Math 8271: News and Announcements, Fall 2015

o 12/24/15: I submitted the grades on 12/21/2015. You must be able to see them online. Thank you for a great semester. Happy holidays! See you next term.

o 12/6/15: I have posted Homework 7, and made it due Friday, December 18, at noon to my mailbox.

o 11/30/15: Zeshen Gu pointed an error in Problem 5.7, which is on the homework, to me today: we must assume that A is strictly upper-triangular. It is an unnoticed typo in the text.

o 11/26/15: I have removed one problem from Homework 6, as I have not noticed it was part Theorem 5.29 (2) and (4). The final count of problems is seven.

o 11/26/15: I posted Homework 6, due Friday, December 4, partially yesterday and completed it today. There are eight problems altogether.

o 11/17/15: I have added the word (generalized) to matrix coefficients in HW Problem 2: working with a basis is not essential in that problem.

o 11/16/15: I have corrected a typo in the formula for the action Rg in HW Problem 2: it should be f(hg) on the right-hand side.

o 11/16/15: I have updated the homework very slightly again and elaborated the hint to Problem 7: Apply the Peter-Weyl theorem to a function which is 0 at 1 and greater than 1 outside of a neighborhood of 1. Where will the kernel of a representation whose matrix coefficient (or a linear combination of such) approximating this function lie?

o 11/16/15: I have updated the homework very slightly by specifying that U(gl) meant the universal enveloping algebra of the Lie algebra gl.

o 11/13/15: I have updated the homework, having removed Section 5.2 from the reading assignment.

o 11/11/15, 9:16 p.m.: I forgot to add problems on the universal enveloping algebra to the homework. I am adding just one problem now, so as the total count of problems is eight in the final version of the homework.

o 11/11/15, 5:30 p.m.: There was so much formula writing in Homework 5, that I ended up writing a LaTeX file and posting a pdf file on the Homework page.

o 11/10/15: I have posted Homework 5, due Friday, November 20, partially. There are not enough suitable problems in the text, and I will add more hand-written problems on Wednesday.

o 10/31/15, 6:01 p.m.: Homework 4, due Friday, November 6, has been posted.

o 10/31/15: A couple of corrections: When I was talking about the Kirillov orbit method the other day, I should not have excluded 0 from the dual space of the Lie algebra. The zero functional corresponds to the trivial representation, that is to say, the representation on the standard one-dimensional space C on which the Lie group acts as identity and the Lie algebra as zero. Another correction refers to an error, pointed out by one of you, in the argument showing that the standard n-dimensional representation of SO(n,R) in Cn is irreducible. We will talk about this on Monday in class. Do not forget about the time switch!

o 10/31/15: Guys, I am still working on the homework. Plan to post it by 6:30 p.m.

o 10/15/15: Homework 3, due Friday, October 23, has been posted.

o 10/14/15: Correction: the differential equation for Z(t) = μ(tx,y), where μ(x,y) is the group law in the logarithmic coordinate: exp(μ(x,y)) = exp(x) exp(y) for x, y in the Lie algebra of a Lie group is not exp (ad x), but rather a Todd series, namely
Z'(t) = log (etad x ead y)  (x),
etad x ead y - 1
which may be expanded into a series in (etad x ead y - 1) applied to x. This implies the Baker-Campbell-Hausdorff formula.

o 10/8/15: Hint to Problem 2.8: Show that Ad X: g → g for G a subgroup of GL(n,K) is just (Ad X)y = XyX-1 by taking the directional derivative of X exp(y) X-1 in the direction y.

o 10/8/15: Hint to Problem 3.2: The intuitive reason for this to work is that when you want to compare how two elements of G multiply in different coordinate charts, you use the change of coordinate map and its Taylor expansion, which is useful to write through its linear, quadratic, etc., parts, as in the proof of Lemma 3.11, to compare the bilinear parts of the group law. Since the quadratic part of the Taylor expansion is symmetric in all the variables, it can mess up only the symmetric part of the group law when changing coordinates. Thus, it is easier to solve a more general problem: if you write the group law in two different coordinate charts f1 and f2: g → G near 1 in G, both mapping 0 to 1, and identify their bilinear parts B1 and B2, then the antisymmetrizations of the bilinear parts are related by the linear part T1 = T* of the Taylor series of the change of coordinates map T = T1 + T2 + ... = f2-1f1 as follows:

T1(B1(x,y) - B1(y,x)) = B2(T1x,T1y) - B2(T1y,T1x).
Finally, to show this, start with
T(x + y + B1(x,y) + ...) = Tx + Ty + B2(Tx,Ty) + ...
and expand both sides up to degree two.

o 10/2/15: In doing the Homework, you may assume that πi(Sn) = 0 for i < n, a standard fact of Algebraic Topology, which follows from Sard's theorem.

o 10/1/15: Homework 2, due Friday, October 9, has been posted.

o 9/23/15: Starting from this Friday, I have decided to modify my office hours slightly and start them at 11:15 on Wednesday and at 10:10 on Friday. Thus, my office hours from now on will be Mon 11:15-12:05, Wed 11:15-12:05, Fri 10:10-11:00, or by appointment.

o 9/18/15: I have just posted the first Homework, due Friday, September 25. I am sorry for the delay: I am still terribly jet-lagged after Japan and fell asleep on your homework a few hours ago. ☺ Now it is just past midnight on September 19. The homework will be collected or graded. Getting together with other students (that is, in study groups) is a very effective way to do homework. However, you have to write solutions on your own.

o 9/16/15: I have added a link to the list of errata for the text to our main course page.

o 9/6/15: I am out of town, participating in a workshop on Braids, Configuration Spaces and Quantum Topology at the University of Tokyo, Japan, during the first week of classes at the U, through September 12. Thus, the first class of the semester will be on Monday, September 14. No office hours during the first week, either: if you need to contact me, please write me at voronov@umn.edu . I apologize for the delay — I know you are all eager to start learning the amazing Lie theory. I look forward to meeting you and starting the class, too!

o 9/6/15: I recommend the following way to study for this class. Attend each class, take notes, participate in class actively. After each class review your notes and study the corresponding part of the text. You can find out which part of the text at the Class Outlines page. Then do the assigned homework problems pertinent to that material. Some students find it helpful to read the material before it is covered in class, some prefer to do reading after class.

o 9/6/15: If you need to register for this class, please, send a message to Ms. Lawson at ugrad@math.umn.edu and ask for a permission number. If permission is granted, go to OneStop and register.


Last modified: (2016-01-19 17:26:02 CST)