Physics 451 Quantum mechanics I Fall 2012 Dec 3, 2012 Karine Chesnel.

Slides:



Advertisements
Similar presentations
Energy is absorbed and emitted in quantum packets of energy related to the frequency of the radiation: Planck constant h= 6.63  10 −34 J·s Planck constant.
Advertisements

Physics 451 Quantum mechanics I Fall 2012 Dec 5, 2012 Karine Chesnel.
Lecture Notes # 3 Understanding Density of States
CHAPTER 3 Introduction to the Quantum Theory of Solids
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Exam Study Practice Do all the reading assignments. Be able to solve all the homework problems without your notes. Re-do the derivations we did in class.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
The Quantum Mechanical Picture of the Atom
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
PHYS3004 Crystalline Solids
Project topics due today. Next HW due in one week
Chapter 6: Free Electron Fermi Gas
Electron Configuration
Physics 451 Quantum mechanics I Fall 2012 Nov 30, 2012 Karine Chesnel.
Physics 451 Quantum mechanics I Fall 2012 Sep 10, 2012 Karine Chesnel.
Physics 451 Quantum mechanics I Fall 2012 Nov 12, 2012 Karine Chesnel.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Physics 451 Quantum mechanics I Fall 2012 Nov 5, 2012 Karine Chesnel.
UNIT 1 FREE ELECTRON THEORY.
EEE 3394 Electronic Materials
Physics 451 Quantum mechanics I Fall 2012 Nov 7, 2012 Karine Chesnel.
The Modern Model of The Atom Chapter 4. Rutherford’s Model Discovered the nucleus Small dense and positive Electrons moved around in Electron cloud.

Ch 4 Free and Confined Electrons EE 315/ECE 451 N ANOELECTRONICS I.
Physics 451 Quantum mechanics I Fall 2012 Sep 12, 2012 Karine Chesnel.
Chapter 35 Quantum Mechanics of Atoms. S-equation for H atom 2 Schrödinger equation for hydrogen atom: Separate variables:
Quantum Mechanics Tirtho Biswas Cal Poly Pomona 10 th February.
NEEP 541 Ionization in Semiconductors Fall 2002 Jake Blanchard.
BASICS OF SEMICONDUCTOR
The Quantum Theory of Solids Allowed and forbidden energy bands Pauli Exclusion Principle In any given system, no two electrons can occupy the same state.
Nanoelectronics Chapter 5 Electrons Subjected to a Periodic Potential – Band Theory of Solids


Kronig-Penney model and Free electron (or empty lattice) band structure Outline: Last class: Bloch theorem, energy bands and band gaps – result of conduction.
The Quantum Mechanical Model of the Atom
Electrical Engineering Materials
Metallic Solids Metallic bond: The valence electrons are loosely bound. Free valence electrons may be shared by the lattice. The common structures for.
Announcements Added a final homework assignment on Chapter 44, particle physics and cosmology. Chap 42 Homework note: Binding energy is by convention positive.
Review of solid state physics
Band Theory of Electronic Structure in Solids
Do all the reading assignments.
QM2 Concept test 7.1 Choose all of the following statements that are correct. (1) The Fermi energy is only defined for fermions. (2) The degeneracy pressure.
Quantum mechanics I Fall 2012
Tightbinding (LCAO) Approach to Bandstructure Theory
ECEE 302: Electronic Devices
Band Theory of Solids So far we have neglected the lattice of positively charged ions Moreover, we have ignored the Coulomb repulsion between the electrons.
Condensed Matter Physics: review
Band Theory The other approach to band theory solves the Schrodinger equation using a periodic potential to represent the Coulomb attraction of the positive.
Physics 342 Lecture 28 Band Theory of Electronic Structure in Solids
Chapter 7 Atomic Physics.
Solids and semiconductors
Quantum mechanics I Fall 2012
Quantum mechanics II Winter 2011
Quantum mechanics I Fall 2012
Quantum mechanics I Fall 2012
Quantum mechanics II Winter 2012
Quantum Theory.
Quantum mechanics I Fall 2012
Quantum mechanics I Fall 2012
Band Theory of Solids 1.
Quantum mechanics I Fall 2012
Quantum Theory.
Quantum Theory.
Quantum mechanics II Winter 2012
Quantum mechanics I Fall 2012
Quantum Theory.
Quantum mechanics I Fall 2012
Quantum mechanics II Winter 2011
Presentation transcript:

Physics 451 Quantum mechanics I Fall 2012 Dec 3, 2012 Karine Chesnel

Homework Quantum mechanics Last two assignment HW 23 Tuesday Dec 4 5.9, 5.12, 5.13, 5.14 HW 24 Thursday Dec , 5.16, 5.18, Wednesday Dec 5 Last class / review

Periodic table Quantum mechanics Hund’s rules First rule: seek the state with highest possible spin S (lowest energy) Second rule: for given spin S, the state with highest possible angular momentum L has lowest energy Third rule: If shell no more than half filled, the state with J=L-S has lowest energy If shell more than half filled, the state with J=L+S has lowest energy

Quiz 32a Quantum mechanics What is the spectroscopic symbol for Silicon ? A. B. C. D. E. Si: (Ne)(3s) 2 (3p) 2

Quiz 32b Quantum mechanics What is the spectroscopic symbol for Chlorine ? A. B. C. D. E. Cl: (Ne)(3s) 2 (3p) 5

Solids Quantum mechanics e-e- What is the wave function of a valence electron in the solid?

Solids Quantum mechanics e-e- Basic Models: Free electron gas theory Crystal Bloch’s theory

Free electron gas Quantum mechanics e-e- e-e- lzlz lyly lxlx Volume Number of electrons:

Free electron gas Quantum mechanics e-e- 3D infinite square well 0 inside the cube outside

Free electron gas Quantum mechanics e-e- Separation of variables

Free electron gas Quantum mechanics Bravais k-space

Free electron gas Quantum mechanics Bravais k-space Fermi surface Free electron density

Free electron gas Quantum mechanics Bravais k-space Fermi surface Total energy contained inside the Fermi surface

Free electron gas Quantum mechanics Bravais k-space Fermi surface Solid Quantum pressure

Solids Quantum mechanics e-e- Bravais k-space Fermi surface Number of unit cells

Solids Quantum mechanics e-e- Bravais k-space Fermi surface Pb 5.15:Relation between E tot and E F Pb 5.16:Case of Cu: calculate E F, v F, T F, and P F

Solids Quantum mechanics e-e- Bravais k-space Fermi surface Number of unit cells

Solids Quantum mechanics V(x) Dirac comb Bloch’s theorem

Solids Quantum mechanics V(x) Circular periodic condition x-axis “wrapped around”

Solids Quantum mechanics V(x) Solving Schrödinger equation 0 a

Solids Quantum mechanics V(x) Boundary conditions 0 a

Solids Quantum mechanics V(x) Boundary conditions at x = 0 0 a Continuity of  Discontinuity of

Solids Quantum mechanics Quantization of k: Band structure Pb 5.18 Pb 5.19 Pb 5.21

Quiz 33 Quantum mechanics A. 1 B. 2 C. q D. Nq E. 2N In the 1D Dirac comb model how many electrons can be contained in each band?

Solids Quantum mechanics Quantization of k: Band structure E N states Band Gap Band (2e in each state) 2N electrons Conductor: band partially filled Semi-conductor: doped insulator Insulator: band entirely filled ( even integer)