interactions of quasiparticles

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Interactions of Quasiparticles Electro ns, holes Phonons Photons Defects Rayleigh Scattering (Section 5.3) Rayleigh Scattering (Section 5.3) Dipole, quadrupole Interaction (Section 5.2) Plasticity theory Nonlinear Optics (Chap. 7) Anharmonic Scattering (Section 5.4) Coulomb scattering, spin-spin interaction (Section 5.5) Deformation potential, Piezoelectric, Frölich Scattering (Section 5.1) Acousto- optics Elastic scattering Adapted from Snoke’s Solid State Physics

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Defects in Solids Mechanical and electrical properties of solids depend strongly on amount of defects Surface/interface reconstruction polystyrene spheres for self-assembled photonic crystals with intentional low-dimensional defects for defect-mode pass-band in stop-band of photonic bandgap

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Page 1: Interactions of Quasiparticles

Interactions of Quasiparticles

Electrons, holes Phonons

Photons DefectsRayleigh Scattering

(Section 5.3)

Rayleigh Scattering

(Section 5.3)

Dipole,quadrupoleInteraction

(Section 5.2)

Plasticity theory

NonlinearOptics

(Chap. 7)

AnharmonicScattering

(Section 5.4)

Coulombscattering, spin-spin

interaction(Section 5.5)

Deformation potential, Piezoelectric, Frölich

Scattering (Section 5.1)

Acousto-

opticsElasticscattering

Adapted from Snoke’s Solid State Physics

Page 2: Interactions of Quasiparticles

Defects in Solids• Mechanical and electrical properties of solids

depend strongly on amount of defects • Surface/interface reconstruction

Page 3: Interactions of Quasiparticles

Interactions with Defects - Types of Defects

Vacancy

Interstial

Substitutional

Ideal Crystal

Page 4: Interactions of Quasiparticles

These are Point Defects

– Consist of only one or a few atoms, does not necessarily involve foreign atoms

– Vacancies: missing atoms, modeled by considering the energy required to break the bonds between an atom inside the crystal and its nearest neighbors

– Frenkel defects: atom displaced from regular site to interstitial site• Vacancy + displaced atom = Frenkel pair

Page 5: Interactions of Quasiparticles

Dislocations

• Two-dimensional defect• Dislocation is a common one• Results from local elastic stress• Described by Burgers vector

– Constructed via closed loop around dislocation core

– Edge dislocation: Burgers vector perpendicular to dislocation line

– Screw dislocation: Burgers vector parallel to dislocation line

is a line defect

Screw dislocation

34

3

4

Page 6: Interactions of Quasiparticles

• One case is a twin boundary (plane) – Essentially a reflection of atom positions

across the twinning plane.

• Stacking faults– For FCC metals an error in ABCABC packing

sequence– Ex: ABCABABC

Planar Defects in Solids

Adapted from Fig. 4.9, Callister 7e.

Page 7: Interactions of Quasiparticles

Defects in Metallic Crystals

– Most metals crystallize in bcc, fcc or hcp structures– Changing pressure or temp. can interchange these forms for a

metal– Soft and malleable metals usually have fcc structure (copper)– Harder and more brittle metals usually have the hcp structure

(zinc)» Atoms can slide past each other and then realign into crystal form» Dislocations (imperfections in lattice) make it easier to bend» Impurities (imperfections in atom type) allow slippage of layers» Work Hardening means hammer until impurities are together» Heat: can soften by dispersing impurities or harden if control

cooling