PHY Statistical Mechanics 12:00* -1:45 PM TR Olin 107

Slides:



Advertisements
Similar presentations
Lecture 27 Electron Gas The model, the partition function and the Fermi function Thermodynamic functions at T = 0 Thermodynamic functions at T > 0.
Advertisements

Classical and Quantum Gases
Statistical Mechanics
Statistical Mechanics
Bose-Einstein Condensation Ultracold Quantum Coherent Gases.
MSEG 803 Equilibria in Material Systems 9: Ideal Gas Quantum Statistics Prof. Juejun (JJ) Hu
Lecture 22. Ideal Bose and Fermi gas (Ch. 7)
1 Lecture 5 The grand canonical ensemble. Density and energy fluctuations in the grand canonical ensemble: correspondence with other ensembles. Fermi-Dirac.
Introductory Nanotechnology ~ Basic Condensed Matter Physics ~
Lecture 23. Systems with a Variable Number of Particles. Ideal Gases of Bosons and Fermions (Ch. 7) In L22, we considered systems with a fixed number of.
Lecture 25 Practice problems Boltzmann Statistics, Maxwell speed distribution Fermi-Dirac distribution, Degenerate Fermi gas Bose-Einstein distribution,
Statistical Mechanics
Bose Einstein Condensation Condensed Matter II –Spring 2007 Davi Ortega In Diluted Gas.
1/21/2014PHY 770 Spring Lecture 3 & 41 PHY Statistical Mechanics 12:30-1:45 PM TR Olin 107 Instructor: Natalie Holzwarth (Olin 300) Course.
Chapter 18 Bose-Einstein Gases Blackbody Radiation 1.The energy loss of a hot body is attributable to the emission of electromagnetic waves from.
2/6/2014PHY 770 Spring Lectures 7 & 81 PHY Statistical Mechanics 11 AM-12:15 PM & 12:30-1:45 PM TR Olin 107 Instructor: Natalie Holzwarth.
Lecture 21. Grand canonical ensemble (Ch. 7)
Blackbody Radiation Wien’s displacement law : Stefan-Boltzmann law :
Statistical mechanics How the overall behavior of a system of many particles is related to the Properties of the particles themselves. It deals with the.
4/17/2014PHY 770 Spring Lecture 231 PHY Statistical Mechanics 12:00 * - 1:45 PM TR Olin 107 Instructor: Natalie Holzwarth (Olin 300) Course.
2/20/2014PHY 770 Spring Lecture 121 PHY Statistical Mechanics 12:00-1:45 PM TR Olin 107 Instructor: Natalie Holzwarth (Olin 300) Course.
4/22/2014PHY 770 Spring Lecture 241 PHY Statistical Mechanics 12:00 * - 1:45 PM TR Olin 107 Instructor: Natalie Holzwarth (Olin 300) Course.
18.3 Bose–Einstein Condensation
2/18/2014PHY 770 Spring Lecture PHY Statistical Mechanics 11 AM – 12:15 & 12:30-1:45 PM TR Olin 107 Instructor: Natalie Holzwarth.
4/08/2014PHY 770 Spring Lecture 201 PHY Statistical Mechanics 12:00 * - 1:45 PM TR Olin 107 Instructor: Natalie Holzwarth (Olin 300) Course.
Chapter 7 Bose and Fermi statistics. §7-1 The statistical expressions of thermodynamic quantities 1 、 Bose systems: Define a macrocanonical partition.
Physics 541 A quantum approach to condensed matter physics.
2/26/2014PHY 770 Spring Lecture 131 PHY Statistical Mechanics 12:00 * -1:45 PM TR Olin 107 Instructor: Natalie Holzwarth (Olin 300) Course.
Statistical Physics. Statistical Distribution Understanding the distribution of certain energy among particle members and their most probable behavior.
6.The Theory of Simple Gases 1.An Ideal Gas in a Quantum Mechanical Microcanonical Ensemble 2.An Ideal Gas in Other Quantum Mechanical Ensembles 3.Statistics.
4/10/2014PHY 770 Spring Lecture 211 PHY Statistical Mechanics 12:00 * - 1:45 PM TR Olin 107 Instructor: Natalie Holzwarth (Olin 300) Course.
Thermal Conduction in Metals and Alloys Classical Approach From the kinetic theory of gases ) where, l is mean free path.
Chapter 6 Applications of
PHY Statistical Mechanics 12:30-1:45 PM TR Olin 107
PHY Statistical Mechanics 12:00* - 1:45 PM TR Olin 107
Electrical Engineering Materials
Advanced Solid State Physics
PHY Statistical Mechanics 12:00* - 1:45 PM TR Olin 107
Department of Electronics
The units of g(): (energy)-1
Solid State Physics Lecture 11
Ideal Bose and Fermi gas
6. The Theory of Simple Gases
16 Heat Capacity.
Lecture 25 Practice problems
Recall the Equipartition
Wave Particle Duality Light behaves as both a wave and a particle at the same time! PARTICLE properties individual interaction dynamics: F=ma mass – quantization.
Bose-Einstein Condensation Ultracold Quantum Coherent Gases
Lecture 22. Ideal Bose and Fermi gas (Ch. 7)
Thermodynamics and Statistical Mechanics
Recall the Equipartition Theorem: In Ch 6,
PHY 752 Solid State Physics Superconductivity (Chap. 18 in GGGPP)
Classical and Quantum Gases
16 Heat Capacity.
Chap. 20 in Shankar: The Dirac equation
PHY 341/641 Thermodynamics and Statistical Mechanics
Lecture 23. Systems with a Variable Number of Particles
Quantum mechanics II Winter 2012
Recall the Equipartition
Fermi statistics and Bose Statistics
Chap. 17 in Shankar: Magnetic field effects – atoms, charged particles
Lecture 27 Electron Gas The model, the partition function and the Fermi function Thermodynamic functions at T = 0 Thermodynamic functions at T > 0.
Group theory and intrinsic spin; specifically, s=1/2
Chap. 20 in Shankar: The Dirac equation for a hydrogen atom
Reading: Chapters #5 in Shankar; quantum mechanical systems in 1-dim
“Addition” of angular momenta – Chap. 15
PHY 741 Quantum Mechanics 12-12:50 AM MWF Olin 103
Thermodynamics and Statistical Physics
“Addition” of angular momenta – Chap. 15
Thermodynamics and Statistical Physics
Presentation transcript:

PHY 770 -- Statistical Mechanics 12:00* -1:45 PM TR Olin 107 Instructor: Natalie Holzwarth (Olin 300) Course Webpage: http://www.wfu.edu/~natalie/s14phy770 Lecture 14 Chap. 6 – Grand canonical ensemble Fermi-Dirac distribution function Bose-Einstein distribution *Partial make-up lecture -- early start time 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Suggestions available upon request. Reminder: Please think about the subject of your computational project – due next week. Suggestions available upon request. 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Examples of grand canonical ensembles – ideal (non-interacting) quantum particles in a cube of length L with periodic boundary conditions -- Fermi-Dirac case In the absence of a magnetic field, the particle spin does not effect the energy spectrum, and only effects the enumeration of possible states spin (g) 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Fermi-Dirac case -- continued 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Fermi-Dirac case -- continued 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Fermi-Dirac case -- continued 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Fermi-Dirac case -- continued 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Fermi-Dirac case -- continued 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Examples of grand canonical ensembles – ideal (non-interacting) quantum particles in a cube of length L with periodic boundary conditions -- Bose-Einstein case (assumed to have spin 0) 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Bose-Einstein case Fermi-Dirac case 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Bose-Einstein case Fermi-Dirac case 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Case of Bose particles Non-interacting spin 0 particles of mass m at low T moving in 3-dimensions in large box of volume V=L3: Assume that each state ek is singly occupied. 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Case of Bose particles at low T 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Critical temperature for Bose condensation: condensate “normal” state 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Case of Bose particles at low T 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Critical temperature for Bose condensation: condensate “normal” state 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Summary: 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Some convenient integrals g3/2(z) g5/2(z) z 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

g3/2(z) z 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

3/18/2014 PHY 770 Spring 2014 -- Lecture 14

T/TE 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

87Rb atoms (~2000 atoms in condensate) http://www.colorado.edu/physics/2000/bec/three_peaks.html 87Rb atoms (~2000 atoms in condensate) 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Other systems with Bose statistics Thermal distribution of photons -- blackbody radiation: In this case, the number of particles (photons) is not conserved so that m=0. 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Blackbody radiation distribution: T3>T2 T2>T1 T1 n 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Other systems with Bose statistics Thermal distribution of vibrations -- phonons: In this case, the number of particles (phonons) is not conserved so that m=0. 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Other systems with Bose statistics -- continued Thermal distribution of vibrations -- phonons: 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Effects of interactions between particles – classical case 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Effects of interactions between particles – classical case -- continued 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Effects of interactions between particles – classical case -- continued 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Effects of interactions between particles – classical case -- continued 3/18/2014 PHY 770 Spring 2014 -- Lecture 14

Effects of interactions between particles – classical case -- continued 3/18/2014 PHY 770 Spring 2014 -- Lecture 14