorem is only missing in name, not in content.
> The typesetting is also a crime against humanity - they should be done similarly to the Feynman lectures, so typed up in LaTeX rather than whatever they are now
The typeseting of the french edition of L&L is extraordinarily beautiful. I'm not sure that is is possible to reach this typographical elegance with freely available LaTeX packages. On the other hand, the re-typed Feynman lectures are a disgrace, and an objectively worsening in quality from the first editions.
I may have been a little vague when I said typesetting - the actual typesetting is a bit dull but the thing that is a disgrace, I should clarify, is that the fonts are terrible, and the text has that "Cheap Dover book" print quality (not far off a good typewriter).
For one of the volumes, a reviewer even posted a picture of his edition with subscripts printed so faint/partially that they were basically missing, and he had to Google the proper formulas!
Do you have any recommendations for good stat mech books? I guess the two volume set by Kardar is trendy right now, but I'm always curious about other options.
Beyond that the usual suspects are good enough for me, I just don't like L&L. I'm probably forgetting something.
It's not exactly statmech but I really like McComb's introductory renormalization methods book.
While I have not seen either of those books before, I have another book by the author of the first one, Stephen Blundell. It's Quantum Field Theory for the Gifted Amateur, and I think you might like it. Not as a standalone quantum book, but perhaps as a supplement to a more "serious" treatment.
edit: I just saw you recommended this below!
I got it when I was 17 and it was an absolute godsend as its really cheap.
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