Presentation on theme: "Electrical and Thermal Conductivity"— Presentation transcript:
1Electrical and Thermal Conductivity Main Topics from Chapters 3-5 Due to time, not all topics will be on test. Some problems ask to discuss the meaning or implication.Lattice Dynamics (Monatomic, Diatomic, Mass Defect, 2D Lattices)Strain (compliance, reduced notation, tensors)Harmonic Oscillator (Destruction/Creation, Hamiltonian & Number Operators, Expectation Values)Energy Density and Heat Capacity (phonons, electrons and photons)Quasiparticle Interactions (e-e, e-phonon, e-photon, defect interations)Electrical and Thermal Conductivity
2Lattice VibrationsWhen a wave propagates along one direction, 1D problem.Use harmonic oscillator approx., meaning amplitude vibration small.The vibrations take the form of collective modes which propagate. Phonons are quanta of lattice vibrations.Longitudinal WavesTransverse Waves
3Monatomic Linear Chain The force on the nth atom;aaThe force to the right;The force to the left;Un-1UnUn+1The total force = Force to the right – Force to the leftThus, Newton’s equation for the nth atom isDiatomic benzetEqn’s of motion of all atoms are of this form, only the value of ‘n’ varies
4Brillouin Zones of the Reciprocal Lattice Reciprocal Space Lattice:2p/a3rd Brillouin Zone2nd Brillouin Zone1st Brillouin Zone (BZ=WS)Each BZ contains identical information about the latticeThere is no point in saying that 2 adjacent atoms are out of phase by more than (e.g., 1.2 =-0.8 )Modes outside first Brillouin zone can be mapped to first BZ
6Diatomic Chain(2 atoms in primitive basis) 2 different types of atoms of masses m1 and m2 are connected by identical springs(n-2) (n-1) (n) (n+1) (n+2)KKKKm2a)m1m1mm2ab)Un-1UnUn+1Un+2Un-2Since a is the repeat distance, the nearest neighbors separations is a/2Two equations of motion must be written;One for mass m1, and One for mass m2.
7A when the two atoms oscillate in antiphase As there are two values of ω for each value of k, the dispersion relation is said to have two branchesOptical Branchл/a2–лkwABCUpper branch is due to thepositive sign of the root.Acoustical BranchNegative sign: k for small k. Dispersion-free propagation of sound wavesAt C, M oscillates and m is at rest.At B, m oscillates and M is at rest.This result remains valid for a chain containing an arbitrary number of atoms per unit cell.A when the two atoms oscillate in antiphase
8Number and Type of Branches Every crystal has 3 acoustic branches, 1 longitudinal and 2 transverseEvery additional atom in the primitive basis contributes 3 further optical branches (again 2 transverse and 1 longitudinal)
92D Lattice Write down the equation(s) of motion Ul,m+1 Ulm Ul-1,m KUlmUl-1,mUl+1,mWhat if I asked you to include second nearest neighbors with a different spring constant?2D LatticeUl,m-1
10Identify the values of at k=0 and at the edges. Ul,m+1CSimilar to the electronic bands on the test, plot w vs k for the  and  directions.Identify the values of at k=0 and at the edges.UlmUl-1,mUl+1,mGot here in 50 minute classUl,m-12D Lattice
11Specific Heat or Heat Capacity Classical Picture of Heat Capacity The heat energy required to raise the temperature a certain amountThe thermal energy is the dominant contribution to the heat capacity in most solids. In non-magnetic insulators, it is the only contribution.Classical Picture of Heat CapacityWhen the solid is heated, the atoms vibrate around their sites like a set of harmonic oscillators.Therefore, the average energy per atom, regarded as a 3D oscillator, is 3kT, and consequently the energy per mole is=Dulong-Petit law: states that specific heat of any solid is independent of temperature and the same result(3R~6cal/K-mole) for all materials!
12Thermal Energy & Heat Capacity Einstein Model Energy of oscillatorAverage energy of a harmonic oscillator and hence of a lattice mode at temperature TThe probability of the oscillator being in this level as given by the Boltzman factor
13Mean energy of a harmonic oscillator High Temperature Limit <<Low Temperature Limitexponential term gets biggerZero Point Energyis independent of frequency of oscillation.This is a classical limit because the energy steps are now small compared with thermal/vibrational energy
14Heat Capacity C (Einstein) Heat capacity found by differentiating average phonon energywhereThe difference between classical and Einstein models comes from zero point energy.Area =T(K)The Einstein model near T= 0 did not agree with experiment, but was better than classical model.Taking into account the distribution of vibration frequencies in a solid this discrepancy can be accounted for.Points:ExperimentCurve: EinsteinPrediction
15Debye approximation has two main steps Approx. dispersion relation of any branch by a linear extrapolationEnsure correct number of modes by imposing a cut-off frequency , above which there are no modes. The cut-off freqency is chosen to make the total number of lattice modes correct. Since there are 3N lattice vibration modes in a crystal having N atoms, we choose so that:Einstein approximation to the dispersionDebye approximation to the dispersion
16Density of states (DOS) per unit frequency range g() The number of modes/states with frequencies and +d will be g()d.# modes with wavenumber from k to k+dk=for 1D monoatomic lattice
17Debye Model adjusts Einstein Model The energy of lattice vibrations will then be found by integrating the energy of single oscillator over the distribution of vibration frequencies. Thusfor 1DMean energy of a harmonic oscillatorIt would be better to find 3D DOS in order to compare the results with experiment.
183D Example: The number of allowed states per unit energy range for free electron? Each k state represents two possible electron states, one for spin up, the other is spin down.
19kx,ky,kz(all have positive values) Octant of the crystal:kx,ky,kz(all have positive values)The number of standing waves;LLAnother view
20The Heat Capacity of a Cold Fermi Gas (Metal) Close to EF, we can ignore the variation in the density of states: g() g(EF).By heating up a metal (kBT << EF), we take a group of electrons at the energy - (with respect to EF), and “lift them up” to . The number of electrons in this group g(EF)f()d and each electron increased its energy by 2 :kBTThe small heat capacity of metals is a direct consequence of the Pauli principle. Most of the electrons cannot change their energy.
21Otherwise metals would have infinite conductivity On average,I go about seconds betweencollisionselectronBam!Random Collisionsphononwith phonons and impuritiesThe thermal vibration of the lattice (phonons) will prevent the atoms from ever all being on their correct sites at the same time.The presence of impurity atoms and other point defects will upset the lattice periodicityElectrons colliding with phonons (T > 0)Electrons colliding with impuritiesimp is independent of T
22r(E) is the ‘density of states available at energy E’. Fermi’s Golden Ruler(E) is the ‘density of states available at energy E’.Transition rate:Quantum levels of the non-perturbed systemTransition is inducedPerturbation is appliedSee Fermi‘s Golden Rule paper in Additional Material on the course homepage
23This process is stimulated absorption (or simply absorption). When the ground state finds itself in the presence of a photon of the appropriate frequency, the perturbing field can induce the necessary oscillations, causing the mix to occur.This leads to the promotion of the system to the upper energy state and the annihilation of the photon.This process is stimulated absorption (or simply absorption).Einstein pointed out that the Fermi Golden Rule correctly describes the absorption process.- degeneracy of state f
24⇒ Quantum Oscillator Atoms still have energy at T=0. What is <x2> for the ground state of the quantum harmonic oscillator?(1D Case)For 3D quantum oscillator, the result is multiplied by 3:⇒
25These quantized normal modes of vibration are called PHONONSPHONONS are massless quantum mechanical particles which have no classical analogue.They behave like particles in momentum space or k space.Phonons are one example of many like this in many different areas of physics. Such quantum mechanical particles are often called“Quasiparticles”Examples of other Quasiparticles:Photons: Quantized Normal Modes of electromagnetic waves.Magnons: Quantized Normal Modes of magnetic excitations in magnetic solidsExcitons: Quantized Normal Modes of electron-hole pairs
26Conditions for: elastic scattering Phonon spectroscopy =Conditions for: elastic scatteringinConstraints:Conservation laws ofMomentumEnergyIn all interactions involving phonons, energy must be conserved and crystal momentum must be conserved to within a reciprocal lattice vector.
27Stress tensor 𝜎, Compliance C, Stiffness S birefringenceElastic anisotropyDeformation tensorStress tensor 𝜎, Compliance C, Stiffness SMessage: Wave propagation in anisotropic media is quite different from isotropic media:There are in general 21 independent elastic constants (instead of 2 in the isotropic case), which can be reduced still further by considering the symmetry conditions found in different crystal structures.There is shear wave splitting (analogous to optical birefringence, different polarizations in diff. directions)Waves travel at different speeds depending in the direction of propagation
28The cubic axes are equivalent, so the diagonal components for normal and shear distortions must be equal.And cubic is not elastically isotropic because a deformation along a cubic axis differs from the stress arising from a deformation along the diagonal.e.g.,  vs. Zener Anisotropy Ratio:x=(a-b)/2 or