1. 1 lectures accompanying the book: Solid State Physics: An Introduction,by Philip Hofmann (1st edition, October 2008, ISBN-10: 3-527-40861-4, ISBN-13: 978-3-527-40861-0, Wiley-VCH Berlin.Philip Hofmann Wiley-VCH Berlin www.philiphofmann.net

2. 2 This is only the outline of a lecture, not a final product. Many “fun parts” in the form of pictures, movies and examples have been removed for copyright reasons. In some cases, www addresses are given for particularly good resources (but not always). I have left some ‘presenter notes’ in the lectures. They are probably of very limited use only. README

3. 3 Dielectric Solids / Insulators

4. 4 Macroscopic description dielectric polarisation dielectric susceptibility dielectric constant microscopic dipole (> 0)

5. 5 Plane-plate capacitor High capacitance can be achieved by large A or small d. Both approaches give rise to several problems.

6. 6 Plane-plate capacitor with dielectric For any macroscopic Gaussian surface inside the dielectric, the incoming and outgoing electric field is identical (because the total average charge is 0). The only place where something macroscopically relevant happens are the surfaces of the dielectric. polarizable units: for the solid

7. 7 Plane-plate capacitor with dielectric capacitance increase by a factor of ε so the E-field decreases by a factor of ε

8. 8 The quest for materials with high  l gate area required charge to make it work d

9. 9 The dielectric constant materialdielectric constant ε vacuum1 air1.000576 (283 K, 1013 hPa) rubber2.5 - 3.5 SiO 2 3.9 glass5-10 NaCl6.1 ethanol25.8 water81.1 barium titanate100-1200

10. 10 Microscopic origin: electronic polarization for the solid for one atom

11. 11 Microscopic origin: ionic polarization

12. 12 Microscopic origin: orientational polarization

13. 13 The local field From the measured ε can we figure out α? average field: external plus internal simple but unfortunately also incorrect!

14. 14 (next few slides optional)

15. 15 The local field at a point in the dielectricum field by external charges on plates field by surface charges depolarization field field from inside this cavity average macroscopic field total local field field from the surface dipoles of a spherical cavity large against microscopic dimensions

16. 16 The local field at a point in the dielectricum calculation of the cavity field (z is direction between plates) in z direction surface charge density on sphere

17. 17 The local field at a point in the dielectricum calculation of the field inside the cavity for a cubic lattice field of a dipole (along z) field at centre for all dipoles in cavity

18. 18 The local field at a point in the dielectricum calculation of the total local field it follows that

19. 19 (end of optional slides)

20. 20 The local field What is the electric field each dipole ‘feels’ in a dielectric? the actual local field is higher Clausius-Mossotti relation

21. 21 The dielectric constant materialdielectric constant ε vacuum1 air1.000576 (283 K, 1013 hPa) rubber2.5 - 3.5 glass5-10 NaCl5.9 ethanol25.8 water81.1 barium titanate100-1200 Clausius-Mossotti relationor

22. 22 plane wave complex index of refraction Maxwell relation all the interesting physics in in the dielectric function! Frequency dependence of the dielectric constant

23. 23 Frequency dependence of the dielectric constant Slowly varying fields: quasi-static behaviour. Fast varying fields: polarisation cannot follow anymore (only electronic polarization can). Of particular interest is the optical regime.

24. 24 Frequency dependence of the dielectric constant Slowly varying fields: quasi-static behaviour. Fast varying fields: polarisation cannot follow anymore (only electronic). Of particular interest is the optical regime. materialstatic εε opt diamond5.685.66 NaCl5.92.34 LiCl11.952.78 TiO 2 946.8 quartz3.852.13

25. 25 Frequency dependence of the dielectric constant: driven and damped harmonic motion We obtain an expression for the frequency-dependent dielectric function as given by the polarization of the lattice. The lattice motion is just described as one harmonic oscillator (times the number of unit cells in the crystal).

26. 26 + + + - - - light E-field (almost constant over very long distance)

27. 27 Frequency dependence of the dielectric constant: driven and damped harmonic motion We obtain an expression for the frequency-dependent dielectric function (dielectric function) as given by the polarization of the lattice. The lattice motion is just described as one harmonic oscillator (times the number of unit cells in the crystal). This model is very simple and very general. It can be extended to describe electronic excitations at higher frequencies as well

28. 28 Frequency dependence of the dielectric constant: driven and damped harmonic motion we start with the usual differential equation driving field (should be local field) harmonic restoring term friction term

29. 29 Frequency dependence of the dielectric constant: driven and damped harmonic motion solution real partimaginary part

30. 30 Frequency dependence of the dielectric constant: driven and damped harmonic motion for sufficiently high frequencies we know that electronic / atomic part ionic / lattice part

31. 31 Frequency dependence of the dielectric constant: driven and damped harmonic motion combine with to get the complex dielectric function to be

32. 32 Frequency dependence of the dielectric constant: driven and damped harmonic motion 32

33. 33 The meaning of ε i instantaneous energy dissipation use on average the dissipated energy is

34. 34 energy dissipation ε imaginaryε real

35. 35 The meaning of ε i energy dissipation

36. 36 Frequency dependence of the dielectric constant: even higher frequencies (optical) image source: wikipedia (Si) and http://woelen.homescience.net (CdSe, CdS)http://woelen.homescience.net SiCdSeCdS

37. 37 Frequency dependence of the dielectric constant: even higher frequencies (optical)

38. 38 remember the plasma oscillation in a metal: even higher frequencies We have seen that metals are transparent above the plasma frequency (in the UV). This lends itself to a simple interpretation: above the plasma frequency the electrons cannot keep up with the rapidly changing field and therefore they cannot keep the metal field- free, like they do in electrostatics. values for the plasma energy

39. 39 Impurities in dielectrics Single-crystals of wide-gap insulators are optically transparent (diamond, alumina) Impurities in the band gap can lead to absorption of light with a specific frequency Doping with shallow impurities can also lead to semiconducting behaviour of the dielectrics. This is favourable for high- temperature applications because one does not have to worry about intrinsic carriers (e.g. in the case of diamond or more likely SiC)

40. 40 Impurities in dielectrics: alumina Al 2 O 3 ruby blue sapphire amethyst white sapphire topaz emerald image source: wikipedia

41. 41 Ferroelectrics Spontaneous polarization without external field or stress Very similar to ferromagnetism in many aspects: alignment of dipoles, domains, ferroelectric Curie temperature, “paraelectric” above the Curie temperature.... But: here direct electric field interactions. Direct magnetic field interactions were far too weak to produce ferromagnetism.

42. 42 Example: barium titanate ferroelectric

43. 43 Frequency dependence of the dielectric constant: driven and damped harmonic motion we start with the usual differential equation LOCAL field harmonic restoring term friction term

44. 44 Applications of ferroelectric materials Most ferroelectrics are also piezoelectric (but not the other way round) and can be applied accordingly. Ferroelectrics have a high dielectric constant and can be used to build small capacitors. Ferroelectrics can be switched and used as non-volatile memory (fast, low-power, many cycles).

45. 45 Piezoelectricity applying stress gives rise to a polarization applying an electric field gives rise to strain

46. 46 Piezoelectricity equilibrium structure no net dipole applying stress leads finite net dipole

47. 47 Applications (too many to name all....) Quartz oscillators in clocks (1 s deviation per year) and micro-balances (detection in ng range) microphones, speakers positioning: mm range (by inchworms) down to 0.01 nm range inchworm pictures

48. 48 Dielectric breakdown For a very high electric field, the dielectric becomes conductive. Mostly by kinetic energy: if some free electrons gather enough kinetic energy to free other electrons, an avalanche effect sets in (intrinsic breakdown)