MIT Amorphous Materials

Transcription

1 MIT Amorphous Materials 10: Electrical and Transport Properties Juejun (JJ) Hu 1

2 After-class reading list Fundamentals of Inorganic Glasses Ch. 14, Ch. 16 Introduction to Glass Science and Technology Ch band gap, band diagram, engineering conductivity 2

3 asics of electrical conduction Electrical conductivity niziei vi i i E Einstein relation D i ikt Ze i : electrical conductivity n : charge carrier density Z : charge number e : elementary charge : carrier mobility D : diffusion coefficient v : carrier drift velocity E : applied electric field 1 Z e 2 n D i i i oth ions and electrons kt i contribute to electrical conductivity in glasses 3

4 Ionic conduction in crystalline materials Vacancy mechanism Interstitial mechanism 4

5 Ionic conduction pathway in amorphous solids Comparison of Li transport pathways figure removed due to copyright restrictions. See: Figure 8: Adams, S. and R. Prasada Rao. "Transport Pathways for Mobile Ions in Disordered Solids from the Analysis of Energy-scaled ond-valence Mismatch Landscapes." Phys. Chem. Chem Phys. 11 (2009): There are low energy sites where ions preferentially locate Ionic conduction results from ion transfer between these sites Ionic conduction is thermally activated 2-D slices of regions with Li site energies below a threshold value in Li 2 O-SiO 2 glasses Phys. Chem. Chem. Phys. 11, 3210 (2009) 5

6 A tale of two valleys Electric field E = 0 Assuming completely random hops, the average total distance an ion moves after M hops in 1-D is: r d M Average diffusion distance: r r 2 D (1-D) 6 D (3-D) 1 2 D d 2 (1-D) 1 2 D d 6 (3-D) + Average spacing between adjacent sites: d For correlated hops: D 1 f d 2 0 f 1 6 Ion hopping frequency: 6

7 A tale of two valleys Electric field E = 0 Attempt (vibration) frequency: 0 Frequency of successful hops (ion hopping frequency): DE a v v 0 exp kt 1 2 E D fv d exp 0 D a 6 kt + arrier height DE a Equal probability of hopping along all directions: zero net current 7

8 A tale of two valleys Energy difference between adjacent sites: ZeEd Hopping frequency : v 1 v 2 0 DEa exp kt Hopping frequency : Electric field E > 0 DE a + ZeEd v 1 v 2 0 DE exp a ZeEd kt Net ion drift velocity: 2 v0 ZeEd DE a v v v d exp 2kT kt 8

9 A tale of two valleys Electric field E > 0 Ion mobility 2 v0zed DEa exp 2kT kt Electrical conductivity (1-D, random hop) 2 0 Einstein relation (3-D, correlated hops) nv Zed DEa exp 2kT kt + ZeEd DE a 1 0 Zed DE E a 0 D a e nd exp exp kt 6kT kt T kt Z 2 fnv 2 9

10 Temperature dependence of ionic conductivity Slope: DE k a Dispersion of activation energy in amorphous solids leads to slight non-arrhenius behavior DEa ln T ln0 kt 1/T ( 1,000) (K -1 ) Phys. Rev. Lett. 109, (2012) 10

11 Theoretical ionic conductivity limit in glass DE fnv0 exp T kt 6k 0 a 0 Zed 2 Note that 0 has a unit of W cm/k When T, 0 /T Extrapolation of the Arrhenius plot agrees with infrared spectroscopic measurements in ionic liquids (molten salts) Solid State lonics 18&19, 72 (1986) Annu. Rev. Phys. Chem. 43, 693 (1992) 11

12 Fast ion conductors / superionic conductors Acta Mater. 61, 759 (2013) 12

13 and structures in defect-free crystalline solids All electronic states are labeled with real loch wave vectors k signaling translational symmetry All electronic states are extended states No extended states exist in the band gap 13

14 and structures in defect-free crystalline solids Figure removed due to copyright restrictions. See Figure 12, Chapter 7: Kittel, Charles. Introduction to Solid State Physics. Wiley, In the band gap, wave equation solutions have complex wave vectors k Kittel, Introduction to Solid State Physics, Ch. 7 14

15 Anderson localization in disordered systems Localization criterion: V 0 / J > 3 P. W. Anderson Image is in the public domain. Source: Wikimedia Commons. Disorder leads to (electron, photon, etc.) wave function localization 15

16 Anderson localization in disordered systems Extended states (loch states) Localized states 16

17 Density of states (DOS) in crystalline and amorphous solids E Conduction band E Conduction band and gap Defect states Urbach tail Mid-gap states Mobility edge Valence band Valence band DOS DOS Crystalline solids Amorphous solids 17

18 Extended state conduction Extended state conductivity: ex ne ex Electron drift mobility in a-si:h ex 1 ftrap 0 0 : free mobility f trap : fraction of time in trap states Drift mobility ex increases with temperature (T, f trap 0) Extended state conductivity follows Arrhenius dependence Electron mobility in c-si: 1400 cm 2 V -1 s -1 R. Street, Hydrogenated Amorphous Silicon, Ch. 7 18

19 Hopping conduction via localized states Fixed range hopping: hopping between nearest neighbors Hopping between dopant atoms at low temperature Variable range hopping (VRH) Hopping between localized states near E F E Mobility edge exp R E F R y g DOS z x 19

20 Variable range hopping DE Hopping probability P exp2r VRH kt Within distance R, the average minimal energy difference DE is: DE Rg Optimal hopping distance: R min DE 2R 4 k T 9 gk T 8gk T 9 14 VRH exp T 14 exp R R z y x 20

21 DC conductivity in amorphous semiconductors ln Extended state conduction ex exp T 1 VRH is most pronounced at low temperature Measured DC conductivity Variable range hopping VRH exp T 14 1/T 21

22 VRH in As-Se-Te-Cu glass Near room temperature, mixed ionic and extended state conduction At low temperature, variable range hopping dominates J. Appl. Phys. 101, (2007) 22

23 Summary asics of electrical transport Conductivity: scalar sum of ionic and electronic contributions niziei vi ie Einstein relation Ionic conductivity Occurs through ion hopping between different preferred sites Thermally activated process and non-arrhenius behavior i 1 ikt D Z e 2 n D Z e k T i i i i i i DE fnv0 T k T 6k 0 a exp 0 Zed 2 23

24 Summary Electronic structure of amorphous semiconductors Anderson localization: extended vs. localized states Density of states E Mobility edge and tail and mid-gap states Extended state conduction Free vs. drift mobility Thermally activated process Localized state conduction Conduction band Urbach tail Mid-gap states Mobility edge Fixed vs. variable range hopping Valence band Mott s T -1/4 law of VRH DOS 24

25 MIT OpenCourseWare Amorphous Materials Fall 2015 For information about citing these materials or our Terms of Use, visit: