"Lecture" for Weeks 13 and 14

Position papers
Sometime in the next few days each of you will get a personalized response (and a grade) to your essay. I will not scan the papers this time, for two reasons. So, this time I'll keep the critiques very general (and mostly favorable). I won't correct every typo or stylistic blunder, but I will point out factual errors and misspellings of names and I'll question an occasional questionable assertion.

I'll make a discussion list for posting your essays and debating them. You might want to wait till you see my critique, so that you can make minor revisions.

Good-bye for awhile
I will spend the week after Thanksgiving at a conference in Germany. I'll leave Sunday, Nov. 26, and I'll be back Monday morning, Dec. 4. I do not know what Internet access I'll have there, so it's prudent to assume that I'll be incommunicado.

As you see, I have set up all the rest of the course. The last 3 chapters are short, and it would be reasonable to have the final homework assignment due soon after Thanksgiving, leaving you a week with nothing to do except finish your term papers. However, in the interest of flexibility, I've divided the assignment into two parts; the exercises on the 20th century may be delayed till Dec. 4. I'm sure it will help Valentina if you get them in earlier, however.

Please look over the exercises soon and try to get any questions of interpretation (like the one this week abour what identities we can assume in differentiating ax) to me by noon Saturday Nov. 25 at latest. I've tried to help on 19.11 and 20.4 by the little essay below.

Quaternions and Grassmann units
For definition of quaternions, see p. 424 of Katz, or p. 7 of the linear algebra reading. What Hamilton and Katz write as a + bi + cj + dk is what Pauli and Fulling write as a sigma0 - b i sigma1 - c i sigma2 - d i sigma3 (where the i in the second version is, as usual, the square root of -1). Quaternions with a = 0 are closely related to
  1. 3-dimensional vectors equipped with the vector cross product (see p. 3 of the linear algebra reading);
  2. Grassmann's "extensive quantities": what Grassmann and Katz (p. 486 and Ex. 19.11) call b epsilon1 + c epsilon2 + d epsilon3;
  3. 3 x 3 antisymmetric matrices (see p. 4 of the linear algebra reading)
More precisely,