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Quiz 2

modified 21Apr2018 at 4:08PM by Paul Crowell  

You can take up to three hours, although the quiz is not nearly that long! There are no extensive calculations. As always, clear explanations of your reasoning are very important. The quiz is closed book, but you can use a calculator, and a rule will be useful for one problem. If you are confused by a question, stop and send me an email. I will try to check my email regularly on Saturday and Sunday.

Week 13

modified 16Apr2018 at 12:26PM by Paul Crowell  

Reading: Kittel, Chapters 17 and 18 (Surfaces and Interfaces, Nanostructures) These cover a broad range of topics, mostly at a superficial level. Some material may refer to quantum mechanics you do not know, particularly the sections on electrons in a magnetic field (e.g., quantum Hall effect). My goal here is simply to expose you to the phenomenology, and I do not expect you to understand it all. If you find something too heavygoing, just skip it. I am posting Chapter 4 of Davies, which is a compendium on the solutions of the Schrodinger equation for various forms of quantum confinement. This is good as a reference. It is essentially "just math," but I will emphasize some points in class. Problem Set 9 (due Thursday 4/19) is now posted. Note that I posted a revised version on Saturday. The revised version contains a hint on Problem 3 and makes clear that you need to know the donor density for Problem 1(a). I will post Quiz 2 on Thursday.

Quiz 2

modified 10Apr2018 at 6:16PM by Paul Crowell  

Quiz 2 will be available Thursday, April 19th and will be due the following Tuesday. It will be a timed takehome like the first quiz. It will cover material up through Problem Set 8. I am attaching Quiz 2 from last year and solutions.

Lecture Slides

modified 17Apr2018 at 12:50AM by Paul Crowell 

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Problem Sets

modified 21Apr2018 at 6:40PM by Paul Crowell  


Week 12

modified 6Apr2018 at 8:10PM by Paul Crowell  

We will continue with semiconductors, moving onto semiconductor heterostructures. There is going to be some material in Tuesday's lecture (and on Problem Set 8) that will be unfamiliar to those who have not had statistical mechanics, but I will do my best. In the end, recognizing the role of the Boltzmann factor and whether or not the energy scale is set by the gap or the donor (or acceptor) binding energy is going to be sufficient. I am attaching pages from Ashcroft and Mermin as well as Davies (the chapter on heterostructures) that you should read over the next week. I will do the pn junction on Thursday. Given the composition of the class, I am going to do more optics this year, and I will come up with some readings for the following week. I apologize for some of the very uncreative problems on Problem Set 8. Spend your time thinking about the Anderson localization problem.

Week 11

modified 2Apr2018 at 11:08PM by Paul Crowell  

As a reminder, I will hold an office hour on Monday, April 2, from 1:30  3:15. Problem Set 7 is due Tuesday. Problem Set 8 is now posted. It will be due Thursday, April 12. This week, we will go back to Chapter 8 (semiconductors), but first we will conclude our discussion of transport in the "semiclassical model" and its application to metals (particularly in the presence of a magnetic field). To this end, it will be helpful to read through p. 194 by Tuesday's lecture. Note the key fact: \hbar dk/dt = F, where F is the external force (e.g. the Lorentz force). This may puzzle you, because \hbar k is NOT the electron momentum, and so this does not appear to be consistent with F=ma at first glance. The truth comes out on p. 193. The electron is acted on by both the external force and the periodic potential. When both the lattice and the electrons are included (see Eqs. 8.15 and 8.16), then \hbar k is a momentum (the crystal momentum). The semiclassical model leads to some reasonably intuitive phenomena such as magnetooscillations, which are really just an extension of cyclotron motion to periodic systems, and some nonintuitive ones, such as Bloch oscillations (p. 217). In the latter case, a constant electric field leads to oscillations in the group velocity. If you understand Bloch oscillations, then you understand crystal momentum. I am adding below a "simple" derivation of the expression (Kittel 9.37) for the period of magnetooscillations. In class,I will just write down this expression, but for Fermi surfaces with a circular crosssection, it is possible to derive it accepting only the fact that the energies must be quantized in units of the cyclotron energy.

Week 10

modified 29Mar2018 at 12:57AM by Paul Crowell 

We will do metals (Chapter 9) before semiconductors (Chapter 8). Read Chapter 9, particularly 221  242. The remainder of the chapter (after p. 242) may be heavy sailing. Do not worry about it. I will return to the topic of electrons in a magnetic field in a couple weeks. If you wish, you can skip this section for now. Pages 232  240 cover various approaches to calculating band structure. Among these, tight binding is by far the most important, and is the only one I will discuss in any detail. Problem Set 7 is posted. It will probably be due Tuesday, April 3. I will have an office hour from 1:30  3:15 on Monday, April 2nd.

Week 9

modified 9Mar2018 at 3:10PM by Paul Crowell 

I am assuming that you will read the section on magnetotransport and the Hall effect (pp. 152  155), which I did not get to in lecture. We will start with Chapter 7 on March 20. This chapter is in a sense the crux of the class. What happens to electronic states (originally planes waves in an empty box) when we "turn on" the periodic potential? Although this is a difficult problem to solve analytically (except in some special cases), there turn out to be some global rules (such as Bloch's theorem) that allow us to make sense of what is going on. My goal is for you to understand why gaps form, the relation to symmetry, and how this impacts the behavior of real materials. Problem Set 6 is now posted and will be due on March 27th. 
Week 8

modified 1Mar2018 at 9:31PM by Paul Crowell 

We will continue with Chapter 6. In all likelihood I will not start Chapter 7 until after spring break, but read pp. 163  167 by Thursday, March 8. The solutions to Quiz 1 are now posted. Professor Valls will lecture on Tuesday. The topics will be thermodynamics of the electron gas (e.g. specific heat) and transport in the relaxation time approximation. I will return on Thursday (I hope) and do magnetotransport (a first pass), thermal transport, and perhaps an aside on optical properties of metals. Problem Set 5 is due Thursday, March 8. 
Quiz 1 is posted here.

modified 9Mar2018 at 6:48PM by Paul Crowell 

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Week 7

modified 25Feb2018 at 8:17PM by Paul Crowell 

Tuesday's lecture will cover some more topics in quantum mechanics, some of which appear in Kittel's Chapter 6, including spin, FermiDirac statistics and the FermiDirac distribution. I will then continue with a discussion of Dirac notation and matrix mechanics. Thursday's lecture will cover most of the remainder of Chapter 6, through approx. p. 152. Problem Set 5 is posted. It will be due Thursday, March 8. My office hour this week will start at 3:15, and I will shift it from 3:15  5:00. 
Week 6

modified 17Feb2018 at 12:37PM by Paul Crowell 

Problem Set 4 is posted and will be due Friday, February 23rd, by 5 PM. You may either put the problem set under my office door (PAN 220) or upload a SINGLE PDF file to the class Moodle Page: https://ay17.moodle.umn.edu/course/view.php?id=10110 The lecture on Tuesday, February 20 will cover material in the second part of Chapter 5, including the generalization of the phonon density of states, van Hove singularities, anharmonicity, and thermal transport. We will start Chapter 6 (electrons) the week of February 27. There will not be a lecture on Thursday, February 22nd. I cannot overemphasize the importance of the density of states, and how we start with a density of states in kspace, which is always (L/2\pi)^d, (where d is the dimensionality) and, with knowledge of the dispersion relation E vs. k, calculate the density of states with respect to energy (or frequency). Depending on the type of particles we are dealing with (phonons, electrons, etc.) the dispersion relation and hence the form of the density of states with respect to energy will vary. In contrast, the details of the Debye calculation are not important. If you have not had statistical mechanics, do not worry about it. You should know that the acoustic phonon contribution to the heat capacity scales as (T/\Theta_D)^d (where d is the dimensionality). We will discuss the contribution from optical phonons on Tuesday. 
Quiz 1

modified 14Feb2018 at 11:43AM by Paul Crowell  

The first quiz will be available (by download from the web site) next Thursday. It will be similar in format to the quiz from last year, which is posted here. This year's quiz will only cover material up through Chapter 5 (phonons). I will probably give you 2 hours, but I am inclined to make it closed book (so that I can ask easier questions!). You can take it when you wish and hand it in on Tuesday, February 27. There will not be a lecture on Thursday, February 22nd.

Week 5

modified 14Feb2018 at 10:06AM by Paul Crowell 

Problem Set 4 is posted and will be due Friday, February 23rd, by 5 PM. You may either put the problem set under my office door (PAN 220) or upload a SINGLE PDF file to the class Moodle Page: https://ay17.moodle.umn.edu/course/view.php?id=10110 Reading: Kittel Chapters 4 and 5. Analogous chapters in Ashcroft and Mermin are Chapters 22  24. Tuesday's lecture: Phonon dispersion relations, optical and acoustic modes, phonons and momentum Thursday's lecture: Phonons: thermal properties Problem Set 3 is due Thursday 
Week 4

modified 8Feb2018 at 2:34PM by Paul Crowell 

Reading: Kittel, Chapter 4. This material is covered (much more thoroughly) in Ashcroft and Mermin, Chapter 22. A&M have four chapters on phonons. Neutron scattering gets its own chapter (24) as do anharmonic effects (25). Tuesday's Lecture: We will spend the first few minutes discussing a couple points from the problem set. After that, I will turn to topics in quantum mechanics (the PHYS 5012 students can leave at that point). Thursday's Lecture: I will conclude the brief review of chemical bonding and then start on phonons. Problem Set 3 will be posted shortly. It will be due Thursday, February 15th. 
Week 3

modified 2Feb2018 at 12:21AM by Paul Crowell  

Problem Set 2 is posted. It will be due Tuesday, February 6th. Because on Thursday I mutilated the discussion of the Miller indices (hkl) in terms of the shortest reciprocal lattice vector perpendicular to a set of lattice planes, I am attaching a discussion here. Both lectures this week will be on "core material" (i.e., no special quantum mechanics lecture). I will probably start the material in Chapter 3 of Kittel (crystal binding) in the second half of Thursday's lecture. I will have relatively little to say about this beyond what is in the text. For those looking for more, I recommend Chapters 19 and 20 of Ashcroft and Mermin.

Office Hours

modified 18Jan2018 at 7:19PM by Paul Crowell 

My office hours will be Wednesday 2:45  4:30 and by appointment. 
Week 2

posted 18Jan2018 at 7:11PM by Paul Crowell 

The lecture on Tuesday, January 23 will continue the "primer on quantum mechanics" from last Tuesday. I will cover Hilbert space, Dirac notation, operators, expectation values, and the matrix formulation of quantum mechanics. I will probably not get to spin. The lecture on Thursday, January 25th will continue our discussion of crystal structure, with the concept of reciprocal space and the basics of diffraction. Problem Set 1 will be due on Thursday, January 25th. Note that the last problem (on diffraction) does not have to be handed in this Thursday. It is on there to give you a head start on next week. 
Week 1

posted 16Jan2018 at 6:01PM by Paul Crowell 

Reading: Kittel, Chapters 1 and 2 We will spend the first two weeks on "structure and symmetry," with an emphasis on the important crystalline systems and the notion of reciprocal space. I am not going to emphasize the mathematical aspects of symmetry, such as point groups and space groups. If you are interested, Ashcroft and Mermin address these (slightly) in their Chapter 7. The first problem set is posted. Because we are interleaving the first couple lectures on quantum mechanics, I may adjust the due date, but for the moment assume it is due Thursday, January 25. 